OO lm ean — aaa ae 7 Sera $7 ; : 38TH oe HOUSE OF REPRESENTATIVES. © § Mis. Doc. lst Sessvon. : = 1 No, $3. *% ¥ = = . °. “ANNUAL REPORT | OF 4% THE BOARD OF REGENTS OF THE SMITHSONIAN INSTITUTION, SHOWING THE * OPERATIONS, EXPENDITURES, AND CONDITION OF THE INSTITUTION FOR THE YEAR 1863. bi WASHINGTON: GOVERNMENT PRINTING OFFICE. 1864,- : * q \ : . & » * ‘se !) Pee Le ' . - ed a es o In THE House oF REPRESENTATIVES, June 28, 1864. _ " _ Resolved, That five thousand extra copies of the Report ef the Smithsonian Institution be | * printed—two thousand for the Institution. and three thousand for the use of the members of ; if thi Hougé. % ® S » e ss. ‘ i's .* vr, | ey . i . * f. ANNUAL REPORT OF THE BOARD OF REGENTS ¥ OF THE SMITHSONIAN INSTITUTION, SHOWING N THE OPERATIONS, EXPENDITURES, AND CONDITION OF THE INSTI- _ TUTION UP TO JANUARY, 1864, AND THE PROCEEDINGS v ' OF THE BOARD UP TO MARCH 16, 1864. . To the Senate and House of Representatives : In obedience to the act of Congress of August 10, 1846, establish- ing the Smithsonian Institution, the undersigned, in behalf of the Regents, submit to Congress, as a report of the operations, expendi- tures, and condition of the Institution, the following documents: 1. The Annual Report of the Secretary, giving an account of the operations of the Institution, during the year 1863. 2. Report of the Executive Committee, giving a general statement of the proceeds and disposition of the Smithsonian fund, and also an account of the expenditures for the year 1863. 3. Proceedings of the Board of Regents up to March 16, 1864. 4, Appendix. Respectfully submitted, ‘ R. B. TANEY, Chancellor. JOSEPH HENRY, Secretary. : 3 . : : we mR ee | . r . * o : a oe ta ‘ ‘ Fy >” L T ‘ ® , : e > : . TER 3 od | _ s ee re ; | * "¢ SECRETARY OF THE SMITHSONIAN INSTITUTION, 27° ca . + , - comme xiituaix eG e- ‘ THE ANNUAL REPORT OF THE OPERATIONS, EXPENDITURES, - AND CON- DITION OF THE INSTITUTION FOR THE YEAR 1863. * > » - s = JUNE 28, 1864.—Read, and ordered to be printed. ih ene . ‘* SMITHSONIAN InstITUTION, Washington, June 27, 1864. ‘Sir: In behalf of the Board of Regents, I have the honor to submit to the House of Representatives of the United States the annual report of the operations, expenditures, and condition of the Smithsonian In- - stitution for the year 1863. T have the honor to be, very respectfully, your obedient servant, , JOSEPH HENRY, : Secretary Smithsonian Institution, Hon. S. Courax, ~ e Speaker of the House of Representatives. . . : = ieee ead T 6 od ' i. te @e ee * : + % ~~ >» Ss « ” . » * # a % + “?* i ¥ ° 7 * * OFFICERS OF THE sMIT HSONIAN INSTITUTION. a ‘\“ ms 864. /*~@ ° Rwy # *, A ; , ‘*€ ABRAHAM LINCOLN, Ew oficio Presiding: Officer of the Institution. °2 RoGaE B. TANEY,* ‘Chancellor of the Institution. ey JOSEPH HENRY, Secretary of the Institution. co ae a. Assistant Secretary. ee ee easurer. WILLIAM J HEES, Chief Clerk. * A. D. BACHE, JOSEPH G. TOTTEN, $ Executive Committee. R. WALLACH, J ‘ 2 | e% REGENTS OF THE INSTITUTION. H. HAMLIN, Vice-President of the United States. ROGER B. TANEY, Chief Justice of the United States. R. WALLACH, Mayor of the City of Washington. W. P. FESSENDEN, member of the Senate of the United States, (Maine. ) L. TRUMBULL, member of the Senate of the United States, (Illinois. ) GARRETT DAVIS, member of the Senate of the United States, hoe ) S. S. COX, member of the House of Representatives, (Ohio. ) J. W. PATTERSON, member of the House of Representatives, (New Hampshire.) H. W. DAVIS, member of the House of Representatives, (Maryland. ) W. B. ASTOR, citizen of New York. W. L. DAYTON, citizen of New Jersey. T. D. WOOLSEY, citizen of Connecticut. LOUIS AGASSIZ, citizen of Massachusetts. ALEXANDER D. BACHE, citizen of Washington. 1 - JOSEPH G. TOTTEN, citizen of Washington. . MEMBERS EX OFFICIO OF THE MNS a .*” Bi « 4 We 1 - ee ue © SRS", : _ 3 : p 0 iia rus ‘oe . oe ae - Ra . : e ¥ ‘ UO Plone 2 . 2 rae « a * ° , ‘ . - a i mF et : ' ** ” ABRAHAM LINCOLN, President of the United States. a) a HANNIBAL HAMLIN, Vice-President of the United States. * ** ’ ___ W. H. SEWARD, Seeretary of State. ' +. S. P. CHASE, Secretary of the Treasury. S oe . E. M. STANTON, Secretary of War. ’ a G. WELLES, Secretary of the Navy. i? M. BLAIR, Postmaster General. e = 4 E. BATES, Attorney General. ° xy : ROGER B. TANEY, Chief Justice of the United. States. e D. P. HOLLOWAY, Commissioner of Patents. - ~ RICHARD WALLACH, Mayor of the City of Washington. ? - * s HONORARY MEMBERS. * BENJAMIN SILLIMAN, of Connecticut. J. P. USHER, Secretary of the Interior, (ez officio t; a ; = ) PROGRAMME OF ORGANIZATION ‘SMITHSONTAN INSTITUTION. [PRESENTED IN THE FIRST ANNUAL REPORT OF THE SECRETARY, AND ADOPTED BY THE BOARD OF REGENTS, DECEMBER 13, 1847.] INTRODUCTION. General considerations which should serve as a guide in adopting a Plan of Organization. 1. Witt or SurrHson. The property is bequeathed to the United States of America, ‘‘to found at Washington, under the name of the SMITHSONIAN INSTITUTION, an establishment for the increase and dif- fusion of knowledge among men.”’ 2. The bequest is for the benefit of mankind. The government of the United States is merely a trustee to carry out the design of the testator. 3. The Institution is not a national establishment, as is frequently supposed, but the establishment of an individual, and is to bear and perpetuate his name. 4. The objects of the Institution are, Ist, to increase, and, 2d, to diffuse knowledge among men. 5. These two objects should not be confounded with one another. The first is to enlarge the existing stock of knowledge by the addition of new truths; and the second, to disseminate knowledge, thus in- creased, among men. 6. The will makes no restriction in favor of any particular kind of knowledge; hence all branches are entitled to a share of attention. 7. Knowledge can be increased by different methods of facilitating and promoting the discovery of new truths; and can be most exten- sively diffused among men by means of the press. 8. To effect the greatest amount of good, the organization should be such as to enable the Institution to produce results, in the way of increasing and diffusing knowledge, which cannot be produced either at all or so efficiently by the existing institutions in our country. 9. The organization should also be such as can be adopted pro- visionally; can be easily reduced to practice, receive modifications, or be abandoned, in whole or in part, without a sacrifice of the funds. 10. In order to compensate, in some measure, for the loss of time occasioned by the delay of eight years in establishing the Institution, 8 ' PROGRAMME OF ORGANIZATION. a considerable portion of the interest which has accrued should be added to the principal. , ; 11. In proportion to the wide field of knowledge to be cultivated, ‘the funds are small. Economy should therefore be consulted in the construction of the building; and not only the first cost of the edifice should be considered, but also the continual expense of keeping it in repair, and of the support of the establishment necessarily connected with it. There should also be but few individuals Dagenonehy sup- ported by the Institution. 12. The plan and dimensions of the building should be determined by the plan of organization, and not the converse. 13. It should be recollected that mankind in general are to be benefited by the bequest, and that, therefore, all unnecessary ex- penditure on local objects would be a perversion of the trust. 14. Besides the foregoing considerations deduced immediately from _ the will of Smithson, regard must be had to certain requirements of the act of Congress establishing the Institution. These are, a library, a museum, and a gallery of art, with a building on a liberal scale to contain them. SECTION I Plan of Organization of the Institution in accordance with the foregoing deductions from the will of Smithson. TO INCREASE KNOWLEDGE. It is proposed— 1. To stimulate men of talent to make original researches, by offer- ing suitable rewards for memoirs containing new truths; and, 2. To appropriate annually a portion of the income for particular researches, under the direction of suitable persons. TO DIFFUSE KNOWLEDGE. It is proposed— 1. To publish a series of periodical reports on the progress of the different branches of knowledge; and, 2. To publish occasionally separate treatises on subjects of general interest. DETAILS OF THE PLAN TO INCREASE KNOWLEDGE. I.—bLy stimulating researches. 1. Facilities to be afforded for the production of original memoirs on a branches of knowledge. . The memoirs thus obtained to be published in a series of vol- ae in a quarto form, and entitled Smithsonian Contributions to Knowledge. No memoir on subjects of physical science to be accepted for ae which does not furnish a positive addition to human knowledge, resting on original research; and all unverified specula- tions to be rejected. 4. Hach memoir presented to the Institution to be submitted for examination to a commission of persons of reputation for learning in ’ PROGRAMME OF ORGANIZATION. 9 the branch to which the memoir pertains; and to be accepted for publication only in case the report of this commission be favorable. 5. The commission to be chosen by the officers of the Institution, and the name of the author, as far as practicable, concealed, unless a favorable decision be made, = 6. The volumes of the memoirs to be exchanged for the transac- tions of literary and scientific societies, and copies to be given to all the colleges and principal libraries in this country. One part of the remaining copies may be offered for sale; and the other carefully preserved, to form complete sets of the work, to eupply the demand from new institutions. 7. An abstract, or popular account, of the contents of these me- moirs to be given to the public through the annual report of the Regents to Congress. Il.—By appropriating a part of the income, annually, to special objects of research, under the direction of suitable persons. 1. The objects, and the amount appropriated, to Pe recommended by counsellors of the Institution. 2. Appropriations in different years to different bicele so that, in course of time, each branch of knowledge may receive a share. 3. The results obtained from these appropriations to be published, with the memoirs before mentioned, in the volumes of the Smithso- nian Contributions to Knowledge. 4, Examples of objects for which appropriations may be made. (1.) System of extended meteorological observations for solving the problem of American storms. (2.) Explorations in descriptive natural history, and geological, magnetical, and topographical surveys, to collect materials for the formation of a physical atlas of the United States. (3.) Solution of experimental problems, such as a new determina- tion of the weight of the earth, of the velocity of electricity, and of light ; chemical analyses of soils and plants; collection and publi- cation of scientific facts accumulated in the offices of government. (4.) Institution of statistical inquiries ee reference to physical, moral, and political subjects. (5.) Historical researches and accurate surveys of places celebrated in American history. (6.) Ethnological researches, particularly with reference to the dif- ferent races of men in North America; also. explorations and accurate surveys of the mounds and other remains of the ancient people of our country. DETAILS OF THE PLAN FOR DIFFUSING KNOWLEDGE. 1.— By the publication of a series of reports, giving an account of the new discoveries in science, and of the changes made from year to year wm all branches of knowled ge not strictly professional. 1. These reports will diffuse a kind of knowledge generally inter- esting, but which, at present, is inaccessible to the public. Some of 10 PROGRAMME OF ORGANIZATION. . ” the reports may be published annually, others at longer intervals, as the income of the Institution or the changes in the branches of knowledge may indicate. : 2. The reports are to be prepared by collaborators eminent in the different branches of knowledge. ' 3. Each collaborator to be furnished with the journals and pubii- cations, domestic and foreign, necessary to the compilation of his report ; to be paid a certain sum for his labors, and to be named on the title-page of the report. 4. The reports to be published in separate parts, so that persons interested in a particular branch can procure the parts relating to it without purchasing the whole. 5. These reports may be presented to Congress for partial distri- bution, the remaining copies to be given to literary and scientific institutions, and sold to individuals for a moderate price. The following are some of the subjects which may be embraced in the reports : ° JT. PHYSICAL CLASS. 1. Physics, including astronomy, natural philosophy, chemistry, and meteorology. 2. Natural history, including botany, zoology, geology, &c. 3. Agriculture. 4, Application of science to art. . Il. MORAL AND POLITICAL CLASS. 5. Ethnology, including particular history, comparative philology, antiquities, &c. 6. Statistics and political economy. . 7. Mental and moral philosophy. 8. A survey of the political events of the world, penal reform, &c. Ill. LITERATURE AND THE FINE ARTS. _9. Modern literature. 10. The fine arts, and their application to the useful arts. 11. Bibliography. 12. Obituary notices of distinguished individuals. Il.— Ly the publication of separate treatises on subjects of general interest. 1. These treatises may occasionally consist of valuable memoirs translated from foreign languages, or of articles prepared under the direction of the Institution, or procured by offering premiums for the best exposition of a given subject. 2. The treatises should, in all cases, be submitted to a commission of competent judges previous to their publication: 3. As examples of these treatises, expositions may be obtained of the present state of the several branches of knowledge mentioned in the table of reports. | PROGRAMME OF ORGANIZATION. 11 SECTION II. Plan of organization, in accordance with the terms of the resolutions of the Board of Regents providing for the two modes of increasing and diffusing knowledge. 1. The act of Congress establishing the Institution contemplated the formation of a library and a museum ; and the Board of Regents, including these objects in the plan of organization, resolved to divide the income* into two equal parts. 2. One part to be appropriated to increase and diffuse knowledge by means of publications and researches, agreeably to the scheme before.given. The other part to be appropriated to the formation of a library and a collection of objects of nature and of art. 3. These two plans are not incompatible one with another. 4. Tocarry out the plan before described, a library will be required, consisting, first, of a complete collection of the transactions and pro- ceedings of all the learned societies in the world; second, of the more important current periodical publications, and other works necessary in preparing the periodical reports. 5. The Institution should make special collections, particularly of objects to illustrate and verify its own publications. 6. Also, a collection of instruments of research in all branches of experimental science. 7. With reference to the collection of books, other than those men- tioned above, catalogues of all the different libraries in the United States should be procured, in order that the valuable books first pur- chased may be such as are not to be found in the United States. 8. Also, catalogues of memoirs, and of books and other materials, should be collected for rendering the Institution a centre of biblio- graphical knowledge, whence the student may be directed to any work which he may require. 9. It is believed that the collections in natural history will increase by donation as rapidly as the income of the Institution can make pro- vision for their reception, and, therefore, it will seldom be necessary to purchase articles of this kind. 10. Attempts should be made to procure for the gallery of art casts of the most celebrated articles of ancient and modern sculpture. 11. The arts may be encouraged by providing a room, free of ex- pense, for the exhibition of the objects of the Art-Union and other similar societies. 12. A small appropriation should annually be made for models of antiquities, such as those of the remains of ancient temples, &c. 13. For the present, or until the building is fully completed, be- sides the Secretary, no permanent assistant will be required, except one, to act as librarian. *= The amount of the Smithsonian bequest received into the Treasury of the Dinihedy Statesiise.< 25 2 -cat eens. ceca esoee sy Sear esiecelissen=nin = $515,169 00 Interest on the same to July 1, 1846, (devoted to the erection of the build- BND) eee seen = Jae en aewaen soe. Coeacd voewen sean e = eiesiac-ss cane 242,129 00 Annual income from the bequest .....-...-.0- s-ec----- a, ae tee ee 30,910 14 12 PROGRAMME OF ORGANIZATION. 14. The Secretary, by the law of Congress, is alone responsible to the Regents. He shall take charge of the building and property, keep a record of proceedings, discharge the duties of librarian and keeper of the museum, and may, with the consent of the Regents, employ assistants. 15. The Secretary and his assistants, during the session of Congress, will be required to illustrate new discoveries in science, and to exhibit new objects of art; distinguished individuals should also be invited to give lectures on subjects of general interest. This programme, which was at first adopted provisionally, has become the settled policy of the Institution. The. only material change is that expressed by the following resolutions, adopted Jan- uary 15, 1855, viz: : Resolved, That the 7th resolution passed by the Board of Regents, on the 26th of January, 1847, requiring an equal division of the in- come between the active operations and the museum and library, when the buildings are completed, be, and it is hereby, repealed. Resolved, That hereafter the annual appropriations shall be appor- tioned specifically among the different objects and operations of the Institution, in such manner as may, in the judgment of the Regents, be necessary and proper for each, according to its intrinsic impor- tance, and a compliance in good faith with the law. REPORT OF THE SECRETARY. To the Board of Regents: GENTLEMEN: I have the honor to present, at the commencement of another session of your honorable board, the annual report of the condition and transactions of the Smithsonian Institution during the year 18653. The general operations of the Institution are so uniform from year to year that the several annual reports can differ but little from each other; the usual order will, therefore, be observed in this com- munication, with only such variations as the special incidents of the year may require. It will be seen by the report of the Executive Committee that the finances of the Institution are in as favorable a condition as the state of public affairs would authorize us to expect. First. The whole amount of money originally derived from the bequest of Smithson is still in the treasury of the United States, bearing interest at six per eent., paid semi-annually, and yielding $30,910. Second. Seventy- five thousand dollars of an extra fund are in bonds of the State of Indiana, at five per cent. interest, also paid semi-annually, yield- ing $3,750. Third. Fifty-three thousand five hundred dollars of the same fund are in bonds of the State of Virginia, twelve thousand in those of Tennessee, and five hundred in those of Georgia, from which nothing has been derived since the commencement of the war. Fourth. A balance of upwards of $32,000 is now in the hands of the treasurer of the Institution. The unsettled accounts at the close of the year do not exceed two thousand dollars. From this statement it appears that the Institution, after erecting a building, accumulating a large library and an extensive museum, supplying the principal museums of the world with specimens of natural history, and publishing a series of volumes which have been distributed to all first-class libraries abroad, and still more extensively at home, has upwards of one hundred thousand dollars in addition to the money received from the original bequest. In addition to this, the stocks of Virginia and Tennessee are quoted at about half , 14 REPORT OF THE SECRETARY. — = * their par value, and it may be a question whether they should not be disposed of and the money otherwise invested. A part of the original bequest, amounting to £5,015, was left by Mr. Rush in England, as the principal of an annuity to be paid to the mother of the nephew of Smithson. The annuitant having died, a power of attorney was sent, in November, 1862, to Messrs. Fladgate, Clark & Finch to collect the money; but it has not yet been received. Although the whole legacy was awarded to Mr. Rush in behalf of the United States, after an amicable suit in chancery, various objections have been raised to allowing the small remainder to be sent to this country. These objections appear to be principally of a technical character, and are scarcely compatible with an equitable interpretation of the facts of the case. There should be no prejudice in England in regard to the construction placed upon the terms of the bequest and the policy which has been adopted, since one hundred and sixty- nine institutions in Great Britain and Ireland are recipients of the Smithsonian publications and specimens of natural history, and have enjoyed the advantages of its system of international exchange. Although the financial affairs of the Institution are still in a favor- able condition, its ability to produce results is materially diminished on account of the advanced prices of labor and materials, and espe- cially the high rate of exchange under which its foreign operations are necessarily conducted. Still, all parts of the general system have been carried on with less abatement than might have been expected, as will be seen from the following account of the various operations : Publications. —The publications of the Institution, as stated in pre- vious reports, consist of three series: Ist, Contributions to Knowl- edge ; 2d, Miscellaneous Collections ; and, 3d, Annual Reports. The Contributions include memoirs, embracing the records of origi- nal investigations and researches, resulting in such new truths as are considered interesting additions to knowledge. Twelve volumes in quarto of this series have been published, and the thirteenth is nearly ready for distribution. The Miscellaneous Collections include works intended to facilitate the study of the various branches of natural history, to give instruc- tion as to the method of observing phenomena, and to furnish a variety of other matter connected with the progress of science. Of this series four large octavo volumes have been issued, and two more ¥Z nearly completed. ” % geet OF THE SECRETARY. 15 The Annual Reports to Dobinens consist, each, of an octavo volume of 450 pages. They contain the report of the Secretary on the operations and condition of the Institution, the proceedings of the Regents, and an appendix, giving a synopsis of the lectures delivered at the Institution, extracts from correspondence, and articles of a character suited to meteorological observers, to teachers, and other persons especially interested in the promotion of knowledge. The thirteenth volume of the Contributions has been completed, and is now in the hands of the binder. It contains the following original papers: 1. Tidal Observations in the Arctic Seas; by Elisha Kent Kane, M. D; made during the second Grinnell Expedition in Search of Sir John Franklin in 1853-55. Reduced and discussed by Charles A. ee assistant United States Coast Survey. . Meteorological Observations in the Arctic Seas ; by Sir Leopold McClintock : made on board the Arctic searching yacht ‘‘ Fox’’ in Baffin’s Bay and Prince Reg ent’s Inlet in 1857~’59. Reduced and dis- cussed by Charles A. Schott, assistant United States Coast Survey. 3. Ancient Mining on the shores of Lake Superior. By Charles Whittlesey. 4. Discussion of the Magnetic and Meteorological Observations made at the Girard College Observatory, Philadelphia, in 1840—'45. Part II. Investigation of the Solar-Diurnal Variation of the Magnetic Declination and its Annual Inequality. By A. D. Bache, Superin- tendent Coast Survey. 5. Part ILI. Investigation of the Lunar Effects of the Magnetic Declination. By A. D. Bache. 6. Parts IV, V, VI. Horfontal Force. Investigation of the ten or eleven year period, and of the disturbances of the horizontal component of the magnetic force ; investigation of the solar-diurnal variation and of the annual inequality of the horizontal force, and of the lunar effect on the same. By A. D. Bache. 7. Records and Results of a Magnetic Survey of Pennsylvania and parts of adjacent States in 1840, 1841, with some Additional Records and Results of 1834, 1835, 1843, and 1862, and a Map. By A. D. Bache. 8. Researches en the Anatomy and Physiology of Respiration in the Chelonia. By S. Weir Mitchell, M.D., and George R. More- house, M. D. Accounts have been given in previous reports of all the papers contained in this volume, excepting that’ on the Chelonia. This 16 REPORT OF THE SECRETARY. Fe , paper, by S. Weir Mitchell, M. D., and George R. Morehouse, M.D., of Philadelphia, is a very complete study of the anatomy and physi- ology of the breathing organs in turtles. It seems that, although at one time, and by a single observer, the true mode of the breathing of these animals was partially understood, it had long been neglected, and modern physiologists have taught that turtles forced air into the lungs as do frogs. Drs. Mitchell and Morehouse have shown that turtles breathe like mammals, by drawing air into the lungs by the aid of muscles situated in the flanks and on the outside of the lungs. Their paper contains a detailed account of the anatomy of the breath- ing organs of turtles, and is illustrated with numerous wood-cuts. The most novel discovery described by the authors is that of a chiasm or crossing from side to side of a portion of the nerves which supply the muscles of the larynx. Except the well-known facts as to similar crossings within the skull, no previous author has described any simi- lar extra-cranial arrangement of nerves. The physiological uses of the laryngeal chiasm has been fully studied by Drs. Mitchell and Morehouse ; and more recently Professor Wyman, led by their dis- covery, has described similar nerve arrangements in serpents and in certain birds. The authors express their indebtedness to the Smithsonian Insti- tution for the aid with which they were furnished in obtaining the requisite specimens for experiments and for dissection. The following papers have been accepted for publication, and will form parts of the fourteenth volume of Contributions : Ist. Three additional parts of the series of discussion of the mag- netic observations at Girard College, by Professor A. D. Bache. 2d. The result of a series of microscopical studies of the medulla oblongata, or the upper portion of the spinal marrow, by Dr. John Dean. 3d. A memoir on the paleontology of the Upper Missouri, by F. B. Meek and F. V. Hayden. , 4th. An account of the photographical observatory and various experiments in regard to this subject, by Dr. Henry Draper, of New York. 5th. A monograph of the ‘‘Larida’’ or gulls, by Dr. Elliott Coues. All these memoirs, except the last, are in the hands of the printer, or in process of illustration by the engraver. In several of the preceding reports an account has been given of a series of reductions of the magnetic observations made from 1840 to 1845, inclusive, at Girard College, Philadelphia, by Professor Bache. sos REPORT OF THE SECRETARY. 17 The first two of the papers of this series related to what is called the eleven-year period of the variation -of the needle, which corresponds with the recurrence and frequency of the spots on the sun. The third paper relates to the influence of the moon on the variation of the needle. The fourth refers to the change in the horizontal part of the force of the earth’s magnetism coinciding with the eleven- year period of the spots on the sun. The fifth relates to the effect of the sun in producing daily and annual variations in the horizontal component of the magnetic force. The sixth relates to the lunar influence on the horizontal magnetic force. A particular account has been given of the result of all these inves- tigations, which tend fully to corroborate the conclusions arrived at from observations in other parts of the world, that both the sun and moon are magnetic bodies, and exert an influence upon the polarity of the earth ; and also that the magnetism of the sun has variations in intensity which are in some way connected with the appearance of spots on its surface, giving rise to the variations in those perturba- tions of the needle which have been called magnetic storms, and which present a periodical recurrence at an interval of about eleven years. The influence of the moon is much less marked than that of the sun, and appears: to be more analogous to the temporary magnetism induced in soft iron. Parts VII, VIII, and IX of this series, now in the press, are a con- tinuation of the same subject. Part VII contains the discussion of the effect of a change of temperature on the readings of the vertical force instrument. If a magnetic needle could be supported perfectly free in space, so as to assume the direction into which it would be brought by the magnetic action of the earth, it would arrange itself in the line of what is called the dip, or the inclination of the needle. At the mag- netic equator of the earth such a needle would be parallel to the horizon, but, departing from this line either to the north or the south, the inclination would increase continually until we arrive at the mag- netic pole, when it would be vertical. It is plain that the full magnetic force of the earth, in the line of the dip, may be resolved into two others, viz., a horizontal force, or that which draws the ordinary magnetic needle back to the meridian when it has been deflected from this position; and, second, the vertical force which tends to draw the end of the needle down into the line of the dip. The fre- 2s 18 REPORT OF THE SECRETARY. quency of vibrations of a magnetic bar suspended by an untwisted +hread, so as to be horizontal, gives the horizontal component of the force of the earth, while the vibrations of a similar bar placed in the plane of the dip, and poised horizontally like a*scale-beam on two knite-edges, gives the variations in the vertical force. These vibra- tions, however, will be affected not only by the changes in the mag- netism of the earth, but by that in the bar itself; and as the latter is affected by the temperature of the place, a series of observations and discussions was necessary to ascertain the corrections due to this cause. For this purpose the room was artificially heated and cooled ; but the value of the correction was finally deduced from an investi- gation of the whole series of regular observations compared with the changes of temperature indicated by the hourly register of the ther- mometer. The corrections for temperature were afterwards applied. to all the observations. The larger disturbances were then separated from the body of the series in the same manner as had been done with ' regard to the horizontal force, by which means the effect of the monthly and yearly disturbance of the sun is exhibited analytically and graphically. From the results it appears that the number and aggre- gate amount of disturbances were least in 1844; that in each year the greatest number of disturbances occurs in March and September, and the least number in June, or, in other words, the maximum about the equinoxes, and the minimum about the solstices. In an appendix to this paper the connexion of the appearance of the aurora borealis with the disturbances of the direction and force of the earth’s magnetism is discussed. From the result of this dis- cussion it appears that there is a periodicity of about eleven years in the recurrence of the frequency of the aurora, as well as in that of the great disturbances of the needle, and that these are coincident with each other and with the appearance of the spots on the sun. The eighth part of the series gives the discussion of the daily and yearly variations due to the action of the sun on the vertical compo- nent of the magnetic force. The mean variation of the force is deter- mined for each hour during each month and for the whole year, and also for the summer and the winter separately. These are expressed analytically and graphically, and an examination of the curve shows a principal maximum about 1 p. m., and a principal minimum about 9a.m. There is an indication of a secondary maximum about 2 a.m., and a secondary minimum about 4 a. m. REPORT OF THE SECRETARY. 19 _In summer the curve appears to have but one greatest and one least ordinate occurring about noon and midnight. In winter the double feature of the curve becomes quite conspicuous. The vertical force appears greater in May, June, July, and August, and less in the remaining months, with a range of about a hundred ind five hundred thousandth part of the whole force. The ninth part gives the investigation of the influence of the moon upon the vertical force ; also upon the direction and intensity of the total force. The methods of investigation are the same in this as in the preceding parts. The daily effects of the moon exhibit a prin- cipal maximum a little before the planet passes the upper meridian, and a principal minimum about three hours after it passes the lower meridian. The average epoch of the tide of vertical force is about one and a half hour in advance, apparently, of the culmination of the moon. A secondary variation of this force, though noticed, is very feeble. The subject of the time of greatest lunar disturbance is yet very imperfectly developed, and more observations in regard to it are desirable. A comparison is also given in this paper between the observations _ made at Toronto and Philadelphia, and their accordances or differ- ences are stated. The effect of the moon upon the direction and inten- sity of the total force is obtained by a combination of the vertical and horizontal components. From this part of the investigation it appears that the dip is greatest at 8 and 20 hours, and least at 3 hours and 153, the range being equal to 3.6 seconds; and also that the maximum strength of the earth is greatest at half-past 12 and 11, and least at 74 and 17 hours, the results, from the observations at Toronto and Philadelphia, being remarkably coincident. The next paper of the foregoing list is that by Dr. Dean, which comprises the anatomy of the medulla oblongata, both human and comparative, from the lowest roots of the hypoglossal nerve, through the upper roots of the auditory, including the hypoglossal, nasal, glossopharyngeal, abducens, facial, and auditory nerves. The ob- jects of the investigation were principally as follows : Ist. To illustrate the topography of the medulla oblongata by means of aseries of photographs, which might completely map out all the principal changes in structure as they successively occur, connected with the development of the different nerves, with the details which accompany the development of their nuclei and accessory ganglia. 2d. The study of the more minute histological details, such as the course of the nerve roots, their entrance into their respective nuclei 20 REPORT OF THE SECRETARY. and connexion with nerve cells, the connexion of the nuclei with each other by nerve fibres passing from the roots and from the nerve cells, the structure of the olivary bodies which possess a peculiar interest from their resemblance in convoluted structure to the cere- brum and cerebellum. 3d. An attempt to show, notwithstanding the apparent difference of structure between the spinal cord and medulla oblongata, a difference which appears very considerable at first sight, that the plan of struc- — ture of the two is identical, that the general arrangement of parts strictly corresponds, that the relation of the nerve roots to their nuclei or cell groups is the same, and moreover the connexion estab- lished between the different nuclei is carried out on the same plan. The illustrations for this work were taken by the author himself directly from the microscopic dissections by photography. For the general edition the photographic illustrations have been copied on stone with great care by L. H. Bradford. The steel plates were en- eraved by J. W. Watts. Besides these, a limited number of photo- graphic prints from the original negatives have been prepared by Dr. Dean himself for private distribution, and from these negatives other copies may be obtained either on direct application to the author or through the medium of this Institution. 3 . This paper, which is the result of over two years of constant study, was referred to Dr. W. A. Hammond, of the United States army, and Professor Jefiries Wyman for critical examination, and was recom- mended by them for publication as a valuable addition both to human and to comparative anatomy. The third paper accepted for publication is on the Paleontology of the Upper Missouri, by F. B. Meek and F. V. Hayden. _ This work contains figures and descriptions of all the known inver- tebrate fossil remains of the various geological formations of Idaho, Dakota, Nebraska, and portions of Kansas. About 370 species, nearly all of which are new, are fully described, and the descriptions are accompanigd by remarks on the relations of each species to allied forms from other districts in this country and Europe, both living and fossil—its geological range, geographical distribution, &c. The illus- trations consist of about one thousand. carefully drawn figures, occu- pying forty-five quarto plates. In addition to full descriptions of species, the work also contains extended accounts of all the genera to which these fossils belong, with the synonymy of each genus, and remarks on its affinities to other genera, both living and extinct ; and assigns the probable period of © REPORT OF THE SECRETARY. ay its introduction, the time when it appears to have attained its maxi- mum development, and that at which it is supposed to have died out, if not represented in our existing seas. At the head of each generic description the etymology of the name and the type of the genus, when known, are given. Full descriptions of each of the families including these genera are likewise given ; and at the end of each family description the names of all the genera, whether living or ex- _ tinct. The introduction contains detailed descriptions of the various formations in which these fossils existed, with remarks on their synchronism with other American and Kuropean deposits. A considerable portion of the specimens described and figured were collected by Dr. F. V. Hayden in the several expeditions into the regions of the Upper Missouri and Yellowstone, sent by the govern- ment under the command of Lieutenant (now Major General) G. K. Warren, of the United States Topographical Engineers, to whose scientific zeal and liberal encouragement we are indebted for much of the material upon which the work is fotnded. But besides these, a large number were collected by Dr. Hayden himself previous to his connexion with the exploring expeditions of the government. The specific descriptions of the fossils described in this work are therefore to be regarded as appearing,in the joint names of Meek and Hayden, while the descriptions of the genera, and families, and the discussion of their relations, geological range, geographical distribution, &c., are to be accredited to Mr. Meek alone. The first sketch of this work was prepared as a part of the report to Congress of the explorations of the above-mentioned regions, but Mr. Meek has since devoted almost three years exclusively to extend- ing and completing the investigations; and as it is probable that Con- gress will make no provision for its publication, it has been adopted by the Institution, at the earnest recommendation of several eminent naturalists, and will be published in successive parts. All the speci- mens described are in the collections of the Institution, and as saon as the work is completed the numerous duplicates will be distributed, as types of the species, to various scientific institutions at home and abroad. Miscellaneous Collections. —Several series of articles forming parts of the Miscellaneous Collections, as stated in previous reports, have been undertaken, of which some have been completed, some are still in hand, and others have been printed during the past year. The first of these series is that relating to the shells of North America, and will consist of the following works : 22 REPORT OF THE SECRETARY. 1. Check lists of North American shells, by P. P. Carpenter, &c. 2. Circular relative to collecting shells. 3. Hlementary introduction to the study of conchology, by P. P. Carpenter. 4. List of the species of shells collected by the United States ex- . ploring expedition, by the same author. 5. Descriptive catalogue of the shells of the west coast of the United States, Mexico, and Central America, by the same author. 6. Descriptive catalogue of the air-breathing shells of North America, by W. G. Binney. 7. Descriptive catalogue of several genera of water-breathing fresh water univalves, by the same author. 8. Descriptive catalogue of the Jiclaniade, or the remainder of the water-breathing fresh water univalves, by George W. Tryon. 9. Descriptive catalogue of the Corbiculade or Cycladide, a group of bivalves principally inhabiting fresh water, by Temple Prime. 10. Descriptive catalogue ‘of the Unionide, or fresh water mussels. 11. Descriptive catalogue of the shells of the eastern coast of the United States, by William Stimpson. 12. Bibliography of North American conchology, by W. G. Binney. 13. Check list catalogue of cretaceous and jurassic fossils of North America, by F. B. Meek. The first and second articles of this list were published in 1860, and described in the report for that year. The third was published in 1861 as a part of the annual report for 1860. A new edition would have been printed before this time, as a part of the Miscellaneous Collections, had we not been disappointed by a delay in procuring the expected use of wood-cuts for the illustration ef the work from the British Museum. We have just learned, however, that the Mu- seum has liberally granted the use of these wood-cuts; that they are now being copied in stereotype in England; and consequently the work will be completed without further delay. The fourth and fifth articles are still in the hands of Mr. Carpenter, who has reported progress, which leads us to expect that they will be ready for the press during the present year. Of the 6th, 7th, and 8th, the first draughts of the manuscripts have been completed, and a preliminary sketch of the conclusions of the authors as regards the names of the species has been printed in the form of proof-sheets, and distributed to conchologists, with a view to elicit criticisms and suggestions prior to final publication. REPORT OF THE SECRETARY. 23 Many important additions and corrections have been obtained in this way which will add much to the value of the works. The request has been made that these proof-sheets should not be considered as express: ing the final views of the authors, but only intended to obtain the information above mentioned. The ninth article of the series, by Mr. Prime, is well advanced in printing, and will be completed in 1864. In addition to the purely North American species, it will contain descriptions and wood-cut figures of those of Central and South America, as well as of the West Indies, thus embracing all the members of the family found in the New World. The tenth and eleventh articles are still in process of preparation, and the engraving of the wood-cuts for their illustration has com- menced. The twelfth article—the first part of the Bibliography of North American conchology by Mr. Binney, mentioned in the last report as in press—has been completed and distributed. It forms a volume of 650 pages, and contains a list of the publications of American aug thors relative to conchology in general. As might reasonably be expected, some omissions have occurred of titles of papers overlooked or not met with, but copies have been sent to all the working con- chologists of the country, with the request to furnish rectifications and additions to be: inserted in an appendix to the second part. This second part, which is now in the press, is intended to include an account of the writings of foreign naturalists relative .to American conchology, and will also contain, beside the additions and corrections of the first volume, copious indexes of authors and names of genera and species. About 250 pages are stereotyped, and the whole work, probably filling over 500 pages, will be finished during 1864. The thirteenth article, check list by Mr. Meek, has been completed and put to press. It contains a list of all the species of cretaceous fossils described by authors up to the end of 1863, and will constitute an important aid in the labor of cataloguing and labelling collections, being prepared in the same style as that of the check-lists of North American shells, published by the Institution some years ago, which have been so much sought after by conchologists and amateurs. Another series of works belonging to the miscellaneous collections is intended to facilitate the study of American insects. Of this series the several articles are as follows: 1. Instructions for collecting and preserving insects. 2. Catalogue of the described Diptera (flies, musquitoes, &c.) of North America, by Baron Osten Sacken. 24 REPORT OF THE SECRETARY. 3. Catalogue of the described Lepidoptera (butterflies, moths, &c,) of North America, by Dr. Jno. G. Morris. 4. Classification of the Coleoptera (beetles, &c.) of North America, by Dr. Jno. L. Le Conte. 5. Synopsis of the described Neuroptera (dragon-flies, &c.) of North _ America, with a list of the South American species, by H. Hagen. 6. Synopsis of the described Lepidoptera of North America, part {. Diurnal and Crepuscular Lepidoptera, by Dr. Jno. G. Morris. 7. List of the Coleoptera of North America, with descriptions of new species, by Dr. Jno. L. Le Conte. 8. Monograph of the Diptera of North America, by H. Loew, with additions, by Baron Osten Sacken. 9. Monographs of Homoptera and Hemiptera, (chinches, roaches, &c.,) of North America, by P. R. Uhler. 10. Descriptive Catalogue of the Hymenoptera, (bees, wasps, &c.,) of North America, by H. De Saussure. These have all been described in previous reports. * Of No. 8, (monograph of Diptera,) the first part was published in 1862. During the past year the second part has been printed, and forms a volume of 339 pages. The manuscript of a third part is in an advanced state of preparation by Dr. Loew, and when received will, as in the case of the two preceding parts, be intrusted to Baron Osten Sacken for translation under his direction. We must again, in this connexion, express our obligations to Baron Osten Sacken for his valuable assistance in the preparation and publication of these works. Of No. 9, monographs of Homoptera and Hemiptera of North America, by P. R. Uhler, the manuscript is nearly completed, and will soon be received from the author. Of No. 10, the manuscript of the first part (Catalogue of Hymenop- tera) was received from the author during the past summer, and placed in the hands of Mr. EH. Norton, of New York, who kindly offered to translate it from the original French and superintend its publication. It is now in the press, and will soon be completed. In addition to the publications relating to shells and insects, the following, belonging also to the Miscellaneous Collections, have been prepared for the Institution: 1. Check-list of Minerals, by Thomas Egleston. 2. Instructions relative to Ethnology and Philology, by George Gibbs. 3. Comparative Vocabulary, by George Gibbs. 4. Dictionary of the Chinook Jargon or Trade (ae of Oregon, by George Gibbs. REPORT OF THE SECRETARY. 25 5. Monograph of the Bats of North America, by Dr. H. Allen, United States army. . No. 1 of these works has been prepared to aid in arranging and cataloguing the Smithsonian collection of minerals and the distribu- _ tion of duplicate specimens, but it will also be of value in facilitating the study of mineralogy by furnishing printed labels and check-lists for exchanges. It presents a list of all the described species of min- erals, with their chemical symbols and systems of crystallization, indi- cating those which are peculiar to the United States, the whole arranged according to the method*adopted by Professor Dana in the last edition of his Manual of Mineralogy. For important additions and corrections, this work is indebted to the principal mineralogists of this country, to whom the proofs were submitted, and especially to Professor Dana, Professor Brush, and Dr. Genth. This list is completed, and will shortly be ready for distribution. No. 2 of these works was printed in the Smithsonian annual report for 1861, but a large demand having arisen for it, it has been reprinted with corrections and additions, and now includes instruc- tions for philological observation, rules for recording sounds and vo- cabularies, &c. In the latter part of the work Mr. Gibbs has received important assistance from Professor W. D. Whitney, of Yale College. It includes directions for the collection of various specimens, hints for special inquiry, &c. Among the former are the skulls of Ameri-* can Indians, which in some cases are difficult to obtain, on account of the jealousy with which the natives guard the remains of their dead. Numerous tribes, however, have become extinct, or have removed from their former abodes. The remains of victims of war are often left where they fall, and the bones of slaves and of the friendless are neglected. Relics of these can be obtained without offence to the living. It is, however, of essential importance that most positive information should be obtained as to the nation or tribe to which a particular skull belongs. This may frequently be learned from the history of the migrations of the tribe, or from the character of the ornaments and utensils found with it. _ Among the specimens of art which are designated as desirable are dresses, ornaments, bows and arrows, lances, saddles with their furniture, models of lodges, cradles, mats, baskets, gambling imple- ments, models of canoes, paddles, fish-hooks, carvings in wood and stone, tools, &c. American antiquities are especially indicated as objects of interest. They include the tools found in the northern copper mines, articles 26 REPORT OF THE SECRETARY. inclosed in mounds, images, pottery, also the contents of ancient shell beds found on the sea-coast and bays, often deeply covered with earth and overgrown with trees; human remains, or implements of human manufacture, bearing the marks of tools or of subjection to fire, found in caves, beneath deposits of stony material formed by drop- pings from the roof; similar articles in salt-licks, likewise in deposits of sand and gravel, or such as evidently belonging to the drift period. Among other desiderata mentioned are the names of tribes, geo- graphical position, number of individuals, physical constitution, such as stature, proportion’of limbs, facial angle, color of skin, hair, and eyes; inscriptions, ‘dress, food, dwellings, arts, trades, religion, government, social life, ceremonies, mode of warfare, medicine, literature, method of dividing time, history, &e. These directions also include a list of words most important to be used in forming the vocabulary of a language. The pamphlet con- sists of thirty-four pages, and is distributed gratuitously to all who are desirous of aiding investigations of this character. No. 3 is a vocabulary of the principal words of which the equivalents are desired in the languages of the American Indians. It has been prepared with, great care by Mr. Gibbs after the usual models, presenting in parallel columns the words selected in English; French, Spanish, and Latin, leaving a blank column to be filled by the required equivalents in the dialect of any given tribe. It forms a pamphlet of eighteen pages, including two hundred and eleven different words, and is printed on letter paper? for convenience in filling up the blanks. No. 4, the Chinook Jargon, is a collection of phrases made up from various languages, Indian and civilized, and constitutes the sole medium of communication with the Indian tribes of the northwest. In 1853 the Smithsonian Institution published a brief dictionary of this language, from a French manuscript presented by Dr. B. R. Mitchell and edited by Professor W. W. Turner. The article was in great demand, and the edition was soon exhausted. Mr. Gibbs, having paid particular attention to the Jargon during his long resi- dence in Washington Territory, kindly offered to prepare a new edition with corrections and additions. This offer was readily ac- cepted, and the dictionary has been published during the past year. The vocabulary of the Chinook contains words of two dialects, the Chinook proper and the Clatsop, and perhaps also of the Wakiakum. The nation or rather family to which the generic name Chinook has been applied, formerly inhabited both banks of the Columbia river REPORT OF THE SECRETARY. at from its mouth to the Grand Dalles, a distance of about one hundred | and seventy miles, and was, as is usual among the sedentary Indians of the west, broken up into numerous bands. Mr. Hale, in his Eth- nography of the United States Exploring. Expedition, has divided these into the Upper and Lower Chinook. The present vocabulary belongs to those nearest the mouth of the river, of which there were five principal bands. The language of the bands further up the river departs more and more widely from the Chinook proper ; indeed, so much so that the lower Indians could not have understood the upper ones without an interpreter. This vocabulary is not as full as could be wished, and the only reason for publishing it in its present condition is that the Indians speaking the language are so nearly extinct that no better digest is likely to be made in future. In regard to the 5th article of the above series, the Monograph of Bats of North America, it may be stated that the mammalia of this continent have been studied and described generally by Audubon, ‘Bachman, and also by Professor Baird of this Institution. These authors, however, have not included in their descriptions the cheirop- tera, or bats. * To supply this deficiency, Dr. Allen, of Philadelphia, has given his attention for several years to the careful study of the specimens of this animal in the principal museums of this country, and has presented the result of his labors to the Institution in the form of the monograph above mentioned. In this a detailed descrip- tion is given of each of the genera and species with wood-cut figures of the skulls, heads, eass, and tails of such species as require this mode of illustration. The wood-cuts of this paper have been completed and the manuscript is now in the hands of the printer. I may mention that the Institution is indebted to Mr. Figaniere, Portugese minister, for a very graphic account of an immense assem- blage of bats which had been colonized for years in the upper part ~ of a mansion house which he had purchased in Maryland. This ac- count will be republished in the appendix to this report, as well as in the paper of Dr. Allen just described. Reports. —The annual reports to Congress are printed at the ex- pense of the government as public documents, with the exception of the wood-cuts, the cost of which is paid by the Institution. Previous to 1853 the reports were principally confined to an exposition of the operations of the Institution, and were published in pamphlet form; but since that date an appendix has been added to each report, which, with the other matter, has increased the size to that of a volume of four hundred and fifty pages. These reports now form a series of ten 28 REPORT OF THE SECRETARY. volumes, beginning with that of 1853, and in order that this series might contain a history of the Institution from the beginning, the will of Smithson, the enactments of Congress-in regard to it, and the sev- eral reports of the Secretary, previous to 1853, were republished in the appendix to that volume. The report for 1862 contains, in the appendix, a eulogy on the late Senator Pearce, by Professor Bache ; a course of lectures on Polarized Light, by F. A. P. Barnard, late president of the University of Mis- sissippi; a course of lectures on Ethnology, by Professor Daniel Wilson, of the University of Toronto ; an introduction to a course of lectures on the Study of High Antiquity, by A. Morlot, of Switzer- land, translated for the Institution by the author ; an account ‘of the Articles on Archelogy, published by the Smithsonian Institution, copied from the ‘‘ Natural History Review,’’ of Engfand ; a history of the French Academy of Sciences; eulogies on Von Buch and Thenard, a continuation of the series of memoirs of distinguished members of the French Academy, translated by C. A. Alexander, - esq.; a Memoir of Isidore St. Hilaire, by Quatrefages, translated by a lady ; a prize Memoir on the Catalytic Force, by T. L. Phipson ; on Atoms, by Sir John Herschel ; Classification of Books, by J. P. Lesley ; Account of Human Remains from Patagonia, and Prize Questions of Scientific Societies. Of this report the usual number of 10,000 copies was printed, of which 4,000 copies were given to the Institution, to be distributed in accordance with the following rules: ‘ 1. To all the meteorological observers who send records of the weather to the Institution. 2. To the collaborators of the Institution. 3. To donors to the museum and library. 4, To colleges and other educational establishments. 5. To pubtic libraries, and literary and scientific societies. 6. To teachers, or individuals who are engaged in special studies, and who make direct application for them. Owing to the many changes which have taken place in the resi- dence and occupation of the correspondents of the Institution since the commencement of the war, it has not been thought advisable to send the reports to all whose names are on the record of distribution, but in most cases to wait until direct application is made by letter or otherwise for a copy of the work. Whenever a report is sent to any address a separate announcement is made of the fact enclosing @ blank receipt to be signed and returned to the Institution. REPORT OF THE SECRETARY. 29 On account of the large amount of printing required by the gov- ernment in consequence of the war, the public printing office has been taxed to its utmost power ;,documents not required for immediate use have been delayed, and among others the report of the Institution for 1862 is still not quite completed. It is expected, however, that it will be ready for distribution in the course of a few weeks. The number of copies of the report ordered to be printed by Congress has varied in different years, and consequently in the increasing de- mand some of the volumes have been entirely exhausted. It may be a matter of consideration whether a new edition of the report for 1856, and perhaps for other years, might not be reprinted. To pre- vent the future exhaustion of the supply of the reports, Congress authorized the stereotyping of the last volume and the printing at any time, from the plates, of the whole or any part of its contents. In view of the great cost of paper and the space required for storage, it has been thought advisable to stereotype the Contributions and Mis- cellaneous Collections, and to strike off only as many copies of each article as are required for immediate distribution. By the adoption of this plan, the ability to supply, to any extent, copies of works published hereafter will always exist, while no more need be printed than are actually required. - Ethnology.—From the first, the Institution has given considerable attention to the various branches of ethnology. Besides the addi- tions to Indian archelogy which are to be found in the several volumes of its Contributions to Knowledge, it has published : everal papers on languages. In the report for 1860, a list of original manu- scripts was given relating to the languages of the northwest cast of America, which had been received through the assistance of Mu. Alex- ander 8S. Taylor, of Monterey, California. Several of these were copied at the expense of the Inst:tution, with the intention of securing their preservation and subsequent pub- lication. It has also been stated that a number of these manuscripts had been presented to Mr. J. G. Shea, of New York, to be published in a series which he has established under the title of ‘‘ Library of American’ Linguistics.’? By presenting these to Mr. Shea for pub- lication and purchasing from him for distribution to learned societies a number of copies, encouragement has been given to a laudable en- terprize, undertaken solely to promote a favorite branch of learning, and with but little comparative expense to the Smithsonian fund. I regret, however, to state that the diminution of the effective income of the Institution will prevent further appropriations at present for this purpose. The following is a list of the works of Mr. Shea’s 30 REPORT OF THE SECRETARY. series, of which the Institution has aided the publication by purchas- ing copies for distribution: 1. Grammar of the Mutsun language, spoken at the mission of San Juan Bautista, Alta California; by Father Felipe Arroyo de la Cuesta. 2. Vocabulary of the language of San Antonio mission, California, by Father Bonaventure Sitjar. 3. Grammar and dictionary of the Yakama language, by Rev. Mie. Cles. Pandosy. : . 4, Vocabulary or Phrase Book of the Mutsun language, of Alta California, by Rev. Father Felipe Arroyo de la Cuesta. 5. Grammar of the Pima or Névome, a language of Sonora, from a manuscript of the XVIII century. The first of these, the Mutsun grammar, was described in the last report. The second, the vocabulary of the native inhabitants of the San Antonio, or Sext&pay, mission ; it was printed from a manu- script forwarded to the Institution by Alexander S. Taylor, of Cali- fornia. The mission of San Antonio de Padua was founded in 1771. in the Sierra of Santa Lucia, twenty-five leagues southwest of Mon- terey ; the authors of this vocabulary being the first missionaries. The tribe is sometimes knownas Tatché, or Telamé, though Mr. Taylor calls it Sextapay. It is gradually disappearing ; not more than fifty Indians still remain, although it is said they were, at one time, so numerous that the dialects spoken by them amounted to twenty. The third is the grammar and dictionary of the Yakamas, a people inhabiting the region of the Yakama river—a stream rising in the Cascade range of mountains, and emptying into the Columbia above the junction of the Snake river. The name signifies the ‘‘ stony ground,’’ in allusion to the rocky character of the country. The au- thor of the grammar, Father Pandosy, was for many years a resident among these Indians, and became well acquainted with their language. In the destruction of the buildings of the mission by fire, during the Indian war in Washington Territory, the original of the grammar was . lost, and the translation, published by Mr. Shea, which was made some time previously, alone remained. It is to be regretted that a more extended dictionary than the one now published was also de- stroyed at the same time. The fourth article is a vocabulary of the same language, of which the grammar constitutes the first of this series, and is by the same author ; the words are given in the Mutsun and Spanish languages. The fifth, the grammar of the Pima, with a vocabulary in the same language and in Spanish, was obtained in Toledo, Spain, and tran;- REPORT OF THE SECRETARY. 62 lated by Buckingham Smith, esq. This manuscript was probably taken to Spain after the suppression of the order of the Jesuits in Mexico, in 1767. The Pima language was spoken by the tribes from the river Yaqui, in Sonora, northward to the Gila, and even beyond the Colorado, eastward beyond the mountains in the province of Taraumara, and westward to the sea of Cortez. The phrases given in these works will preserve the knowledge of what constituted the food of the inhabitants ; their manner of living, their character, and native customs, &c. This may prove of historic interest hereafter, if the facts be nowhere else more circumstantially authenticated. Meteorology.—From 1856 to 1861 an appropriation was made from the agricultural fund of the Patent Office for assistance to the Insti- tution in collecting and reducing statistics relative to the climate of the United States. This was commenced while the Patent Office was under the direction of Judge Mason, but was suddenly discontinued under a change of administration. The pr8priety of an appropriation for this purpose, from the fund above mentioned, must be evident to every one who reflects on the intimate connexion between meteorology and agriculture. A knowledge of the peculiarities of the climate of a country is an essential requisite for the adoption of a system of scientific culture. The average temperature of the spring, autumn, and of the growing season; the ratio of the number of unfavor- able to favorable years; the amount of rain, and moisture ; the average time of the occurrence of late and early frosts, are all facts of importance in the economical adaptation of the crops to a given lo- eality, in order to obtain the maximum of produce from a definite amount of labor. The money received from the Patent Office was expended in assist- ing to defray the expense of the reductions of the observations, and as soon as the appropriation was stopped we were obliged to discon- ‘tinue this part of the operations. The Institution, however, still con- tinues to derive some benefit from its association with the Patent Office, in receiving through it, free of postage, the returned registers from the different observers. Unfortunately, the postage law adopted at the last session of Con- gress prevents the correspondents on agriculture and meteorology from sending their reports by mail unless prepaid. This arrange- ment almost entirely stops the reception of these articles, for, since the service rendered is gratuitous, the observers cannot be expected to bear this additional burden. It is to be hoped that Congress will so modify the law as to remove this obstruction to a correspondence of great importance to the agricultural interests of the country. ' 39 REPORT OF THE SECRETARY. Owing to this restriction, the number of meteorological registers received during the past year has been diminished, and the transmis- sion of nearly all of them would have been discontinued had not the Commissioner of Agriculture, in view of their value to his department, decided to advance to some of the observers the neces- sary postage stamps to affix to their registers. He would willingly have sent stamps to all, but the tax would have been too heavy for the office; he therefore found it necessary to limit the number, and in doing so endeavored to make such a selection as would secure registers from districts distributed as uniformly as possible in all the States. Those observers, therefore, who have not been supplied with stamps should infer from this no disparagement of their observa- tions, for among those who have been omitted from the list are some whose registers are highly prized for their regularity and accuracy. Before it was known that this arrangement would be made by the Commissioner a circular was sent from this Institution to all the ob- servers, mentioning the new feature in the postage law, and requesting them to continue their observations, and retain the records until the law should be modified, or some arrangement could be made by which the observers would not be subject to the burden of postage.* Under the new organization of the Department of Agriculture a renewed interest has been manifested by the Commissioner in the collection of meteorological statistics, and he has expressed the desire to co-operate with this Institution in continuing and extending the system of records of the weather which it had established with so much labor and expense. In order to obtain and diffuse a knowledge of facts of immediate importance to agriculturists, the Commissioner has commenced the publication of a monthly bulletin giving the state of the crops, the condition of the weather, and various other items of importance which are daily received from observers, and which would lose a considerable portion of their value were they suffered to remain unpublished until the end of the year. For this bulletin the Institution supplies the meteorological materials, consisting of the mean, maximum, and minimum temperature and amount of rain for each month in different States, and also, for the purpose of comparison, the mean temperature and amount of rain for a series of five years, grouped by States ; * This law has been changed since the above was written, and observers can send their meteorological registers, or other communications, to the ‘‘ Commissioner of Agriculture,” with out prepayment of postuge. REPORT OF THE SECRETARY. 33 together with tables of important atmospheric changes, and notices of auroras, meteors, and other periodical phenomena. The publica- tion has been received with much favor by agriculturists, and is regarded with great interest by the observers, who are thus fur- nished promptly with a general summary of the principal features of the meteorology of each month in all parts of the country, with which they can compare their own observations. In view of the value of the information thus furnished by the Institution, it is hoped that the previous appropriation will be renewed, and that the reductions which have been discontinued for the last four years may be resumed. The second volume of the Results of Meteorological Observations made for the Institution, from 1854 to 1859, and reduced by Professor Coffin, is still in the press, its completion being delayed by the great pressure, upon the public printing office, of government work relative to the war. : We are indebted to the courtesy of Captain (now General) George G. Meade, of the topographical engineers, superintendent of the survey of the north and northwestern lakes, and of his successor in office, Lieutenant Colonel J. D. Graham, for a continuation of the favor formerly extended to the Institution in furnishing us with copies of the meteorological observations made at the different stations estab- lished for the survey. These records are very valuable, being made with full sets of instruments and at important places. They em- brace observations made three times a day, at the same hours with the Smithsonian system, 7 a. m. and 2 and 9 p. m., and at ten sta- tions, extending from Superior City in the State of Wisconsin, at the western extremity of Lake Superior, to Sackett’s Harbor in New York, on the east end of Lake Ontario. The Bureau of Medicine and Surgery of the Navy Department also continues to furnish us with the meteorological records kept at the naval hospitals at Chelsea, New York, and Philadelphia. For several years previous to the commencement of the war a large map was exhibited in the Smithsonian Institution on which was daily represented the direction of the wind and face of the sky over the greater portion of the United States; and in previous reports we have frequently called attention to the fact that a properly organized sys- tem for giving daily or half daily changes of the weather in distant parts of the United States would be of great practical importance to the shipping interests of the country; we have also stated the fact that we are much more favorably situated for predicting the coming 38 34 REPORT OF THE SECRETARY. weather than the meteorologists of Europe. The storms in our lati- tude generally move from west to east, and, since our seaboard is on the eastern side of a great continent, we can have information of the approaching storm while it is still hundreds of miles to the west of us. Not so with the meteorologists of Europe, since they reside on the western side of a continent, and can have no telegraphic dispatches from the ocean. The proposition, however, to furnish constant information of this kind could not be carried out by the limited means of the Smithsonian Institution, and, indeed, can only be rendered properly and fully serviceable.under the direction and at the expense of the government. New and interesting features have been introduced into the daily meteorological bulletin published by the Imperial Observatory at Paris. As mentioned in the last report, these bulletins are litho- graphed each day from records of the barometer, thermometer, wind, and face of the sky, compiled from telegraphic reports transmitted to the observatory from various parts of Europe. In addition to these, they now contain daily a small outline chart of Europe upon which are drawn diagrams showing the barometric curve of the day through the various stations, together with the temperature and direction and force of the wind. For the use of vessels about to leave port, a state- ment is also given of what will probably be the direction of the wind the next day. Chambers of commerce and intelligent seamen have acknowledged in strong language the benefit of these daily bulletins, thus adding to the ever-accumulating testimony in favor not only of the speculative interest but also practical benefits of meteorology.‘ At Bordeaux, Havre, and other important ports, as soon as the bul- letins are received, the telegraphic announcement of the weather and the probable direction of wind for the following day are posted in public places and furnished to the principal newspapers for publica- — tion. The bulletin also contains extracts from the correspondents of the observatory on astronomical and other subjects as well as meteo- rology. With the number for December 20, a supplement was issued with a diagram exhibiting the indications of the self-registering instru- ments at the Royal Observatory, Greenwich, during the great storm on the English coast in the first three days of December, 1863. Laboratory.—The principal work which has been done in the laboratory during the past year is an extended series of experiments on the properties of different kinds of oil intended for light-house purposes. For a number of years past the price of sperm oil has been constantly increasing, and from a dollar per gallon it had ad- REPORT OF THE SECRETARY. 35 vanced last year to two dollars and forty-three cents. It became, therefore, animportant matter to the Light-house Board to determine whether some other burning material could not be introduced in the place of so expensive an article. The investigation of this subject was given in charge to myself, as the chairman of the Committee on Experiments. The result of the investigations not only revealed a number of new phenomena. of interest to science, but also estab- lished the important practical fact of the superiority of winter strained lard oil over standard sperm oil in the intensity of the light, the steadiness and persistence of the flame, and the less care required in attendance. This fact must have an important bearing on the cost of lighting the extended coast of the United States, as well as upon the commercial value of one of the staple products of the western part of our Union. The price of lard oil is, at present, considerably less than one-half of that of sperm, and while the supply of sperm oil has remained stationary, or even diminished with an increasing de- mand, the sources of lard oil in the country are abundant, and the quantity which can be produced will be sufficient to meet almost an unlimited consumption. Another series of experiments was made for determining the proper arrangements of reflectors and lenses for illuminating distant ob- jects either by the electric or the calciumlight. These experiments were instituted at the suggestion of the Navy Department, but as no appropriation was made for their being carried into practice, they were discontinued, and the knowledge obtained remains unapplied. Collections of specimens of natural history, &c.—In several of the preceding reports a distinction has been drawn between the collec- tion of specimens of natural history made through the agency of this Institution, and what is called the Smithsonian museum. The object of making large collections of duplicate specimens is, first, to advance science by furnishing to original investigators new materials for critical study; and second, to assist in diffusing knowledge, by providing colleges, academies, and other educational establishments, with labelled specimens to illustrate the various productions of nature, while the principal end to be attained by the public museum of the Institution is the gratification and instruction of the inhabitants and visitors of the city of Washington. The collecting and distributing of a large number of specimens, for the purpose stated, is an important means of increasing and diffusing knowledge, and, as such, is in strict accordance with the will of the founder of the Institution. It has, therefore, from the first received 36 REPORT OF THE SECRETARY. much attention, and has been attended with a commensurate amount of beneficial results. Among the collections received during the past year have been specimens of great interest, either the results of explorations, undertaken by the Institution, or of exchanges with individuals or local societies. The materials thus collected belong principally to two classes, namely, to specimens of new or rare forms intended to advance natural history and duplicates of such as are to be labelled and distributed for the purposes of education. Among the former are the collections of Mr. Kennicott, whose explorations . have been mentioned in previous reports. They are of a very valu- able character, illustrating the natural history and ethnology of. the northwestern portions of the continent of North America. The specimens received in 1863, from this exploration, filled forty boxes and packages, weighing, in the aggregate, 3,000 pounds. They em- brace in the line of natural history thousands of skins of mammals and birds, eggs, nests, skeletons, fishes, insects, fossils, plants, &c. * In the line of ethnology are skulls, dresses, weapons, implements, | utensils. instruments of the chase, in short, all the requisite material to illustrate the peculiarities of the Esquimaux and different tribes of Indians inhabiting the northwest regions. In addition to the collections obtained from the British possessions in North America, by Mr. Kennicott, specimens have been received from other points and other parties. Among these are a series of | birds and eggs from Labrador, gathered by Mr. Henry Connolly, and. a large amount of new material from Mexico, collected by John Xantus, — under the auspices and at the expense of the Institution, consisting of birds, fishes, reptiles, shells, &c. Another series from the same country’ has been presented by Dr. Sartorius, who has, for a number of years, been one of the meteorological observers of the Institution. Inter- esting collections have been received, also, from Dr. A. Van Frantzius, | of Costa Rica; from Mr. Osbert Salvin, of Guatemala; from Captain) J. M. Dow, of Panama; specimens from Cuba have been presented! by Mr. C. Wright and Prof. Poey; from Trinidad, by Mr. Galody, | United States consul; from Jamaica, by Mr. W. T. March; from Ecua:: dor, by the Hon. C. T. Buckalew, now of the United States Senate. A valuable contribution of birds and mammals has also been received from Prof. Sumichrast, of Orizaba. These collections are all intended to illustrate the natural history of the American continents, to the investigation of whose extended regions the Institution has especially directed its labors. | In order to facilitate the preparation of a work on the birds of America, by Prof. Baird, a circular from the Institution was dis- REPORT OF THE SECRETARY. at tributed through the State Department to the consular and diplomatic agents of the United States in Central and South America, asking aid in completing the collection of birds, and we doubt not that much new and valuable material will thus be obtained. The following are the rules which have been adopted in regard to the disposition and use of the collections: First. To advance original science, the duplicate type specimens are distributed as widely as possible to scientific institutions in this and other countries, to be used in identifying the species and genera which have: been described. Second. For the purposes of education, duplicate sets of specimens, properly labelled, are presented to colleges and other institutions of learning in this country. Third. These donations are made on condition that due ae is to be given the Institution in the labelling of the specimens, and in all - accounts which may be published of them. Fourth. Specimens are presented to foreign institutions, on condi- tion that if type specimens are wanted for comparison or other use in this country they will be furnished when required. Fifth. In return for specimens which may be presented to colleges and other institutions, collections from localities in their vicinity shall be furnished when wanted. In the disposition of the undescribed specimens of the collection, the following considerations have been observed as governing prin- ciples: first. The original specimens are not to be intrusted for descrip- tion to inexperienced persons, but to those only who have given evi- dence of ability properly to perform the work. Second. Preference is to be given to those who have been engaged in the laborious and difficult enterprise of making complete mono- graphs. Third. The investigator may be allowed, in certain cases, to take the specimens to his place of residence, and to retain them for study a reasonable time. Fourth. The use of the specimens is only to be allowed on condition that a series of types for the Smithsonian museum will be selected and properly labelled, and the whole returned in good condition. Fiih. In any publications which may be made of results derived from an investigation of the materials from the Smithsonian collection, full credit must be accorded to the Institution for the facilities which have been afforded. 38 REPORT OF THE SECRETARY. During the past year the assorting and labelling of the specimens have been continued, as well as the distribution of duplicates. The whole number of entries on the record book of the Smithsonian collection, at the end of the year 1861, was 66,075; at the end of 1862, 74,764, and at the end of 1863, 86,847; but each entry indi- cates a lot consisting of a number of specimens. The whole number of duplicate specimens distributed to different institutions in this country and abroad, up to the end of the year 1863, has been 94,713. As these specimens are distributed on the express condition that full credit is to be given to the Institution on the labels, and in all pub- lications which may relate to them, the name of Smithson, even through this distribution alone, would become familiarly known in every part of the civilized world. It has been, from the first, one of the prominent objects of the Institution to collect the most ample materials for illustrating the entire natural history of North America; to determine the different species of plants and of animals; to ascertain the distribution of the former, and the migrations of the lftter. This object it has endea- vored to accomplish through the agency of the different surveying expeditions of government ; through explorations instituted at its own expense, and by enlisting the co-operation of individuals interested in science, and of local scientific societies. In all its efforts in this line it has been heartily supported, and it is believed that its labors have been productive of valuable results. The collections thus made have been intrusted to competent investigators for examination and description, and the results published in the different Smithsonian series, in transactions of societies, and in various government reports. For a list of what has already been prepared and published, either by the Institution or under its direction, I would refer to a report on this subject in preparation by Professor Baird. ' Museuwm.—The additions to the museum, in the line of natural his- tory, are principally confined to the type specimens which have been collected and described at the expense of the general government, or under the immediate auspices of the Institution. Even thus restricted, the specimens increase in number more rapidly than the portion of the Smithsonian fund which can be devoted to their support will authorize. Few persons have an idea of the labor, constant care, and expense which attends the proper preservation of a series of objects of natural history ; but those who have had the necessary experience know that large miscellaneous collections can only be properly sup- ported by governments , and, in the establishment of provincial socie- REPORT OF THE SECRETARY. 39 ties, the rule has been strongly recommended of attempting to pre- serve nothing except what is strictly local. ‘‘It is the experience of societies,’ says Dr. Jardine,* the celebrated Scotch naturalist, ‘‘that general collections are encumbrances, and in most instances get destroyed for want of care, or they are dispersed. Within these few years the really fine and valuable collection of the Zoological Society of London, chiefly presented by the late N. A. Vigors, a first-rate scholar and naturalist, and containing many unique things from our scientific exploratory voyages, has-been sold. That of the Entomological Society has also been sold, and the greater part of that belonging to the Linnzan Society was sold during the last month, because there was not sufficient space to keep what had been pre- sented to them. The collection of the Royal Society of Edinburgh is now undergoing the same process.’’ During the past year the work of labelling the specimens in the museum, so that the common, as well as the scientific name of each article may be distinctly exhibited, has been continued. Explorations.—The only explorations during the past year, under the auspices and at the expense of the Institution, are, Ist, the con- tinuation of that of Mr. Xantus on the western coast of Mexico ; and, 2d, that by Mr. Meek in New Jersey and the lower part of Virginia. The explorations of Mr. Xantus extended several hundred miles along the western coast of Mexico in a region little known, and very abundant in interesting objects. The exploration of Mr. Meek related to the collection of complete series of shells to illustrate the tertiary formation of the seaboard of New Jersey and Virginia. Several series of shells were obtained, which are in the process of being accurately labelled, and are intended for distribution to some of the principal colleges of the country. Exchanges.—The important aid rendered to science and literature by the system of international exchange which has for many years been actively carried on by the Institution, is still everywhere highly appreciated. Our operations in this line are becoming more and more extensive, requiring an additional amount of time, labor, and attention, as well as largely increasing in expense. ‘The great liber- ality of many of the transportation companies alone enables us to carry on the system in its present extent, and we again tender our acknowledgments, especially to the following parties, who have * Address of Sir W. Jardine, president of the Dumfriesshire and Galloway Natyral History and Antiquarian Society, December, 1863 40 REPORT OF THE SECRETARY. assisted us in this respect: The North German Lloyd, between Bre- men and New York; the Hamburg and New York steamship line ; the Cunard line ; the Panama Railroad Company ; the Pacific Mail Steamship Company ; Adams’s Express Company, and the Hudson’s Bay Company. During the past year it was deemed advisable to establish a new agency of exchanges for Holland and Belgium, and Mr. Fred. Muller, bookseller, at Amsterdam, who was appointed the agent, has entered upon the discharge of his duties with zeal and efficiency. The numbers of the transactions of the societies in the countries referred to necessary to complete the sets in the Smithsonian library, as well as much other valuable scientific and literary material, have been procured by him. The other foreign agents of the Institution are still Dr. Felix Flugel, Leipsic, Mr. Wesley, London, and Gustave Bossange, Paris. From the tabular statement given by Professor Baird, it appears that during the year 1863 there have been sent to foreign countries 1,426 packages, each containing a number of articles, enclosed in 61 boxes, measuring 447 cubic feet, and weighing 10,286 pounds. The number of packages received in return for societies and individuals in this country was 1,522, included in which, for the Smithsonian Insti- tution, were 4,589 books and pamphlets, besides specimens of natural history. LInbrary.—The policy in regard to the library as has frequently been previously stated, is to form a collection as perfect as possible of all the tranactions and proceedings of the learned societies of the world. The success of the Institution in this enterprise has been fully commensurate with the expectations entertained, and the collection of works of this class, if the accumulation continues under the same favor- able conditions, will soon rival any other of a like kind in the world. The liberal distribution which the Institution has made of its own pub- lications and those of government has produced a rich return in series of transactions which, although existing as duplicates in some of the older libraries of Europe, can scarcely be obtained by purchase. It was mentioned in the last report that the number of transactions and proceedings of learned societies contained in the library of the Institution had increased so much that a new edition of the cata- logue previously published had become necessary. This work has - since been put to press, and will be printed as rapidly as the care necessary to insure acccuracy will permit. Copies of this catalogue REPORT OF THE SECRETARY. 41 will be distributed to all the principal libraries of the country, and with the liberal policy which has been adopted in regard to the books of the Smithsonian collection, will serve to render the library more generally useful. By exchanges there have been received 719 octavos, 167 quartos, and 24 folios ; of parts of volumes and pamphlets, in octavo, 2,119; in quarto, 779; in folio, 581; maps and charts 200 ; total, 4,589. In addition to these about 400 volumes were purchased. Among the valuable works received during the year, are the fol- lowing : : 55 volumes from the Royal Library of Stockholm. Comptes-Rendus, 1859, 1860, 1861, with atlas, from the Commission Imperiale Ar chelogique, St. Petersburg. 12 volumes and 18 parts of volumes from the Koninlijk Institut des Ingenieurs, d’ Gravenhage. 52 volumes and 94 pamphlets from the Nederlandsch Maatschappig ter Bevordering van Nijverheid, Haarlem. 10 volumes of its own publications from the Société pour la recherche et la conservation des Monuments Historiques du Grand Duché de Luxembourg, Luxembourg. 24 volumes‘and 12 parts from the Kaiserliche Akademie der Wis- senschaften, Vienna. 9 volumes and 29 charts from the Etablissement Géographique de Bruxelles. 21 volumes of Proceedings from the Société d’ Agriculture, Com- merce, Science et Arts du Dept. de la Marne. 24 volumes of Proceedings and Transactions from the Institution of Civil Engineers, London. 36 volumes and 114 charts from the Board of Admiralty, London. Large donations from the Royal University of Norway. Braddam’s Memoirs of the Royal Society of London, vol. ix 1745, from Mrs. Mary A. Malthie, Syracuse, New York. 26 volumes from the Regents of the University in behalf of the State of New York. Lectures.—The usual course of lectures has been commenced for the present season, and will embrace the following : Five lectures, by Rev. John Lord, of New York, on the ‘¢ Fall of the Roman Empire.’’ Subjects——I. The grandeur and glory of the Ancient Civilization—The external splendor of the Roman Em- pire in its latter days. II. The internal hollowness and defects 42 REPORT OF THE SECRETARY. of the old Roman civilization—The shame and miseries of society— The vices of self-interest, and preparation for violence and inev- itable ruin. III. The fall of the empire, and the desolations pro- duced by the barbarians—The destruction of the old fabric of so- ciety. IV. The reasons why the old conservative influences of paganism did not arrest the ruin—The failure of art, literature, and science, and the mechanism of governments. V. The reasons why Christianity did not save the Empire, and the ideas which the church incorporated with subsequent civilizations—The foundation of the new Teutonic structure. Three lectures, by Professor Louis Agassiz, of Cambridge, Massa- chusetts, on the ‘‘ Glacial period.” - One lecture, by Professor J. L. Campbell, of Wabash College, on ‘t Galileo.’’ Seven lectures, by Dr. Reinhold Solger, on ‘The Races of Men.’’ Six lectures, by Professor W. D. Whitney, of Yale College, on “Philology.’ I. History and objects of linguistic science—Plan of these lectures—Why and how do we speak English—How language is preserved and perpetuated—Its constant change—The study of language an historical science. II. Ilustration of the processes of growth and change in language—Formation of words by combination of old materials—Mutilation and corruption of existing forms—Change and development of meaning—Rate of progress of these changes. III. Statement and illustration of the influences causing the growth of dialects, and those checking and counteracting this growth—Our language a Germanic dialect, with partly French vocabulary languages with which it is related—Branches of the Indo-European family of languages, and proof that they are of common descent— Place, period, and grade of civilization of the original tribe. IV. His- torical and linguistic importance of the Indo-European race and lan- euage—History of the language—Its development from monosyllabic roots. V. Survey of the other great families of language, Semitic, | Scythian, Chinese, Polynesian, Egyptian, African, and American— Isolated languages not included in these families. WI. Comparative value of linguistic and physical evidence of race, and their relative bearing on the science of ethnology—Relation of the study of language to the question of the unity of the human race—origin of language— Its character and value to the human race.* The number of applications for the use of the lecture-room has * A synopsis of this course of lectures has been furnished by the author for insertion in the appendix to this report. REPORT OF THE SECRETARY. . 43 been much less since the adoption of the rule restricting its use to the purposes of the Institution exclusively has become more gener- ally known. This rule, which has been widely approved of by the - enlightened public, has precluded a large amount of unprofitable cor- respondence and enabled the Institution to avoid an embarrassing and inauspicious connexion with sensational expositions of the exciting subjects of the day. From the preceding account of the present condition of the Insti- tution, and of its operations during the past year, as well as from the examination of the collections and publications, it is hoped that, not- withstanding the unfavorable condition of the country for scientific research, and the diminished means at our command, it will appear that the line of policy and of action originally adopted has been pur- sued with unabated ardor and with corresponding success. Respectfully submitted, JOSEPH HENRY, Secretary. WASHINGTON, 1864. ’ ‘ ‘ APPENDIX TO THE REPORT OF THE SECRETARY. SMITHSONIAN INSTITUTION, Washington, December 31, 1863. Sir: I have the honor to present herewith a report, for 1863, of the opera-’ tions intrusted to my charge, consisting especially of those relating to the printing, the exchanges, and the collections of natural history. Very respectfully, your obedient servant, SPENCER F. BAIRD, Assistant Secretary Smithsonian Institution. Prof. Joseru Henry, LL.D., Secretary Smithsonian Institution. PRINTING. An accompanying table will show the works printed during the year, and also those now in press. ‘The total number of pages belonging to works finished within the year is: OE quarto papers... =~... -- te oe idm alone a le aie 350 pages, 3 plates. Octavo Miscellaneous Collections ---..2.---22------ 1,313 pages. Of works still in press there have been printed : Of quarto RVOLIGA MRIDOUbL caterer eis ie 108 pages. OCT MCI a ei carbo ce relate (cb Toiee RePEc Lata OR EE ee 443 pages. _ Making a total of 458 quarto pages, and 1,756 octavo, exclusive of the annual report to Congress, nearly finished, and to fill 450 pages. EXCHANGES AND TRANSPORTATION. The system of exchanges has been in a highly successful condition during 1863, both the receipts and transmissions being fully equal to the average of any previous year. ‘The attendant expenses of this branch of operations are, however, great and increasing, and would long since have become almost pro- hibitory but for the liberality exhibited by various transportation companies in carrying the boxes and parcels cf the Institution free of any charges for freight. It is not too much to say that thousands of dollars are thus presented by the com- panies as a recognition on their part of the great importance, domestic as well as international, of these operations of the Institution. Ameng the parties de- serving of especial mention in this connexion are the proprietors of the Cunard steamers between New York and Liverpool, and New York and Havana; the North German Lloyd, between New York and Bremen; the Hamburg American Packet Company, between New York and Hamburg; the Panama Railroad Company ; the Pacific Mail Steamship Company ; the Hudson’s Bay Company ; the Adams Express Company, &c. REPORT OF THE ASSISTANT SECRETARY. 45 The Institution is under especial obligations, for important services rendered in this connexion, to the Hon. Hiram Barney, collector of the port of New York, and to his assistant, Mr. George Hillier; to Mr. A. B. Forbes and Mr. Hubbard, of the Pacific Mail Steamship Company, in San Francisco, as well as to the regular agents of the Institution. During the year, 1863, a new literary agency of the Institution was established for Holland and Belgium. Mr. Frederick Miller, bookseller, of Amsterdam, was placed in charge, and he has already rendered much service. The other foreign agents of the Institution—Dr. Felix Fliigel, of Leipsic; Gustave Bossange & Company, of Paris; and Mr. William’ Wesley, of London—continue to dis- charge their duties with efficiency, and to the full satisfaction of the Insti- tution. The number of institutions and individuals, at home and abroad, making use of the facilities of scientific exchanges offered by the Smithsonian Institution is continually on the increase, and it is believed that any interruption or suspen- sion of this part of the programme of operations would be considered as a serious calamity. In 1862 the Institution distributed four volumes of Miscellaneous Collections, one volume of Annual Reports, and one thick quarto volume of Meteorological Records and Reductions. In 1863, owing to various circumstances, the Annual Report for 1861 was the only volume distributed, although many copies of separate papers were sent abroad. For this reason the bulk of sending, in 1863, was less than that of previous years, but it is expected that the difference will be fully made-up in 1864. The following tables exhibit the details of the operations in the line of ex- change during 1863: A. Receipt of books, &c., by exchange in 1863. Volumes : ACTA cisk i, ideals vie ge ara SS oo 5's Ree Utne ao NANG Ns cise er ME yer ffs Bas pst tie 167 HONIG Rtsbre, 3 hes eee eaarnemcAtee eines issu. See 24 910 Parts of volumes and pamphlets : MC EAVO «acer terete arate Co Gane ret eke tee ieee 2,119 Oidarto. . < - JEEP A oe ee laos pee wks ABE 779 Polign.. swage ipeoreite ses uaa ae. \eniss:e - cai 581 3,479 meempeanta Charts.) sams Poa ae SS eo ley Uy Saree Ba kee f 200 Total! sob Bees a4 pbik it etak ease eeee ACE se 4, 589 emer iTE DOG) LeSe Re ALI ee SUR Ne Se ee 2, 886 Reem igw HE POG 2”... icin eres PRN oe EU ae Le 5, 035 46 APPENDIX TO THE REPORT OF THE SECRETARY. ; B. Table showing the statistics of the exchanges of the Smithsonian Institution an 1863. ' 4 q m 3 3 So Bo i a 32], | 94 | #28 | 2 Agent and country. wa | we | Ok iS Se ‘oe Qa ore = O'S * ol oy 5 5 3 Cer A A & E Dr. FELIX FLUGEL, Letpsic— Ricamdinavinesosie6 o-6,ncieen eon 1 MV E03.2 2 .nllenoeeeee | eotecreee Soredenecee anne cease entisaclle 13 She leads See) Se eee aes Norway --------- --------------- 4 EE cite a mm VEIT eee ioe = ee sin oan amin 13 SL 5.2 3-2 a eee eee RUINS IGiee ore aie So oiele aisle mio ataieiain i=l 42 COU Pconc0n|| Joie eee ste Some ees Germany .-....-.---- ---------- - 265 AOS iiss fete ab Pe oneeee RppbAeR ANC weep lee mnie tsieteeta cian in 30 ESE Sa ate alia eS eee All ek Ee Belgium ....-------------------- 10 A 2 ees See) ce crue (ered ae eiesie Piel PRU am re 378 690 | _ 26 202 | 3,500 FREDERICK MULLER, Amsterdam— PLO barid ereete oo sine = totata eialateiere alate 40 Ble ee eee wecers sae ecener ee ple eh siccule cetera eee 40 81 | 4 31} 1,006 GuSTAVE BossanGE & Co., Paris— IBTANCAe een = alos esee etait sate 107 NSO- Rete cece leceocees lowes Maly yaa epee re larele (= - <5) tee a een ge cele wo = 672 United States National Observatory: -2....¢- 22222022... 149 Hinited: States. Patenta@inee 7.0) 502) Bee ee es oo 465 pupetintendent- of -Gonsasy=3.:o-cn ose te ye ss 200 Mme abt Serge 3 yee ote yg ER ete TOE Re 15 Wi indsor, Nova Scotia— ere 4 EO Wk ene eRe eee creat ene TLD ah Ame 18 3,316 48 APPENDIX TO THE REPORT OF THE SECRETARY. D. Addressed packages received by the Smithsonian Institution from Europe, for distribution in America, in 1863. No. of packages. No. of packages. | ALBANY, NEW YORK. BOSTON, MASS.—Continued. ATban ty INStUtG oo. o es cee eS a enke 2 || Professor C. J. Jackson...--.....-.. 1 AIDBDVRUNDTAM ee. fee ke conn ccs mse 1 |) Professor Rogers. 2=-)-- yet ee eee ee 1 Dudley Observatory ......---------- GO") SEL. Seudders. 25252) sy aa enees 1 New York State Agricultural Society..| 29 || Charles Sprague..........-----.--.- 1 New York State Library.... -..- ---- al |\iGeorre- Lieknor's..--2--2 ee eee eee 1 New York State Medical Society - ---- 1 New York State University.......... 4 BRATTLEBORO’, VERMONT. Droweeemmonss 255-52 2s.4 Soe Ss 1 Protesson James Hall. 2. ccsssrm< sc 4 ||, Asylumitordmsane® © a8 eee aero 1 AMHERST, MASSACHUSETTS. BRUNSWICK, MAINE. Amherst Caller’: 0025 s-5-0 Sets 2-1 4 || Historical Society of Maine......--.. 2 DP Pew hatehcock5— = <= veccre mance 2 Charles H:-Hitehcock--....2 2... 2255 J BURLINGTON, IOWA. Professor Charles Upham Shepherd. -. 2 Iowa Historical and Genealogical In- ANNAPOLIS, MARYLAND. stitute. .-.- - wn aetekics, canes s See Binteibraiy ee sor te 4 BURLINGTON, VERMONT. University of Vermont.....-----.-.- I ee eee CAMBRIDGE, MASSACHUSETTS. Mbsonvatoly.sconce = =) couse erceee 2 || American Association for Advance- Te STUN OW as ec mc miseloisie se siaie re 4 MeNt Of SCiGNCe --as ese eee 21 Astronomical Journal....-..-......- 2 AUGUSTA, MAINE. Harvard. Colleges: =. ¥- see sae one il Observatory of Harvard College...-.-- 21 State Wuibrary ic <6 en aoe coee cee nee 4 || Professor. Agassizie--syee ee eee 40 G. PweBond. 3-2-2. ae— poco sere eee 4 BALTIMORE, MARYLAND. Professor El... Clarks-seccemere caer 1 Professor’ J. P:/Cooke ee asaser sso ee 1 Maryland Historical Society ......... 2) Dr. John Dean. So jaceceeree sens cee 1 Peabody: Institute... <5. 22s... J. - 1. || Hon. Edward Hverett-.--.-. 5-2. ...- 1 DOT tyds GIANGs Socess -nciees aaceee EN. Dr. BY A. Gouldetc-eesteesacesceciae 8 WrrwouniG: Moms: saccececes cece. 4 || Professor Asa Gray =-s2 esse -2 ese sees 8 ete, Uber. cose ee eeee de tees: 2 || Professor H. W. Longfellow. .-...-.-- 1 Professor J. Lovering-~-----. ..-. << 1 BOSTON, MASSACHUSETTS. Professor Jules Marcou ..... .......- 2 Professor B. Pemcenea-2-- ---e-- ene 8 American Academy of Arts and Sci- i, SW tPutnamecseeeeees tie eee 1 GUCOS sree antes = = ee aeciesenae S6)|(#Dr, aE Sano eeeeseae=eseseaaee 2 Boston Society of Natural History...) 65 || Professor G. A. Schmit...........-. 1 IDowalch library. o-2-. 8 scone Jo Mar., Luttle.. 2 SSae ee cee a ee Se J Bee Berti 6 Masta | a (ORR NR Massachusetts Historical Society. .-... 3 || Academy of Sciences ---.. ----- oe 6 si England Historico-Genealogical Mechanics’ Institute -....-...-..--.- j BOGIOi rer cree oid dame cece! aciee 1 X North asses REVIOW sane sccecnes 1 See peso Perkins’ Institute for the Blind....-. 1 || Astronomical Observatory -..---.---- 7 Prison Discipline Soviety........--.- 1 || Dental Register of the West. ..-.---- 1 Pnblic UaibPar ys top acraw => woe carne s 4 || Historical and Philosophical Society State Library 2.2 5500255. Eee iene mee 4 Of Ohio..:: ake ee eee eeeee ce eoeeneee 1 ite &: hs. Abbatteseeeee css oan x cee 1 || Mercantile Library -..-.-. .-..------ 1 SEs D0 W0 5 ERBIOIR aso Sitiy Sein eina inte A's 1 | John G. Anthony 72-2 ence. e-em 1 REPORT OF THE ASSISTANT SECRETARY. 49 D.—Addressed packages received by the Smithsonian Institution, §¢.—Continued. CLINTON, NEW YORK. Observatory of Hamilton College Dr. C. H. F. Peters COLUMBIA, MISSOURI. Geological Survey of Missouri....--- COLUMBIA, PENNSYLVANIA, Professor S. S. Haldeman .....-....- COLUMBUS, OHIO. Ohio State Board of Agriculture ALO SOTA Yee sie ie cas Sree tices ee ele oe Leo Lesquereux CONCORD, NEW HAMPSHIRE. New Hampshire Historical Society... State Library DES MOINES, IOWA. State Library DETROIT, MICHIGAN. Michigan State Agricultural Society - - Lieutenant Colonel J. D. Graham..-. Dr. Tappan DORCHESTER, MASSACHUSETTS. Dr. Edward Jarvis EAST GREENWICH, NEW YORK, Asa Fitch EASTON, PENNSYLVANIA. Bbrore yi. Cotiny 2202.02.50 eee FRANKFORT, KENTUCKY, Geological Survey of Kentucky State Library GAMBIER, OHIO. Kenyon College GEORGETOWN, D. C. Georgetown College 13 dS a eee Se ass aa siren ac stern seid “ ee ———————————eeeeeeeeoeaoaoaoaoaoamaaaaaaaa9aaaaaaaaqaaaoaaoaaaeaeoaoaoaoaaoeaeeeEeeEeaeEeeEeoeaeEeeEeEeeeEeEeaeaeeEeaaEeaeEeaeaeaEeEeaeaEeaeEeEeEeEeEeEeEeEeEeEee—— eee No. of packages. | woe _ Se DO | ! e HARRISBURG, PENNSYLVANIA. State Library State Lunatic Asylum HARTFORD, CONNECTICUT, Historical Society of Connecticut State Library HAVANA, CUBA. Royal Economical Society...--..-.-.- HUDSON, OHIO. Western Reserve College...-....-.-- Professor Charles A. Young INDIANAPOLIS, INDIANA. Indiana Historical Society State Library IOWA CITY, IOWA. State Wmiversitiy y= crc sees ser JACKSONVILLE, ILLINOIS. Institution for the Blind-..---....--- JANESVILLE, WISCONSIN. State Institution for the Blind... .--- JEFFERSON CITY, MISSOURI. Historical Society of Missouri State Library LANCASTER, OHIO. Dr. J. M. Bigelow LANSING, MICHIGAN. State Agricultural College State Library LEON, NEW YORK. T. Apoleon Cheney LITTLE ROCK, ARKANSAS. State Library LOUISVILLE, KENTUCKY. Colonel Long Professor J. Lawrence Smith Dy. L. P. Yandell No. of packages. = om be ee > bom Jock fed 50 APPENDIX TO THE REPORT OF THE SECRETARY. D.— Addressed packagesreceived by the Smithsonian Institution, §c.—Continued. . MADISON, WISCONSIN. Historical Society of Wisconsin. ----- Skandinaviske Presse-Forening - - - --- State Agricultural Society. -.---.----- State fabranyeases.2-2~--- -4- Beers MONTPELIER, VERMONT. Historical and Antiquarian Society of WennOntea <== -4.2ee: avec re les DiALOMPNDKAl Veco | n-/osaece ccs an Miberi Acer: -\-26s45 f-keldenesee MONTREAL, CANADA EAST. Natural History Society....----.---- Professor Billings...-..--.---.------ Thomash. Blackwell- =. ..<- 22-2... Professor J. W. Dawson....--------- DITA W OPEN. colon = sacs rotesporl Ss unt eee asaeee = M. Toly de Lotbiniere .----- ---..-<- NEW BRUNSWICK, NEW JERSEY. Geological Survey of New Jersey.--. Professor George H. Cook...-..-.---- NEW HAVEN, CONNECTICUT. American Journal of Science and Arts- American Oriental Society. .-..-.---- WaleiCollere: sateen cmc's Sase 58 Professor Ji. W): WManasss45 5h 52 tye 253 IProvesson beuoomiseecesscee ose L ee NEW ORLEANS, LOUISIANA. New Orleans Academy of Natural Sci- NEW YORK, N. Y. American Acriculturist.............. American Ethnological Society. ...... American Geographical and Statistical PUCOUV Eee coe in eee note AStOTeMipIatyes se ee - nee ee ek coe ee Farmer and Mechanic. ..........--.- Histompalepocienyen =>. .oe-2. Journal of Pharmacy -.--........- ae Bodical Cols wees ek a syas deeue New York City Lunatic Asylum. .... New York Dental Journal.-.......-. New York Lyceum of Natural History . No. of packages. | — CO Set ~ —OQ— bet et QD CD woe wD CO WR OTE or No. of packages. | NEW YORK, N. Y.—Continued. University. eacst. aeeeecee ee eee Wi. Coopers = a... ataaeens eee nee ee Dr. Dimper-o aan ieee see eee Dr: Daniel Maton=os--5--saeese esse DEIR STOR ra no 5 ere a ere ee ee DD. Ge lick -. aes te Aeee eee Dr... Harper 3224 -62> es - eee CoBGUUNG 8 soc... once ee G. Ni vluewrenes:. .< ija-26. gasses eee Temple Primeracies sissies -idt-me eee John Redtielimee re. classe sees dames TRenwiCk © pds annen tees ee Dry Johmyloueyers seater eeeee ae Mr. Wiheatlowen ce gaat deta ctaebee Prt pet Bt et CD SE CD mt OD OD bet fet et et 0 CO tt NORTHAMPTON, MASSACHUSETTS. OLYMPIA, WASHINGTON TERRITORY, FRermtonal Wibranyinac seems meets 2 OMAHA, NEBRASKA, State Wibrany:i<.--,.5.4-0deaieseaee 5 OWEGO, NEW YORK. Mr. Pumpelly- 2. oo- <2 s_sstieees vee 5 PEORIA, ILLINOIS, Dr, Brendel. eco ee eee eee 1 PHILADELPHIA, PENNSYLVANIA. Academy of Natural Sciences....-... 114 American Philosophical Society... --- ; Central, High School... .-..- .=-2-2 Dental! Cosmos seeaever seen e = =o = ee Entomological Society .-..-.-...---- PRaniclin, Dn siitite ies ee ee ence aeioee Historical Society of Pennsylvania. -- Institution for the Blind.-..---.----- Wagener Free Institute.............- (Dr. Alien Jo eemstac saa ses ssa ene A.D... Brownisaeecisecceme =< acceer ou —_ ee OOOO RE REPORT OF THE ASSISTANT SECRETARY. 51 D.—Addressed packages received by the Smithsonian Institution, &¢.—Continued. PHILADELPHIA, PA.—Continued. Prd osephseidy . 22. -5- ose seule - Hee Narrone 22248 vs ee Bia AO) rime mes Ss oEEE8 Cig pee os William Sharswood.......--..------ H. S. Tanner George W. Tryon PTOLESSOTVV BONED oes. a5- 1. ose Floratio C.pWioed se. 2-254 2/.+ seasons PRINCETON, NEW JERSEY. Pralempr A. Giyob\. 5... =... --\---< PROVIDENCE, RHODE ISLAND. Rhode Island Histoxical Society... --- State Librar ENGICssOn Ae Oaswelle sete fou sc ke QUEBEC, CANADA EAST, Astronomical Observatory....-.....- WavalyWiniversity... 2c Series lk Literary and Historical Society ..---. QUINCY, ILLINOIS. Dr. John Ritter ROCK ISLAND, ILLINOIS, WP VCN Cie ers). = <=. soe sine esis Benjamin D. Walsh RYE, NEW YORK. Tok a rn eee SACRAMENTO, CALIFORNIA. EY 6 a ao oan cnn an cece ST. LOUIS, MISSOURI. Deutsche Institute fur Férderung der Wissensehatien 5.26.22. s25e5 St. Louis Academy of Sciences. .----- St. Louis University......-.-.------ Dr. George Bernays Dr. George Engelmann .....--..-..-- re Adams Hammer: -....-2.-25esate een Ey SHUMAT A. (== niin) ins neice RNS on ne ola iow wen yer aeroene No. of packages. — Leek fad freed feed fe et et OD GD DO DW DO WO & 0 Wee — ao Se OT et ST. PAUL, MINNESOTA. Historical Society of St. Paul...--.--- SALEM, MASSACHUSETTS. ISSexe LNSbbn Leta voce eee ee SAN FRANCISCO, CALIFORNIA, California Academy of Natural Sci- SANTIAGO, CHILI. Universityscos2 secese sss ecmeie eee SPRINGFIELD, ILLINOIS. State Agricultural Society -..---..... State Library STOCKTON, CALIFORNIA, State Lunatic Asylum TORONTO, CANADA WEST. Bureau of Agriculture and Statistics -. Canadian Institutes. 2) 222s s2j2222 2. Magnetical and Meteorological Obser- vator TOPEKA, KANSAS. State Library TRENTON, NEW JERSEY, State Library UTICA, NEW YORK, State Lunatic Asylum WASHINGTON, D. C. Bureau of Ordnance and Hydrography Library of Congress National Observatory .------4-..-..- Navy Department Ordnance Bureau. -.--...-. Revenue Department .-.-.....------ Secretary of State -----). 22.2... 32 Surgeon General United States Army- Topographical Bureau United States Coast Survey United States Patent Office ......---- No. of packages. 2 Se te oO fet CD eet et DD CD CD eet 52 APPENDIX TO THE REPORT OF THE SECRETARY. D.— Addressed packages received by the Smithsonian Institution, §c.—Continued. si wd ~ 2 | ne os | os Ag Ags ee Fe WASHINGTON, D. C.—Continued. WASHINGTON, D. C.—Continued. War Departmentic.--2-.1- +--+ =-=— 6 | T.. Posche*.0-0 ope eee es 1 Colonel J. Gaberti=-22=.--2--.----- 4 || Captain John Rodgers -...-....----- 1 Professors. WS Bache!.2---- 2-2. 20 |S.) W..iSimim). steerer eee 1 NO Tig © OUCH pee ee ine oa ae! = mmm yare ole ae 1, || HR. Schooleratt ==> =--) eee ee ee J MeO Melber yea mince ee ee 1. ||, Dr. Wi: Stimpson... ---seeee ee fone 5 Captain. M. Gilliss ......- 2252-222] 24. | WevAS tread way 72-eero een ee 1 Generalieimoryesessns ose ene eek 2 || Ul e-store 0 tatoo toto tenner 1 Mien GlOveNeea = eaisae nee a sste ea ala ae L Barons VionsGerolt) 255255 20 sees 1 Dr PSV eleven hos toy oes bas 1 || Captain Charles Wilkes. ........--.- 2 Professor Hubbard. ..---. =.---- ==: 1) SiO bMS emis aces = oe eee ee eee 1 General A. A. Humphreys-.-.-...-.-- 1 Colonelis wi wliono wo eee- ss. o> = = - 1 WORCESTER, MASSACHUSETTS. DP Smith MeCauleyise 5-22-22 ek. -- 1 Professor G. A. Matile --..-.-...---- | 1 | American Antiquarian Society .....-- TRG CEP ENC OS SC ae ete tee ert 273 STNG AN TOO ip A CONS aw wwe et te ttl eee 1, 522 MUSEUM AND COLLECTIONS. It is gratifying to be able to state that the interest in the subject of natural history, which received so material a check in 1861, and showed symptoms of revival in 1862, has continued to manifest itself still more strongly during the year 1863. No better indication of this could be found than in the increase in the number of collections received by the Institution, which amounted to 264 distinct donations in 1863, while, in 1862, there were but 124. Among the collections received have heen many specimens of great interest ; some, the results of special explorations under the auspices of the Institution for developing the natural history of portions of this continent; others, the sponta- neous offerings of correspondents; and others, again, exchanges received in return for donations of specimens on the part of the Institution. No additions have been made by purchase, the Institution not having funds at its command for this purpose. It has, nevertheless, been found that’ a given amount of money can be better applied in meeting the expenses of explorations in particular regions than in buying collections already made. he results thus obtained are usually more varied in their character, and more important, from having been accomplished under definite instructions, and with special reference to the acquisition of facts and information additional to that which would be furnished by the specimens themselves. It is not merely specimens of natural history that are secured in the course of the several explorations, but information is obtained respecting the habits of animals, the ethnological peculiarities of human races, the meteorology, the physical geography, the geology of the country, &c. EXPLORA'TIONS. Among the explorations wholly or partially carried on under the auspices of the Smithsonian Institution, and furnishing results of more or less interest, may be mentioned the following : Explorations by Mr. Kennicott—A brief mention was made in the last report of the return of Mr. Kennicott, late in 1862, after an absence of nearly four years in the north, his movements while there having previously been indi- REPORT OF THE ASSISTANT SECRETARY. 53 cated in the reports of 1859, 1860, and 1861. By the arrival of all his collee- tions, and those of gentlemen connected with the Hudson’s Bay Company, who have so liberally aided him and the Institution in the effort to develop a knowledge of the natural and physical history of the north, we are now enabled better to realize the magnitude of the results of these operations. The collee- tions received in 1863 (which include some which should have arrived in the end of 1862) filled forty boxes and packages, many of them of large size, and weighing, in the aggregate, about 3,000 pounds. ‘They embraced thousands of kins of birds and mae ial eggs of nearly all the birds nesting in the north, numerous skulls and skeletons a animals, fishes in alcohol and preserved dry, insects, fossils, plants, Xe. Not in any way inferior in interest and importance to the natural history collections were those relating to the ethnological peculiarities of the Esquimaux and different tribes of Indians inhabiting the Arctic regions. It is believed that no such series is elsewhere to be found of the dresses, weapons, implements, utensils, instruments of war and of the chase, &c., &c., of the aborigines of Northern America. The cataloguing and labelling of the specimens last received is now nearly completed, and Mr. Kennicott will then proceed to make a detailed report of the scientific results of his operations, as well as those of the various gentlemen of the Hudson’s Bay service who co-operated in the work. The materials at his command will serve to fix with precision the relationships of the arctic animals to those of more southern regions, their geographical distribution, their habits and manners, and other particul: us of interest, and to extend very largely the admirable records presented by Sir John Richardson relative to arctic zoology. The Institution has already acknowledged, in many ways, its indebtedness to the Hudson’s Bay Company, as well as to its officers, for their numerous favors—the company itself, through its secretary, Mr. Thos. Fraser, of London; the governors, Sir, George Simpson and Mr. Dallas; Mr. E. M. Hopkins, the secretary at Montreal ; the chief factors, Governor Wm. MeTavish, Mr. George Barnston, Mr. John McKenzie, Mr. J. A. Grahame, Mr. Wm. Sinclair ; the chief traders, Mr. B. R. Ross, Mr. W. L. Hardisty, Mr. R. Campbell, Mr. Jas. Lockhart, and others, together with Mr. R. W. MacFarlane, Mr. Le Clarke, Mr. S. Jones, Mr. J. S. an the Rev. W. W. Kirkby, Messrs. Andrew and James Flett, Mr. C. P. Gaudet, Mr. John Reid, Mr. Harriot, and others—all have lent their aid towards the accomplishment of the work—every possible facility was given to Mr. Kennicott, every privilege granted within the rules of the company. At all the posts he was an honored guest, and he and his col- lections and outfit were transported from point to point in the company’s boats and sledges without charge. In addition to collections from the region traversed by Mr. Kennicott in his four years’ exploration, some valuable specimens have been received from other points of British North America. Conspicuous among these is a series of birds and eges ae Rigolette, in Labrador, gathered by Mr. Henry Conolly, of the Hudson’s Bay Company’ s service, and brought to Boston, without charge, by Mr. J. W. Dodge. ‘This collection embraced. specimens of the rare Labrador falcon, and Sinai of much interest. A collection of birds and other objects of natural history, made at Moose Factory, for the Institution, by Mr. John McKenzie, has reached London by ship from Hudson’s Bay, and may shortly be expected in Washington. Exploration of Western Mexico by Mr. Xantus.—In iy last report I men- tioned that Mr. John Xantus, so long and so well known in connexion with explorations about Fort Riley, Kansas, Fort Tejon, California, and Cape St. Lucas, was about proceeding to a new field of operations. He left New York on the 11th of December, 1862, for Manzanillo, Mexico, the Panama Railroad 54 APPENDIX TO THE REPORT OF THE SECRETARY. Company and the Pacific Mail Steamship Company, with that liberality they have so steadily exhibited in their transactions with the Institution, having given free passage over their respective routes to himself and his outfit. Mr. Xantus arrived at Manzanillo early in January, 1863, and making this and Colima his principal points of departure, extended his explorations in various directions, especially among the mountain regions. He is still occupied in his labors, the field being very extensive and of varied interest. Many of his col- lections have already been received, and found to contain numerous species of birds, reptiles, fishes, shells, &e., new to science, while others throw much light on the eeographical distribution of the plants and animals of Mexico and Central America. Explorations in Costa Rica—For some time past much attention has been directed by naturalists toward the natural history of Costa Rica, a region which, from its peculiar physical conformation, indicated a fauna quite different from that of the adjacent states. ‘The birds were particularly sought after owing to the many remarkable forms, brought to light by travellers. It was, therefore, with no little gratification that a collection of birds, made by Dr. A. Von Frant- zius, an eminent naturalist and physician, resident in Costa Rica, aided by the Hon. Ci. N. Riotte, United States minister, and Mr. J. Carniol, was received a few mouths ago at the Institution. A careful examination of these specimens proved that the peculiar interest of the fauna had not been overestimated, a large proportion of the species being either new, or but recently described. Additional collections, shortly expected from Dr. Von Frantzius, will, it is hoped, increase still more our knowledge of the species. Miscellancous explorations in Mexico—F ox several years past a highly valued meteorological correspondent of the Institution, Dr. Charles Sartorius, of Mira- dor, has made contributions of specimens of the natural history of his vicinity. During the year several collections were received from him of much interest and importance, especially certain species of Mexican deer, recently described, and but little known. As Dr. Sartorius, aided by his son, Mr. Florentin Sartorius, is now engaged in preparing an account of the animals of eastern Mexico, with special reference to their habits, &c., it is a source of gratification to us to have it in our power to aid him by identifying the species from his specimens, which his remoteness from large collections and libraries prevents him from doing for him- self. Prof. F. Sumichrast, of Orizaba, has also made valuable contributions of birds and mammals of Mexico, and proposes to renew these whenever the con- dition of the internal affairs of Mexico will allow of the transmission of his collections. Dr. G. Berendt, of Tabasco, is also occupied in a similar manner in the interest of science and of the Institution. Explorations in Guatemala and the west coast of Central America.—Mr. Osbert Salvin, an eminent English ornithologist, who has spent many years in the exploration of Guatemala, has transmitted to the Institution a second col- lection of the birds of that region. As these contain specimens of most of his new species, and all have been carefully compared, as far as practicable, with the types, his series of birds is of especial value, as furnishing standards for the identification of other collections. Additional collections of much interest continue to be sent to the Institution by Captain J. M. Dow, of the Panama Railroad Company, so frequently men- tioned in my previous reports. Certain rare birds and fishes collected by him are especially noteworthy. Trinidad.—A collection of nearly fifty species of birds of Trinidad was pre- sented by Mr. Galody, United States consul at Antigua, embracing many species not formerly in possession of the Institution. Jamaica.—Myr. W. 'T. March, from whom the Institution has already received extensive collections in Jamaican zoology, has again made an important contri- REPORT OF THE ASSISTANT SECRETARY. D9 bution of an extensive series of birds’ nests and eggs, the materials upon which he based a memoir on the birds of Jamaica, transmitted to the Institution, to be published by the Philadelphia Academy of Natural Sciences, and printed in its proceedings for November, 1863. Cuba.— Additional collections were received during the year from Mr. Charles Wright and Professor F’. Poey, embracing new and rare species of birds, shells, reptiles, and fishes. Some collections, transmitted by Dr. J. Gundlach, have not yet reached us. Ecuador —The Hon. C. R. Buckalew, now United States senator, while United States minister, resident at Heuador, made quite an extensive collection of the birds of that country, which he has lately presented to the Institution. Nearly all of the species thus obtained were new to the cabinet. ? No collections of magnitude, from regions or localities other than American, have been received during the year. It is not the intention or expectation of the Institution to make general collections of the natural history of the globe, neither its space nor available funds warranting so broad a field of operations. By limiting its labor to America, a hope may be entertained of possessing, in time, a complete series of the animals of the continent. Exotic collections, as far as they are spontaneously offered, and especially such as are necessary to illustrate the characters of American species, are always acceptable, and the specimens gathered by the government exploring expeditions, of which the Smithsonian Institution is the custodian, will always be carefully preserved; but any especial efforts towards the increase of the museum may advantageously be confined, as a general policy, to the New World. The most important additions, it will be readily seen, relate to the class of birds. Desirous of extending the observations upon the birds of North America, as published in the ninth volume of the Pacific railroad report, a cir- cular was issued by the Institution, which has been distributed by the State Department to the consular and diplomatic officers of the United States in the foreign portions of America, asking aid in completing the collection of birds ; and important additions are expected from the request thus extended. The materials received will be used, in connexion with those already in possession of the Institution, in the preparation of catalogues and monographs relative to American ornithology. Among the specimens received by the Institution during the year should especially be mentioned the great Ainsa or Tucson meteorite. This meteorite was first discovered by the Jesuit missionaries in Sonora, by whom it was considered a great curiosity, exciting much speculation as to its origin. In 1735 the “Gran Capitan de las Provincias del Occidente, Don Juan Baptista Anza, was induced to visit the erolite,”’ and found it at a place called * Los Muchaches,” in the Sierra Madre, and, struck with its appearance, under- took to transport it to San Blas, then the nearest port of entry, with the view of carrying it to Spain. With this object it was brought as far as the Presidio, near ‘Tucson, in Arizona, and left there on account of “the ditheulty of carrying it any further. After the withdrawal of the Spanish garrison it was taken into the town of Tucson, set up vertically, and used as a kind of public anvil, of which it bears marks at the present time. In this condition it was seen and reported upon by various travellers; among others it was visited by John R. Bartlett, July 18, 1852, at the time Commissioner of the United States and Mexican Boundary Survey. Mr. Bartlett gives a short account of it, (Personal Narrative, volume II, p. 297,) accompanied by a figure, (the lower one on the plate,) where it is represented as resting upon two legs, owing to the lower part of the ring, of which it consists, being buried in the ground. His estimate of six hundred pounds as its weight falls far within the actual amount. 56 APPENDIX TO THE REPORT OF THE SECRETARY. In 1857, Dr. B. J. D. Irwin, United States army, then stationed at Fort Buchanan, south of Tucson, found this meteorite lying in one of the by streets of the village, half buried in the earth. As no one claimed it, he publicly announced his intention to take possession of it and forward it to the Smith- sonian Institution, whenever an opportunity offered. Some time after, assisted by Mr. Palatine Robinson, of Tucson, (near to whose house the meteorite lay,) he succeeded in having it sent, by the agency of Mr. Augustine Ainza, to Hermosillo, where it remained for some time at the hacienda of Don Manuel Ynigo, father-in-law of Mr. Ainza. In May, 1863, Mr. Jesus Ainza, brother of Mr. Augustine Ainza, and grand- son of Dota Ana Ainza de Iglas, the daughter of Don Juan Bautista Ainza, visited Sonora, and on his return brought the meteorite with him to San Fran- cisco, where it was delivered by his brother, M. Santiago Ainza, to the agent of the Smithsonian Institution, Mr. A. B. Forbes, of the Pacific Mail Steamship Company, and forwarded by him, vza the Isthmus, to Washington, where it arrived in November, and is now on exhibition, and the great object of attraction to visitors in the Smithsonian hall. It is proper to state that, although Dr. Irwin was authorized to expend whatever was necessary to secure the trans- mission of the meteorite to San Francisco, beyond some small expenses paid by him for placing it upon the truck in Tucson, no charge was made by the Ainza family for the cost of transportation to Guaymas and delivery to the Pacific Mail Steamship Company, performed partly with their own wagons and partly by other means of conveyance. It was brought free of charge from Guaymas to San Francisco by the Flint and Haliday line of steamers. While on the route to New York the Pacific Mail Steamship Company and the Panama Railroad Company, with that liberality which has ever characterized their intercourse with the Smithsonian Institution, transported it without expense to Aspinwall, and thence to New York. The meteorite is in the shape of an immense signet ring, much heavier on one side, where it is nearly flat on its outer surface, and presents the face used as an anvil. ‘The greatest exterior diameter is 49 inches; width of thickest part of the ring 9 inches, the least 38 inches ; the greatest width of the central opening, 23 inches; width of thickest part of the ring, 174 inches. The weight is now 1,400 pounds, but some portions have been removed from time to time, probably reducing it considerably. Its composition is principally of iron, with small specks of a whitish silicious mineral diffused through it. A careful chemical and physical examination of the meteorite will be made by Professor G. J. Brush, of New Haven, to whom the Smithsonian Institution has committed the subject for a detailed report. As the erolite was first brought from the mountains north of Tucson by the great grandfather of the gentleman to whose exertions in transporting it to Washington the Institution owes so much, it is proposed to call it the “ Ainsa meteorite.”’ To Dr. Irwin, of the United States medical department, the Insti- tution is also under great obligations for his agency in securing this specimen. Dr. Irwin states that the inhabitants of Tucson have a tradition that a shower of these meteorites took place in the Santa Catarina mountains about two hun- dred years ago, and that there are many other masses of a similar character yet remaining in those mountains. This meteorite is among the largest known, and in this country is only exceeded a little in weight by the Gibbs meteorite in the cabinet of Yale Col- lege, New Haven, while it surpasses the latter in size, being disposed in the form of a ring instead of a solid mass. The Smithsonian Institution also possesses the third largest meteorite in the country in the “Couch meteorite,” weighing 252 pounds, and brought from Northeastern Mexico by Major General D. N. Couch, and by him presented to the Institution. ‘ REPORT OF THE ASSISTANT SECRETARY, 57 IDENTIFICATION OF SPECIMENS. Continued progress has been made during the year in the determination and arrangement of the species in the Smithsonian collections, and the cabinet is gradually becoming more and more useful for reference and study. Any appa- rent shortcoming in this respect will be excused in view of the fact that the work done is mainly a voluntary contribution on the part of gentlemen engaged in making special examinations of the Smithsonian collections, and the Insti- tution is under many obligations for their assistance. DISTRIBUTION OF SPECIMENS. In accordance with the plan of the Institution, as fast as the identification of the species is satisfactorily accomplished, the duplicate specimens are set aside. for distribution to such museums at home and abroad as appear to be suitable recipients. The total number of objects thus distributed to the end of the year 1863, all properly determined and labelled, amounts to 26,651 species, and 50,601 specimens, as shown by the following schedule: Statement of specimens of natural history distributed by the Smithsonian Insti- tution up to December 31, 1863. Prior to 1854. 1854 to July, | 1861 to August, Total. Special distribu- 1861. 1863. tion of shells of Exp’g Exp’n. Specimens. 5 wn mn m wm ro] : 8 i 5 : § é 5 k 8 2 z 2 & 2 & 2 | & 2 & o ° O° o oC 9 2° o oO ° o o o Oo Sz o oO o oO oO Se a a a a a a a a nD 2 R RQ D R R RD BS le | Mammals .... ..---- 5 5 404 624 172 | 216 581 SON eects | cores rds ee ene ns 825 | 1,035] 3,162] 4,255| 1,787 | 2,494] 5,774) 7,784 |.--...-. PUERe GPLUCH oes. .<---~ 18 22} 1,470 | 2,356 18 | 180) le oUOn i 26000) |sasee mean aaa MISMIER See pees 2-22) \San oaiciel= deleeoee 1, 623 |< 3,921 20 28))| 516437) 93) 9492 eee eee eee MIFURUACCAYS oo ncn bs :a|em eo oaiarsea mientras 9360) St B94. eee | Rvs teecr 9 360 TAB OS, ee ere ne eee PUHMLOR Mee as 2c bores see lees oon 551 Gale fone e ae | sem os = 551 Uae \eeieme se Serene Moinsis ee Ll. =: - =|. .ttisenltes ga iaiec 588 |} 1,985 310 380 898 | 2,365 | 10,934 | 44,112 Invertebrates, in- | | REMI ER MOC ata c(ala/at |= wiara ee == fas seeee. 216 330 312 400 528 | Le eeaiase anaes paeetete ae Eggs of birds -.--.-- 114 | 307 | 1,537 | 3,558 G28u eestor 219n ol OOM Ee ance meme HIOEHUINVERtEDIALes-|---~-— <-|- 5 nc moe] ae ee | en le 747 | 2,238 747 | yea let et tel IG EMOCOLUCDLALOS =... |Sroia;0 52725 | tac et aes e aeeoen hematin leeeee dee ba R aR Sey eR pee Sac is Senne ete co Sault ee 58 OG ects ae shee ad 5 63 Goa sateen Minerals and rocks.-|.--..--.. |S tena tetera etetettet 211 354 211 | Do eee aaletee = BR Otal er nina a1). 1,020 | 1,527 | 10,487 | 19,650 | 4,210 | 7,368 | 26,651 | 72, 657 | 10,934 | 44,112 In the index to the three volumes of transmissions of specimens for examina- tion, or donation, the names of two hundred and fifty-nine institutions and indi- viduals are entered up to August, 1863. N. B—The preceding enumeration of specimens distributed does not include the specimens (duplicates) retained by collaborators in behalf of certain author- ized collections—as of insects, by Messrs. Leconte, Uhler, Morris, Ostensacken, Saussure, Edwards, Hagen, Loew, Scudder, &c.; of vertebrate fossils, by Leidy, for the Philadelphia Academy; of fishes, by Professor Agassiz; shells, by Messrs. Carpenter, Binney, Tryon, &c.; mammals, by Messrs. Leconte, Allen. &c.; birds, by Mr. Cassin; reptiles, by Mr. Cope; plants, by Messrs. Torrey, Gray, Engelman, and Eaton. ‘These will probably amount to at least 10,000 species, and 20,000 specimens additional. The cataloguing of specimens in the record-books of the Institution has been continued during the year, and, as will be seen by the accompanying table, now amounts to 86,547 entries, being an increase, since 1863, of over 12,000. 58 APPENDIX TO THE REPORT OF THE SECRETARY. Table showing the total number of entries on the record-books of the Smithsonian collection at the end of the years 1861, 1862, and 1863. 1861 1862. 1863 Skeletons and skullsseceiuc-sseco cose creda sche es oeieeeenisets 4,459 | 4,750 6, 275 Mammals = se- ase ee oe mo = oer awicew = eet ere 5,590 | 5,900 7,175 Bria.) nucck see ay Boe on. ec e te eee 23,510 | 26,157 | 31,800 PROpUUOS 6 23 nwo e Som se mem pm wn inne ms ering enema 6,088 | 6,311 6, 325 Bighes See se eee occa ce en 2 clear ineiclelele wicioin miele [atari 3,643 | 4,925 5, 075 Eggs of birds-.-.-.. -.------2---0- 2s nee te - ba ee ae nan nse 4,830 | 6,000 i, 21D Gristicbans eae ~ fone 2 2 edo es coe mice gnte wen l > ate emia Ly Seta le clacet 1, 287 Mollngls este cn eet cies wi biscl. 266 Seee aseee = =e ene — = 9,718 | 10,000 | 10, 450 Hadintet cess. ict blawets- bce aguell-4-edsesesae Gee a 1,800 | 2,675 | 2,725 MOS S1 Betes eto he mec am alata Rae we clel ore oe ee etal setae a et 1,031 | 2,100 2,550 Maret a Geese aa apne eae ein a sok Siena a been ee ee ete 3,500 | 3,725 4, 925 Ethnological specimens --------------------------++---+---- 550 825 875 Aymelids. 22 senieiine sce scr bate en nsinasalle te ala eee eee 105 109 110 Potal sence oa tne ob sisee SS -ha Sos ce snes Sear 66, 075 | 74,764 | 86,847 LIST OF DONATIONS TO THE MUSEUM OF THE SMITHSONIAN INSTITUTION IN 1863. Atkins, L. S—Eggs of birds and shells from Ohio. Aisa, J.—See ian Akhurst, J—Birds from St. rit Roniaa! West Indies. Baer, O. P.—Unionide from Indiana. Baird, S. F.—Iron ore from Hanover station ; series of skins and eggs of birds, mammals, fishes, and invertebrates, from Wood’s Hole and Cohasset, Massa- chusetts. Baird, Mrs. S. F— Leuciscus, from Potomac river. Beadle, Rev. E. R.—Bergen Hill minerals. Bean, W.—Collection of annelids and cirripeds of Great Britain. Behrens, Dr.—Insects from California. Berlin Museum—54 skins of birds of Central and South America. Bethune, Rev. C. S—Skin of Scalops brewert, Canada. Blackman, Mr.—Skins and eggs of birds, [linois. Blake, W. P.—Keg of fishes from Hakodadi, Japan. Bland, Thomas.—Spiraxis, from West Indies. mo” George A——Embryo Canada grouse in alcohol; skins and eggs of birds Bouve, Thomas T.—Large erystale of beryl. Brass, W.—Birds, imataennle) &e., Fort Halkett. Brevoort, J. U—Fresh specimen of Zoarces anguillaris. Bruckart, H. G.—Insects trom Lancaster county, Pennsylvania. Buchalew, Hon. C. R.—Collection of birds of Ecuador. Burling, W.—Skin of Halietus pelagicus from the Amoor river. (Through Samuel Hubbard.) Carniol, J—Skins of Costa Rican birds. Carpenter, P. P.—Yossils from vicinity of Moscow. Carpenter, Robbie S.—Skin of starling, Sturnus vulgaris, Warrington, England. Clark, Lawrence-—A general zoological collection ‘from Fort Rae, Great ‘Slave lake. Coleman, Lyman.—Seeds of Damascus thorn; petrified wood from Cairo. Coleman, W. T.—Birds and eggs from Canada. Comstock, A.—Cuttings of California grapes. REPORT OF THE ASSISTANT SECRETARY. 59 Conolly, H—Skins and eggs of birds from Labrador. Cooper, Dr. J. G.—Shells of California. Coues, Dr. H.—Series of skins of birds of District of Columbia. Cowles, P. W—lInsects trom Vicksburg. Crosier, Dr. E. S—Vorticella, &e., New Albany, Indiana. De Saussure, Dr. H—Skins of Mexican birds, and lacustrian antiquities of Switzerland. Diebitsch, Professor —Rana pipiens. _. Dodd, P. W.—Skulls of animals and eges of birds from Sable island. Dow, Captain J. M—Skins of mammals, and birds, fishes, &c., from west coast of Central America. Drew, Dr. F. P.—Collection of reptiles and eggs of birds from Kansas. Drewsen, Charles—Series of Greenland shells. Drexler, C.—sSeries of skins of birds of the District of Columbia. Egleston, Thomas.—Series of Eurcpean fossils. Elliot, D. G.—Skins of European gulls; skins of humming birds. Elliot, H. W.—tUarge collection of “Uiionides: shells, &e., in aleohol, Ohio. Engelmann, Dr —? ossils from Llinois. Fairbanks, Professor —Box of eggs. . Fay, Joseph S—Chlorastrolite from Lake Superior. Flett, Andrew.—Skins and eggs of birds; Fort Normann. Flett, James —Kges of birds, ‘ke. from in Pierre’s house. Foreman, Dr. H—Vive boxes of minerals from Maryland. Freiburg, Mining Academy of—Box of mineralogical and geological speci- mens Gin Germany. Frick, Dr—Shells of California and Japan, Galody, M.—Skins of birds of Trinidad. Gaudet, C. P—Skins and eggs ot birds, &c., from Peel’s river. Gibbs, George.—Indian curiosities. Gilliss, U. S. N., Captain.—Six boxes of microscopic soundings. Gilpin, Dr. J. B—Series of shrews and mice of Nova Scotia. Goldsmth, Dr. M.—Cricket from the Mammoth Cave, Kentucky. Gould, Dr. A. A—F¥orty species of Melaniade. - Grahame, J. A—Skins of mammals, &c., Norway House. Giebel, Dr. C—Three boxes of insects of Europe, (365 species.) Gruber, Ferd—Skins and eggs of birds from California. Gundlach, Dr. J—Specimenus of Gundlachia, Cuba. Gunn, Donald.—Skins and eggs of birds from Red River settlement and Lake Winipeg. Haideman, Professor S. S—Types of the species of Melaniade described by him. Hall, W. F.—DBirds and eggs from Massachusetts. Hamilton, R—Collection of skins and eggs of birds from Great Whale river, (through Mr. George Barnston.) Hardisty, W. L.—Birds, mammals, &c., from Fort Liard. Harris, W. O.—Minerals from Chester county. Harriot, Mr—Skins of birds from Fort Anderson. Hays, Dr. W. W.—Fishes, &c., from Sacramento river. Hayden, Dr. F. V.—Al\coholie specimens, Beaufort, South Carolina. Haymond, Dr. R.—Cypris from Indiana. Hephurn, James.—Skins and eggs of birds from the Pacifie coast. Hibbard, Francis —Lead ore from New Brunswick. Hibbard, James.—Antimony ores, New Brunswick. Hitz, R. B. § George.—1,200 eggs, of twelve species of birds, from Northamp- ton county, Virginia, with shells: &e. (See also Stimpson.) Fossils from Aquia creek. 60 APPENDIX TO THE REPORT OF THE SECRETARY. Hoge, Mr.—Skin of boa from the Serapiqui river. Hope, John.—Eggs of birds, fishes, &c., Great Bear lake. Hotaling, C. F.—Rock salt from Louisiana. Hoxie, W—Insects from Massachusetts. Hoy, Dr. P. R.—Nests and eggs from Racine. Hunt, General L. C—Indian knife, Klamath lake. Irwin, Dr. W. W., and J. Ainsa-—Meteorite from Tucson, weighing 1,400 pounds. Jeffreys, Mr.—Box of minerals of Chester county, Pennsylvania. Jones, Strachan.—Kggs of birds, &c., from the Yukon. Julian, A. A.—Series of fishes, &c., Sombrero island. Keep, Rev. Marcus R—Moose horns from Maine. Kennedy, Dr. H. W.—Collection of reptiles of Uruguay. Kennicott, R—Insects, eggs, &c., from Illinois. Kennicott, R., and others ——Fitteen boxes, three bales, one keg, and one chest of Arctic collections. Mr. Kennicott’s collections principally from the mouth of the Porcupine river, Peel’s river, Fort Good Hope, La Pierre’s house, Fort Resolution, &e. Kirtland, Dr. J. P-—Two boxes of western Unionidae. Krefft, Dr. G., (through W. Cooper.)—Collection of Australian reptiles. Krider, John —Mounted hawks. Lapham, I. A.—Unionide of Wisconsin. Lawrence, George N—Skins of birds from Central America and Panama. Lea, Isaac—Box ot Unionidae, and one hundred species of Melaniade. Lewis, James, Dr—tWLarge collection of land and fluviatile shells from the in- terior of New York. Lockhart, James.—Large series of zoological specimens, principally birds’ eggs, from the Yukon; skins of birds, mammals, eggs, &c., from Fort Resolution. Lykins, W. H. R.—Fossils from Kansas. MacFarlane, R. W—A general zoological and ethnological collection from vicinity of the Anderson river, Arctic America. McGuire, J. C—Two boxes of Unionide. Mc Kenzie, Hector —Birds’ eggs from Red river. McKenzie, J—Birds, &c., from Fort Resolution. Mc Kenzie, Roderick.—Birds’ eggs from Lake Manitobah. McMurray, W.—Birds’ eggs from Winipeg river. Mac Tavish, Gov. William.—Skins and eggs of birds, &c., from the Red River country. : Mann, William.—Skins of Pinicola canadensis, Lake Superior. rene W. Thomas.—Three boxes of skins, nests and eggs of Jamaican irds. Meck, F. B.—Series of fossils from New Jersey and Maryland. Moore, Carleton R—Double tail of Limulus. Michener, Dr. E.—156 crania of birds, and 54 of mammals; two boxes of minerals. Onion, J. S—Plants, eggs, &e., from Fort Good Hope. Palmer, Dr. E.—F¥ossils, minerals, &c., Pike’s Peak. Parker, Rev. H. W.—Marine shells, United States, and two boxes of minerals from New Bedford. Parkinson, D. T—Skins and eggs of birds, Indian skulls, plants, &c., Fort Crook, California Philadelphia Academy of Natural Sciences —Seventy species of Melaniade. Piper, Col., (10th regiment New York volunteer artillery.}—Rock specimens and fossil wood from Fort Meigs, near Washington. Poey, Prof. #.—Collection of bats and Neuroptera ; fishes from Cuba. Poole, Henry —* Cone in cone” in slate. From a shaft sunk in the Harbor Vein coal seam, Little Glacé Bay, Cape Breton. REPORT OF THE ASSISTANT SECRETARY. 61 Prentiss, D. W.—Series of skins of birds of the District of Columbia. Quackenbush, Leslie R.—Fossils of the Utica slate. Reed, John —Skins and eggs of birds from Big Island, Great Slave Lake. One collection through L. Clarke, jr. Reed, Peter —Sorex platyrhinus, Washington county, New York. Richards, Thos.—Skins of birds, &c., from 'Temiscamingue. Riotte, Hon. U—Reptiles and insects in alcohol, skins of birds, shells, &c., Costa Rica. Ritchie, J. P—Skin and egg of Buteo pennsylvanicus from Massachusetts. Rodgers, Commodore John—Ethnological collections of the North Pacific Ex- ploring Expedition. Ross, B. R.—A general zoological collection from Fort Simpson and vicinity. Rousseau, E.—Box of shells from New York. Saemann, L.—Box of European minerals. Salisbury, Dr. S. H.—Scalops in alcohol from Fairfield county, Ohio. Salle, A—Skins of Mexican birds. Salvin, O.—Collection of birds of Guatemala, (150 species.) Sartorius, Dr. C—Collection of birds, mammals, alcoholic specimens, &c., Mexico. Schmidt, Dr—Birds from the vicinity of Washington, collected by the late Chas. F. Schmidt. Sclater, Dr. P. L.—Skins of Mexican birds. S¢mpson, George B.—Copper spear-head, and other relies. Sitka, Governor of.—Box of crustacea. (Through Mr. Jas. Hepburn.) Springer, P. M.—Skins and sterna of birds, [inois. Stimpson, Dr. W.—Three boxes of marine invertebrates of Great Britain; two of American. Stimpson, Dr. W. and R. B. Hitz —Three boxes shells, eggs, &c., Northamp- ton county, Virginia. Sumichrast, Prof. F—Mammals and birds of Mexico. Surgeon General—Tertiary fossils, Suffolk, Virginia. Swan, J. G.—Indian curiosities, skins of birds, eggs, shells, fishes, &c., from Puget Sound. - Thomson, J. H —Box of New England shells. Tolman, J. W.—Skins and eggs of birds of Illinois. Trumbull, George—Wavellite from Chester county. Tryon, G. W.—One hundred and twenty-five species of Melaniade. Olke, H.—Skins of birds from Wiinois. Van Cortlandt, Dr. E—Mammals in alechol, skins of Lepidosteus, &c., from Ottawa. Frantzius, Dr.—Collection of birds and mammals from Costa Rica. Velie, Dr. J. W—Eges of Protonotaria citrea, &c., from Illinois. Vienna Gevlogisches Reichs- Anstalt——Collection of Austrian fossils. Walker, R. O—Fishes, shells, skulls, &c., Allegheny county, Pennsylvania. White, Dr—Marine shells and skulls of mammals, Isthmus, Panama. Willis, J. .—Shells, eggs, and fishes of Nova Scotia. Williams College Lyceum,— Eggs of Greenland birds. Wilson, N.—Seeds of plants from Jamaica. (Through Thos. Bland.) Wingate, J. D.—Box of shells, Bellefonte, Pennsylvania. Woodworth, Dr. J. M—Reptiles and insects from Memphis. Wouton, W. G.—Skins and eggs of birds of Nova Scctia. Wright, Chas.—Birds, shells, and insects of Cuba. Wynne, Dr. Jas —Specimen of sphinx or hawk moth from Central America. Xantus, John—Fourteen boxes of mammals, birds, and other animals, plants &c., from Manzanillo, Colima, &c. 62 APPENDIX TO THE REPORT OF THE SECRETARY. LIST OF WORKS PUBLISHED IN 1863. (155.) Ancient Mining on the Shores of Lake Superior. By Charles Whit- tlesey. 4to., pp. 32, and one map. (Published April, 1863.) — (146.) Meteorological Observations in the Arctic Seas. By Sir Leopold McClintock, R. N. Made on board the Arctic searching yacht “ Fox,” in Baflin’s Bay and Prince Regent’s Inlet in 1857, 1858, and 1859. Reduced and discussed at the expense of the Smithsonian Institution by Charles A. Schott, Assistant United States Coast Survey. 4to., pp. 160, and one map. A small edition of this work was published in May, 1862, but the final issue, with corrections and additions, took place in 1863. (166.) Records and Results of a Magnetic Survey of Pennsylvania and parts of adjacent States in 1840 and 1841, with some additional Records and Results of 1834, 1835, 1843, and 1862,and a map. By A. D. Bache, LL.D., F. R. S., Member of Corresponding Academy of Sciences, Paris; President of National Academy of Sciences ; Superintendent United States Coast Survey. 4to., pp. 88, and one map. (Published October, 1863.) (169.) Researches upon the Anatomy and Physiology of Respiration in the Chelonia. By S. Weir Mitchell, M. D., and George R. Morehouse, M.D. 4to., pp: 50. (Published April, 1863.) (156.) Catalogue of Minerals, with their Formulas, &c. Prepared for the Smithsonian Institution by T. Egleston. 8vo., pp. 42. (140.) List of the Coleoptera of North America. Prepared for the Smithso- nian teen by John L. Leconte, M.D. PartI. 8vo., pp.60. (Published March, 1863. (167.) New Species of North American Coleoptera. Prepared for the Smith- sonian Institution by John L. Leconte, M.D. Part I. 8vo., pp. 94. (Pub- lished March, 1863.) (142.) Bibliography of North American Conchology previous to the year 1860. Prepared for the Smithsonian Institution by W. G. Binney. Part I. American authors. 8vo., pp. 658. (Published March, 1863.) (171.) Monograph of the Diptera of North America. Prepared for the Smith- sonian Institution by H. Loew. Part II. Edited by R. Ostensacken. 8vo., pp. 340. (Published January, 1864.) (160.) Instructions relative to the Ethnology and Philology of America. Prepared for the Smithsonian Institution by George Gibbs. 8vo., pp. 36. (Published March, 1863.) (161.) A Dictionary of the Chinook Jargon or 'Trade Language of Oregon. Prepared for the Smithsonian Institution by George Gibbs. S8vo., pp. 60. (Published March, 1863.) Systematic index to the list of foreign correspondents of the Smithsonian Institution, corrected to January, 1862. S8vo., pp. 16. Appendix to the list of foreign correspondents of the Smithsonian Institution, corrected to January, 1863. 8vo., pp. 7. (170.) Comparative Vocabulary. Reprinted from the Smithsonian Instruc- tions relative to ethnology and philology. 4to., pp. 20. (Published May, 1863.) WORKS STILL IN PRESS. (174.) Bibliography of North American Conchology. By W. G. Binney. Part II. 8vo., 239 pages stereotyped. (143.) Synopsis of Air Breathing Shells. By W.G. Binney. 8vo. (144.) Synopsis of North American Vivipara, &e. By W.G. Binney. S8vo. (145.) Monograph of American Corbiculade. By'Temple Prime. 8vo., (42 pages in type. (177.) Check-list of North American Fossils; cretaceous formation. By F B. Meek. 8vo. REPORT OF THE ASSISTANT SECRETARY. 63 (172.) Paleontology of the Upper Missouri. By F. B. Meek and F. V. Hayden. 4to. (165.) Monograph of North American Bats. By Harrison Allen, M.D. 8vo. a On the Microscopic Structure of the Medulla Oblongata and the 'Tra- pezium. By Dr. John Dean. 4to. (175.) Discussion of the Magnetic and Meteorological Observations of Girard College. By Prof. A. D. Bache. Part VII, VIII, IX. 4to. (179.) List of publications of learned societies, periodicals, and encyclopedic works in the library of the Smithsonian Institution, July 1, 1863. (178.) Monograph of North American Hymenoptera. By H. De Saussure. Part I. Edited by Edward Norton. 8vo. LIST OF METEOROLOGICAL STATIONS AND OBSERVERS SMITHSONIAN OF THE FOR THE YEAR 1863. INSTITUTION Name of observer. BRITISH AMERICA. Acadia College Baker, J. C Clarke, Lawrence, jr Connolly, Henr Delaney, Edward M. J..-. Everett, Prof. J. D........ Flett, Andrew Hall, Archibald, M. D McFarlane; R.....-..-.- ; Magnetic Observatory Murdock iG 25 -S.o.5-25 526 Phillips, H Rankin, Colin Richards, Thomas MEXICO. Laszlo, Charles Sartorius, Dr. Charles CENTRAL AMERICA. Riotte, C. N White, William T., M. D-. WEST INDIES, United States Consul Julien, Alexis A BERMUDA. Royal Engineers, (in the Royal Gazette.) SOUTH AMERICA. Hering, C. T * A signifies Barometer, Thermometer, Psychrom- eter, and Rain Gauge. B signifies Barometer. T signifies Thermometer. colony of Surinam, Dutch Guiana. P signifies Psy chrometer. R signifies Rain Gauge. N signifies no instrument, t Above Lake Ontario. g g ® Station. = sy 8 . a 2 at a Z z e) 5 3 2 © A A e je) 4 Cm ek Feet. Wolfville, Nova Scotia --.---------- 45 06 | 64 25 Ooi eA Stanbridge, Canada East -.-....----.- 45 ).083|\ ava) OOM =): = 5 ec TD Sscen Port Rae Greatislaye wakes. <-—ee]. ose o> as) sobre taelpeeees ae ese Lat Gis MW eG ly ee Se eee aaa ee 55 loss saaac eae acsos eS os Colonial Building, St. John’s, New- | 47 35 | 52 40 TO Be eka = foundland. : King’sCollege, Windsor, NovaScotia-| 44 59 | 64 07 DOONAN avec. | Fort McPherson, Hudson’s Bay Ter- | 68 00 | 135 00 OCT teeeme eer ritory. Montreal, Canada Bast ....---.----- 45 30 | 73 36 57 || Avas some HorteAmdersoniesseeeeeeeeaeeiee eee 68530 Te SOR ee eta el aati ROT GOT Be ete te et chet] eee te rete itera Saisie sie Toronto, Canada West ----.--..-... 43 39 | 79 21 TLOB HACE tees Sta doliney Newari 8 yy closer eete | cleat [teeter = reciente tern Niagara, Canada West.........-.-.- 43 09 | 79 20 hn PAs ecuatates Michipicoton, Canada West -..--.--. A756) “Bo OGNieo eee Bre = Kenogumissee, Hudson’s Bay Terri- | 49 50| 8400, 1,000} T....... tory. San Juan Bautista, Tabasco........ 17 47 | 92 36 BONIPAC Se saree Mirador Wer Orogicnss-cceise = cece 19 15)|" 963255 eS TGOU MAL ane Sani 0s6), Costa Rica... -.acccre science 9) 540 Ran OGn S72) | ME eee npn yale eee ee ane sae aaa D1 Oa a eee se ees cities TMurkisslsland & == qe cec ats ais ne wie celal | = a\x acc aime | eaters balstmter atmo (eieimteeentister ie Sombrerotisland!=~--ecvensacte nan 18 55 | 63 27 AS | At eee. Centre Signal Station, Saint George’s.|........|.-------|-------- PAs iniiein ats Government Plantation Rustenberg, |...--.--|.----0+-|-...--0- AG a aiaants No. of months received, e PA MRR PNWOWN w Bm Wr TI a) ll 12 12 12 METEOROLOGICAL OBSERVERS. List of meteorological stations and observers, §:c.—Continued. S 3 . 2 z z Name of observer. Station. County. 3 a ; = 4 S a 5 = é 2 2 A = 5 a CALIFORNIA. a rae Feet. Ayres iW. ©. Mi. D-.-- -- | San Francisco ..-| San Francisco---| 37 48 | 122 27 130! | Aveo Belcher, W. C....-------- | Marysville .....- Mapas 26eeee. 2 39 29 | 121 30 80 | B.T.R.. forott) Cnaries....-+--—-. - - Sacramento .-.--. Sacramento -.-.--. 38 31 | 121 29 60: Ree Dunkum, Mrs. Elizab’h S-; Honcut -.....-- Wuba 2. S25 2+. SO SoA S0NT: <3. eee se sen Logan, Thomas M., M. D..| Sacramento -«--- Sacramento. ..-- 38 35 | 121 28 AL Abscess Parkinson, David F -.---- Presidio of San | San Francisco--.| 37 48 | 122 22 |.--..-.-. AS sea Francisco. mith, Ma 2. ..<---..--- Spanish Ranche-.| Plumas---..----- 39 56 | 120 40} 3,700 | B.T.R.. COLORADO. Ly Lutirell, James-..-.-..-..-.-- Montgomery .. --| Park .........-- 39 00 | 106 00 | 13,000 | T..----- CONNECTICUT. ; Gane Jarvis. s-<=220<5-- Canton 52 2062 Hartford 22%... 4200} 73 00 ODL EE RA eee Hunt, Rey. Daniel -.----- Wonifret=- 33. - 22 Windham ....-... 41 52| 72 23 SBT PGA. 25 eciee Johnston, Prof. John ...-- Middletown - ....| Middlesex -.....- 41 32) 72 39 LTO RAPS Ruse Learned, Dwight W-.----- Plymouth .....-- Litchfield - ....-- 4) 40 | 73 03 |~...--. ae es Leavenworth, D. C-.-.-.---- New Haven..... New Haven ...-. 4118] 7256 40)). BAR 3 Rockwell, Charlotte ------ Colebrook ....--.- Litchfield. ....... AD, OOH S37 0G) 3556-55 Ps ade Yeomans, William H..--. Columbia. .....-. Tolland ......... 41040) |S i242) \. 2. 5 Te ess DAKOTA. Williams, Herbert G.--.--- Peet N Eee alae ela nites ADE la ee Odeo on eee aerate DELAWARE. Hedges, Urban D., M.D--.| Wilmington ..... Dey Cast ener ee eer eee oat Te oe ee DISTRICT OF COLUMBIA. MacKee, Rey. C. B ..-.--.-- Georgetown ..... Washington ..... eae Adm CeSh nism (a wie/a,s AR Feats Smithsonian Institution-..| Washington -.... Washington ...-- 38 53 | 77 01 600) Areas FLORIDA. Dennis, William C.-....-.-. Key West -..-...- Monroe, 24 =~ aa 24 33 | 81 28 16) (Bits Be: IDAHO. nein © 2-5 5-—------ Morinsramie. 22) |se sees 4210} 104 47} 4,472) T....... imosseau, M1. ©.......-.--- Rorts Benton +2 .: |2e==ee aes 47 A9\\ VO 36: 1! °2) TSO Nese ILLINOIS. wmidrich, Werry ..--------- TUuNKi Wall. oo Bureau ...-=-5-- 4115! 89 66 69.0 eS re BSBHEOCKG, Ur == 565------ = Riley 22-0 sss McHenry. .-..-.--. 4211] &8 20 1604 Reais s BACON eon aa ns - Willow Creek 2.-/ ee. ----- = -<-2-2 41 45)) 88 '56') 10405) Nose e et Baker, Nathan T......--. | Belleville........ Sti Clanineis =: 38 2 90 06 600 | B.T... Ballou, N. E., M. D.--.--- Sandwich ..----. Doe) Kalbiciie'..2 2: 41 31 | 88 30 663) ake 22 Bandelier, Adolphus F.,jr-| Highland - ..-.... Madison ........ 38 45 69046) .ceeeees BT. 2. Blanchard, Orestes A-.... Mimira.-.5-s eee Pankey eae AT 327) 2SOito} aes ae ote 2 Boettner, Gustav A...--.- @hicapoe--e ess Cooks. stn semase 41 54 SOr4Dt le sso Bee oss) Brendel, Frederick, M. D..| Peoria .-.. --.--- Peoria... sce eee 40 43 | &9 3 AGO} AY 2) 2258 Brookes, Samuel..-...--. Chicago -2 2. 2-5 Cooks eee Ee 42.00 | 87 30 |.....-.. T4255 22 | Byrne, ArthurM ..--...-. Chicago. 22e=2 8 Gopkssse ee: 32 41 57 | 87 38 Sok EDar ee Ee: Himothy-<-... Jacksonville -. ..| Morgan. ........ 39 30} $0.06 GO| TR et meme; PON =- 2 5-2... - | 2 Grant, Miss Ellen._.._... Manchester -..... SEOth oo. = oa Soe |} 3933] 90 34 683 "(SAS ose Griffing, Henry .-.. ...-.- Hazel Dell..--.--- Cumberland -- --. 39 OOH 88100) |--- =. ine eeees | Little, J. Thomas .--..... Dixon :.2..s-seee eee 30. 2 AWA SOS) S22 ----- ee Saoe| Livingston, Prof. Wm -...| Galesburg -.----. Ranoxye. soc aet [een ae -F| aareee le oceans Aner ee on Mead, 8. B.)MD.......: | Augusta .... <--- Hancock’: 2: << ./-. 4010); 91 00 R204 | eevee oc Merwin, Mrs. Emily H....| Ottawa.-..------ Ba Salle-se222 =e 41 20} 88 47 SAMO | RR are NOC SS Ol: . Pekin -..2.2c-cee Tazow ellisee AQ*S60|TaeOros||.—.-/--- iB: Doss Rogers, O. P. and J. S....| Marengo....--..-. MeHoenty 29228 32 4214| 8&3 842 ) B. T. R.. Tolman, James W.....--. Winnebago De- | Winnebago .....| 4217] 89 12 900 | B. T. R-. pot. INDIANA, Anderson, Henry H...... Rockville -.. .-.. Parke': soca <2 oon 36 00} 8700] 1,100; T.R... Burroughs, Reuben.....-. South Bend - .... St. Joseph. -.-... 41 39 | 86 7] 600), P.BRe e8 * Above low-water mark at Quincy. os of months received. No. rer A WOHPH MOO He DH ON Ww b Hh mo _ 2M WO WWVWMWH Wh —, = 66 APPENDIX TO THE REPORT OF THE SECRETARY. List of meteorological stations and observers, §c.—Continued. : oS 3 3 Name of observer. Station. County. 3 a 3 3 m o ° b 2 | = INDIANA—Continued. or Cray Chappellsmith, John. .-..-. New Harmony..-| Posey ----------- 38 08 | &7 50 Crozier, Dr. ©. S...-.---- New Albany.-.---- Floyd ---.-.------ 38 02 | 8&5 29 ve Claas: Spesee.6. | Hemry ----.-.--- 39 55.| 85 20 Dawaon, William -- -- ) | Spiceland . ...... Henry -} a Feet. ° Brat Wee ae Baie aon 1 1,060 | T.R .. A, Sosa Bo: 600 | T.R-.- jase eee Bay = 600 | T.R.. 800); Nijee ee 698 | TLR -.a. 800 | T. P. R-: 1,000) | Bass 2s eaiae ae BRB A ae masons | TT Bisse Tot WAS secon ae ings =¥ Se Wt Bases nie raie Sate Ni =. 438 AQ PRR? a. a5 eae IN| tekiaese pas |, SSR. 6S6a | PA eee 950 | T.R. 1500) eee: Ae gtk TTR era Cleon BE aoe 14258) Re) 22 Gol An cee L eee er ee Sie ae re OO! | PAU is erniate etal PRR oko SSR #Nigss2- <= 1300) aR, ose GOR AER ae clasts ANOOON eke Ree S77 ON pki eeee ee 940 || PAss ase: creo are A thats STOMA ooycece sbaieiaasaente TP ae 100") PAs ee 90 | B. T.R..| 8000] Rese 130 | T.R....| SOU -Ateeesk = ‘ re oe | ae iar 1) Bun 2s Se cidiate Sha Ninctieeeg pine Bie ae wea. ORe os ss 700) Eee 2 TT anaes | 700) || Dae: Res oe wera eee DB ce cme QD) || A eiee sate | No. of months received. , WWRAAWwCeNwoens | w me ~— I BK ne wo VW ACHKRUG JN at ae WKwWP WW AW = 12 i0 12 METEOROLOGICAL OBSERVERS. List of meteorological stations and observers, §c.—Continued. 5 S oO ™ ; a): By) aa : 3 = # a3 Name of observer. Station. County. = = 5 as 3 a ‘ é % a S a 5 $3 5 2 2 % a" ’ A = ss a A MARYLAND—Continued. ’ oy oo Feet. Hanshew. Henry L..-..-.-. Frederick ...--.- Frederick . -...-- BO AS MlerO) | a = =e Aa jeee 1 Lowndés, Benjamin O....] Bladensburg.--.. Prince George’s..| 38 57 | 76 58 dd. | eet nhE Stephenson, Rey. James-.-| St. Inigoes....... St. Mary’s-..-..-- 38 10} 76 41 49~|| Ba coors © 12 MASSACHUSETTS. Astronomical Observatory.| Williamstown ...| Berkshire . ....-. 42 43 | 73 13 686 | B. T. R..- 7 Bacon, William =. ......-- Richmond...-.-.-- Berkshire .....-- 42 23.) 73 20 TWO OM Sas Rayer = 6 Barrows, N., M. D....--- Sandwich . ....-. Barnstable ...... A TASY | FORO | Ses aie ayes cient we 9 Caldyvell, John H......... Topaheld’: 22. -=-| UR8OX =o 25s Se so PEO K He So osc Tae 8 Davis, Rev. Emerson... .. Westfield. .....-.. Hampden .-.-.---.| 4206 | 72 48 USLON NESS WSS 12 Dewhurst, Rey. Eli -..--- Baldwinsville. ...| Worcester ....--. 42 37 | 72 05 847 | B. T.R 10 Palion, John ages: =. ---.- Lawrence ....-.. EISs@X) 2 :.enesrmcies 42 42) 7111 Tada Aseey =65- 3 fetcalf, John Geo., M.D-..}| Mendon ..-.-...... Worcester -..-..- 4206) | ile Saee. 2s ee Bod; He. 12 rentiss, Henry C., M. D-.| Worcester ......- Worcester =<.---- 42 16| 71 438 SRO eA. 2s es 7 Rodman, Samuel ..--..--.. New Bedford....| Bristol .....-.-.. 41 39 | 70 56 OO) | av cm roe 11 Spell) Prot by Sy. . 222. -- Amherst .... +... Hampshire --...- 42 22 | 72 34 BT a eA a ues Bes 12 MICHIGAN. Blaker, Dr. G. H...---- : Pern {| Marquette ......- Marquette ....... 4633 | 8733] 620| A...... 7 Kedzie, Prof. R. C.-.----.. ansinp)-2.)34-.2 Tn ham tetra ye AAD) | Banos | hm «oe Josd Ais 3.6824 5 Schetterly, Henry R.--.-. Northport -.----. Leelenaw - .-...- 49: 23:4) .80). 24) |... .--5. Dec erna 6 Bren ea. Ene ei cet. Holland <-):..5...) Ottawa .c.2--2 42 00 | 86 00 6800 a 12 Van Orden, Wm., jr------ Clifton). $25 2)4.<: Keweenaw ...... 47 0G | 88 00 800) ace aes Ls Whelpley, Miss Florence E.| Monroe..--.-.... Monroe sees-- + 41 56 | 83 23 590 | T.R 12 Woodard) (CS. ac. -nioon Ypsilanti........ Washtenaw ..... 4215] 83 47 COL AS oe acces 10 MINNESOTA. Grave, Mary A..-.-\.-.-.. Tamarack ....... FLORMG PIN bese ac collate cine |S oe cle TS ee 6 CO appli aan ian 2c) IN fo ee oes ae eee AMON) 5 faden es: 45 15 | 93 28 S061 | ler 3 Paterson, Rev. A. B.,D.D.| St. Paul -.......: Ramsey)---.:.=-. 44 57 | 93 05 S000) aR. =. 12 mimith, Henry I.....-...- Forest City-...--. Meeker, = si-- cs: AD AS) || (OS 28) ais. ser Tits 11 PAGING Cette aia t ooinin nal Beaver Bay -..... akew == )- me 47 17) 91 18 | 657 | B.T . 12 MISSOURL Christian, John........... Harrisonville >. ..5|) Casseo-2b5 oas-it|o<= sasedueneees|s 206. oo viene 12 Engelmann, George, M.D-.| St. Louis..-..... St. Louis....-.-. 38.37 | 90 15 481 |) A step ates if Fendler, Augustus. .....-. Sty Mouisten se. - 3 Sti Donises-ccc.: 32 37 | 90 16 470 |) Bo Donk e 6 Sa is a Laborville ...... Stlonisssacsa5 Se oon eQOhMss |... . 2. <2 {Rea 1 ONE DEAE clocie wans =~ Kirksville ....... A dairmeeaysaeen\ 40 38 | 9250] 1,000 | N....-..- 2 ney, George P.-.....---. Canton --5 4h! We wis seses,t-% BOT ARO dnd Bl = = 6/0 = cra ieee 12 Tidsweil, Miss Mary Alice-| Warrenton ..-.-.. Warren ......-.| 3837 | 9116 820) | iveeeeeea 7 NEBRASKA. Bowen, Miss Anna M. J...| Elkhorn City ....) Douglas -......-. A 235) 967125) 1,000) | Mie cece 12 HAR, GON ....£-- 2-2 -. Fontenelle ...... Washington ..... 41 31 96 45 MS OOOs Wee ktanere 5 Hamilton, Rev. Wm....-- Bellevue seee- 2 Sarpy: sete serene AL TOBN pe Qo eon |ereretaieral ste ISVS taj ll NEW HAMPSHIRE, Brown, Branch .-.. --.-... Stratford ........ C008) 225 - =< <-sa08 BOOB Fails ote eel OUD! einen Rare lara 12 SeUHAG, TIMMS >. <2 .. = Claremont ...... Sullivan ........ 43 22 | 72 21 539 | B. T. R 12 French, Isaac §., M. D..-.| Loudon Ridge ...| Merrimack .. .-.-. 43 20 | 71 25 4734) TE Bsa 2 Nason, Rey. Elias .-....-.. FXeLer 55 sae oe Rockingham... .. 42 58 | 70 55 125) 0B. hie 9 Odell, Fletcher .... ...... Shelburne -....-- Coon = 2; o=sh. 3-5 44 23 71 06 1005). 2 12 Pitman, Charles H.-...... North Barnstead.| Belknap.....---. ASvOSul sede | 2 inie<.< 5 eee ees 10 eetith, Hennes ots North Littleton ..| Grafton... ...... BAO RW ELON S22... oe Bo 3 Whiting, Robert C........ Littleton -...-.... Grafton’ <-.:/-.5 44 20 Wee 2n00!|,....5.-. FDR, Gas 10: NEW JERSEY. Beans, Thomas J......... Pragress: -=\.. .2--- 41 22| 74 02 180 8 South Trenton. -.-.} Oneida --.-..----- 43 DOM OVA Dane: <5 eee 2 Vermillion. .-..--- Oswego -..------- 43 26 | 77 26 Sele Dee Ee 12 Skaneateles - ---- Onondaga ......- 43 00 | 76 30 932 | B. T 11 Baldwinsville. ...| Onondaga -.----. 431045) WGA. esse TEES.see 12 Seneca Falls----- Senecaeo.----—- 42 54] 76 51 463 | B.T 4 AnD ooo se = Cayuga -..-.....- 4255 | 74 28)}........ eee iz Fishkill Landing.) Dutchess..-...-. 41 34} 7418 42|)B.T.R 12 Rochester - ------ Monroe ... .....- 43 08 | 77.51 516 | Be TR 11 Theresa ....--- ..| Jefferson ....--.- 4412] 75 48 365: (DR .oe2| We Ogdensburg --.-.-. St. Lawrence....| 44 43 | 75 37 279) Neeeeces trove ceatesestate Rensselaer -- .--. 42 44] 73 37 58. | AMR .... Walson- pase == Niagaras--o---< 43 20 | 78 56 250)|) Tee seas Waterford .. ..-.. Saratoga .......- 42 47) 73 39 10) |e ene Nichols...-.---.- ADO P Bee ates AZTOO MM ONS ee sincnie mele eee 12 South Hartford ..| Washington -.-... AS VS Fave 400: | TIR 2: 5 Flatbush .......- Kan piles eer se 40 37 | 74 02 54 | B.T.R.- 8 Fort Ann...--.-- Washington ...-. 42 3 7344 | 1,430) TR... 2 Oswego... .-...- Oswego .-.------ 43 28 | 76 30 250 | B. T.R. 12 Rochester . -.-.-- Monroeeeee eee 43 08 | 77 51 D2) || PAs ae ee 12 New York......- New York..-..-.-.. 40 43 | 74 05 25) Adee 12 Clinton 222 =2se-5 Q@neidat2ees- 3 - 43 03 | 75 15 600, |) ee Re 12 Fredonia ....---- Chautauqua ..... AQ 260M FONB4 ie woe sae Ba, es: 1 Jamestown --.-.- Chautauqua ..... 42.06 | 7919) 1,454) TR... 1 Gouverneur -.-.. St. Lawrence....) 4419} 75 29 |.....--.. BTR 12 Wampsville -.--. Madison ....-...- 43 04 | 75 50 500 | T.R--- 12 Marathon . ..---.- Cortland’S. =. -...- 42 24 \MeTGKOD) | 55. x0==' TS Ries 5 New York .:...- New York...-... 40 44} 73 59 41 | (As eaeacee 1 NUerniee = eee Rockland - .--.--- AD 30s) WES cepa ye i Cazenovia .. .... Madison ....-..-. £2.55'| 75 46) 1,260) A 2. 2222 6 White Plains -...| Westchester ..... A105) |. TBRAON E.-cecs Doe Sees 12 Welshfield ...-.-. Geauga 225-565 41 23 | (81 12))" 1) 2050/- ik << 12 Marietta. --=~' Washington ...-.. 39 25 | 81 31 630 |e 1 Saybrook - ...-.-. Ashtabula -..-.-- 41 52} 81 OL G50 Nien e ca 2 New Lisbon ...-.. Columbiana -...-. 40 45 | 80 45 961 | B. T. R-- 12 Medina, ==... --.=. Medina) 25% <>. == 41 O7 BL 47) Teh eAvSs ac 2 Cleveland ....... Cuyahoga .-....-- 41 30} 81 40 Gbps | MEroeaeen 12 Portsmouth... --- Scioto 22k... 38 45 | 82 50 eau Poa tleee 1 Betheliz sc 2 22 =~ Clermont - ...:.- 39 00 | 84 00 Boule teers 12 Newark ......--. ickmps seer). 40 07 | 82 21 B25) ple eee 8 Austinburg -.. -. Ashtabula .....- 41 54} 80 52 BL6) |) Bo Re 12 Portsmouth....-- SLIGO =e eae al 38 42] 82 36 Dot |\eopaeke at 9 Little Hocking -.| ‘Washington -.... 39 25) USMOON eer nae. Nee ee 2 College Hill -.-.. Hamilton. ..-....| 3919 | 84 26 800" MR Sse a2) Cincinnati ..-.--- Hamilton > ----.* 39 06} 84 27 M5008] ave seats 12 Westerville. ---.-.-. Mranklin:. 25s. - AD 04: ||) "83V000)| 6... 225 Avie taiata ital 8 Kingstones-----= FRUOSS ieee ieee = 39 29 | 83 00 (OSP) | WANES Saee 3 Dallasburg -....- Warren .. ...---| 39 30] 84 31 SOOM Ntseeeeee a Kelley's Island...| Erie...........-- 41 36 | 82 42 OST i) asso hear 12 | Cleveland .. .. ..] Cuyahoga ....... 41 30} 81 40 643) | Bo. wae 12 Savannah -.....- Aphlandj- ==. 4WISh| MB2I3I")" 1, 098i) AS yseerl 7 New Westfield.-..} Hood...-...-.--- 4113] 88 49 692)| INR 2 Madison .. ...-.- WGK) ceemac se - 41 50 | 81 00 6205). DoR eee 2 Waton secre ea Preblavwess.. 2. =< 40 GO} -74200)) 1,400.) Lis. 22222 | 1 EN OV eterna Miaminese ve... 40 03 | 84 06 DP LOSs We lephee 5 Yast Fairfield. ...| Columbiana - .... AD ATs WOOra4s yd, 152") AC Sai sce 12 Bullsborouph +. - =| (huebland:- <2 c- < 5) <<. c eeemel eteerettall eiarelae = 2) Bie 6 Norwalk 222-25: is ith [eee AUIS tee aOee se =e pier Re 12 Bowling Green...| Wood .......---- 41 15°} 83 40 | 700 | B. T.R-- 12 Garrettsville..... Portage =¢ -=..2.|- 41 050 sh 10 900) | 0 sae 3 Cincinnati ----.-- Klamilton 2.5... 2 39 06 | 84 27 540 | B.T.R. 12 Hillsborough ....| Highland - :. ....).....<- HaGretese ck 1.2205) eas 2 Cardington ...-.- LODO eet ane © 40 30 | 83 00 |j.+...-.. Neeser | 1 Kenton... s2c.0. Hardinijeoe-c- = AL BON GARA Ew 2A B.S) 1 Milnersville . ....] Guernsey . ....-. 40M OM MEURD)|. none] aes | eee * Above low-water in the Ohio river at Cincinnati. ra) Or Ie Sa \ METEOROLOGICAL OBSERVERS. . . ? . List of meteorological stations and observers, §c¢c—Coutinued. Name WPobserver: oH10—Continued. Thompson, Rey. Elias. --. Thompson, Prof. H. A... Trémbley, J. B., M. D.--. Ward, Rev. Ll. F..---..... RV HUGGE ALAS! Jooosseass Williams, Prof. M. G Nyason werot. J. H..--..-- Young, Prof. Chas. A--.. ; PGhG. 0. (Ole a eciacasis OREGON. a Tronside, R. B.. BE eosa ss Willis, PoWassts22-cse-=- PENNSYLVANIA. Atwater, H. H Bentley, E. T Overs), Wi kee=----" =--=- PICK ATEN. Go... sa.. << Brugger, Samuel......... Darlington, Fenelon Eggert, John Friel, P Hance, Ebenezer Heisiey, Dr. John HHCKOR Nine =5<= 22% «ote Hoffer, Dr. Jacob R.-.--.-- Jacobs, Rev. Mo... -2-.: SIBCONS EES Bio 5/6 55 Kirkpatrick, Prof. Jas. A Kohler, Edward Lyceum, Jefferson College Martindale, Isaac C....--- Meehan, Thomas...-.-- Meehan, J Muller, Prof. Rudolph- --. Ralston, Rev. J. Grier. .-. Ricksecker, Lucius E...-. Savery, Thos. H Smith, Wm., D. D.-..----- Swift, Dr. Paul Taylor, John Walker, Robert L Weeks, James A ..-..-..--.- | RHODE ISLAND. Caswell, Prof. Alexis..--. Sheldon, H. C SOUTH CAROLINA. Marsh, M. M., M. D.... ; BMA A MRE a 5. - TENNESSEE. Stewart, Prof. Wm. M.... UTAH. Pearce, Harrison Phelps, W. W VERMONT. Buckland, David Chickering, Rev. J. W --- Cutting, Hiram A Marsh, M. M., M. D...... Station. Croton Westerville... -.- Toledo Weliington -.---. Cincinnati -4.-<.- Urbana College Hill Hudson AMDUINN 22 s2. csc Salem Susquehanna De- pot. Tioga Blairsville Silver Spring. --. Fleming Parkersville Berwick Shamokin Philadelphia .-. -. Morrisville Harrisburg Harrisburg Mount Joy Gettysburg .@. .. Philadelphia -. -. North Whitehall. Cannonsburg.... Byberry Germantown .... itis DET ee a Norristown...... Nazareth Altoona Cannonsburg ---. West Haverford. . Conneilsville -. - . Moorhead Oil City Providence Providence Beaufort Clarksville St. George..---.. Salt Lake City .. Brandon Springfield Lunenburg Montpelier seeeee County. Licking Franklin Lucas: -6s-22eee Loraine Hamilton - Champaign .-..-- Hamilton - ...-..- Summit. 225... Baker Marion Susquehanna... Tioga Indiana Lancaster Centresssccctsc es Chester Columbiathes---- Northumberland - Philadelphia -. -- Bucks Dauphin Dauphin Lancaster Philadelphia -- -- Lehigh Washington Philadelphia .. -. Philadelphia Alleghany Montgomery .. -. Northampton ..-. Blair Washington Delaware. -....- PY LG) 2a aleinaicie Alleghany Providence Providence Washington Salt Lake Rutland Essex a North latitude. 40 13 40 04 41 39 41 08 39 08 40 06 39 19 41 15 44 37 44 56 40 31 40 05 40 55 39 54 41 05 40 45 39 57 40 12 40 16 40 20 40 08 39 49 39 57 40 40 40 17 40 05 40 30 40 08 40 43 40 35 40 16 40 00 40 00 41 49 41 50 36 28 37 00 40 45 43 45 43 18 44 28 44 17 West longitude. 80 46 87 13 114 00 111 26 73 00 | 72 33 71 41 72 36 481 Instruments. 69 No. of months received. Be ee RPRONRMOOCW WwW wow me _ Clio m to * e ‘ 70 APPENDIX TO THE REPORT OF THE SECRETARY. List of meteorological stations ae observers, &c.—Continued. . oO m 7 = 3 a @ is a jes Name of observer. Station. County. = a 8 BE = o Pe) a e a 5 Ss 3 . o 5 3 2 $ ie : A = 5 4 A VERMONT—Continued. o 4 SLs Feet. Mead, Stephen O--...---- Rutland -........ Rutland (ayers seedee eee | eee ee eee Ni eet tics 5 Paddock, James A Craftsbury ----- Orleans --.- -.-.-. 44.40))) 72:29 | 1,100) BR -.-- 12 Parker, Joseph.....-.-.--. West Rupert ....| Bennington. .--.| 43 15] 73 11 C2700 CPaoe ee 3 Petty, McK ----.......... Burlington ....-.. Chittenden ...--- 44 27 | 7310 BOX Wane nese 12 Pollard, © 5. sos... Brookfield .. .--- Orange = -- ------ 44:02 )) T2i36)|-.--- 4. DRY, Seats 5 Tobey, James K ......... Calais -... -...-- Washington ..--. Aa 22 NV NFeO9 ace De Bie wets 1 WASHINGTON, Swan, JamesG.......-..-. Neeah Bay ...---|--.0+e+--0-------- 28 41 | 124 37 400 ee eatces 12 WISCONSIN, Armstrong, § ...-..------ Waterford ...-.. Racine - ..-..---- 42 48 | 88 13 |....---- eee 5 STS VeaN ae ene =e Rocky Run..---. Columbia. -.----- ASe26n| |) TOO PCO |= =n oe TUR sess 8 Ellis, Edwin, M. D...-.--- Odanah........- Ashland .. .----- 46 33 | 91 00 610); BARrosee 9 Gridley, Rey. John.....-.- Kenosha .. .----- Kenosha -. ------ 42 35 | 87 50 600 | B.T. R-- 1 Kelley, Charles W--.----- Delafield’ --—- 2. Waukesha .. ----. 43 06 | 88 36 900)) BAe 6 Lapham, Iner’se A., LL.D-| Milwaukee--.---- Miwaukee-..---- 43 03 | 87 59 POS N e Ate esters Uy TUDE, SACOD = --- = -2a-=- Manitowoc ..---. Manitowoc - -...| 44 07 | 87 45 6587 | Bios 12 Mann, William ..-.- -.---- Superior .- -..--. Douglas .-.. --.. 46 46 | 92 03 680) Wi Sen 6 Mathews, George..--.---- Brighton 2s... - Kenosha .. ...--- 42 36 | 88 03 700.) Nb 2a. ee 6 LUGE TR ONC ROSE rn aopeseoe— Waupaca. ...--- Waupata - --..-- ASOD BOM | arc cre een 1 Porter, Henry D ......... Beloit. Jefe 22 Rock, est eessne 42 30 | 89 04 750, | Bar wR 12 Sterling, Prof. John W.--.-| Madison .. .....- Dane oe sete === 43.05 | 189925 | 1,068} A -- -—. 10 Whiting, Wm. H..-.--.--. Geneva ........- Walworth .. .... 42 205 |7a8OVal joo. oa Pe cnscs 8 Winkler, Carl, M. D..-.-.- Milwaukee-...... Milwaukee- 43 03 | 87 57 600 | B. T. R-- 2 Woods, William ......-... Weyauwega..... Waupaca.......- 4415} 88 50 BO) eae 12 DEATHS OF OBSERVERS. Dr. 8. P. Hildreth, Marietta, Ohio, July 24, 1863. ’ 'T. F. Pollard, Brookfield, New Hampshire, August 19, 1863. Hon. Robert Hallowell Gardiner, Gardiner, Maine, March 22, 1864. David Buckland, Brandon, Vermont, July 19, 1864. Colleges and other institutions from which meteorological registers were recerved during the year 1863, included in the preceding list. : INO) SOORES soopecmoseosse Acadia College ....-.- © Soa. 5G coeeee eer Wolfville. King’s; College sse2 <._.- an See eee 2s Windsor. (Canada cess aaae = soe eet Grammar Schooltes2-2 --=- 2s eee eee Niagara. Maonetic Observatery.-....-.-.. ----...- Toronto. Wonnechicuteees=r esses see Wesleyan University 5. =~... -sseeeesseee-— Middletown. INOS eae lo eee ILombard) Wniwersitiy ---<- 5 qe ee ee a Galesburg. University of Chicaco..2.- -s-sen eee Chicago. Oye eee ape ee ae ae Comell (Collere.. 3-22. te peeeeeee cone Mount Vernon. Griswold College): —-- .. == Amherst. State Lunatic Hospital.......2-2..------- Worcester. Walliams; Collero ~.- =. 2 98e- eeesee sone Williamstown- Michigan, sei se eee State Agricultural College..........------ Lansing. New Jersey... oss'Coee bens Fréechold Instiiateso. .... ~ snes Institution for Deaf and Dumb. -..-.------- New York. Erasmus Hall Academy..-.....5--..----- Flatbush. University of Rochester -........-..----- Rochester. METEOROLOGICAL CONTRIBUTIONS. 71 ‘. : Colleges, §c., from which meteorological registers were received, §c.—Continued. eet es. eee eee | Farmers’ College eM a cota) aU bin aid ete College Hill. | Halcyon Academy.-..-.........---.---- Croton, | | Otterbein Universities 2.22220. Sos 2 2 Westerville. | Wrbanat Universitgee = -52.-- 23522. S22 2 Urbana, | Western Reserve Kclegs Be hoe | Hudson. | Woodward EhohiSchoole- 22.2... 2. Cincinnati. SOPOT estate ital elem iel= = Willamette University-------..-----. 2. Salem. jeenhsylvania -.----- ----=: Central High School. -2.-2-2-2- --2..----: Philadelphia. | iHlavertord @ollese=* pa emere === ==] West Haverford. Jefferson College -....---. -------------- | Cannonsburg. Biiode island... 252.2022. io eeyl VR hh Heo oS Ibe see eS seesoe Providence. PlenuMenseos- 2. ss.-2. Luss | Stewart College. .--.--..-------.--..---- Clarksville. iMermonti= 2 cjacnsda suis 2 ' University of Vermont ..--.-.--..-----.- Burlington. WISCONSIN: 2.22\222p$4be=28 Beloit) College -jassae a Seto s dalle orate Beloit. | Wisconsin University -.----.------------ Madison. METEOROLOGICAL MATERIAL CONTRIBUTED IN ADDITION TO THE REGULAR OBSERVATIONS. Abbott, Francis —Abstract of observations made at eight stations in T'as- mania, or Van Dieman’s Land, during the six months ending June, 1862, for the papers and proceedings of the Royal Society. Caswell, Prof: A., D. D—Summary for the year 1863, and comparison with the previous thirty-two years, at Providence, Rhode Island. Printed in the Providence Daily Journal. Dabney, William H—Temperature of the valley of Orotava, Island of Tene- riffe, compared with that of London, Paris, Pan, Nice, Rome, and Madeira. Extracted from the pamphlet of the Baron of Belcastel. Dreutzer, O. E., (consul, Bergen, Norway.)—Summary of meteorological observations for each month in the year 1863, kept at the hospital in Bergen. The readings of the barometer reduced to inches, and the thermometer to Fah- renheit scale, by Mr. Dreutzer. Gardiner, R. H—Printed summary of observations during the year 1863, at Gardiner,. Maine, and monthly mean temperature and amount of rain for a period of tw enty-seven years, from 1837 to 1863, inclusive. Goddard, C. W.—Daily observations at Constantinople, from October, 1862, to September, 1863, inclusive. Also a summary for the year 1862. Gregory, S. O—Diagram showing the changes of the wind every day in the year 1863, at Theresa, New York. Graham, Colonel James D.—Register of water-level and meteorological ob- servations, made at the following places, under the direction of Captain George G. Meade, topographical engineers, until August, 1863, and subsequently under the direction of Colonel James D. Graham, corps of engineers, superintendent of the survey : Sackett’s Harbor, New York.—July, 1861. to December, 1863. Charlotte, New York.—July, 1861, to December, 1863. Fort Niagara, New York.—July, 1861, to December, 1863. Buffalo, New York.—June, 1860, to December, 1863. Cleveland, Ohio—June, 1860, to December, 1863. Monroe, Michigan.—July, 1861, to December, 1863. Detroit, Michigan.—January, 1860, to December, 1863. Tawas City, Michigan.—July, 1861, to December, 1863. Thunder Bay Island, Michigan.—July, 1861, to November, 1863. Sugar Island, Michigan.—November, 1863, to December, 1863. Grand Haven, Michigan.—July, 1861, to July, 1863. Ontonagon, Michigan.—July, 1861, to December, 1863. ‘ Superior, Wisconsin.—June, 1861, to December, 1863. TZ APPENDIX TO THE REPORT OF THE SECRETARY. > 9 - . Ives, William—Summary of observations at Buffalo, New York, during the year 1863, newspaper slip. Kirkpatrick, Professor James AA general abstract of the meteorological ob- servations made at Philadelphia during the year 1863, and a comparison with those of the last twelve years. Printed sheets from the Journal of the Franklin Institute. ‘ Lake Winnipisseogee Cotton and Woollen Manufacturing Company, New Hampshire-—Amount of rain for each month in 1863, at the outlet of Lake Winnipisseogee, in the town of Laconia, New Hampshire, and also at Lake Village, about four miles south on the same stream of water. Lapham, I. A., LL.D—Table showing the direction and force of the wind for each hour during the month of September, 1863, at Milwaukee, Wisconsin, taken from the autographic record made by Burnell’s anemograph. Prepared for the Commissioner of Agriculture by I. A. Lapham, LL.D. Summary of observations at Milwaukee, Wisconsin, with a full set of instru- ments, during the year 1863. (Printed slip from the Milwaukee Sentinel.) Lewis, James, M. D—Hourly record of the temperature at Mohawk, New York, during the year 1863, from the register made by his metallic self-recording thermometer; also, monthly and half-monthly means, and hourly mean for the whole year 1863. Lippincott, James S—Meteorological observations made by Benjamin Shep- herd near Greenwich, Cumberland, New Jersey, from March, 1856, to June, 1861. Tabulated and reduced by James 8. Lippincott, Haddonfield, Camden county, New Jersey, for the Smithsonian Institution. Logan, Thomas M., M. D—Monthly summaries of the meteorology and necrology of Sacramento, California, reported for the Sacramento Daily Union by Thomas M. Logan, M. D., secretary of the Board of Health. Contribution to the Physics, Hygiene, and Thermology of the Sacramento River, by Thomas M. Logan, M.D: From the Pacific Medical and Surgical Journal. 8 pp. 8vo. Magnetical Observatory, Toronto, Canada West, (Professor G. T. Kingston, M. A., director.)—Mean meteorological results for the year 1862; also, a com- parison of the same with a series of preceding years. Mayhew, Royal—Mean temperature at Indianapolis, Indiana, for the hours of sunrise, 7 a. m., 12 m., and 2,6, and 9 p. m., during each month in the years 1861, 1862, and 1863; also, the amount of rain in each month during the same period. Morris, Prof. Oran W.—Summary of observations for 1863, giving maxi- mum, minimum, mean, and range of all the instruments for each month, as kept at the Institution for the Deaf and Dumb, New York. Murdock, G—Appendix to Agricultural Report, being hints on meteorology, with summaries of observations made at Saint John, New Brunswick, in the years 1851 to 1862, inclusive, by G. Murdock, superintendent of water-works at St. John. 8vo. 34 pages. Nason, Rev. Elias.—Record of events in Exeter, New Hampshire, during the year 18638, containing notices of the weather. No. 3, by the Rey. Elias Nason. 12mo. 24 pages. Ohio State Board of Agriculture —Fifteenth Annual Report of the board to the general assembly of Ohio for the year 1860. Contains articles on the influence of forests upon soil, climate, rain, and winds. P. 255 to 274. Report for 1861. ‘'The atmospheric conditions, showing the value of ba- rometers for agricultural purposes,”’ by C. A. Richard, of Columbus, Ohio. P. . 234 to 275. Osservatorio del Collegio Romano.—Bulletino Meteorologico del’ Osservatorio del Collegio Romano con corrispondenza e bibliografia per ’ avanzamento della fisica terrestre. Published at Rome twice a month, beginning March, 1862. METEOROLOGICAL CONTRIBUTIONS. ta al o Paine, H. M., M. D—Summary of observations at Clinton, New York, for 1862 and 1863, with a full set of instruments, giving the monthly and annual means, maxima, and minina. Paterson, Rev. A. B—Meteorological notes for December, 1863, at St. Paul, Minnesota, with a comparison with the previous four years. (Newspaper.) Rrotte, C. N.—Printed summary of observations made at seven stations in Costa Rica in the year 1863. Sartorius, Charles—Summary for the year 1863, with full set of instru- ments, at Mirador, Mexico. Secchi, P. Angelo—Alcune richerche meteorogiche sulle tempeste oecorse nel 1859-’60 memoria del P. Angelo Secchi. Estratta dagli Atti della accademi de’ Nuovi Lincei Sessione III, dell’ Anno XIII, del 5 febbraro 1860. Rome. 1860. 28 pp. quarto. State Department.—Statistical report on the weather and health of Frankfort- on-the-Main during the year 1863, by William W. Murphy, consul. Vaughan, Captain D.—Meteorological Journal and Report relative to the cur- rents, climate, and navigation of that. portion of the lower St. Lawrence forming the Strait of Belle-Isle. Second edition. Compiled by Captain D. Vaughan, Quebec. Svo. 62 pp. Whitehead, W. A—Summary of observations during the year 1863 at Newark, New Jersey. Printed slip from Newark Daily Advertiser. Also, an article on the “ Climate of Newark,” being an examination and comparison of the observations made there during the last twenty years. Wislizenus, A., M. D—Monthly and yearly mean of positive atmospheric ’ electricity, of temperature, and of relative humidity, in 1861, 1862, and 1863, at St. Louis, Missouri, based upon daily observations at 6, 9, 12, 3, 6, and 9 o’clock. Published in the St. Louis Medical and ere Journal. Vol. I, No.4. - REPORT OF THE EXECUTIVE COMMITTEE. The Executive Committee respectfully submit to the Board of Regents the following report of the receipts and expenditures of the Smithsonian Institution during the year 1863, with estimates for the year 1864: General Statement. RECEIPTS. The whole amount of the Smithson bequest deposited in the treasury of the United States is $515,169, from which an annual income at 6 per cent. is derived of ..........-....-- $30,910 14 ‘The extra fund of unexpended income is invested as follows, viz: In $75,000 Indiana 5 per cent. bonds, yielding (less United States GA) wre ermal oiats.= « isis SUAS Ie Loe ane LC eles cared als 3,749 50 In $53,500 Virginia 6 per cent. bonds. In $12,000 Tennessee 6 per cent. bonds. In $500 Georgia 6 per cent. bonds. In $100 Washington city 6 per bonds, yielding............-.- 6 00 SE OTANI CONG :r's.0:215 = pepe Rae Laie Re ee ee 34,665 64 Balance in the hands of the treasurer, senuary, 1863.5. loses 29,509 61 otal receipts: s+. 2.1 3e ake SREP ote MA ASe ey sn ae 64,175 25 EXPENDITURES. For building, furniture, and fixtures............. FO Ad a Wie Hor Seneral expensesec ec x. Sad wectenessctas 11,688 69 For publications, researches, and lectures .....-.-. 10, 761 65 For library, museum, and @allery Ob Carts. 2 co. 192595238 SL Oooo Balance in the hands of the treasurer, January, 1864...-. 32, 353 90 STATEMENT IN DETAIL OF THE EXPENDITURES OF 1863. Buudine incidentals:: 22s... 662 2 hb oe $1, 598 '79 eramonpoere and LXTULES ee. ie .o, 2 35.6 elec cq! ho see ol2 99 —— $2,111 78 Meetings of the Board of Regents................ 104 50 SURI En eae te ecss als a Oe es » 343 71 ET CCti renee ns ik A cee ae ML 1,090 75 BOStAgb epee oe ak osha eke s ld eee 421 46 Pransportauign, weeneral ook als Saale, cass shee 374 05 BiCHAN OCS are ee ena ak Cee ee 1,357 76 PAMALLONCRY |... ae eerie eyecare etn ee 486 09 REPORT OF THE EXECUTIVE COMMITTEE. 75 erercneral pringms.... 00022200 2 pares nee $3 50 RMR ar ats we 2 se West cte 531 98 ME sie a oa ee gs o's wad 129 59 Marre i PCO OTA neo ais = 5: a cee eas 3 584 65. Meera Clefi hire: ©. c's... £2. ue eee ee 311 65 PRUMIPEPRCCICEATY «co sce eee eet 3,500 00 Salaries, chief clerk, bookkeeper, laborers, &c..- - - 2,389 00 $11, 688 69 Prnibnsonian. Contributions - .. << .-2 - 0. > ms nt oe penne ea ene ae 10, 500 For publications, researches,-and lectures.........--...-.-+.---- 10, 500 For library, museum, aud wallery of ati. -22-2tsccee Ae ee eee eee ee 9, 000 Mota + 3. ee ee ee a ee Ce ee ee a eee $32, 000 The actual expenditure on the building is very nearly the same as the amount appropriated. For general expenses the amount is larger than the estimate, and this is due to the increased cost of materials. For publications, &c., the actual expenditure is nearly the same as the estimate. For library, museum, and gallery of art, the expenditure is nearly three thousand dollars less than the estimate, but this is on account of the expend- iture on the collections of the remainder of an appropriation from Congress for the distribution of the specimens. For the year 1864 the same estimates are recommended as those made for 1863. The committee have examined the books and accounts of the Institution for the past year, and find them to be correct. Respectfully submitted. A. D. BACHE, RICHARD WALLACH, Committee. . \ 4 : rR ° a : - JOURNAL OF PROCEEDINGS fo, BOARD OR REG Nees THE SMITHSONIAN INSTITUTION. WASHINGTON, January 20, 1864. In accordance with a resolution of the Board of Regents of the Smithsonian Institution, fixing the time of the beginning of their annual session on the third Wednesday of January of each year, the Board met this day in the Regents’ room, at 104 o’clock a. m. Present: Hon. 8. 8. Cox, Hon. J. W. Patterson Hon. R. Wallach, General J. G. Totten, and Professor Henry, the Secretary. A quorum not being present, the Board adjourned to meet on Monday, January 29, at 73 p- m. Monpay, January 25, i864. A meeting of the Board of Regents was held this day at 74 o’clock p.m Present: Hon. H. Hamlin, Vice-President of the United States, Hon. W. P. Fessenden, Hon. L. Trumbull, Hon. J. W. Patterson, Hon. H. W. Davis, Hon. Rt. Wallach, Mr. William B. Astor, General Joseph G. Totten, Professor A. D. Bache, the treasurer Mr. Seaton, and Professor Henry, the Secretary. In the absence of the chancellor, Mr. Hamlin was called to the chair. The Secretary announced the election, by joint resolution of the Senate and House of Representatives, of Professor Agassiz, of Massachusetts, as a Regent in place of Mr. Badger, the reappointment by the Speaker of Hon. S. 8. Cox, of Ohio, and the appointment of Hon. J. W. Patterson, of New Hampshire, and Hon. Henry Winter Davis, of Maryland, as Regents from the House of Representatives. The general statement of the funds of the Institution and of the receipts and expenditures during 1863 was presented by the treasurer. The Secretary submitted the annual report of the operations of the Institu- tion during the past year, which was read in part. The Secretary made a statement as to the policy which had been adopted in regard to bequests and donations having special conditions attached to them, » 78 ' PROCEEDINGS OF THE BOARD OF REGENTS. and gave the reasons for declining to accept a herbarium which had recently been bequeathed to the Institution. ~ On motion it was ; Resolved, That the action of the Secretary in this case be approved.. ~ The Secretary called attention to the unexpected delays and embarrassments which had oceurred in obtaining the remainder of the original bequest of Smithson left in England as the principal of an annuity to the mother of the nephew of Smithson, and read the correspondence on the subject with the attorneys, and also a letter from Hon. C. F. Adams, the American minister to England. On motion it was Resolved, That a committee be appointed, consisting of. the Secretary, Mr. H. W. Davis, and Professor Bache, to confer with the Secretary of State and the British minister relative to the action of the English authorities in regard to the money due the Smithsonian Institution. On motion, the Board adjourned to meet on Wednesday, January 27, at 74 o’clock p. m. WEDNESDAY, January 27, 1864. A meeting of the Board of Regents was held at the Institution at 74 o’clock p-m. Present: Hon. H. Hamlin, Vice-President of the United States, Hon. G. Davis, Hon. R. Wallach, Mr. William B. Astor, Professor A. D. Bache, and the Secretary. Mr.’Hamlin was called to the chair. The minutes of the last meeting were read and approved. Professor Bache presented the report of the executive committee, which was read and approved. The Secretary presented the remainder of his annual report, which was read and adopted. He also presented a series of letters illustrating the correspondence and operations of the Institution.* On motion, the Board adjourned to meet at the call of the Seeretary. Turspay, March 15, 1864. A meeting of the Board of Regents was held this day at 104 o’clock a. m. Present: Hon. H. Hamlin, Vice-President of the United States, Hon. S. S. Cox, Hon. J. W. Patterson, Hon. R. Wallach, Professor L. Agassiz, Professor A. B. Bache, and the Secretary. Mr. Hamlin was called to the chair. The minutes of the last meeting were read and approved. The Secretary presented a series of works on natural history, which had been prepared and printed at the expense of the Institution, and also the * See end of the Proceedings, page 80. PROCEEDINGS OF THE BOARD OF REGENTS. 79 manuscripts of several others which had been offered for publication. All of these, he stated, had been referred for critical examination to Professor Agassiz, who would favor the Board with some remarks in regard to them. Professor Agassiz stated that, so far as he had had an opportunity of examining the original papers, he considered them worthy of publication; that he would give the whole series of works on natural history, which constitute portions of what is called the Miscellaneous Collections, a critical examination, and present a report upon them at a future time. At present he would beg leave to make a few remarks on the importance of adopting measures for in- creasing the efficiency of the active operations of the Institution by relieving them of the expense of the support of the museum, library, and gallery of art. Unless this could be done, many valuable contributions to science offered for publication would have to be postponed or refused. He thought that the resources of the Institution were inadequate to carry on at the same time its active operations, and maintain a museum, a library, and a gallery of art upon the only footing upon which they can truly be creditably supported. Without, therefore, making a definite motion, he would submit for future consideration the propriety of asking the government to take charge of the museum, the library, and the building now occupied by the Institution, with a view of main- taining them on a more extensive scale, and relieving the Smithsonian Institu- tion of a large expenditure which, for the advancement and diffusion of science, had better hereafter be devoted to the active operations of the Institution. He hoped that if such a plan would be carried out, the resources reverting to the Institution from the transfer of the museum and library to the government, either to form an independent organization or to be carried on hereafter as before by the Smithsonian Institution, the active operations of the latter would be greatly extended. The Secretary stated that the suggestions of Professor Agassiz were in accordance with the views which had been entertained by the majority of the Board of Regents from the first discussion of the organization of the Institu- tion; that the present disposition of the funds was a necessity which was im- posed upon the directors by the requirements of the law of Congress establish- ing the Institution, and that he had always entertained the hope that the sup- port of the building and collections would in due time be provided for by the general government, and a national museum be founded which would be com- mensurate with the intelligence, extent, and resources of the country. Professor Bache fully concurred in these remarks, and moved the following resolutions, which were adopted : Resolved, 'That a committee be appointed to report to the Board of Regents any suggestions for extending the active operations of the Smithsonian Institu- tion, and for the separate maintenance of the collections. Resolved, That this committee consist of Professor Agassiz, the Secretary of the Institution, Mr. Fessenden, Mr. Patterson, and Mr. Cox. The Board then adjourned sine die. ‘ : 80 PROCEEDINGS OF THE BOARD OF REGENTS. LETTERS PRESENTED TO THE BOARD OF REGENTS TO ILLUSTRATE THE CORRESPONDENCE AND OPERATIONS OF THE INSTITUTION. Communication from Dr. B. A. Gould, on a new discussion and reduction of the observations of Piazzi of Palermo. CamsBripGe, May 16, 1863. My Dear Sir: For many years I have been strongly convinced that an extremely valuable contribution to astronomical science might be made by a new discussion and reduction of the observations of Piazzi at Palermo. This eminent astronomer, with his assistants, was engaged, during the twenty- two years from 1792 to 1813, in observing the positions of the principal fixed stars. He was provided with the best instruments which could be obtained at that time, and his observations have been, and must continue to be, our prin- cipal and most trustworthy source of information as to the places of between seven and eight thousand fixed stars at the beginning of the present century. As nearly as I can estimate without an actual count, he must have made about ninety thousand determinations of right ascension, and from sixty to seventy thousand of declination, the original records of which observations still exist. From these he censtructed his two well-known catalogues—the first in 1803, the second in 1814—containing the mean places for 1800.0 of 7,646 stars. His methods of observation, while, of course, far inferior in many respects to those of the present day, were the best in use at that period; and the care and fidelity with which they were used seem to have been unsurpassed ; and, al- though the reductions upon which the catalogue was based seem to have been incommensurate in precision with the observations themselves, still this cata- logue has, for the past fifty years, been a standard authority with astronomers, and, fora great part.of that time, their chief dependence for both the right ascensions and declinations of stars. The original observations of Piazzi were sent by him for safe keeping to his friend Oriani, in Milan, and have been carefully preserved at the Observatory of the Brera in that city. In 1845, Professor Littrou, the director of the Impe- rial Observatory of Vienna, incited specially, as he says, by Argelander, and encouraged by Bessel, Gauss, Schumacher, Struve, &c., commenced the printing of these original observations as part of the series of Annals of the Vienna Observatory, and they have thus been for several years accessible to astronomers. When organizing the Dudley Observatory in 1856-58, it formed an integral part of my plan, not merely to institute new observations of the heavenly bodies, but to carry on such computations, reductions, &c., as might render available past observations of this and the last century, which would otherwise be either useless or of inferior value to astronomy. Various undertakings of this kind were planned, but the first of all to be begun was the re-reduction of the whole series of Piazzi’s observations, using the best values of the constants of pre- cession, ‘aberration, and mutation, and investigating all the instrumental errors with care; and I made considerable progress in arranging the details of the computation. After communication with Professor Littrou, and an extended correspondence with Professor Argelander on the subject, in which this distin- guished astronomer gave me many very useful suggestions, the whole plan was completed, and, but for the misfortunes which interfered with the usefulness of the Dudley Observatory before its activity had fairly begun, the new cata- logue would doubtless now have been in the hands of astronomers. My health and opportunities of labor being now greatly improved, I am anxious to resume this work, and write to ask for your influence and aid, as far as possible, in furtherance of the plan. Knowing, as you do, the nature of the ’ PROCEEDINGS OF THE BOARD OF REGENTS. 81 % work proposed, it is almost needless to dwell upon its value to science. The one consideration, that Piazzi’s observations must, for long years to come, fur- nish the only means of determining the proper motions of more than five thousand stars, is of itself sufficient. For the other stars observed by him, they constitute a most important element in the determination. The huge number of stars, observed in zones by Lalande, at almost the same period—more than fifty thousand—depend for their reduction and value almost solely upon Piazzi’s results; and the formation of a new catalogue of the latter will give an altogether new value to the results of Lalande. The great mass of independent observations thus rendered more accurate can speak for themselves, and it is manifest that their usefulness will be far greater than that of the same number of new observations made now. Unfortunately, Piazzi’s observations do not afford all the elements now known to be needed for their reduction, and it will doubtless be necessary to reduce them differentially, thus greatly increasing the labor. Not merely ques- tions of azimuth, zenith point, and clock correction, but also questions of graduation, of irregularity of pivots, and even of refraction, must be discussed, thus rendering the undertaking one of no small magnitude ; still it would, I am sure, be labor well bestowed, and, as Professor Argelander wrote me in 1857, “it would be a grand thing, * * * * and one of the most important things that could be done.” The first process required is the reduction to the mean equinox of 1800.0 of all the observations just as they were given by Piazzi. This is a work which could be carried on by ordinary computers, and would in itself be of great service, even were the discussions of the observations to be omitted. It would consti- tute nearly two-thirds of all the labor, and possesses the great advantage that whatever is done, be the amount large or small, is immediately available. The best estimate that I am able to make gives about $5,000 as the probable cost of this reduction, to which from one-quarter to one-third should be added for the expense of checking, comparing, and correcting mistakes. Therefore, be- fore beginning, I desire to make sure that at least $6,000 will be available for the purpose. There is scarcely a limit to the number of computers who could be employed at once upon this part of the work. It might easily be accom- plished in a single year, or it might be slowly and regularly carried on for a long time, the expense being not very different in the two cases. This process being completed, the remainder of the work, consisting of various investigations, in addition to the discussion of the instrumental corrections, and the formation of a catalogue from the observations after all reductions have been applied, would, of course, require more deliberate study. Ft would probably occupy at least two years, but I think the expense would be decidedly inferior to that of the first process. Indeed, I have convinced myself that all the out- lays needed for the whole undertaking in all its branches would not exceed $10,000, and that if this sum were now available, the work might be completed in two years, inasmuch as parts of all the processes could go on simultaneously. My sense of the usefulness of this work, and my conviction that astronomers everywhere would agree in this opinion, are so strong that I have determined to appeal to you for aid, well knowing that your interest and moral support will, under any circumstances, not be wanting. It is precisely such an under- taking as the plan of the Smithsonian Institution would lead it to encourage ; and although I can readily see that the amount needed is larger than the Smith- sonian would probably be able to apply at any one time to the furtherance of any one science, still I come to you with my plan, well assured that you will willingly do what you can in its behalf, whether by some gradual appropriation year after year, from the Smithsonian funds, in aid of what I have called the first process, viz.: The computation of the correction to the mean equinox of 68s 82 PROCEEDINGS OF THE BOARD OF REGENTS. 1800.0, or in some still more active way, by enlisting interest and securing aid from other sources. For several months past I have devoted such time and means as I could to the preliminary steps, and, as you are aware, I now desire only the means of defraying the indispensable outlays, wishing to contribute my own services in behalf of the work. ee I am, dear sir, very respectfully and truly yours, aga a ni B. A. GOULD. Professor JosppH Henry, Secretary of the Smithsonian Institution. Project of an outline history of public education in the United States, by Frederic A. Packard. The proposed volume, to contain from 600 to 800 pages royal 8vo, to be put up in a cheap form, in the manner of legislative documents, with ample tables, indexes, &c., for easy reference. If it shall be thought best, the form might be changed to to volumes—one embracing the original thirteen States, and the other the remaining States and Territories. The plan of the work would comprise the following topics : ke I. Of universal education, considered as an essential element of free political institutions, what should be its character and extent ? Il. An historical sketch of the laws of the several States on the subject of education, and the establishment of public schools, academies, and colleges. In this connexion would be given the provisions for education under the colonial government, and their influence on succeeding legislation. III. An abstract or synopsis of all laws now in force in the several States touching public education, and of contemporaneous judicial expositions of the law, so far as they affect the essential principles of the system. IV. A sketch of the present state of public education in the country : (a.) Of the division of territory for school purposes, what and how made ? (®.) Of the manner of raising money for the support of schools, and the amount raised and expended in each decade of years, of the present century. (c.) Of the permanent revenue for the support of schools—if derived from a fund—when and how was such fund created, and what is its amount and in- vestment ? what portion of the annual school expense is derived from it, and what is its effect to stimulate or depress the working of the system ? (d.) Of the number and average age of children under instruction, distin- guishing the sex; the number in attendance, in proportion to the whole popu- lation, and the average time of attendance. (e.) Of the mode of employing teachers and determining their qualifications. (f.) Of the number of teachers employed, distinguishing the sex ; the compen- sation allowed; the average age of teachers, male and female separate ; and the average amount of time employed in daily teaching, making distinct heads of summer and winter schools. (g.) Of the branches taught in the public schools, and the proportion of time devoted to each. (i.) Of the preparation and introduction of school-books ; character of them in early schools—improvements in them; expense of them, and by whom borne ; and the number and variety of them, in the different branches, which are in use in the different schools. V. Of normal schools, number, when organized, how supported, number of pupils, terms and condition of admission; what proportion of pupils pursue teaching for a livelihood, and what proportion of these succeed. PROCEEDINGS OF THE BOARD OF REGENTS. 83 VI. Of school-houses, their number, average capacity, manner and means of building, and improvements in respect to site, ventilation, heating, furniture, out-houses, &c., &e. VII. Of school librarces, number of schools supplied with ; how and by whom selected ; funds to purchase, and the amount and source of the same; number and character of volumes ; cost, mode of distributing, preserving, and extent of circulation. VIII. Of the religious element in public schools; if less than formerly, why? To what extent necessary and practicable ? IX. Of popular manners and customs in the schools ; habits of thinking and acting; domestic and social character, and qualifications for citizenship, as they are influenced by our systems of public education. X. Of physical education, what time appropriated to it; what facilities and encouragements are afforded; what methods adopted, as drill, gymnasium, or athletic games ; and what part teachers take therein. XI. Of infant schools. XII. Of Sunday schools. XIII. Of colleges and other public literary institutions, so far as they afford aid to, or receive aid from, the public schools. XIV. Of the comparative expense and value of public education at different periods of our history. XV. Of lyceums, mechanics’ institutes, evening schools, and other methods of adult education, to make other means of ,education available, or to compensate for the want or neglect of early advantages. XVI. Number of persons of school age that are under instruction, the pro- portion of the population that can both read and write; the qualifications of the pupils, upon leaving school, to engage in the active pursuits of life, with a superior physical, moral, and intellectual character. The materials being thus collected, would be arranged under the title of éagh State, respectively, whatever is peculiar in its educational history and statisties ae placed under specific heads, and what is common to all under general heads. For example, Maine might occupy the first chapter or section of the volume— and we should first refer to Massachusetts for all matter preceding 1820, when it ceased to be a province. Then would come a succinct account of all legisla- tion on the subject, including an abstract of existing laws; then the origin, amount, and mode of distributing any school fund. Next, a bird’s-eye view of the actual condition of the schools, government, discipline, construction of buildings, character of teachers, text-books, and the obvious fruits of the sys- tem. Whatever peculiarity there may be in the climate, in the habits and pursuits of the people, or in the condition of society, affecting favorably or otherwise the interests of education, would find a place in aon After completing the circle of States in this way, a condensed chronological, historical, and statistical survey of the entire country would be in place, and pee nciplcs or conclusions as are established by the facts stated and illus- trated. It will be observed that the plan contemplates the history of each State complete in itself, and if prepared by an individual selected for the purpose, might bear the author’s name, like contributions to a biographical dictionary or an encyclopedia. Of course it would serve a valuable Joca/ purpose, and if properly prepared, would secure a share of public patronage, while the whole volume would furnish highly interesting and important information to the country at large and to foreign inquirers. When the outline thus sketched is well digested and matured, my purpose would be to forward a schedule of the subjects to some qualified patriotic person in each State, requesting his co-operation. The great advantages of having the 84 PROCEEDINGS OF THE BOARD OF REGENTS. 4 work done by a resident of the States, respectively, are the accuracy, fidelity, and fulness which would be secured, the facilities for obtaining materials, and the authority which it would bear. These considerations might induce one or more suitable persons in each State to encounter some personal inconvenience, especially as the service is one of vast and permanent importance, and can be better done now than at any future period. , The President of the Chamber of Commerce of Bordeaux to the Secretary of the Smithsonian Institution at Washington: Sir: I am not ignorant that the Institution of which you are the Secretary, and which labors with the most praiseworthy zeal to promote the progress of the different branches of human knowledge, maintains relations of exchange with the Imperial Academy of Sciences, Belles Lettres, and Arts of Bordeaux. The Chamber of Commerce, anxious in its turn to co-operate, as far as pos- sible, in the realization of the plans which you pursue, feels pleasure in trans- mitting to you a copy of its publications. They comprise a collection of its proceedings since 1850, the first volume of the catalogue of its library, &c. It is hoped that these various publications will find a place in your collections. The Chamber has, on its own part, founded a considerable library, which is open to the public, and it would be happy if the Smithsonian Institution should think proper to send us some of the volumes which it publishes, and which are filled with documents of the greatest interest on America, and on different ques- tions of importance. These works would thus be at the disposal of a consid- erable number of studious persons, and they would contribute to make the seryices of the Institution of which you are the organ appreciated in all their extent in Europe. Be pleased, sir, to accept the assurance of my most dis- tinguished consideration. CARTE DEL Paxasio, MILAN, October 31, 1862. Sir: Through the kindness of your agent, Mr. Bossange, of Paris, we have received the Annual Report of the Board of Regents, presented by the great and liberal Smithsonian Institution to the Carte del Palasio’s Agricultural As- sociation, of which we are directors and regents. Reading your valuable re- port, we have seen with the greatest satisfaction that the interesting and useful results of yourjabors have been approved and commended by intelligent men everywhere. hilst expressing, honored sir, our warmest thanks for having been deemed worthy by your Institution to participate in the gifts which the liberality of the Smithsonian Institution renders to men devoted to science, it will be a source of pleasure to us to endeavor to reciprocate your kindness. To promote knowledge and facilitate its progress by stimulating men of science to undertake general and extensive researches, and to offer the means of con- tinuing them, is the most useful service which can be rendered to mankind. The very extensive means which your great Institution has at its command, the ardor with which your officers and regents began and continue their difficult work, are infallible indications of the greatest results which will be produced. And we do not doubt that the material and moral progress of individuals, with that of science in general, will fully realize the anticipations of the founder, and amply recompense the continued labors of the distinguished directors of the Smithsonian Institution. PROCEEDINGS OF THE BOARD OF REGENTS. 85 As directors of a new institution, which we hope will also soon produce im- portant results in agriculture, we shall be content if, in reciprocating your kindness, we can also in any way serve the laudable purposes of your Institu- tion by presenting the results of our own labors and researches. Again expressing our thanks, we have the pleasure of sending some of the publications relating to our institution, with the hope that they will be placed in the Smithsonian library. They are the following: 1. Programme of organi- zation of the Carte del Palasio’s Agricultural Association. 2. Annual Reports of the Association for 1859-’61. 3. Agricultural Annals, by Dr. Gaetano Can- toni, professor of agronomy. * * * * * * % * Your most obedient servants, Sta. ANTONIO RESCHIN, Direttore. Dr. GAETANO CANTONI, Professor. * Orrice’Sur’t U. S. Minirary GENERAL HospIvats, Memphis, Tennessee, September 5, 1863. My Dear Sir: I am in receipt of your letter of the 25th ultimo, by which I learn the pleasing intelligence that the “ great Tucson meteorite” is in a fair way of getting to Washington at last. 1 amsure you will feel proud of it when you see it. J knew the “Carlton specimen” was not ours, as I had‘ sent it to Hermosilla before I left Arizona. ‘That sent in by General C. is about 750 pounds, while ours is about twice that weight. The only history I can give you is a vague one, as there is no written record of its advent in Tucson. The old inhabitants of that place all agree that it was brought there from the Santa Catarina mountains, which lie to the north of Tucson, about midway between the Rio San Pedro and that town. li was brought in by the military stationed at the old preszdio, where it remained until after the withdrawal of the Spanish garrison. It was then taken into town, set up on end, and used as a kind of public anvil for the use of the inhabitants. The smaller one was used in a blacksmith’s forge for similar purposes. In 1857 I found-the large one lying in one of the by-streets half buried in the earth, having evidently been there a considerable time. No person claimed it, so I publicly announced that I would take possession of it in behalf of the Smith- sonian, and forward it whenever an opportunity offered. Mr. Palatine Robinson, near whose house the iron‘was, assisted me in getting it sent to Hermosilla. There was some expense attending its hoisting into the truck-wagon that took it down to Sonora, which I paid to Mr. R. Mr. Ainsa agreed to take it, or have it taken, to Guaymas, Sonora, for fifty dollars. | The people of Tucson all agree that a shower of these meteorites fell in the Santa Catarina mountains some two hundred years ago, and I have been told that there were plenty of them remaining in the mountains. I never was in the immediate portion of the mountain range where they report the specimens are to be found, so I cannot vouch for the correctness of their reports. As the country is volcanic almost entirely, I have often thought, from the fact that iron ore is abundant in several of these mountains, that it might have been that masses of iron mineral were reduced to the metallic state by voleanic heat. See in the case of the famous ‘“Planchas de plata” silver mines, some one hundred miles south of the Santa Catarina, where large pieces of pure silver have been found reduced to the pure state by fire, which has left everything in its vicinity in a state of calcination. One piece weighing 1,500 pounds was found and cut in two to allow its removal to the city of Mexico by the Spanish authorities. I think you will find allusion to those interesting and once rich mines in Brantz Mayer. : 86 PROCEEDINGS OF THE BOARD OF REGENTS. T believe I have given you some data about the Tucson meteorites in a monogram published by the War Department in 1860; Medical Statistics of United States Army, 1855-60. I wish I could give you full information on this matter. Please let me know when you receive it, and be assured that when I go to Washington I will pay my respects in person to you and it. I am very busy, so you will excuse this hurried letter, and believe me Yours, very respectfully, B. J. D. IRWIN, Surgeon United States Army. SAN Francisco, Cau., Judy 2, 1863. Dear Sir: The aerolite which had remained so long at Alamito, for want of a proper person to bring it here, was brought by one of my brothers, Jesus M. Ainsa, who visited Sonora lately. We have been induced to retain it here for a short time, to satisfy the curiosity of the San Francisco people. The State Geological Society asked to be allowed to have a small piece for their collection, which request was, of course, granted. With this exception the aerolite has been preserved entirely in the same condition in mich it was found in Arizona, and by the 13th of this month we will have the pleasure to ship it to New York, under the care of the Pacific Mail Steamship Company. I take this opportunity to offer my services to the Institution. I remain, respectfully, : SANTIAGO AINSA. Professor Henry, \ Smithsonian Institution, Washington, D. C. San Francisco, Oa, August 26, 1863. Dear Sir: I have the pleasure to acknowledge your favor of July 31, and I take pleasure in complying with your request. In fact I intended to do this before, but, owing to many engagements on hand, I have been postponing it to this moment. y I announced in my last that the meteorite would be sent by the following steamer from that date; but we were asked to retain it some time longer by some scientific men, who wished to examine it closely. The history of this aerolite we have from our grandmother, Dofia Ana Anza de Islas, daughter of Don Juan Bautista Anza, our great grandfather. The | Jesuit missionaries had the earliest knowledge of this curiosity. ‘There were various theories entertained about it; but it was generally believed to proceed from some iron mine in the vicinity, which belief holds to this day in Sonora. In an expedition made by Don Juan Bautista Anza, then “Gran Capitan de las Provincias del Occidente,” about the year 1735, to the country about Tucson, he was induced to visit the aerolite, and he undertook the work of transporting it to Spain. The place where it was found is called “Sierra de la. Madera,” on a spot called Los Muchadios. Through the want of proper means and the bad state of the roads, (having to carry it to San Blas, then the uearest port of entry,) the work of transportation was given up, and they were satisfied to take it as far as Tucson. ‘There it remained ever since, until my brother, Agustine Ainsa, undertook to transport it, in 1860, and present it to the Institute. His intentions, however, were never carried out ‘antil May last, Wises aire ee SD ce i i = PROCEEDINGS OF THE BOARD OF REGENTS, 87 when another of my brothers, Jesus M. Ainsa, visited Sonora and brought it with him on his return. By the time of the receipt of this the aerolite must be already in Washington, as we delivered it to the agent of the Institute about a month ago, to have it transported to you. Your. agent spoke to us about expenses ; but we wish not to deprive ourselves of the honor of having presented it to the Institute, and as such we desire that you should accept it. I would be thankful if you would send me a copy of the analysis, and of other informat*on about the aerolite; and if you find it not too troublesome, to send the same, with my compliments, to St. J pea s College, Fordham, New York, where I was educated. I have the honor to remain, your obedient servant, SANTIAGO AINSA. JosePH Henry, Esq., Smithsonian Institution, Washington, D. C. [This meteorite is now in the museum, and is an object of special interest to visitors. ] LirTLeE GuLacE Bay, Care Breton, Nova Scortta, * October 25, 1868. My Dear Sir: I send you a specimen of “cone-in-cone,” which I have lately obtained in sinking a shaft at this place upon the Harbor Vein seam of - coal described in Professor Lesley’s report of this coal-field last year. It was found in the band that corresponds to the black bituminous shales below the one inch of cannel coal, and 23 feet above the Harbor series of five feet of coal. It was only obtained on the northwest side of the shaft, thinning out to the south and east, or towards the “crop.” The greatest thickness of the bed was about 7 inches. The largest “cone-in-cone’’ was 54 inches in diameter. The journal of the strata sunk through differs somewhat from Professor Lesley’s taken at the shore. ft. in. ueanedbtt-dxitt and ipravel..0e i) s2252e. Se Se oe ee 10.0 Blue shales, with cyclas shells, fish teeth, and other remains........ 3.0 Cone-in-cone s cloke id Scie eee eee eo Pee Leen CRO Haat eet tL aug sion a Brown band, with coprolites.........--...... LUE So Oks one 3 Blue arenaceous shales ......- Beeb deee ys tet foot Jen) gl ie ee 1.0 EMAIL RAT CBUOIC « < Saipabeaiakie Dek we leie oss sleek Ol IE 2.0 Seam penis ot shales “fucomMa? sor sek 22 ee Peo. ee ee 33 eee AAMT 34. 22. Ai RR Pe OU Mae SL DARREL es A een acontun shales 239 eos seis koe ised same CRU OE OST VEL on 2.6 Sandstone, black mark, like the fruit “‘cardeocarpon”’........---.--- 1.04 PINE EMN A hs [221 2). ce I eS RUE ee oe a I Sic ad DIMER ICRG), 2). 2s Glee ie. 28 IRE Ste ee SUC UE LC Ouck ec 3.10 IRENE 2 os): is wc as Se he I ee RPI cok LR s6 4 mesaesnd ironstone: ballse soos! 52. WAnae = 42 ois. s 2. 7.5 Rennes.) 492 1c). Sua 1S ad per er lara eras wie 5.5 41.11 I cannot find in any work that I possess anything exactly like them, so think they may be of interest to add to your museum. The points of the cones are downwards. ? 88 PROCEEDINGS OF THE BOARD OF REGENTS. . T shall be glad to hear from you about them after they have been examined. I have sent a specimen to Dr, Dawson, Montreal, but fear the season is too late for him to get it this year. I remain, my dear sir, your obedient servant, HENRY POOLE. JosEPpH Henry, Secretary Smithsonian Institution, Washington. The above relates to a very interesting specimen of a remarkable concretion of a clayey material, which occurs in thin slabs, entirely formed of cones, the axes of which are all at right angles to the parallel surfaces of the slabs. The only explanation which occurs to us of the mode of formation of this structure is that of percolation of water charged with earthy material through a porous rock, and filling a horizontal crevice with parallel sides, with a series of stalac- tites and stalagmites. es HUNGARIAN NATIONAL Museum, Pesth, October 15, 18638. Sir: In reply to your esteemed letter of the 29th of May, I have the honor to inform you that the birds sent us through Dr. Flugel have been duly re- ceived, and I beg leave to return the Hearth thanks oF our institution for the same. Full acknowledgments have also been made in our reports, and in the newspapers, of our obligations to the-Smithsonian Institution, which stands so high in public opinion everywhere. AUGUST V. KUBINYI, Director. JosePpH Henry, Esq., Secretary Smithsonian Institution, Washington. CuristTiaAna, Norway, November 4, 1863. Sir: Having been appointed director of the Ethnological Museum at the University of Christiana, I have perused a letter of the “6th May, 1862, from the secretary of the Smithsonian Institution to the secretary of this university. As this letter alludes to the endeavors of your excellent Institution for the collection of ethnological objects from North America, and the utility of estab- lishing a system of exchange for European curiosities, I have made use of the opportunity to offer you what we have in this line. The aboriginal population of this country are the Laps or Laplanders, living at present on vihe mountains and sea-coasts farthest north of Norway, Rovedent and Russia. ‘Their language proves them undoubtedly to be of the Mongolian stock in Asia, and, as such, related to the red man of America. ‘The Laps are a remarkable instance of this race, as they are converted to Christianity and have adopted the habits and industry of civilization, modified by the severity of the arctic climate in their country and their peculiar mode of subsistence as nomads with flocks of reindeer. We have procured a set of models made by the individuals of the people themselves, and illustrative of their present mode of existence. In offering this small collection for your acceptance, we hope that it may serve a scientific purpose in comparing the red man with his yellow brother in the old continent. If it should be in your power to afford us some correspond- ing objeets from your field of research, that is so immensely more extensive, a a ll PROCEEDINGS OF THE BOARD OF REGENTS. 89 ‘very great desideratum in our collection would be supplied that would engage our most earnest attention. The articles in question are— I. Three casts, in plaster, taken from living individuals, viz: 1, an unmixed Lap, 39 years old; 2, a man whose father was a Fin from Russian Finland, and whose mother was a Lap, 42 years old; 3, a man whose grandmother was a Swede, (of the Teutonic stock, ) Cihernine Lap, 43 years. If. Four photographie portraits: 1, mixture of Lap and Fin, 28 years; 2, 74 years; 3, 28 years; 4, 38 years—pure Laps. Iii. A reindeer, harnessed with its sledge. The sledge is canoe-shaped, so as to be able to move upon the deepest and softest snow whut going down into it. IV. A pair of snow-shoes, being very long pieces of thin onde with which the Lap can walk upon soft snow. They have straps or stirrups to put the feet into. ‘The man moves on with the staff. V. A pair of pack-saddles, with. which they move their luggage in summer on the back of the reindeers ; included is a model of a wooden tub and a cask ; two flat pieces of wood to lay across the back of the reindeer are attached. Vi. A trunk, in which is included the wooden bowl for preserving the rein- deer milk, and the press for making cheese out of it. VI. A spade for removing the snow. VIII. Two large wooden bowls. IX. A tent; in the middle the fireplace and two pots hanging over it; behind is a scaffolding of wood for their stores, raised upon poles, so that it may not be attacked by dogs. Confiding in your interest for the advancement of science, I remain, very respectfully, your obedient servant, LOUIS KR DAA. JosePH Henry, Esq., Secretary Smithsonian Institution, Washington. [These articles are now in the museum. |} KAISERLICHE-KGNIGLICHE GEOLOGISCHE REICHS-ANSTALT, Vienna, December 11, 1863. Sir: I have the honor to transmit to you for the Smithsonian Institution a series of tertiary fossils from the Vienna basin, viz: Seupmre On eria DEUS SL cern tesa ve.2 oa ett 2 Sata /se eo ae 3 6 species. Seanmne @erithium beds ts skeet 2s eee a oe 10 species. Sammie vearine beds... See FP Ee eee 270 species. Pporebe ei '.s. Cee RE A i es Meare Ree 286 species. In the box prepared to be sent you will find, 1, the present letter; 2, a sys- tematic éatalogue, with tabular reference to the localities; 3, a catalogue in which the localities are kept separate; 4, a guide of geographical reference for the localities. 'The number of specimens or lots in catalogue 3 is 622. Beside these there are a number imperfectly determined or not belonging to Austrian localities. The rest will give a pretty fair idea of the leading or type mollusca of our Vienna basin. The series here offered has been composed or selected under the auspices of Dr. Hérnes, director of the Imperial Museum of Miner- alogy, and he placed it at the disposal of our Imperial Geological Institute, so that I beg you will consider it as a joint offer from both establishments. I have the honor to be, dear sir, ever most truly yours, W. HAIDINGER. 9 PROCEEDINGS OF THE BOARD OF REGENTS. British Museum, December 30, 1863. Dear Sir: I have to acknowledge the receipt of your letter of this day’s date, and to acquaint you that the trustees have acceded to the request made by Professor Henry, on behalf of the Smithsonian Institution, and that I have instructed Dr. Gray to give you every facility with a view to such elecirotype impressions being made for that Institution as are required from our wood engravings illustrative of the conchology of the North American continent. I shall be happy. to see you, and to give you any assistance in my power when + — ever it may be convenient for you to call at the museum, as you propose. Believe me, dear sir, yours truly, : A. PANIZZI. Dr. P. P. CARPENTER. 31 PFEIDEMARKET, HampBure, February 4, 1864. Dear Sir: I duly received your very kind letter of the 6th of January, in- forming me that the director of the Smithsonian Institution would have the kindness to send me five of the American perennibranchiates for investigation. A few days afterwards the box was delivered into my hands, containing— 1. Menopoma Alleghaniense. 2. Menobranchus lateralis. 3. Siren lacertina. 4, Amphiuma tridactylum. 5. Siredon pisciformis. All these amphibia being of the greatest importance for my studies, I cannot but express to you my most sincere thanks for this most valuable assistance. You will allow meto pay to yourrenowned Institution, in the mean time, my thanks for the reports and other valuable works, particularly on the Zodlogy and Anatomy of Amphibia, published at Washington, and directed to me some years ago. I should feel most happy if you would give me a direction how I might pay my thanks in a more material manner. You will, therefore, oblige me very much by informing me of the desiderata in your collections. Perhaps there might be some European fishes or amphibia which I might be able to procure for you. Of sea snakes, which family of snakes I have described some years ago, there are also some few species in my own possession. In minerals I am pretty rich, having the best private collection of this branch that exists in our place. It is only on the supposition that I might be able to furnish to the Smithso- nian Institution some equivalent that I take the great, and, perhaps, immodest liberty to mention, that one specimen more of the genera amphiuma, siren, and menopoma, would be of the greatest importance for my studies. It would be very difficult to decide all the anatomical questions concerning the named amphibia after the investigation of only one specimen. Having the intention to describe in a comparative manner the bones, muscles, and nerves of the famous Salamandra Japonica, with relation to the other genera of Ichthyodea, I feel myself in a high degree advanced by the specimens which I owe to your kind- ness, and would be induced to hope that my little work might not remain quite imperfect, if there would be any chance to acquire still one specimen more of the above-mentioned three genera. Finally, you will allow me to say that I am not now in any connexion with the Hamburg Museum, as the address of your letter said, but that, though being on very friendly relations with the directors of our collections, I have given up my place among them. With the highest regards, I am yours, very respectfully, Dr. J. G. FISCHER. [The specimen requested was sent to Dr. Fischer.] PROCEEDINGS OF THE BOARD OF - REGENTS. 91 : Vienna, February 9, 1864. My Dear Sir: Permit me to enclose here an invitation to join in a subscrip- tion for a gold honorary medal to be presented to our most worthy Professor Ch. Fr. Ph. von Martius, of Munich, on his fiftieth anniversary of medical dociorship on the 30th of March, 1864. Our most honored friends on the other side of the Atlantic should not fail in the list; only I am sorry that by various impediments I was prevented from * writing at an earlier period. It is now’so late that only by very good luck it will be possible that an answer may arrive previously to the 15th of March, to be entered in the first list which must be printed, embellished, and then bound up, and sent to Munich from Vienna before the 30th of March. Whatever is brought to notice later than the 30th will be appended, and what comes to hand after the 30th up to the end of June will be given in the first complementary report to be published on the 1st of July. Nothing will be lost, as even what comes after that period will be published afterwards. Every subscriber, of course, will have a bronze copy of the medal, and the votary tablet sent to him. Subscriptions should be three florins Austrian silver money, or more, which is about one and a half dollar American silver. By this time you may already have received our last box with tertiary fossil types of several localities of the Vienna basin, being a joint parcel from the Imperial Mineralogical Cabinet and our own Geological Institution. I am happy to hear you have now the Ainsa Tucson meteoric iron. I shall send some of these days a paper of mine on the Carleton Tucson, which ap- peared in the Vienna Academy Proceedings. I enclose impression from the surface, cut, polished, and etched, and galvanographed positively and negatively. We shall be happy, as soon as you may fix on cutting some slices off the block, to receive a bit from you for our Imperial Mineralogical Museum of the Ainsa Tucson too. With all the most cordial wishes, ever most truly yours, W. HAIDINGER. Professor JosePH HENRY, Secretary to the Smithsonian Institution, Washington. Orrice Hupson’s Bay Company, Montreal, February 26, 1864. My Dear Sir: Absence from home and subsequent indisposition have pre- vented my acknowledging receipt of your letter of 19th ultimo at an earlier date. The settlement you have made of Mr. Kennicott’s account is quite satisfac- tory. There was a small deficiency in consequence of a change in the rate of exchange when your draft reached me}; but that matter can be arranged when we receive Mr. Mactavish’s final statement of Mr. Kirkby’s account. The kind expressions of thanks contained in your letter are very gratifying. We have always felt pleasure in promoting scientific research; but, in Mr. Kennicott’s case, this was enhanced by his amiable character and prudence. It is no easy part to play, going as a stranger into a territory inhabited by men bound to a foreign government, and with exclusive views on many points. But Mr. Kennicott knew how to meet the circumstances ; and from his arrival among us until his departure was always popular, and I believe inspired a sincere friendship and esteem among those with whom he most associated. If in Washington, pray offer him my kind regards. Hoping some day to have the honor and pleasure of forming your personal acquaintance, believe me, sir, very truly yours, EDW. M. HOPKINS. JosePpH Henry, Esq,, Smithsonian Institution, Washington, D. C. ——————————————————— 7 —_— ——_—__ + GENERAL APPENDIX REPORT FOR 1863. The object of this appendix is to illustrate the operations of the Institution by reports of lectures and extracts from correspondence, as well as to furnish information of a character suited especially to the meteorological observers and “ other persons interested in the promotion of knowledge. LECTURES. BRIEF ABSTRACT OF A SERIES OF SIX LECTURES ON THE PRINCIPLES OF LINGUISTIC SCIENCE, DELIVERED AT * THE SMITHSONIAN INSTITUTION IN MARCH, 1864. BY WILLIAM D. WHITNEY, PROFESSOR OF SANSKRIT IN YALE COLLEGE, NEW HAVEN, THE scientific study of language is of modern date. Only its scanty and im- perfect germs are to be found in ancient times. It lacked that wide and com- prehensive basis of observed and collected facts on which alone such a science can be founded. The active and searching curiosity of the past century, with the facilities for investigation given by trade, travel, and philanthropic effort, could not but call it into being. No single circumstance has so powerfully aided its development as the introduction of Sanskrit to the knowledge of Hurope. This, the most ancient and primitive of Indo-European tongues, laid the sure foundation of the comparative philology of the Indo-European family, out of . which has ‘grown the general science of language. The objects of this science are twofold: 'l'o discover the nature and history of language itself, and to elicit information respecting human history. Both are invested with q very high degree of importance. The value of language to man, and the absorbing interest of inquiry into its character, are palpable, and attested by the labors and speculations of generations of scholars and thinkers. It has also quite recently been found that language is the principal means of ethnological investigation, of tracing out the deeds and fates of men during the prehistoric ages. Not only does it determine the fact and the de- gree of relationship among nations, but it gives information which can be ob- tained in no other way respecting their moral and intellectual character, and the growth of their civilization. Linguistic science, as a branch of the study of human history, embraces the whole race at every period of its history. All spoken or recorded speech is its material. The dialects of the lowliest as well as the most highly endowed races are its care. It would fain hold up and study every single fact in the light of every other related fact, since only thus can all be fully understood. To survey in detail, in these lectures, the whole field of linguistic science will be, of course, impracticable. We can only attempt to lay down and illustrate its fundamental principles, to gain some insight into its methods, to determine the nature and force of linguistic evidence, to see how this is elicited from the material containing it, to note its bearing on historical and ethnological study, and to review briefly the principal results hitherto obtained by its means The method followed will be the analytic, establishing principles from facts 96 PRINCIPLES OF LINGUISTIC SCIENCE. within every one’s apprehension, and proceeding from that which is well known or obvious, to that which is more obscure. Illustrations will be sought, mainly from among the phenomena of our own familiar speech, since every living and growing language has that within itself which exemplifies the facts and princi- ples of universal application in all language. We shall also avoid, as much as possible, the use of figurative, philosophical, and technical phraseology, and talk the language of plain fact. Our preliminary inquiry may properly be, Why do we, ourselves, speak Eng- lish? ‘Though a simple question, its correct answer will clear our way of many difficulties. The general reply is obvious: We learned English from those among whom our earliest years were passed. We did not produce the words we use by an internal impulse, by the reflection of phenomena in our consciousness, and the like. As soon as we were able to associate an idea and its uttered sign, we were taught to stammer the names of the most familiar objects, and our instruction advanced with our capacities ; our notions and con- ceptions were brought into shapes agreeing with those they took in the minds: about us, and were called by the names to which these were accustomed. Cer- tain liquids which we saw, colorless and white, had not to be studied and com- pared by us in order to the invention of a title for them. We were informed that they were “ water” and ‘‘milk.”’ The one of them, in certain modes of oceur- rence, we were made to know as “ puddle” and “river.” The words ery, strike, bite, eat, drink, love, hate, and so on, were taught us by being applied to acts and states of which we made experience. Long before any mental analysis of our own would have given us the distinct ideas of trwe and false, they were im- pressed upon our minds by admonition, or something stronger. ‘The ap- pellations of hosts of objects, places, beings, which we had not seen, and per- haps have not yet seen, were fixed in our minds, with the means of attaching some distinctive idea to them. The amount and kind of this training varied greatly in different cases, but we all had it, and by it alone could learn to talk as we do. Language was the first step in our education. It came by educa- tion, and not by inheritance. English blood would never have given us Eng- lish speech. We could just as easily have learned to say wasser or eau as “‘ water,” milch or lait as ‘‘ milk,’ lieben or aimer as “ love,’ &e. An American child is brought up by a French nurse in order that it may speak French first, and it does so. ‘The infant cast on shore alive from a wreck learns the tongue of its foster-parents, and no outbreak of natural speech ever betrays whence it derived its birth. The imported African forgets, in a generation, his Congo or Mendi, and is able to use only a dialect of his master’s speech. It is already clear, then, that English people do not, as some have paradoxi- cally maintained, speak English by inherent natural gift, because they are English, just as all swallows twitter, all bears growl, all lions roar, and so*on. The special forms of spoken language are matters of imitation. 'They are kept up by usage, and transmitted by oral tradition. We thus learn, not English simply, but the particular kind of English which is spoken by our instructors. A few, perhaps, get nothing from the outset but the purest style of the language; but hardly any can escape some tinge of local dialect, of the slang of caste or calling, even of individual peculiarities of our teachers, inelegancies of pronunciation, pet phrases, colloquialisms and vul- garisms, and the like. Often errors and infelicities thus acquired in early life are ineradicable by all the care of after years. Again, this process does not give us universal command of the resources of the language. A child’s vocabulary is very scanty, and goes on increasing to the end of life. The encyclopedic English tongue, as we may call it, contains over one hundred thousand words. Of these, the most uninstructed classes ac- quire only three to five thousand, a frugal stock of the most indispensable words and phrases. ‘To such a nucleus every artisan, in every walk of labor, must PRINCIPLES OF LINGUISTIC SCIENCE. 7 add his own technical language, containing much which most English speakers know nothing of. No small portion of the one hundred thousand words is made up of such special vocabularies. ‘The generally educated man learns much of many of them, but no one learns them all. Every one may find, on every page of our great dictionaries, words which he knows not how to deal with. There are various styles of expression for the same thing which are not at every one’s command. Even the meanings attributed to the same words by different speakers are different. The voluptuary, the passionate, the philosophic, and the senti- mental, for example, mean very different things by “love’’ and “hate.” It is no paradox to maintain that, while we all speak English, no two among us speak precisely the same language, the same in extent, form, or meaning. What, then, is the English language? It is the aggregate of the articulated signs for thought current among the English people ; or, itis their average, that part which is supported by the usage of the majority—a majority counting not by numbers only, but by culture. It includes varieties of every kind; but it has unity, from the fact that all who speak it may, to a considerable extent, and on matters of the most general interest, talk so as to understand one another. It is kept in existence by uninterrupted tradition, in which each individual takes a part, handing down his portion of it, with his limitations and peculiarities— books, a kind of undying individual, greatly assisting in the process. But all traditional transmission is inherently and necessarily defective, and that of language forms no exception. If English were a certain fixed body of words, learned complete by every one, and kept intact, it might more easily be preserved from alteration. As the case stands, it does not remain the same from genera- tion to generation. Its most noticeable mode of alteration is that whichis ever going on in its vo- cabulary, especially its technical vocabularies. New processes ,and products, new views and opinions, new knowledge of every kind, must find their fit ex- pression. No well-informed man can write a chapter now upon what every one _is thinking and talking of which would be intelligible to the well-informed man of acentury ago. There are also changes affecting rather the form than the content of language, of slow progress, and in their inception, in great part, inac- curacies of speech, opposed by the conservative forces, yet as inevitable in the end as the others. They show the influence of the great numerical majority who do not speak with correctness, but whose errors finally become the norm of the language. Thus, we had formerly a special preterit form spake, and good speakers would as soon have said “he come and done it” as “‘ he spoke to me.” Now only spoke is in common use. Three centuries ago we had only Ais as possessive of both de and zt, but popular usage struck out a new possessive, ats, for the latter. You we employ not only as object, according to its ancient usage, but as subject, instead of ye, &c., &c. The influences which brought about such changes are still to be seen in full operation about us, especially among children and uninstructed persons, to whom the communication of the language is imperfectly or incorrectly made. A child substitutes an easy for a hard sound in pronouncing, drops out a syllable or two from a half-under- stood word, says “I bringed” or “I brang” for I drought, says “mang” and “‘mouses,” says “ gooder” and ‘“ goodest,’”’ and the like. Its own and others’ care corrects these errors; but if the caré be wanting, the error remains ; and there are ever in existence, among the lower strata of language-users, hosts of these deviations from correct usage, always threatening, and sometimes suc- ceeding in making their way to the surface, and securing recognition and gen- eral adoption. he conservative forces arrayed against them, aided by school instruction and reading, are now so powerful among us that the language changes but very slowly in this way, yet the examples given are truly typical, and illustrate a force always in action. That, in these and other methods, lan- guage actually undergoes notable change is palpably true. Go back only to 7s oR. PRINCIPLES OF LINGUISTIC SCIENCE. our Bible translation, to Shakspeare, and much is found which is no longer good English. Go back five hundred years, to Chaucer, and our own tongue is only partially intelligible to us. Another five hundred years carries us to the Anglo- Saxon of King Alfred, a totally strange form of speech, as much so as the modern German; and yet each one of the thirty or forty generations between us and Alfred was as singly intent on transmitting to its successor the language it received from its predecessor as is our own. ‘These facts and conditions are of universal occurrence in linguistic history. All language is handed down in the manner described, and is subject to the ‘same disturbing forces. The process of transmission always has been, and al- ways will be, imperfect. No tongue remains the same during a long period-of time. This is the fundamental fact on which rests the whole method of lin- guistic investigation. ; We see now what is meant when language is spoken of as having an inde- pendent existence, as being organic, or an organism, as growing or developing, and soon. ‘These are only figurative modes of speech. Language-has no ex- istence, save in the minds and mouths of those who employ it. It is an aggre- gate of signs of thought, deriving their significance from the intelligent agree- ment of speakers and hearers. It is in their power, and subject to their will. As they maintain it in existence, so their consenting action modifies and alters it. It cannot be changed hastily or capriciously, because it depends upon gen- eral consent, which can be won only for such modifications and extensions as are in accordance with its already established rules. Individuals are constantly trying experiments of alteration upon it, with childish errors of expression, with bad grammar, with slang, with artificial turns of phrase, and arbitrarily coined words. But these are, for the most part, only laughed at as blunders, or put down as mannerisms and vulgarisms. ‘Individual authority, except in special cases, is too weak to force itself upon public opinion. The speakers of lan- guage constitute a republic, in which authority is conferred only by universal suffrage, and for due cause. High political rank does not give power over speech. ‘The grammatical blunders of an emperor do not become the: rule to his subjects. But individuals are allowed to introduce novelties and changes into the general speech; thus, for instance, to name their own inventions or discoveries, if they do it discreetly and suitably ; and great masters of the art of speech, poets, orators, are permitted to touch even the more intimate and sacred parts of language. Is it cailed for? is it in accordance with the usages and analogies of the language? is it offered or supported by good authority !— such are the considerations by which, in any given case, general consent is won or repelled, and this decides whether the proposed change shall be te- jected, or shall become part and parcel of the universal speech. As, then, an organic being grows by the gradual accretion of homogeneous organic matter, as its existing parts and processes form the new addition, in order to help the life and functional action of the being, so language extends by the addition of material accordant with its substance, evolved by its formative methods, and intended to secure the end of its existence, the expression of the thoughts of those who speak and write it. It thus presents striking and in- structive analegies with organic life ; but to call it an organism outright, as some do, and to claim that its growth is independent of human agency, and that its study is, therefore, to be ranked among the physical sciences, is palpably and seriously to misinterpret it. Language is an institution, constantly undergoing, at the hands of those who use it, adaptation to their varying circumstances and needs. Between all determining causes and their results in its development stands, as middle term, the human mind, seeking and choosing expression for human thought. Its every partis ahistorical product. Its study is a historical * science, a branch of the study of the human race, and of human institutions. PRINCIPLES OF LINGUISTIC SCIENCE. 99 As every constituent item of language is the product of a series of changes, working themselves out in history, the method of linguistic investigation must be historical. ‘l’o understand the structure and character of speech, and to penetrate to its origin, we must follow backward the modifying processes to which it has been subjected, endeavoring to understand the influences which have produced and governed them. ‘This can be done to but small extent by means of contemporary records.. We must call to our aid the art of etymological analysis. On etymology, the tracing out of the history of individual wortls, is founded the whole science of language. ‘To illustrate the methods of etymolo- gizing, and to bring to light some of its results, by simple and characteristic examples, is the object of this second lecture. Let us look first at evidence showing the composite nature of words. We are all the time putting together two words to form a compound; as, fear- wmspiring, god-like, house-top, and so on. But the extent to which language is the result of such composition is apparent only on deeper study. Fearful is as clear a compound, on reflection, as fear-inspiring ; yet ful is, to our appre- hension, a kind of. suffix, forming a large class of adjectives from nouns, like the suffix ows, (in peril-ous, riot-ous, &c.;) and its independent origin and meaning are but dimly present to the mind of one who uses the adjectives. Fearless and its like are not less evident compounds; but the ess here is not our word Jess, but the altered form of an older word, meaning “loose, free.’’ Again : ly, in godly, brotherly, &c., is of yet obscurer origin, and we deem it merely a suffix; but a study of the other forms of our language, or a compari-_ son of kindred Germanic dialects now spoken, shows it to be descended from the adjective Zzke, which has been used in all the languages of our family as an adjective-forming suffix; we alone have given it the further and now re- motely derived office of adverbial suffix, employable at will to convert any adjective into an adverb. The d of such words as I loved, I hated, is proved by the form it wears in the oldest Germanic tongues to be a relic of the past tense did: I loved is originally I love did. Sueh and which were once so-like. and who-like, and so on. The same is the case in the Latin part of our lan- guage, and even in its oldest and most essential constituents. The de or ple of double, triple, and so ‘cn, is the root plic, meaning “bend, fold ;” triple is the precise etymological equivalent of three-fold. The two letters of am, which seems as simple a word as aught can be, are relics of two elements: one, the root as, meaning “be ;” the other, the pronoun mz, meaning “me, 1;” am stands for as-mz, “be-I.”’ The third person, 7s, has lost the whole of a second lement, 22, which it once possessed, and of which at least the ¢ is left in nearly 1 the kindred languages ; compare German is¢, Latin est, Greek esti, Sanscrit asti, &c. With few exceptions, all the words of our language admit of such analysis, which discovers in them at least two elements: one radical, containing the fundamental idea; the other formal, indicating its restriction, application, or ‘relation. ‘This is, in fact, the normal constitution of a word; it contains a root and a suffix or prefix, or both, or more than one of both. Thus, inapplicabili- tres contains two prefixes and three suffixes, all clustered about the root pic, “bend ;” and it is, as it were, the fusion and integration of the phrase “ nume rous conditions of not being able to bend or fit to something.” Our examples show that word-analysis is, at least in part, only the retracing of a previous synthesis. We are as sure of the actuality of the process of com- bination by which these words were formed as if it had all gone on under our own eyes. There would have been no such suffixes as :fwl, less, ly, &e., if there had not been before in the language the independent words full, loose, like, &c. No small part of the formative elements of our language can thus be proved descended from independent words ; if a considerable part do not admit like proof, we are not authorized to suppose that their history is different 100 PRINCIPLES OF LINGUISTIC SCIENCE. from that of the others, but only that we have not at command the evidence which would explain it. ! The same examples show not less clearly that alteration, corruption, and mutilation of the products of combination is a rule of the life of language. The reason of this corruption lies in great measure in the fact that, having once struck out a compound, we are not solicitous to keep up the memory of its descent. We accept the word coined as a conventional sign for the idea which it conveys, and give our attention mainly to that. Hence ease and con- venience in the use of the word are consulted; a long vocable is contracted; a hard combination of consonants is mouthed over into more utterable shape; subordinate elements are defaced into conformity with the inferiority of their consequence. So the sailor says bos’n for boatswain, to’gal’nts’ls for topgal- lantsails, &e. This is a part ofthe wise economy of speech, a sign and means of the integration of words, contributing to conciseness and vigor of expression. But it is also a blind tendency, and its effect is in part destructive. It leads to waste as well as economy; ease and convenience being consulted by the sacrifice of what is valuable as well as the rejection of what is unnecessary— if, indeed, it can truly be said that a people not undergoing degradation of character ever sacrifices anything of its language which is really valuable with- out providing an equivalent. A language may thus, at any rate, become greatly altered, giving up much which in other tongues is retained and valued. Our own English offers one of the extremest examples known of the prevalence of these wearing-out tendencies. Thus, for instance, the primitive language from which our own is descended had a full set of terminations for the three persons plural of the verb, viz: masz, tasi, nti—e. g., lagamasi, lagatasi, laganti, “we lie, ye lie, they lie.” In Latin they appear shorn of their final vowel, as mus, tis, nt. In Gothic, the oldest Germanic language, they are reduced to their initial consonants only, m, th, nd—thus, ligam, ligith, ligand. They are still, in this form, pretty distinctive, and sufficient for their purpose. But the prevailing custom of ex- pressing the pronouns along with the verb lessened their necessity} and in Anglo-Saxon they are all reduced to a single form, ath in the present, on in the imperfect. We, finally, have cut them off entirely, and say we lie, ye he, they lie, without any endings designating the person. In the declension of nouns we have effected a revolution not less thorough. Our ancient mother-tongue declined every noun substantive in three numbers, with eight cases in each, and every adjective in three genders besides. With us all adjective declension has disappeared, and of substantive declension we have saved only a genitive and a plural ending, both s. In a few plurals, bs men, mice, teeth, we have seized upon a distinction at first enphonie and acci- dental only, and have made it significant. So also in the conjugation of our “irregular” verbs, as sing, sang, sung ; the change of vowel was at first merely euphonic, then became, as in most German dialects it still continues, auxiliary to the sense, and finally, with us, it is in many cases the only means of dis- tinction of present, preterite, and participle. In one remarkable case, the wearing-out processes have led to the total abandonment of a conspicuous department of grammatical structure. A dis- tinction of gender in nouns, as masculine, feminine, or neuter, marked by dif- ferences of termination and declension, has ever prevailed in the family of lan- guages to which ours belongs. Even in the Anglo-Saxon, nouns were still masculine, feminine, or neuter, not according to their natural character, but in conformity with the ancient tradition, on fanciful grounds of difference, which we find it excessively difficult to trace out and recognize. But in the exten- sive decay and ruin of grammatical’ forms attending the elaboration of modern English from Anglo-Saxon and Norman French, this whole scheme of artificial PRINCIPLES OF LINGUISTIC SCIENCE. 101] distinctions has disappeared, leaving almost no trace behind. Natural gender has replaced grammatical, and the pronominal forms he, she, it, his, him, her, its, are our only means for its indication. These two processes—the production of new forms by the combination of old materials, and the wearing down and wearing out of the forms so produced, are the principal means by which the external life and growth of language are kept up, by whose operation spoken tongues are constantly becoming other than they were. But they are only auxiliary to a not less striking growth in the interior content of specch, in the meaning of words. It is as important a part of the historical study of a word to trace out its changes of signification _as its changes of form; and the former are even richer in curious and unex- pected developments, are fuller of instruction, than the latter. The internal content of language is plastic to the touch of the inspiring mind. But for this, no variability of form or facility of combination could make it aught but a stiff dead structure, incapable of supplying for any time the needs of a think- ing, feeling, observing, and reasoning community. ‘Old words are applied to new uses; the general is individualized, the individual generalized; the con- crete becomes the’ abstract; a pregnant expression, a startling metaphor, is reduced to the level of an ordinary phrase; delicate shades of meaning are dis- tinguished by the gradual differentiation of synonymous words, and so on. ‘The rate at which these processes of change go on is very various. It de- pends, in part, upon subtle and recondite causes, as upon the individual char- acter of different languages and the qualities of the peoples who speak them— qualities, perhaps, which exhibit themselves only in this way, and hardly ad- mit of analysis and recognition elsewhere. In part, it depends also upon ex- ternal circumstances, upon change of surroundings and mode of life, of mental and physical activity. An English family, wrecked on a coral island in the south seas, would soon find a great part of its vocabulary useless, and in a very few generations its language would have become vastly impoverished. A tribe from such an island, again, if suddenly transferred to the midst of northern variety of clime, product, and occupation, would have to expand rapidly its store of speech to keep pace with the growing wealth of its expe- riences. As regards grammatical change, all that assists the purity of linguistic tradition tends to keep language the same; so, especially, culture, literature, the habit of instructién. Careiul and pervading education reduces to a mini- mum that immense and most important class of changes which begins in popu- lar inaccuracies. On the other hand, the intermixture of races of diverse speech, rendering necessary the elaboration, by mutual compromise, of a new dialect for common use, tends powerfully to the disorganization of grammatical structure. It is such a course which has made of our English the language which, above all others, has yielded up most of the grammatical fabric which was its birthright and inheritance. The processes of alteration illustrated in the last lecture are familiarly spoken of as going on in language itself, like fermentation in bread, or deplacement and replacement in animal tissues. But it must not be forgotten that every Separate item of change is the work of an individual or individuals. In lan- guage, the ultimate atoms at work are not dead matter, but intelligent beings, acting fora purpose. Lach, indeed, acts unpremeditatedly, and for the most par unconsciously ; each only wants to use the common possession for his own enefit, at his own convenience; yet cach is also an actor in the great work of preserving and of shaping the general speech. Now, the infinite diversity of circumstances and of characters in the speakers of language tends toward infi- nite diversity in their action and its results; each would, acting independently, impress upon its progress a somewhat different course. Linguistic develop- y 102 PRINCIPLES OF LINGUISTIC SCIENCE. ment is thus the product of an infinity of divergent or ¢entrifugal forces. . The great centripetal foree which holds them in check, and combines them into a single direction, is the necessity of communication. Man is no soliloquist, and that would not be language which was understood and employed by one only. Each person is, in his own way, engaged in modifying language, but no one’s action shapes the general speech unless it be accepted by the rest and become common usage. Hach community must speak alike; whatever changes their tongue may undergo must be ratified and adopted by them all. Communication being thus the force which produces uniformity of speech, it is clear that whatever narrows communication and tends to isolate communities favors separation of a language into dialects ; whatever extends communication and expands the limits of communities, tends to preserve language homoge- neous. When a race is confined within narrow boundaries, however rapidly its tongue may undergo the inevitable: processes of change, all will learn from each and each from all, and they will continue to understand one anothér. But if the race grow rapidly in numbers, spreading over region after region, and sending out distant colonies, only favoring circumstances and conditions can preserve its unity of speech. In a low state of civilization’ a maintenance of the bonds of community over a wide area is impracticable; the tendency is to clannish feeling, to separation into tribes; and multiplicity of dialects is the natural consequence. Culture and enlightenment give a wonderful cohesive force ; political. unity, national feeling, community of traditions and faith, make strongly in favor of linguistic unity also; a traditional literature helps yet more powertully to the same result; but, most of all, a written literature, and a sys- tem of popular instruction. ‘The same causes which restrict the variation of language in time, from generation to generation, restrict it also in space, from region to region. Moreover, as community occasions and preserves identity of speech, so it also has power to bring identity out of dissimilarity. The fusion of communities causes the fusion of their forms of speech; the multiplication and strengthening of the ties which bind together the sections of a people makes for the effacement of differences already existing, the assimilation of dialects, and the production of homogeneous language. Both classes of influences—those which lead to diversity and those which produce assimilation—are always at work, and a consideration of their joint and mutual acjion is necessary to the explanation of the history of any lan- guage, or family of languages’; but the former are more fundamental and in- separable from linguistic growth; the latter are more external and incidental, more varying in their mode and scale of operation. Language everywhere tends to diversity, but circumstances connected with its use check, control, and even reverse the tendency. ‘The division of a formerly homogeneous language into dialects has been the rule in human history; the extinction of dialectic differences, whether by the extinction or fusion with others of the peoples em- ploying them, or by extension of the sway of single dialects, has been the ex- ception, connected with the great facts of history, as the spread of empire and civilization under the auspices of certain races. Misled by a too exclusive at- tention to facts of the latter class, one or two modern authors of high rank have been guilty of the paradox of holding that infinite dialectic division is the normal primitive state of language, which tends to coalescence and assimilation. A greater and more pernicious error could hardly be maintained. ‘The principles h@re laid down teach us how we are to proceed in classifying and arranging the infinity of tongues now prevailing on the earth. Many of them, at least, are the divergent branches of more original stocks. Languages are to be grouped by their affinities: we are to rank together first those which ; PRINCIPLES OF LINGUISTIC SCIENCE. 103 * are of closest and most evident relationship, and gradually to extend our scheme till we have done all which the nature of the case permits ; tifi the evidence on which we found our classification fails us. That the slightly distinguished forms of speech prevailing in the different sections of our own country, and even the more notable dialects which are to be found among the lower orders of population in the British isles, constitute together a single language, is too evident to call for proof. Let the man most ignorant of history go about the world, from British colony to colony, finding here and there, on coast and island, in fortress and city, communities of English- speaking people, and he will not think of doubting that they were all scattered thither irom a common centre, and have their common language by community of linguistic tradition. A like conclusion is almost equally palpable when we seek after kindred for our language on the continent of Kurope. There is a large class of evidently related dialects, occupying the Netherlands, Germany, Denmark, the Scandinavian peninsula, and Iccland, which a very little study ‘shows us to be akin with the more important half of our own tongue, that which comes to us from the Anglo-Saxon. There is another large class in southern Europe, comprising the French, Spanish, Portugticse, Italian, Rheto- Romanie, and Wallachian, which exhibit an equally clear connexion with the non-Saxon part of our familiar speech. If we say true, while the Dutchman says ¢rouw, the German ¢reu, the Swede and Dane tro, &c., it is because we have all received the same word in the same sense by uninterrupted tradition from some community which used a form coincident with one of these, or nearly resembling them all. So, also, if we say verity, while the Frenchman says verité, the Italian verztd, the Spaniard verdad, &e. Recorded history, in fact, fully explains the descent of this latter class of languages from a single mother, the Latin, as it also makes clear why our English is composed of. materials derived from both classes. What recorded history does not explain is the more recondite, but not less undeniable evidence of relationship which we dis- cover between these two classes themselves, as well as between them both and most of the other languages of Europe, together with some of those of Asia. These are, namely, the Greek, ancient and modern; the Slavonic, occupying Russia, Poland, Bohemia, Servia, and other provinces in the eastern part of Austria and the northern of Turkey; the Lithuanic, around the southern shore of the Baltic; the Celtic, of which the scanty remains are now found in Ireland, the Scotch highlands, Wales, and Brittany; and, outside of Europe, the tongues of Iran, as the Persian, with its ancient and modern congeners, and its remoter kindred, Kurdish, Armenian, Afghan, and Ossetie; and, finally, the languages of India, the Sanscrit and its descendants. These various branches go together to make up the great family of related languages which’ we call the Indo-European. Their relation to one another is ‘the same in kind with that of the various Germanic dialects, or the Romanic, and differs only in degree. The resemblances and coincidences which they exhibit are explainable only upon the hypothesis of a common linguistic tradi- tion; their differences are fully accounted for by their divergent growth and development during the ages which have passed since their separation. A few selected specimens of their accordance will be enough to give here, as their relation is now a matter of general knowledge, and few or none are found to doubt or deny it. Examples of words corresponding in all or nearly ail the branches are as follows (the equivalent words in two or three unconnected languages are also added for the sake of more fully exhibiting the value of the coincidences) : 104 PRINCIPLES OF LINGUISTIC SCIENCE: . ' Two. | Three, Seven. Thou, | Me. | Mother. | Brother. | Daughter. | | | Germanic -£2 22 2. - | Twa, | Thri Sibun. Thu. Mik. Muoter. | Brothar. | Dauhtar. Lithuanic ..--.....-.- Du. | ‘Tri | Septyni. Tu. | Manén. | Moter. Brolis. Dukter. Slavonic | Tri, | Sedmi. | Ti. | Man. Mater. | Brat. Dochy. a a a 5 caks| | ‘Tri. Secht. | Tu, Me. Mathair.| Brathair. | Dear. Latin - -- | ‘Tres, , Septem. | Tu. Me. Mater. Prater. | | - 2 cee. Greate 22: | Treis, Hepta. | Su. Me. Meter. Phrator. | ‘Thusatep. RATBIAR fae iajcn doin > y, Tri | Hapta. Tum. | Me, AT AT Se!) aicip iit in | eee Sanscrit Tri Sapta. Twam. | Mé. Matar. Bhratar. | Duhitar. Avabie 011). 19.700 | Ithn. | Thalath. | Sab’, Anta. | Ana. | Umm. | Akh. Bint. atisigh= oof. S25 | Iki. | Uch, Yedi. Sen. | Ben. | Ana. Kardash. | Kiz. Hungarian .-........| Ket. | Harom. | Het. Te: | Engem. | Anya. Fiver. Leany. \ 1 But, to the historical student of language, correspondences of grammatical structure are more unequivocal signs of near relationship than ¢orrespondences of words, being less exposed to imputation of accidental origin. As striking and convincing an example of this kind of evidence, perhaps, as any other is furnished in the inflection of the verbal tenses, as follows: Ihave. | Thouhast. | He hath. | Wehaye. | Ye have. | They have. ———— $s | —_ — | | SeSESSSSSSSSSSSSSFSFeMs MeUMgMS Fe sees Sas v eos cess 3 Haba. Habai-s. Habai-th. | Haba-m. Habai-th. | Haba-nd. NEA WANNG. sce coc aceon sonia sje ein —mi. -si. ti. —me. -te. -ti. RIAVORIO Seth oslo cemanlsacticee se —mi. —si. ti. —mu. -te. —nti, (COLIC eye ok Parisien boa tem eome ee mind |U8 2 Soe ee -d. —m. -d. -t. MATES oe ape Siar oie Sle in serena mers Habeo. Habe-s. Habe-t. Habe-mus. | Habe-tis. Habe-nt. Greek, (dialectic)../2: cn. bans —mi. si. -ti, —mes. —te. —nti, Persian, (modern) .-....-....... =Mpds See ee ae -d, -m. -d. -nd, BaNECiatee eet e hora teehee =mi. =si. -ti, —masi. -tha. -uti. These are specimens, taken from among a host of others which crowd every part of the grammar and vocabulary of the languages in question, and their convincing weight it is impossible to deny. It is certain that at some time in the past, and in some limited region of Asia or Europe, there lived a tribe from whose rude speech have descended all those rich and cultivated tongues now spoken and written by so many great nations of both the eastern and western continents ; but to know just where and when is beyond our power. The claim often set up that the home of the family was in the northeastern part of the Iranian plateau, not far from the mountains of the Hindu-Koh, rests upon no sufficient grounds. he traditions of no race reach back far enough to be authoritative upon such a point. Nor is the testimony derivable from language more conclusive. And to define, even with distant approach to confidence, the time which the tongues of the family must have occupjed in running their career of development is wholly impracticable. That the time of Indo-Euro- pean unity must have been thousands of years before Christ is very certain. Recent discoveries are proving that man’s antiquity is much greater than has hitherto been usually supposed. Respecting the origin of particular races our knowledge is likely ever to continue exceedingly indefinite. As to the grade of civilization and mode of life, however, of the Indo-European family before its dispersion, their language gives us reliable, though incomplete, information. Words which are found in the speech of all the separated branches must have appertained to the mother tongue, and must imply the knowledge or possession, in that primitive period, of what they indicate. By such means we learn that the tribe was not nomadic, and that it addicted itself to agriculture and the raising of cattle. It reared our chief domestic animals. The region it inhabited was varied, and not near the ocean; its most marked season was winter. Barley, and perhaps wheat also, was raised for food. Certain metals were worked, perhaps iron among them. Weaving was practiced. ‘he arms of offence and defence were those usual among primitive peoples—the bow, sword, PRINCIPLES OF LINGUISTIC SCIENCE. 105 spear, and shield. Boats were built and managed by oars. The political organi- zation was probably that of petty tribes. The relations of the family were well and distinctly established. Some of the stars were noticed and named; the moon was the chief measurer of time. The religion was polytheistic—a worship of the personified powers of nature, and its rites were practiced without a priesthood. The present lecture is to be devoted to the further consideration of the Indo- European family, to a brief exposition of its importance, and of the special interest attaching to its language, and to some account of the history of the latter. One source of the especial interest which we feel in Indo-European speech is found in the fact that our own language is one of its branches. This would call for and justify a particular attention to it on our part, even did it lack claims to the same from men of other races. But it does, in fact, possess such claims, and that partly by reason of the historical importance of the peoples which speak it, and their superior gifts, which lend prominent value to inquiries into a matter which illustrates both. Since the first rise of the Persian empire, the various branches of this family have borne a leading part in the drama of universal history. Greece, however, the bitter foe and final conqueror of Persia, was the chief founder of Indo-European greatness, and the most brilliant ex- ample of Indo-European genius; in art and literature what the Hebrew race has been in religion, and exerting an influence as unlimited in space and in time. Rome next, inheriting the fruits of Gréek culture, gained the empire of the world, and impressed upon all nations a political and social unity. Chris- tianity itself, rejected by the Semitic race among whom it appeared, was taken up by Indo-Europeans, and added a new bond of unity, a religious one, to the ties by which Rome bound the world together. The Germans were mainly instrumental in overthrowing the power of Rome; they gave monarchs to nearly every throne in Hurope, and infused new blood into the effete populations; but their devastations ushered in a period of darkness, during which it seemed for a time as if the Semites, inspired with the fury of a new religion, (Mobam- medanism,) were to succeed to the empire of humanity. With their repulse and downfall began the last and most glorious era of Indo-European supremacy, in the midst of which we live; when the races of that family are the undisputed leaders, the acknowledged guardians and propagators of civilization. The establishment of the unity of this family, and the light thrown from language upon its history, constitute the most brilliant achievement of the new science of language, which* began with its recognition, and has developed along with its investigation. Indo-European language furnished such a grand body of related facts as the science needed for its sure foundation. Its dialects have a range, in period and variety of development, to which those of no other family approach ; they illustrate the processes of linguistic growth upon an unrivalled scale. The records of Chinese literature*go back, perhaps, to an antiquity as great, or greater ; but the Chinese language is almost without a history. There are Egyptian written documents which ‘are older than anything else the world has to show, but they are scanty and obscure, and the Egyptian tongue also stands comparatively isolated. ‘The Semitic languages come nearest to offering . a parallel; but they, too, fall far short of it. While their age is nearly the same, their variety is greatly inferior; ‘they are a group of closely related dialects, not presenting greater differences than some single branches of the Indo-European family, as, tor instance, the Germanic. And the other divisions of the human race hardly cover, to any notable extent, time as well as space with their known dialects; they offer us only their extant forms of speech. Now, much may be 106 PRINCIPLES OF LINGUISTIC SCIENCE. done, even with the aid of contemporary related dialects only, toward pene- trating their common history, because one will be found to have preserved one part, another another, of their ancestral tongues; but conclusions so reached will be inferior both in copiousness and in certainty to those which are derived from a comparative study of older and younger dialects, which illustrate the laws of change in their progress, and trace, as it were, currents and courses of development whose direction we can follow backward with confidence. This advantage we enjoy, to the highest known degree, in the Indo-European lan- guages. In the Germanic branch we have several different lines of linguistic descent, extending through a period of 1,500 years; the English going back to the Anglo-Saxon of the seventh century; the German nearly or quite as far; the Scandinavian to a somewhat less remote period; while the venerable Gothie of the fourth century (oldest of all) helps notably to bridge over the interval to the primitive language of the family. Celtie literature is much less rich, and also less ancient, carrying us up.to or beyond the tenth century. The oldest of the numerous Slavonic dialects, the ancient Bulgarian, has monuments a thousand years old. The Lithuanic is of much more recent date, but in many of its forms more antique and primitive than any of the languages hitherto referred to. The Romanic languages, through their mother, the Latin, take us up to a few centuries beyond the Christian era; the Greek to toward a thousand years before Christ. ‘The varied series of Persian tongues comes down from an antiquity nearly equalling the Greek; and the Sanscrit, the sacred language of ancient India, exceeding all the rest in age, and yet more in its preservation of primitive material and forms, reaches in its oldest records an epoch removed nearly 4,000 years from our own day. In investigating this rich and varied body of kindred tongues, the new science of language elaborated its processes and deduced its general laws, ap- plicable, with such modifications as the separate cases require; to other families also. The general method of study is everywhere the same, being conditioned by the nature of language itself, as a thing of historic growth, and by the capacity of related languages to cast light upon each other’s history. Historie analysis, by the aid of an extensive and careful comparison of kindred forms, is the grand means of research. From this its fundamental method, the science, in its growing stage, bore for some time the familiar name of ‘comparative philology.” ‘The comparison must be made in a scientific and orderly manner, proceeding from the nearer to the more remotely connected, from the clearer to the more obscure; but, finally, all language is brought within its sphere, and the full meaning of each linguistic fact is read in the light of every other, diverse as well as correspondent. The history of Indo-European speech has been more carefully read, and is better understood, than that of any other grand division of human language— imperfect as is still our comprehension of much that concerns it, partly owing to the incomplete analysis of evidence still preserved, but partly also to the irreparable loss of evidence. Some of the principal facts in that history are worthy of further attention. . The chief processes in the growth of the languages of our family have been shown to be the combination of old material into new words, with accompany- ing corruption and mutilation of phonetic form and independent meaning. These processes may go on in the future to an indefinite extent, with constant evolution from each form of speech of another slightly differing from it, until the descendants of every existing dialect shall be so unlike their ancestors that their relationship shall be scarcely discoverable. The question arises, whether there has been the same indefinite progress in the past, without traceable sign of an actual beginning. This inquiry is to be answered in the negative; the evidence of language points distinctly back to an earliest con- dition, or commencement of history; our analysis brings us finally to élements PRINCIPLES OF LINGUISTIC SCIENCE. 107 which we must regard as original. First, it must be claimed that our analyses are real, and not imaginary; they are the retracing of the steps of a previous synthesis. This is palpably the case with the latest of them, as in the case of truthful (truthful) and godly (god-like) ; it is equally.clear, too, as regards all the formative apparatus which is peculiar to the Germanic languages, since this must have been elaborated by them from their own materials, since the © separation of the Germanic branch from the rest of the family. But there is no stopping in this series of admissions. Every word-clement, separable by analysis, of which the genesis can be shown, which can be carried back to a word having an independent status in the language, must have been appended as an independent vocable to the words with which it was first connected. And even more. Considering how easily the evidence of origin becomes oblit- erated by the processes of phonetic alteration, we may not deny a former in- dependence to formative elements of which we cannot now trace the genesis. The parts into which etymological analysis separates our words are, as a uni- versal rule, those by the actual putting together of which the words in ques- tion were once made up. In analyzing zrrevocability, for example, we take off affix after aflix, leaving each time a word to which that affix had been added, till at last is left only the syllable voc, which conveys the idea of ‘“call- ing,” and which, though nowhere appearing in its naked form in actual use, we must believe to have existed before any one of the various aflixes with which we find it in combination was appended to it. To suchsyllables, which we call roots, we everywhere arrive by pushing our analytical process to the utmost, and these we believe to be the germs out of which language has actu-+ ally grown. In other words, the Indo-European languages began with an original monosyllabic stage. From monosyllabic roots, by processes not differ- ing in nature trom those which are still in operation, has been developed the marvellous and richly varied structure of our modern speech. ‘Tis is a truth, the recognition of which has been reached, almost with unanimity, by students of language ; the objections which are urged against it by the few who refuse it their belief are founded in misapprehension and prejudice, and are of no avail. The Indo-European roots are of two classes: roots of position, demonstra- tive or pronominal roots, and roots of quality, predicative or verbal roots. The former form chiefly pronouns and prepositions; the latter, verbs and nouns. Pronominal roots denote the relations of things to the speaker as regards place ; their fundamental distinction is between the ¢his and the that, the nearer and the remoter object. They are of the simplest phonetic form, generally a sim- ple consonant with a following vowel, composing an open syllable, and they are but few in number. The verbal roots are more numerous, counting by hundreds, and they are of every variety of form, from a simple vowel toa vowel both preceded and followed by one or more consonants. Instances are: 2 and gd, denoting simple motion; ak, swift motion; std, standing; vas, stay- ing ; sad, sitting; pad, walking; vart, turning; pat, flying; ad, eating; pd, drinking; vid, seeing; vak, speaking; dd, giving; garbh, grasping; dik, pointing out; dbhar, ‘bearing; kar, making; bandh, binding; bid, shining ; bhi, growing, &c., &c. They represent each its own meaning in its naked- ness of all limitations or applications, in a state of indeterminateness from which it is equally ready to take on the semblance of verb, substantive, or adjective. The first beginnings of polysyllabism were made by compounding together roots of the two classes. Thus, the addition to the root wah, “speaking,” of the pronominal elements mi, sz, t, produced combinations to which usage as- signed the meaning “I speak, thou speakest, he speaks,” laying in them the same idea of predication which we put into the ambiguous word dove, when we say “Ilove.” Other pronominal elements, modified or combined to express 108 PRINCIPLES OF LINGUISTIC SCIENCE. duality and plurality, formed the other numbers of this simple verbal tense. The prefixion of an augment, an adverbial prefix, pointing to a “then” or “there” as one of the conditions of the action, gave a past tense; reduplica- tion, symbolizing the completion of the action, produced a perfect. The future and the moods, subjunctive and optative, were chiefly formed by composition with the developed forms of other roots,, signifying ‘to be” and ‘to desire.” Expansions of the verbal scheme, down to such late formations as the Germanic preterit (I love-d = I love-did) and the Romanic future (j’aimer-ai = j'ai & aimer, “1 have to love,’’) are very numerous and various. The same root of action or quality, by the addition of other affixes, in part of pronominal origin, in part derived from other verbal roots, had its indefiniteness limited to expres- sion of the person or thing possessing the quality or exerting or suffering the action, or of the act or quality itself; and the forms so created became the basis of still further modification and combination. Thus arose nouns, substantive and adjective; for the two classes are originally and in idea but one. Things were named as the possessors of qualities or acts, not in the way of definition or complete description, but by seizing on some notable characteristic, and making it stand as representative of the rest. Nouns were provided with case- terminations; these varied the themes to which they were appended, as to num- ber, whether singular, dual, or plural; as to gender, whether male, female, or neither of the two, (and this, as already noticed, upon an ideal scheme of classi- fication ;) and as to case, or kind of relation sustained to the action of the sen- tence, whether as subject, direct object, or indirect object, with implication of the relations which we express by the use of the prepositions ¢o, 7m, with, from, for, and of. Hight such cases were possessed by the primitive language ; the Anglo-Saxon retained five of them; we have saved but one of the oblique cases, the genitive, (our “ possessive.’’) Prepositions, adverbial prefixes to the verb, of mixed pronominal and verbal origin, were from a very early time im- portant aids in directing and limiting the action expressed by the verb; these only later, and by degrees, detached themselves from the verb, and came to belong to the noun, assuming the office of its disappearing case-endings. The article is the part of speech of most modern origin, the definite article growing out of the demonstrative pronoun, the indefinite out of the numeral one. At what rate these processes of growth went on at the beginning, how rapid was the development out of monosyllabic barrenness into the wealth and fer- tility of inflective speech, we can never hope to know. The eonditions of that ancient period, and the degree in which they could quicken the now sluggish processes of word-combination and formation, are beyond our ken. We know only that, before the separation of the Indo-European tribe into the branches which later became the nations of Europe and southwestern Asia, so much of this linguistic development had taken place that its traces remain uneffaced, even to the present day, in the languages of them all; and, also, that the work was accomplished hundreds of years, if not thousands, before the light of re- corded history breaks upon the very oldest member of the family. é Much of what has been shown to be true of the history of Indo-European language is true also of that of other divisions of the human race. All the varied forms of speech which fill the earth have grown into their present shape by development out of such simple elements as we have called roots; roots, too, have been everywhere of the same two classes, pronominal and ver- bal, and the earliest forms have beeh produced especially by the combination of the two. Linguistic families are made up of those languages which have recognizably descended, in the ordinary course of linguistic tradition, from a common ancestor. But these great families are found to differ from one another, not only in their material, but also in their management of it; in their PRINCIPLES OF LINGUISTIC SCIENCE. 109 apprenension of the grammatical relations to be expressed by the combination of elements, and in the general way in which they apply their resources to the expression of these relations. Indo-European languages are what is generally called “inflective.” By this is meant, that they show a peculiar aptitude in closely combining the radical and formal elements, forgetting their separate individuality, and accepting the compound as integral sign of the thing indi- cated; submitting it then, as a whole, to the altering processes of linguistic growth. ‘This tendency shows itself very differently in different constituents of the language: in wntruthfully, for example, the four elements are held in- dependently apart; while in sing, sang, sung, song, inflection has reached its extreme result, substituting an, internal variation for original aggregation. The value of this distinction will appear more clearly as we go on to consider the characteristics of the other great families. We will take them up in an order partly geographical, partly based upon their relative importance. The second family is the Semitic, or Shemitic, so called because the descent of most of the nations speaking its languages is traced in the Bible to Shem. Its principal branches are: 1. The northern, Syriac or Aramaic. 2. The central, Hebrew and Phenician. 3. The southern, Arabic, with its outliers in Eastern Africa, the languages of Abyssinia. It is a strongly marked group, and, though occupying but a narrow territory, is of prime consequence, from the conspicuous part which the race speaking it has played in the history of the world. In the great empires of Mesopotamia the Semitic race first rose to high importance; then in the commercial and civilizing activity of the Phe- nicians, whose colony, Carthage, long disputed the dominion of the world with Rome. Meantime, the politically almost insignificant little people of the Hebrews were producing a religion and religious literature, which, made uni- versal by Christ, were to become the mightiest, elements in history. Finally, in the Mohammedan uprising, the third branch of the race advanced suddenly to a leading place, and for a while threatened even to reduce to vassalage the Indo-European nations; and it is still a conquering and civilizing power in parts of Asia and Africa. The Semitic type of language is also inflective, like the Indo-European, but not in such a way as implies any historical connexion between the two. The Semitic tongues are in many respects of a more strange and isolated character than any others known. ‘Their most fundamental peculiarity is the triliterality of their roots, every Semitic verbal root containing just three consonants. And it is composed only of consonants: their vocalization is almost solely a means of grammatical flexion. Thus, g-t-/ is a root conveying the idea of “killing ;” then gatala means ‘he killed;” qutda, “he was killed;” ugtwl, “kill ;” gat, “killing ;” zgtal, “causing to kill;” gat, “‘murder;” qitl, “enemy;”’ gut/, “murderous ;” and so on. Prefixes and suffixes are also used, but to only a limited extent; there is little left for them to do; the formation of derivative from derivative, by accumulation of affixes, is almost totally un- known. This significant vocalization is, to our knowledge, an ultimate fact in Semitic speech in all its forms, as is the radical triliterality ; but it seems im- possible to regard the latter, especially, as absolutely original ; and many at- tempts are made, with but indifferent success as yet, to reduce the roots to a simpler and less Procrustean form, out of which they should be a development. The different languages are of very near relationship, like German, Dutch, and Swedish, rather than like German, French, and Russian, for instance. Nor have they varied in the course of their gecorded history to anything like the same extent with the Indo-European languages. Everything in Semitic speech wears an aspect of peculiar rigidity. The Semitic verb is strikingly unlike ours in its apprehension of the element of time. It distinguishes only two tenses, whose chief distinction is that of complete and incomplete action: each may be, in different circumstances, either 110 PRINCIPLES OF LINGUISTIC SCIENCE. past, present, or future. Of wealth of modal forms there is but little; distine- tions of the action of transitive, causal, intensive, iterative, reflexive, and the like, by so-called conjugations, are multiplied instead. In their nouns, the Semites distinguish two genders, masculine and feminine, and three numbers ; but cases are almost wanting, only the Arabic separating nominative, genitive, — and accusative. The substantive verb is mostly wanting. ‘The language is poor in particles and connectives ; sentences are strung together, not interwoven into a period. ‘The characteristic stiffness is also shown in the development of signification. Words applied to intellectual and moral uses remain metaphors ; the figure shows through, and cannot be lost sight of. Semitic speech, then, is rather pictorial, forcible, vivid, than adapted to calm and reasoning philosophy. The next family of languages is one of much greater extent and’variety. It covers the whole northern portion of the eastern continent, with most of Central Asia, and parts of both Asia and Europe lying further south. We will call it the Seythian family ; it is known also by several other names, as Ural-Altaic, Tataric, Mongolian, Turanian. It is divided into five principal branches: 1. The Ugrian, or Finno-Hungarian, which is chiefly European in situation, in- cluding the languages of the Lapps, the Finns, and the Hungarians, with their congeners in the Russian territories, on both sides of the Ural. 2. The Samoi- edic, in Siberia, of small consequence. 3. The Turkish, or Tataric, spoken by races who have played some conspicuous part in modern history, especially in the dismemberment of the Mohammedan empire: its subdivisions are numerous, and extend from Turkey in Europe to the lower Lena, in Northern Siberia. 4. The Mongolian, the language of a people who in the 13th century overwhelmed nearly all the monarchies of Europe, and established for a brief period an em- pire the widest the world has ever seen: the Mongols now live in insignificance under Chinese domination. 5. The 'Tungusic, in the extreme east, having for its principal branch the Manchu, spoken by the present ruling dynasty and tribe in China. . The Scythian races have played but a subordinate part in human affairs. War and devastation have been their chief trade: they have shown no aptitude for advancing civilization, and but little for appropriating it. No written mon- uments of their languages carry us back to a past at all remote. But it is claimed of late by students of the Assyrian and Babylonian inscriptions, that one of their languages is a Scythian dialect, of the Finno-Hungarian branch, and even that those who spoke it were the founders of the civilization of that region. If this is established as true, it will greatly modify the aspect of an- cient ethnological history. The linguistic tie which binds together the branches of this great family is but a weak one, much less unequivocal than in the other families we have noted. There is less correspondence between them in linguistic material and forms ; either their separation is very remote, or they have had a peculiarly mobile and alterable structure. Their chief resemblances are of morphological character ; they are all alike “ agglutinative ;” the combinations by which their words are formed are of a loose nature; the root or theme is held apart from the suffixes, and these from one another, with a distinctive consciousness of their separate individuality. All formative elements follow the root to which they are attached ; prefixes are unused; the root, which is monosyllabic, remaining pure and un- changed, whatever accretions it may receive. It, however, usually affects the suffixes, in a manner which constitutes one of the striking phonetie peculiarities of the family. ‘The vowels are divided into two classes, heavy and light, and only vowels of the same class are allowed to occur within the limits of the same word; hence, the vowels of all suffixes are assimilated to that of the root. Thus, in ‘Turkish, from 4a6¢ comes babd-lar-um-dan, “from our fathers ;’? while from dedeh comes dede-ler-in-den, “from their grandfathers.’ This is usually called » PRINCIPLES OF LINGUISTIC SCIENCE. 111 the “law of harmonic sequence of vowels.” Varieties and irregularities of conjugation and declension are almost wholly wanting in Scythian grammar. The rank of the Scythian languages in the general scale of human speech, notwithstanding their euphonious structtre and great wealth of forms in certain departments, is but an inferior one. ‘Those of the western or European branch are decidedly the noblest, and they diminish in value eastward, the Tungusic being the poorest of all. There are those who would give the Scythian family a yet wider extension, even making it include most of the other Asiatic tongues, with those of the islands. Such sweeping classification, in the present state of our knowledge, has no scientific value, and is even opposed to the plainest evidences of lin- guistic structure and material. One group, that of the Tamulic or Dravidian dialects of Southern India, is most confidently, and with most plausibility, claimed as Scythian, and may probably yet be proved such. China and Farther India are occupied by races whose languages form a sin- gle class. Their distinction is that they are monosyllabic; they have never grown out of that original stage in which, as we have seen, Indo-European speech also had its beginning. ‘Their words are still roots, of indeterminate logical form; they are made parts of speech only by the consenting apprehen- sion of speaker and hearer, guided by their order and by the general require ments of the sense. But while the different languages of the class agree in general morphological character, they show great diversity in material, and the nature and degree of their relationship is very obscure. The’ Chinese is infi- nitely the most important among them. Its abundant literature goes back even into the second thousand years before Christ. It has only about 450 different phonetic combinations in its vocabulary; which, however, by change in the tone of utterance, are made into rather more than twice that number of distinct words. Yet this scanty apparatus, by the power which the mind has over its instrument, has been the means of expression of far higher, profounder, and more varied thought, than the majority of highly organized dialects spoken’ among men. China has been the mother of culture to the races lying south, east, and west of her tore the rest of the world she has affected mainly through the products of h€r ingenuity and industry. Those who speak the Malay-Polynesian languages fill all the islands, from the coast of Asia southward and eastward, from Madagascar to the Sandwich group, from New Zealand to Formosa. Only the present spoken dialects are known, and most of those but very imperfectly, sa that their groupings and degrees of relationship are little understood: there may prove to be more than one distinct family among them. Their phonetic form is of the simplest kind. Their roots are prevailingly dissyllabic in form, and of nominal rather than ver- bal meaning. Reduplication is a common mode of their development; the rest is accomplished more by prefixes than suflixes. Anything that can properly be called a verbal form is. hardly to be found in most of the dialects; mood, tense, number, gender, case, are wanting. The oldest dated monuments of ancient culture, the oldest written records, are found in the valley of the Nile. The earliest form of Egyptian speech is preserved on tables of stone and rolls of papyrus held by dead hands; a later, the Coptic, has a Christian literature of the first centuries after Christ, but the Coptic also has been extinct now for more than two centuries. It was of the simplest structure; its monosyllabic roots had value as verbs and as nouns, and only primary derivatives were formed from them; nor were its sutlixes, for the most part, more closely attached than those of the Scythian family. In some of its constructions it was as bald as the Chinese, and even more am- biguous. It agrees with the Indo-European and Semiiic languages in distin- guishing gender in its forms; no other human languages do this. There are apparent signs of relationship betweeu Egyptian and Semitic which lead many 112 PRINCIPLES OF LINGUISTIC SCIENCE. a scholars to entertaifi the confident opinion that the two descend from a com- mon ancestor; this, however, is as yet by no means to be regarded as certain. Many of the tongues of Northern Africa, and the Hottentot and Bushman, in South Africa, are also asserted to exhibit signs of an ultimate connexion with Egyptian. Excepting those dialects which are cither clearly Semitic, or claimed to be of kindred with Semitic or Egyptian, Africa is filled with a — great variety of tongues, forming a distinct family. They are, in a certain © way, rich in forms, and have some striking and peculiar traits. ‘The use of preformatives characterizes them; a root never appears without a prefix of some kind, and the prefixes are varied to accord with that of the dominant word in the sentence, producing a kind of syntactical alliteration. ‘There remains for consideration, of the great families of human speech, only that one which occupies the American continent. It is too ‘vast and varied to be dealt with here in any detail. Isolation of communities and the consequent indefinite separation into dialects have been carried in America to an extreme. Moreover, there is a peculiar changeableness of material, hard to explain and account for, which causes that two branches of a tribe which have been sep- arated but a brief time speak languages which are mutually unintelligible, and of which it is even hard to trace the relationship. But it is believed that a fundamental unity lies at the base of all the infinite variety of American dialects, from the Arctic Circle to Cape Horn; whatever their differences of material, there is a single type or plan on which their forms are developed and their constructions made. It is called the incorporative, or polysynthetic. It tends to the aggregation of the parts of the sentence into one great word; to the substitution of an intricate compound for the phrase with its separated and balanced numbers. No linguistic evidence of any réal value has yet been adduced going to show the affinity of American with Asiatic language, nor has the time yet come for _a fruitful discussion of the question. ‘To make a bare and immediate compari- son of the modern dialects of the two continents is altogether futile. When the comparative philology of the separate families is fully worked out, from the collation and analysis of all attainable material in each, if we shall find ourselves in a position to judge and decide the qu@8tion of Asiatic derivation, we shall have reason.to rejeice at it. What we have to do at present is sim- ply to learn all that we possibly can about the aboriginal languages of this continent ; our national honor and duty are peculiarly concerned in the work, toward which, with too much reason, European scholars accuse us of indiffer- ence and inefticiency. The Smithsonian Institution has recently taken up the subject, under special advantages and with laudable zeal, and all Americans should countenance and assist its efforts by every means in their power. Before closing this cursory and imperfect review of the great families of hu- man language, we should glance at one or two isolated languages or groups, hitherto unclassified. One of the most noteworthy is the Basque, spoken on the borders of France and Spain by the representatives of the ancient Iberi- ans, and perhaps the scanty relic of a race earlier than the irruptions of the Scythian and Indo-European tribes. Another is the Etruscan, of Italy, saved in scanty inscriptions, which offer an unsolved and probably insoluble problem to the linguistic student. In the Caucasian mountains, again, appears a little knot of idioms which have defied the efforts of scholars to connect them with other known forms of speech. Each family has, as may be seen even from our hasty sketch, its own peculiar characteristics, which distinguish it from every other. By such sweeping classifications of them as into monosyllabic and polysyllabic, into isolating, agglutinative, and inflectional, or the like, little or nothing is gained. ‘True classification must be founded on a consideration * . . od PRINCIPLES OF LINGUISTIC SCIENCE. 118 >» of the whole complicate structure of the languages classified ; it must, above | all, be historical, holding together, and apart from others, those groups which give evidence of genetic derivation from a common original. - On reviewing this division of the families of language, any one will be struck by its non-agreement with the divisions based on physical characteristics. This brings up the important question as to the comparative value of linguistic and physical evidence of race. A reconciliation of their seeming discordance must e sought and finally found, for the naturalist and linguist are both trying to work out the same problem—the actual genealogical history of human races— and they cannot disregard each other’s results. Their harmonious agreement can only be the result of the greatly advanced and perfected methods and con- clusions of both. Nothing more can be attempted here than to note certain general considerations bearing upon the subject. In the first place, language is no certain evidence of descent. As was shown in the first lecture, language is not inherited, but learned, and often from teachers of other blood than the learner. Nor does mixture of language prove mixture of race. ‘The Latin part of our vocabulary was brought us by men of Germanic descent, who learned it from Celts and Germans, and they from a mixed mass of Italians. ‘These defects of linguistic evidence have always to be borne in mind by those who are drawing conclusions in linguistic ethnology. But their effect must not be exaggerated ; nor must it be overlooked that physi- cal evidence has quite as important defects. The kind and amount of modifi- eation which external circumstances can introduce into a race-type is as yet undetermined. Many eminent naturalists are not unwilling to allow that all existing differences among men may be the effect of processes of variation, and that the hypothesis of different origins is at least unnecessary. Hence, as a race may change its language, and not its physical type, it may also do the con- trary. Language may retain traces of mixture undiscoverable otherwise. Lan- guage may more readily and surely than physiology distinguish mixed from transitional types. In many respects linguistic evidence has a greatly superior practical value ; differences of language are much the more easily apprehended, described, and recorded. Individual differences, often obscuring race-differences of a physical characte1, disappear in language. Testimony coming down from remote times is much more accessible and authenticable in language. Discord between the two, or question as to relative rank, there is none, or ought to be none. Both are equally legitimate and necessary modes of approaching the solution of the same difficult and, in its details, insoluble problem, man’s origin and history. Each has its notable limitations, and needs all the aid it can get from the other and from recorded history to supply its defects and control its conclusions. But the part which language has to perform in constructing the ethnological history of the race must be much the greater. In laying down grand outlines, in settling ultimate questions, the authority of physiology may be superior ; but the filling up of details, and the conversion of a barren elassi- fication into a history, must be mainly accomplished by linguistic science. Another important question is, what has the study of language to say re- specting the unity of the human race? This question can already be pretty confidently answered, but the answer must be a negative one only. Linguistic science can never hope to give any authoritative decision upon the subject. To show that it can never pretend to prove the ultimate variety of human races is very easy. It regards language as something which has grown by degrees out of scanty rudiments. It cannot assume that these rudiments were preggeed by any other agency than that which made their after combinations. It cannot say how long a time may have been occupied in the formation of reots, or how long the monosyllabic stage may have lasted ; and it must confess it altogether 8s ~ 7 # » 7 | | | 114 |» PRINCIPLES OF LINGUISTIC SCTE sr **on the negative side. If it may possibly be hoped that their connexion will ae | a re > _" a Se %. possible that an original man race should have separated into tribes 2 the formation of any lan e so distinctly developed, and of such fixed forms,, — as should leave traceable fragments in the later dialects of the atindered por- tions. Among all the varieties of human speech there are no differences which are not fully explainable upon the hypothesis of unity of descent. iy That the linguistic student also cannot bear positive testimony in tater such descent is equally demonstrable, although not by so direct an argument There is here no theoretic impediment in the way, buta practical one. It mig be hoped that traces of an original unity would be discoverable in all pa of human language; only examination could show that such is not the cas | investigation, however incomplete, has already gone far enough to le no reasonable expectation of making the discovery. The processes of linguistic change alter the constituent parts of language in — every manner and to every degree, producing not only utter difference between words which were originally one, but also apparent correspondence between those which are radically unconnected. There are no two languages on the face of the earth between which a diligent search may not bring to light resem- blances which are easily proved by alittle historical study to be no signs of rela- tionship, but only the result of accident. Now, the more remote the time of sepa- ration of two related languages, the more numerous will be their differences, the more scanty their resemblances ; hence, the more ambiguous will be the indica- tions of their connexion; until finally a point is reached where it is impossible to decide whether apparent coincidences which we discover are genuine, or only accidental, and evidence of nothing; and, in the comparison of languages, that point is actually reached. When we come to hold together the forms of speech belonging to different families, the evidence fails us. It is no longer of force to prove anything to our satisfaction. The families are composed of such lan- guages as can be seen to have grown together out of the radical stage. If there is community between them, it must lie in their roots alone; and to give the comparison this form is virtually to abandon it as hopeless. To trace out the roots of any family, in their ultimate form and primitive signification, is a task of the very gravest difficulty. By the help of the great variety and an- tiquity of its dialects, and especially by the Sanserit, the task can be somewhat satisfactorily accomplished for the Indo-European tongue; but the Semitic roots, as already explained, are of the most perplexingly developed form. Radi- cal correspondences among the great branches of the Scythian family are hardly sufficient to prove the ultimate relationship of those branches; and to hope that, in the blind confusion of Malay, African, and American dialects,* linguistic analysis will ever arrive at a confident recognition of their primitive germs, is altogether futile. Accidental correspondences are, if anything, more likely to ap- pear among roots than in the forms of developed speech. Authorities are much divided upon the question whether the Indo-European and Semitic families are proved connected, with a decided preponderance of the best and safest opinions | | | | yet be established, with the help of evidence coming from outside of language, the same hope cannot be entertained as to the connexion of either of these with any other family, and yet less as to the inter-connexion of all the families. We come, finally, to consider the origin of language. We may claim that the problem has been greatly simplified by what has already been proved as to the history of speech. Did we find the latter everywhere and always a com- ‘pletely developed and complicated apparatus, we might be tempted to despair of explaining its origin otherwise than by the simple hypothesis of a miraculous agency. But we have seen that the wealth of the noblest tongues comes by slow accumulation from an early poverty. We have only to satisfy ourselves how men should have become possessed, at first, of the seanty and hum bieens of language. And, in the first place, there is no reason for supposing them A i f ; . . ' ” Ce : * e — * 4 ea : vi wr : ; oy e a 7 il i ; ‘ ae oe Me PRINCIPLES OF LINGUISTIC scIENcE. _—-115 | oe . | generated by any other.agency than that which is active in their after combi- nation and development; namely, by the conscious exertion of man’s natural powers, by eee of the faculties conferred upon him for the satisfaction of the necessities implanted in him. In this way, and in no other, is language a di- vine gift. It is divine in the sense that man’s nature, with all its capacities and mar ents, is a divine creation. It is human, in that it is a product of that are, in its normal workings. : , is highly important that we make clear to ourselves what is the directly mpelling foree to the production of language. It is not any internal and necessary impulse to expression on the part of thought itself, although this is ry often maintained; it is the desire of communication. One man alone would never form a language. ‘Two children could not grow up together without ac- quiring some means of exchange of thought. Language is not thought, nor thought language ; noris there a mysterious and indissoluble connexion between the two, so that we cannot conceive of the existence of the one apart from the other. But thought would be awkward, feeble, and indistinct, without the working apparatus afforded it in language. ‘The mind, deprived of such an in- strument, would be, as it were, lamed and palsied. The possession of ideas, cognitions, reasonings, deductions, imaginings, hopes, cannot be denied to the deaf and dumb, even when untaught any substitute for spoken language ; nor, indeed, even to the lower animals, in greatly inferior and greatly varying degree. Thought is anterior to language and independent of it. It does not require ex- pression in order to be thought. The incalculable advantage which it derives from its command of speech, though a necessary implication in the gift of speech to man, comes incidentally, growing out of that communication which man must and will have with his fellow. A word, then, is not a thought; it isthe sign of thought, arbitrarily selected and conventionally agreed upon. It is the fashion to cry down the use of the word conventional as applied to language; but, rightly understood, it precisely expresses the fact. It does not imply the holding of a convention and formal discussion, but the acceptance and adoption into use, on the part of a community, of something proposed by an in- dividual ; and in no other way, as has been shown above, does anything in language originate; nor didit, back to the very beginning. Every root-syllable was first used in its peculiar sense by some one, and became language by the assent of others. ; These considerations relieve the remaining part of our problem of much of its difficulty. Under the outward impulse to communication, thought tends irre- sistibly toward expression: it will have expression, and, were it destitute of articulate speech, it would have sought and found other means—gestures, atti- tudes, looks, written signs, any or all of these. But the voice was the appointed and provided means of supplying this great want, and no race of men, accord- ingly, is found unprovided with articulate speech. It remains to inquire how men should have discovered what the voice was meant for, and have applied it to its proper use. Several theories have been proposed in explanation of this. One, the onomatopoetic, supposes that the first names of objects and acts were generated by imitation of the cries of animals and the noises of dead nature; _ another, the interjectional, regards the natural sounds which we utter when in .a state of excited feeling, our exclamations, as the beginnings of speech ; another compares man’s utterance with the ringing of natural substances when struck, and holds’ that man has an instinctive faculty for giving expression to the rational conceptions of his mind. The last of these is believed to be destitute of all value, as grounded in unsound theory, and supported by nothing in our experience or observation. The other two are so far true that it must be granted that exclamations and imitated sounds helped men to realize that they had in _ their voices that which was capable of being applied to express the movements _ of their spirits. But the study of language brings to light no interjectional 4% =~ Tae ee ' es eae q a 1te 4 PRINCIPLES OF LINGUISTIC SCIENCE. 4 . + roots; and onomatopoetic ones, although sometimes met with, are rare, at least in the better known families of language, and in great part of late formation. Evidence does not show, and theory does not require, that the actual beginnings ‘ of speech should have been of either character. The process of root-making was in much the greatest part a free and arbitrary one; it was, as we may with especial propriety call it, a tentative process, a devisal and experimental pro- posal of signs, to be thenceforth associated by a community with conceptions which pressed for representation. Objective and absolute connexion between sound and sense there was none, except in words of onomatopoetic formation ; of a subjective connexion, a geiding analogy, wee catch occasional glimpses, or seem to catch them; they are too subtle and evanescent to be believed in. with confidence, nor have we ground for suspecting their wide occurrence. There is thus enough of obscurity, of uncertainty, resting upon the earliest pe- riod of linguistic growth ; but of mystery, hardly any ; the process is not beyond our ken, although its details are out of our knowledge. ‘3 Of all animals, man is the only one that has proved himself capable of origi- nating a language. Yor this, the general reason, that man’s endowments are Pe vastly higher than those of the inferior races, is the best that can be given. When philosophers shall have determined precisely wherein lies man’s supe- _‘Mority, they will at the same time have explained his exclusive possession of speech. If, however, it were necessary to say in what mode of action lay that deficiency of power in the lower animals which, more than any other, put lan- guage out of their reach, we should incline to maintain that it was the power of distinct reflection on the facts of consciousness ; of analyzing impressions, and setting their parts so clearly before the internal sense as to perceive that each : is capable of a distinct sign. Many animals come so near to a capacity for lan- guage as to be able to understand and be directed by it, when addressed to them by man; nor is their condition without analogy with that of very young chil- i dren; whose power of comprehending language is developed much earlier and . more rapidly than their power of employing it. It may well be questioned whether, as regards capacity for speech, the distance from the unimpressible * oyster, for instance, to the intelligent dog, is not vastly greater than that from the dog to the lowest and least cultivable races of men. ee ; ye : he « * x e 4 : r + ~ ¥ _ , . . MEMOIR OF C. F. BEAUTEMPS-BEAUPRE, ke BY M. ELIE Wee none , ERPETUAL SECRETARY OF THE FRENCH ACADEMY OF SCIENCES, ‘- - TRANSLATED FOR THE SMITHSONIAN INSTITUTION BY C, A. ALEXANDER, - To this Academy no species of scientific renown is alien; and if such men as la Pérouse, d’Entrecasteaux, Baudin, Dumont d’Urville, have disappeared from the stage of the world without having been numbered in its ranks, it was because an inauspicious destiny arrested their career. Their place here was already marked. To have obtained it would have been to them, next to the consciousness of duty fulfilled, the highest of gratifications. To you, gentle- men, the privilege of crowning their memorable labors by your suftrages would have been a subject of the most just self-congratulation. Those labors death, which has snatched away their authors, has not withdrawn from your domain. ‘It is still grateful to you to extol them, and your committee has concurred with me in thinking that I could prefer no better claim to your favorable attention than by attempting to retrace, on this occasion, the life of a colleague who knew how to obtain and to justify all your sympathies, and whose name invariably recalls those of the heroes of hydrography we have named, of whom he was, with better fortunes and not less daring, the companion, the rival, or the master. Charles-Frangois Beautemps-Beaupré was born August 6, 1766, at Neuville au Pont, a village situated one league north of Sainte Menehold, in that part of Champagne which now forms the department of the Marne. His father was an unpretending tiller of the soil, and the young Francois, who seemed destined to cultivate, in his turn, the rather prosaic fields of that worthy country, passed his first years in youthful sports on the pleasant hills which, branching from the Argonne, agreeably diversify the banks of the Aisne. His constitution, naturally robust, and strengthened by country exercise, received on one occa- sion a severe shock. While heedlessly playing with the rope of the parochial bell he fell with violence, and sustained such injuries of the head as to make trepanning necessary. ‘The operation was no doubt skilfully performed, for the young sufferer became, with advancing years, a man of tall stature, of a noble and expressive mien, and retained, for nearly eighty years, the use of the © exalted faculties which won him a place in this assemblage. I have not been able to recover the name of the modest provincial surgeon to whom, under Providence, our colleague was indebted for life and intelligence, and who, per- haps, never knew the full value of the head he had been instrumental in re- storing. M. Beautemps-Beaupré passed, indeed, only the years of childhood at his’ native village. Among his relations was an eminent geographer, M. Jean Nico- las Buache, the head of a geographical establishment derived by collateral in- heritance from the family of Delisle—a family wholly devoted to science, and known, through more than a century, for its connexion with almost every pub- Tication relating to geography, astronomy, and the marine. M. Buache, visit- ¥ “a . — Arse 8 8 7 + Cee * ’ => aad P os a ‘7 = Bs 118 P MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. - % _ * et r 7 “> eT % * ¥ tenance of his young relative. He was pleased at the idea of associating with himself a docile intelligence which might be trained to the conduct o . > a ; ing Neuville au Pont about the year 1776, was struck with the asc coun- monial business, and readily induced the little Beaupré to accompany him + Paris. Thus the latter found himself installed, at the age of ten years, in the midst of the hereditary traditions of a house which had become, in some sort, — the focus of geographical studies. He was charged with the arrangement and preservation of those charts, atlases, and globes with which we have most of us been occupied at some period of our lives. To this labor, which would have repelled the generality of young persons, he gave himself with unbounded de- — votion. He lived among his dear maps, assorting, adjusting, studying them; hence he was not long in mastering all that was necessary for understanding them. His vocation stood revealed to him; nor, with such innate tastes, could his eventual accession to this Academy be a matter of doubt, provided that for him, also, the condition stipulated in the distich of La Fontaine should be realized : ‘* Little fish to large will grow, If God shall only life bestow.” M. Buache, gratified at the manifestation of so happy a turn, afforded every facility in his power for its development. . The attention of this learned geographer was by no means confined to the commerce of his establishment. He had assisted in the education of the three princes who became, successively, Louis XVI, Louis XVIII, and Charles X, and maintained with the first of these monarchs, himself a distinguished geog- _ rapher, relations of confidence founded ona similarity of tastes and studies. It is to be presumed that he contributed much towards shaping the views of the ~ excellent King in relation to the expedition of la Perouse, and being intrusted, jointly with M. Fleurieu, with the preparation of instructions for. the voyage— instructions strongly impressed with the benevolent spirit of Louis X VI—it became necessary for him to execute in the short space of three months a nu- merous series of charts. Naturally he turned for assistance in this labor to his young coadjutor, with whose talent for this species of design he had been so — much delighted; and, quite as naturally, the youthful enthusiast, in whom there was much more than the material for a draughtsman, grew enamored, as he proceeded, not only of the charts but of the expedition, and eagerly pressed to be allowed to embark on one of the frigates. Happily for himself and for science, M. Buache decided that, at the age of eighteen, there was yet too much for him to learn to make it advisable that he should engage in such an enterprise, and thus prevented his taking part in that fatal expedition from which no one was destined ever to return. The young Beaupré had not, however, escaped the notice of M. de Fleurieu, and was transferred as engineer in 1785 from the department of the Marine, in which he had heretofore served under the orders of M. Buache, to that of the Controls, where, in immediate subordination to M. de Fleurieu, he was required to assist in the execution of the charts of the Baltic Neptune. Meanwhile the expedition commanded by la Perouse had sailed from Brest, August 1, 1785. After having traversed the coasts of the Pacific ocean in all directions, and moored in the harbor of Botany Bay, it had again put to sea, March 10, 1788, in order to prosecute the route marked in its instructions. - From that time nothing had been héard of it, and apprehensions for its safety . & began to be entertained which were unhappily too well founded. The National Assembly having petitioned the King to despatch armed ves- sels in search of the distinguished navigator, two new frigates, Ja Recherche and U iagerance, were designated to sail, under the orders of Rear-Admiral | ntrecasteaux, upon this laudable mission; and this time M. Beau- a Bruny d’ a , > ee e patri- © yi) ‘ S. y | 1 . - eR MEMOIR OF ©. F. BEATEN ES eae e ad ’ ; 4 - ae» eaupré obtained the favor of accompanying the expedition. He was | July 31, 1791, under the title of first hydrographical engineer, to e la Recherche, commanded by the admiral in person, and reported imself at Brest, whither he had repaired in company with M. de la Billardiere, the botanist of the expedition, and destined himself also to become a member of this Academy. ' r The two vessels sailed September 29, 1791, at which time Beaupré was twenty-five years of age. By his labors during six years in the compilation a Neptune of the Baltic sea, he had thus early become an experienced chartographer, and the expedition now departing offered the happiest occasion for the application of his talents in this line; for the admiral, being about to explore with great minuteness all the coasts where traces of la Perouse might be expected to be found, had received orders to determine at the same time their hydrography with all possible compactness. i After having doubled the Cape of Good Hope, the expedition passed in # sight of the isle of- Amsterdam, coasted at a distance the southern shores of New Holland, and came to anchor towards the southeast point of Van Die- men’s Land, at the then desert entrance of the river on which now stands the city of Hobarttown. It next penetrated into the Pacific ocean, followed the western coast of New Caledonia and the northern of New Guinea, passed to the northwest of Amboyna and Timor, to the west of New Holland, explored in detail the south coast of that vast region, and, after having thus made its entire circuit, again cast anchor, January 21, 1793, in the south part of Van Diemen’s Land. Having completed, during the finest month of the austral summer, import- ant hydrographical labors commenced the previous year, and particularly the | | survey of the straits of d’Entrecasteaux, which separate the isle of Bruny from % the main land, the expedition again sailed, February 27, and passed anew into , the wide Pacific. Directing its course towards all the points where la Perouse could be supposed to have touched or to have been driven, after his departure ~ from Botany Bay five years before, the expedition visited Tongataboo, one of = the Friendly islands, and once more shaped its course towards New Caledonia, which was now reached from the northwest. Some idea of the incidents and . ae _ ? a perils of these courses may be conveyed by a few passages of the admiral’s narrative: ‘‘On the eve of our arrival at New Caledonia, April 17, 1793, it blew a hard gale; the atmosphere was thick, but not so dark as to induce me to lose a night off the Cape. I gave orders to proceed under easy sail. About three in the morning it grew very dark, and the cries of numerous birds were heard near the frigate, an almost certain indication at that hour, of the neighbor- hood of land. Although day was not far off, M. Merite, officer of the watch, prudently decided to bring to, and scarcely had objects become distinguishable, when a low coast presented itself to view; an instant after it was discovered’ ~ to be surrounded with breakers on which we should certainly have struck but for the precaution just mentioned; for we had been making two leagues an hour under topsails alone, closely reefed. This dangerous ledge was recon- noitred, and a special draught of it carefully executed. Its length from north to south is from nine to eleven miles, and its breadth, east and west, seven to eight. We saw to the east of this reef two small wooded islands, with a third larger midway between them: these we have named the Beaupre islands.” * Te *The claims of M. Beautemps-Beaupré to a distinction of this kind were incidentally recognized by the distinguished and lamented explorer, Sir John Franklin. Being on a visit i, to Paris, just before his departure on the expedition which was destined to so fatal a result, he called on M. Beautemps-Beaupré, and, speaking of Van Diemen’s Land, of which Sir John had been governor, learned from the lips of our colleague that the latter had been the first explorer of “s a on which now rises Hobarttown, the capital of the island. How: * To edie d * » ae pr: My. ’ he, : " ton . 2" 120 MEMOIR OF Gi F, BEAUTEMPS-BEAUPRE. , ty When his name was thus conferred, M. Beautemps-Beaupré had been daily prosecuting his labors for more than twenty months under the eyes of the admiral and his oflicers, and the testimonial may, therefore, be regarded as the more deliberate and honorable. “The same day,” continues the admiral, “at half after 1 o’clock, we deseried New Caledonia, and in two hours were a mile distant from the reef on the eastern coast of this great island, which seemed to be bordered by it, as the western coast had been ascertained to be in 1792. * * * * Ag the entrance of the harbor of Balade, where I proposed to come to anchor, was only marked by an interruption of the reef which borders the coast, we followed this reef closely in order not to miss the opening. We reached the pass by 2 o’clock, and a favorable tack gave us hopes of gaining the anchorage, when it was signalled that the other frigate, 7’ Esperance, had struck.” Happily the imperilled vessel was safely extricated, and the two frigates finally cast anchor very nearly at tlre spot where Captain Cook had done in 1774. «The naturalists of the expedition repaired, April 25, to the neighboring mountains, and M. Beaupré ascended with them in hopes of discovering the reefs with which the channels of Balade are bestrown, and of fixing their position. The sea was discernible to the east, west, and north, and the isles of Balabra, Reconnaissance, and many other points which had been entered in the maps of 1792 were recognized. The positions of these were determined by M. ‘Beaupré with reference to the observatory of Balade, with the view of con- necting the trigonometrical operations of this year with those of the preceding one. From the top of these mountains the shelf which borders the other side of New Caledonia was perceived, and an interruption distinguished, which, after renewed observations, seemed to correspond with that discovered the previous year in visiting the western coast.” . The expedition left the roads of Balade May’9, 1793, and soon after encoun- tered the dangerous reefs which stretch to the NW. of New Caledonia; these having been examined but imperfectly by Cook, have received the name of the reefs of d’ Entrecasteaux. ‘Twice, at the break of day, were the ships of the last-named navigator found to have so closely approached this barrier, that there was barely room for the evolution by which they were extricated. Direct- ing his course northeastwardly towards the island of Santa Cruz, the admiral gave the name of /a Recherche to an island in the vicinity of the former, whose latitude and longitude were determined to be, within but a few minutes, 11° 40/ south, and 164° 25’ east. During the numerous courses made by the vessels in the archipelago of Santa Urcz, M. Beautemps-Beaupré, favored by fine weather, succeeded in fixing the position of a multitude of points, as well on the principal island as its accessories. According to the method which he had adopted for making his observations, . and which has since become of general use, he first made at each station a | draught of the coast, in which he indicated by letters or numbers not only the ~ most remarkable objects, but wrote the measures of the angles observed, the bearings of the points with respect to one another, the estimate of distances, &c. | The draughts, on which were to be written the results of the observations made > much do I regret,” exclaimed Sir John, ‘‘ that I was ignorant of the cireumstance! I should have bestowed your name on the finest portion of the city.”’ aptain Flinders, who, in 1801-1803, conducted an expedition ‘‘for the purpose of com- pleting the discovery of that vast country” to which he gave the name of Terra Australis, (afterwards changed to Australia,) and who published an account of his voyage in two 4to. volumes, accompanied by an atlas, bears testimony, as wellin notes engraved upon the maps as in passages of the text, to the accuracy of the labors of our colleague. In the introduction to the work it is said: ‘‘’The charts of the bays, ports, and arms of the sea at the southeast end of Van Diemen’s Land, constructed in this expedition by M. Beautemps-Beaupré and assistants, appear to combine scientific accuracy and minuteness of detail, with an uncom- mon degree of neatness in the execution. They contain some of the finest specimens of marine surveying, perhaps, ever made in a new country.” £ ; A : ee a Wok . ; ae MEMOIR OF ©. F. BEAUTEMPS-BEAUPRE. 121 , ? : xe : on board, dull not be taken with too much rapidity, for it was necessary that the ship should not materially change its place during the time of the opera- tion. ‘The principal operations which serve as a foundation for the charts con- structed by M. Beaupré are such as were executed either at midday, or simul- taneously with the observations of horary angles; that is to say, at such times of each day as the position of the vessel was determined by astronomical ob- servations and the chronometer. On these occasions he assembled around him the greatest possible number of observers, and he had found or formed a great many among the officers of the frigate. Just one minute before taking the observations he made a sketch of the coast under view, beginning with those parts of it which, being most remote, would undergo least change of outline by reason of the movement of the ship; then, precisely at the moment when the astronomical observations were taken, he measured the angular distance be- tween the object which he had designated to his assistants as the point of de- parture and one of the remarkable places of the coast, while each of the as- sistants measured the angular distance of the same point of departure from one of the other objects embraced in the survey. The results of these simultaneous observations were afterwards transferred to the sketch which had been made of the outline of the land. All the angular measures were taken with Borda’s _ repeating circle. When the sun was not too high above the horizon, one of the observers measured the distance of that body from one of the remarkable points of the coast; by means of the heights of the sun observed at the same moment by M. de Rossel, and from the distance measured, M. Beaupré obtained the astro- nomical bearing of that point, whence he deduced the bearing of all the points between which angles had been taken. Two compasses were always directed, during the observations, on the place chosen as a point of departure for the angles, and the mean of the bearings given by those instruments was transcribed in the collection of notes, and this whether an astronomical bearing had been obtained or not. In the first case the magnetic indication served to show the variation of the needle, and in the second to supply, though imperfectly, the absence of an astronomical observation. If circumstances, which, however, occurred but rarely, prevented the co-operation of a sufficient number of observers to take simultaneously the angles of all the remarkable points necessary to be determined, M. Beaupré arranged several circles of reflection, so that each observer might promptly take two or three angles, without being obliged to write them on the spot; and these observations, made with a rapidity proportionate to the expertness of the observer, were found to agree almost as exactly as those made simultaneously. M. Beaupré, who drew the chart with as much facility as exactness, found a marked advantage in embodying the results observed as promptly as possible, for he had then all the circumstances of the observations present to his mind. It was not seldom that he was enabled in this way to detest and remedy inad- vertencies committed in writing the angles measured. The precision of his graphic constructions ever rendered it practicable for him to verify, and some- times to correct, with great probability, the positions of the ship, determined “several times a day by astronomical observations, combined with the indica- tions of chronometers and the estimate of courses. The means of verification resulted, in part, from the fact that the observa- tions of each station gave him a series of visual lines, springing essentially from the same point, and forming known angles, whether with one another or with the astronomic meridian, or at least with the magnetic meridian, itself deter- mined by an observation made at nearly the same time. They resulted, more- over, from the circumstance that all the visual lines directed from different stations on the same object, such as a cape or a mountain, must, on the draught, intersect one another at the representation of that object. When, at the first trial, these did * —_ 122 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. % . eo not meet, a series of approximations tending to modify in an admissible degree the position of the ship at the different stations sufficed to establish the neces-— sary junction. ‘The approximations in question might be made with still more rigor by calculation, and one of our most scientific hydrographers, M. de Tessan, has even shown that the method of least squares is here applicable ;* but M. _ Beaupré adhered generally to the graphic method, which he employed with as | much sagacity as precision. The application of this rigorous method fixes the position of the principal points of the chart about to be constructed, as the tops of mountains, capes, &e. The details, such as the outline of coasts, course of rivers, &c., are afterwards described with such degree of precision as time permits; and when a sojourn of some duration renders it practicable to add the soundings taken at sea, as was the case in regard to the straits of d’Entrecasteaux and other parts of the coasts of Van Diemen’s Land, the positions of the points of sounding are fixed by reference to the principal points determined by the bearings, in accordance with the methods which will be presently indicated when we arrive at the hydrographic surveys of the coasts of France. >: The bearings taken from the 19th to the 23d May, in the archipelago of Santa Cruz, enabled M. Beaupré to give a remarkable proof of his skill in applying these processes, which were then new. Faithful to his method of constructing, day by day, the chart of those parts of coasts which he would not again see, he devoted the night of the 21st to describing the details of. the south coast of the island of Santa Cruz; that of the 22d was similarly occupied with the north coast; and, the ships sailing on the 23d for the Solomon islands, he applied himself,-as soon as the land was lost sight of, to the definitive reduction of his chart. This, like all the rest belonging to the voyage of d’Entrecasteaux, was constructed on a scale of three lines for one minute of the equator; and as it presented, for the discussion of which we have been speaking, nearly all the cases to be met with in practice, M. Beaupré has caused it to be engraved in the 19th plate of the atlas, with all his lines of construction, as an example of his manner of operating, and it is here that he has explained his method with de- tails at which we have only been able to give a cursory glance. They may be seen in the appendix relative to this subject at the end of the first volume of _ the voyage of d’Entrecasteaux, an appendix which has become the vade-mecum, and, if I may so speak, the catechism of the constructors of marine charts. In reducing to rule, and in practicing his method, M. Beaupré fulfilled the most cherished wish of the scientific hydrographers, who, at the close of the eighteenth century, employed themselves with the means of giving to nautical science all the precision of which it is susceptible. Borda, after having placed in the hands of navigators the repeating circle of which they still make use, had recommended its employment in preference to the compass, which till then was exclusively relied on for surveys executed at sea. Flurieu had equally recommended astronomic surveys. For naturalizing these scientific processes in the practice of hydrography, it was requisite that some engineer of a peculiar aptitude should devote himself with energy and perseverance to the application of the new instruments and rigorous geometric methods adapted to the accurate measurement of angles. M. Beaupré proved fully equal to this honorable mission, and, thanks to his unceasing efforts, the voyage of d’Entre- casteaux inaugurated the opening of a new era—that of precise hydrography. Like all other branches of human knowledge, hydrography has been advanced by degrees. After the invention of the compass, so far surpassed at a later stage by mew instruments, the discoveries of Christopher Columbus and of Vasco de Gama gave ideas a wholly new direction. Subsequently the adven- So * See Voyage autour du Monde, par le frégate Venus, commandée par M. Abel Dupetit Thouars: Physique, par M. de Tessan, t. v., p. 288. ‘ os en) *. ‘ a ! : sie MEMOIR OF C. F. BEAUTEMPS-BEAUPRE: 123 + turous circumnavigations of the Magellans, Mendafias, Drakes, Tasmans, and Dampiers, made known the principal outlines of the two oceans, but with very imperfect exactness, as may be perceived from a glance at the old globes which are still of frequent occurrence in Paris. That, according to the happy expres- sion of M. Villemain, was the heroic age of the navigation of discovery ; the modern Argonauts went forth in their search for the golden fleece with an ardor little favorable to systematic exploration, and which yet did not prevent them from overlooking the rich auriferous deposits of California and Australia. Towards the middle of the eighteenth century, after Buffon had published his Natural History, the taste for voyages was revived under a form even then much more scientific. In the course of a few years we see Byron, Carteret, Wallis, traverse the Pacific ocean, and make the tour of the world. Cook is sent to Tahiti to observe, June 3, 1769, the passage of Venus over the dise of the sun. He makes two other important voyages, and after having traversed the Pacific in all directions, and penetrated into the frozen regions of both poles, falls in 1779 beneath the weapons of the natives of the Sandwich islands. Cook remains the principal figure and characteristic of this period; but had fate per- mitted the instructions given to la Perouse to have been completely carried out, the voyage of this last would, perhaps, have afforded the best example of what it was possible to accomplish with the hydrographic methods then in use. These different enterprises made known almost all the lands and archipelagos with which the ocean is strown, and furnished charts which already presented their general form with a great degree of fidelity. Last come the hydrographic voyages of precision. If the expedition of d’Entrecasteaux offers the first example of them, the voyage of the Coguille, executed under the command and published under the direction of our distin- guished colleague, Captain Duperrey, must, perhaps, be regarded as the most perfect type of this class of enterprises. To the same class belong the almost too hazardous voyages of Sir John Ross among the ices of the antarctic pole, and those not less daring of M. Dumont d’Urville. The hydrographic study of the archipelago of Santa Cruz, which retained around M. Beautemps-Beaupré some of the most skilful officers of the frigate, did not so exclusively occupy the attention of Admiral d’Entrecasteaux and other chiefs of the expedition as to divert their attention from the main objeet of their mission, which was to seek for traces of la Perouse. They constantly communicated with the shores, questioned the natives, examined the objects in their possession, and observed, among other things, a piece of iron from the hoop of a cask, set as a hatchet; but no one then suspected that there was here a vestige of the expedition of la Perouse. ‘The admiral has minutely recorded the reasons why no importance was attached to the circumstance. Nevertheless the chart of the archipelago of Santa Cruz presents, in its SE. portion, an island on which by a rather singular chance the admiral bestowed the name of la Recherche, after that of his own frigate sent in search of la Perouse. ‘We took the bearing of this island, says M. Beautemps-Beaupré, for the first time from our point of station at 20 minutes after 9 o’clock, 19th May, at a great distance, At noon, the same day, we again took its bearing, and then lost sight of it.’ Situated at the southeast extremity of the archipel- ago of Mendaiia, this island has been in like manner seen and lost sight of by not a few other navigators in whose track it lay, and who little imagined that la Perouse and his companions had paid with their lives for the honor of having previously discovered it. Thus two years earlier than d’Entrecasteaux, Captain Edwards, commanding the English frigate Pandora, had discovered, August 13, 1791, this same island, which he had named Pitt island, and had sailed around its southern shore with- out suspecting that it concealed the remains of a world-renowned shipwreck. Thirty years later, in 1823, Captain Duperrey, among whose officers was M. 4 at 124 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. Dumont d’Urville, passed in the corvette Za Coquille, 2d and 3d August, at — about half a degree to the W.SW. of the island. Strong eastwardly winds prevented him from approaching nearer, but he took numerous bearings which seryed to rectify the position of the island, and then obeyed without thought the wind which bore him away from it, having himself no reason for supposing that this obscure spot presented any trace of the expedition of la Perouse. Yet the veil was about to be withdrawn. Four years after, in December, 1827, and January, 1828, M. Dumont d’Urville was lying with the Astrolabe in the ort of Hobarttown, situated in those parts of Van Diemen’s Land which MM. d’Entrecasteaux and Beautemps-Beaupré had surveyed with so much care while they were still desert. Here reports reached him, vague indeed, and even con- tradictory, respecting a surprising discovery made by Captain Dillon, com- manding an English vessel, engaged in commerce. This mariner, it was said, had acquired authentic information relative to the shipwreck of la Perouse, and had even brought away the handle of a sword which he claimed to have belonged to that celebrated navigator. Notwithstanding the slight authority for these reports, M. Dumont d’Urville thought himself justified in modifying the route which his instructions traced for him. He touched, February 10, at 'Tikopia, where he found among the natives a lascar named Joe, a sailor and native of Calcutta, who was the same that had sold the sword-handle to Captain Dillon. ‘This man, after a little hesitation, acknowledged that some years before he had gone to the Vanikoro asles, which are no other than the group of la Recherche, where he had seen many objects belonging to the vessels of la Perouse; that he had been then told that two very aged whites were still alive, but he himself had not seen them. The next day, February 11, 1828, the Astrolabe sailed for the Vanikoro islands, situated, according to the natives, about forty leagues W.NW. from Tikopia. The vessel came to anchor, February 14, at the place of its destination, and remained till the 17th of March. M. Dumont d’Urville, being quite seriously indisposed, could not quit the corvette, which, besides, was, in more than one respect, not considered in entire safety; but, after having inter- rogated the natives, he despatched in succession several parties commanded by responsible officers, with whom he associated his faithful surgeon, M. Gaimard, whose recent death has been a new occasion of sorrow to the friends of science. The chain of reefs which, at a distance of two or three miles, forms an im- mense girdle around Vanikoro, closely approaches the southern coast near Paiou, in front of a place called Ambi. Here it is but a mile off, and it was here that, on a first visit, the native who preceded M. Jacquinot stopped his canoe in an opening between the breakers, and made a sign to the Frenchmen to look be- neath the water. There; at a depth of twelve or fifteen feet, were clearly distinguishable, scattered here and there, and imbedded in corals, anchors, cannons, bullets, and divers other objects, especially numerous sheets of lead ; the wood had entirely disappeared. 'The position of the anchors seemed to in- dicate that four of them had sunk with the ship, while two others had probably been let go. On a second visit M. Guilbert succeeded in withdrawing from the — reefs the following objects : An anchor of about eighteen hundred pounds weight, without a stock, much rusted and covered with a crust of corals apparently from one to two inches in thickness; a cast cannon, likewise covered with corals, and so much oxydized that the metal readily yielded under the hammer; a small swivel of brass and a blunderbuss of copper in much better preservation, one bearing on its trunnions 548 as its number, and 144 as its weight; the other 286 and 94 for its number and weight respectively, with no other marks ; a pig of lead and large sheet of the same metal, together with some fragments of por- celain. The remains of a kettle had been previously procured at Nama, a vil- _ lage of the coast. MEMOIR OF ©. F. BEAUTEMPS-BEAUPRE. 125 The following is the amount of the information obtained from the natives : About forty years previous to 1828, (which would carry us back to 1788, the date of la Perouse’s disappearance, ) one morning, at the close of a very dark night, during which the wind blew with violence from the SE., the islanders suddenly de- scried on the southern coast, opposite the district of Tauema, an enormous pirogue, stranded upon the reefs. It was rapidly demolished by the waves, and so en- tirely disappeared that nothing was ever recovered from the wreck. Of the persons who manned it a few only succeeded in escaping in a boat and gained the shore. The following day, likewise in the morning, a second pirogue, similar to the first, was discovered on the rocks before Paiou; where, in the lee of the island, and less racked by the wind and sea, stranded moreover on a level shelf of twelve or fifteen feet depth, it remained some time in its position without being destroyed. This, like the first, bore a white ensign. The strangers who manned it landed at Paiou, where they established themselves with those saved from the other ship, and immediately set about constructing a small vessel from the fragments of the ship which had not gone down. ‘Their task was completed in six or seven moons, and, as most, of the savages averred, - all the strangers left the island. A few, however, declared that two remained behind, but that these had not long survived. M. de Fromelin, who also visited these shores in 1828, on the corvette la Bayonnaise, and who had doubtless heard of the discovery of the English Cap- tain Dillon, ascertained by examination the existence of the remains of the French frigate on the reefs of Vanikoro. It was a source of regret to M. Dumont d’Urville that he had not been able, in 1828, to visit in person the place of the shipwreck; hence, when on a last and memorable expedition he traversed anew the great ocean, he caused his ships, the Astrolabe and the Zelée, to lie to, 6th November, 1838, near the -eef of the southern shore of Vanikoro. Landing in a sea too rough to admit f stopping on the reef, he discovered a space cleared of trees, which appeared to him to have been the spot where the parties from the wreck had pitched their camp. Near it he observed a large cocoa-nut tree which had been deeply cut around the trunk at two metres above the ground, besides other traces of the use of the axe at a remote date, but beyond this he noticed no new indications. The two frigates mounted with cannon, which could be none but those of la Perouse, for no others were known to have disappeared in these seas, had _ doubtless encountered, but with more adverse fortune, casualties similar to those + which befell the frigates of Admiral d’Entrecasteaux ; of which one was near being lost on the Beaupré islands at the time of their discovery, and the other struck on a reef of zoophytes in the pass which forms an entrance to the haven of Balade, but was fortunately extricated. It was not an impossibility that the remnant of the crews of la Perouse should be saved in the bark which they had constructed, and on which they put to sea about the close of the year 1788. In fact, the English Captain Bligh, of the ship Bounty, abandoned in the midst of the South sea by his revolted crew, in an undecked shallop only twenty-two feet in length, passed, 18th May, 1789, about fifty leagues to the south, and consequently almost within sight of the isles of Vanikoro, and succeeded, May 29, in reaching the coast of New Holland at the south entrance of Torres’ straits, whence they made their way to Cou- pang, in the island of Timor. True it is, as apyears from the romantic narrative of his adventures, that not to have perished a hundred times was due only to the most astonishing good fortune. This fortune was denied to la Perouse and his companions, though the boat in which they left Vanikoro but a few months before was no doubt larger and better appointed than that of Bligh. In similar circumstances many others have succeeded in being saved. In © _ reading the stirring recital of their various perils, we readily perceive that in the fate of la Perouse there is nothing enigmatical; nor can the conclusion escape se a » . 126 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. us that the expedition of d’Entrecasteaux must have been conducted with as much ability as zeal, when we see on the chart of the archipelago of Santa at % Cruz, by M. Beautemps-Beaupré, two of the lines of survey directed by him upon the island of la Recherche or Vanikoro, meet precisely at the spot where ~ still lie beneath the waves the anchors and cannons of one of the frigates of the illustrious and unfortunate navigator. _ The ships of d’Entrecasteaux continued in sight of the island la Recherche almost the whole of the 19th of May, 1793. Besides the instruments of the , Survey, there was no deficiency of telescopes pointed towards the land, through which, if signals after the European manner had been made, the piercing eyes _of some of the mariners could not fail to have deseried them. But the survi- vors of the wreck were doubtless long departed or dead when the expedition passed, which was not till five years after the disaster. As to finding under the waters of the sea the remains of the shipwreck, that would have been a stroke of good fortune such as seems in general not to have attached to any- thing connected with the expedition of la Perouse. Perhaps, however, d’En- - trecasteaux might have had that melancholy satisfaction, if his officers had paid more attention to the piece of iron, mounted as a hatchet, which was seen in possession of the natives of Santa Cruz, for it had very possibly been pro- cured from the remains of the wrecked frigates. But who will venture to say that in their circumstances he would himself have divined it. + However that may be, the hour had now come for the departure of the ex- pedition. Sailing from Santa Cruz it pursued its prescribed course, and thus separated itself more and more from the principal object of its research; yet, thanks to the indefatigable zeal of M. Beautemps-Beaupré, it continued to ren- _ der eminent service to hydrography. It traversed the archipelagos of the Solo- mon and Louisiade groups, the coasts of New Britain and New Guinea; but a de- plorable incident awaited it on these obscure shores. Admiral d’Entrecasteaux died July 20, 1793, after a short illness which presented some of the symptoms of scurvy. The captain of the frigate ’ Esperance had already fallen a victim to fever in the port of Balade. Very soon scurvy and dysentery had decimated the crews which left France in 1791, while the loss among the higher officers divided itself with impartial severity between Paris and Coblentz. Not that there was any suspension of the surveys, which continued to produce excellent charts, but a feeling prevailed that it was time to desist. The two frigates were turned towards the island of Java, and entered the port of Sourabaya, where the voyagers learned that the day of their arrival was not only October 27, 1793, but, at the same time, the 6th Brumaire of the year IT. The expedition was here broken up and its different members returned sep- arately to Europe. In his passage, M. Beautemps-Beaupré stopped some time at the Cape of Good Hope. He had preserved the minutes of his charts, but the fairly executed transcripts, with other scientific documents collected by the expedition, were captured on the return by the English, by whom, however, they were restored at a later period. Yet, to avoid the possibility of their dis- appearance, he employed the time of his stay at the Cape in making a new copy, which his friend M. Renard, chief surgeon of the expedition, undertook to convey privately to the representative of France in the United States of America. He himself embarked on a Swedish vessel, which landed him at Goth- embourg, where M. Fournier, French consul, procured him the means of re-entering his own country. Arrived at Paris August 31, 1796, after an absence of five years, he rejoined his excellent friend M. Fleurieu, and resumed, under his direction, the prepara- tion of the Neptune of the Baltic sea, being at once named hydrographic engi- neer of the first class, and under-keeper of the general depot of the marine. In 1798 the editing and publication of the charts of the voyage of d’Entrecasteaux were officially confided to him. This great performance, which did not appear *? . * MEMOIR OF C. F. BEAUTEMPS -BEAUPRE. 1% till 1808, was a work of prolonged execution, but the co-operation which he gave it did not engross him exclusively, and from the 20th J uly, 1799, to the 26th June, 1804, he was charged in’ chief with making the hydrographic survey of the course of the Scheldt, and with a succession of other hydrographic mis- _ af sions relative either to the Scheldt or to the coasts of the North sea. [as Admiral Rosily, director of the depot of marine, being designated at the end of the campaign of 1802 to make an inspection of these labors, informed himself. 3 of the methods followed by M. Beautemps-Beaupré, as well in fixing the posi- ; tions of shoals and of soundings as in the construction of the plan. He gave # his complete approbation to these methods, which consisted essentially in the combination of the accurate measurement of angles by means of the circle of reflection, with the employment of the geometric principle of the “ problem of | three points,”’ a combination whose application to submarine topography is one % of the best titles of M. Beautemps-Beaupré to the respectful consideration of hydrographers. In 1804 the Nautical Description of the Coast of the North Sea from Calais to Ostend was published under the auspices of the depot of marine. ‘This work gives in detail the description of the shoals which obstruct the port of Dunkirk, and of those which are comprised between Dunkirk and the entrance of the Scheldt, as well as the nautical instructions necessary for mariners who frequent those shores. The chart which accompanies it was reproduced. at the hydro- graphical office. of London, with an English title, as having been executed by Admiral Beautemps-Beaupré ; for the English were not slow in ascertaining, though a little vaguely, that under that name there existed a hydrographer worthy of the highest confidence. In the following years M. Beautemps- Beaupré explored the course of the Scheldt, till then but little studied, and, for * the first time, demonstrated the practicability of the ascent of that river by ships-of-the-line as high as Antwerp, an indieation which furnished a basis for $ the plans of the Emperor at that point. Charts of minute detail embody the results of these labors, before the termination of which M. Beautemps-Beaupré was advanced in his position as hydrographical engineer and officer of the marine, and was named (August 5, 1804) a member of the legion of honor. He e: had by this time, indeed, become pre-eminently the hydrographer of the Em- peror Napoleon. The latter, when a city or department required an important and difficult construction, was accustomed to say: “ I will send Prony thither.” When the matter in hand was the elaboration of one of those great projects which he had so justly at heart for the re-establishment of our maritime power, he sent, without saying anything, M. Beautemps-Beaupré. After the campaign of Austerlitz and the peace of Presburg, the views of the Emperor were turned towards the coasts of Dalmatia, of which the numerous inlets and islands, with their steep banks and deep channels, present magnifi- cent harbors, equally sheltered from the wind and the enemy, and of great importance to the Venetian marine. M.Beautemps-Beaupré received (February 6, 1806) an order to make the hydrographic survey of the military ports on the east shore of the Gulf of Venice. 'To this object he devoted three campaigns, in 1806,-1808, and 1809. He took plans of the whole coast from Trieste to the mouths of the Cattaro, embracing the port of Pola, and the still more magnifi- cent one of Calamota, near Ragusa. ‘The plans and surveys of coasts which he executed have been published on a reduced scale, but the admirably drawn * originals remain one of the ornaments of the depot of marine. After the battle of Wagram he was sent by General Maureillan, governor of Zara, to the headquarters of the French army at Vienna, as bearer of a conven- tion of armistice relative to Dalmatia. He received, on this occasion, from the hand of the Emperor, the decoration of the iron crown. Being ordered to report himself; with his charts, to the minister of marine at Paris, he had scarcely arrived at that city when he was named member of a commission : a = -+ * ‘ i 128 MEMOIR OF C. F, BEAUTEMPS-BEAUPRE. 1 charged with duties relating to military operations on the coast of Zealand, __ where the English had made a descent. Recurrence to him was the invariable “ie _ rule in everything bearing on the affairs of the Scheldt, and in the intervals of >. his labors in Dalmatia he had been repeatedly required to return thither. His ae indefatigable activity was equal to all demands. .*.. Anew phase in his life now opened to him. The death .of his venerable . master and friend, M. de Fleurieu, had left a place vacant in the first class of the Institute in the section of geography and navigation. M. Beautemps-Beau- pré consented, with much distrust, to become a candidate. To make the report on his titles to a nomination fell to the lot of M. Arago, who, observing the number and variety of his labors, said to him: “ You must have lived a hundred years !”’ He had lived, however, but forty-four, and was nominated, September 24, 1810, by a large majority. One of his principal competitors was Admiral de Rosily, director of the depot of marine, his official chief and constant friend. The transient rivalry produced no change in their feelings or relations. In our peaceful contests, he who loses to-day frequently succeeds to-morrow, and the merit of one aspirant places in higher relief the merits of others. Admiral Rosily was himself an hydrographer of much experience and great knowledge. In 1787, during the voyage of la Perouse, he had executed, by order of the King, on the frigate Venus, which he commanded, the hydrographic recon- naissance of the Red sea. In 1816, zealously supported by M. Beautemps- Beaupré, he, too, became a colleague of the Academy in the section of free academicians. In 1811 the empire had been extended as far as Hamburg and Lubeck. M. Beautemps-Beaupré, who, at the beginning of his career, had labored on the _ Baltic Neptune under M. Fleurieu, was now charged with the hydrographic exploration of the northern coasts of the empire beyond the Scheldt. From 1811 to 1813 he made a series of surveys in the departments of Holland, as well as at the mouths of the Ems, the Weser, and the Elbe, in view of the estab- lishment of a great military port. ‘The decision, founded on his investigations, being in favor of the Elbe, he was charged, with the selection of the most favorable site on the left bank of that river, and made a complete hydrographic survey of its course. | In 1815, during the hundred days, the Emperor, at a reception in the Tuil- leries, stopping abruptly before M. Beautemps-Beaupré, said to him, with an air of chagrin: “ We are still very far from the Elbe—and your charts ?” “ Sire,” replied M. Beautemps-Beaupré, ‘1 considered it my duty to send them to the United States by an American vessel.” “ J¢ zs well,” rejoined the Emperor, gratified at recognizing in this trait the man who had been the confidant and faithful instrument of his great designs. At a later period the charts were remitted to the government of Hanover, and M. Beautemps«Beaupré was named a member of the Royal Society of Sciences of Gottingen. Justly honored for so long a series of services, he might have now resigned himself to a well-earned repose, but his was not the temperament for such an indulgence, and at an age when many think of closing their career he com- menced a new one. Since his return from the Cape of Good Hope in 1796, he had been unable, by reason of. the war, to extend his labors beyond the waters closed to the enemy, and, with the exception of his exploration of the coasts of the North sea, after the peace of Amiens in 1802, he had been obliged to confine himself to some of the rivers of Germany and the equally protected inlets of Dalmatia. The return of peace again made the ocean free, and the opportunity of revisiting it was seized with alacrity by M. Beautemps-Beaupré, for whom it seemed to revive the brightest days of his early manhood. Admiral Rosily, director of the depot of marine, had the merit of imme- diately comprehending what the occasion required and allowed, and Louis — XVIII that of entertaining his proposals with favor, notwithstanding the em- 2 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. 129 barrassments of the times. The ordinance directing the immediate prepara- tion of tlie pilot of the coasts of France was signed June 6, 1814, but the labor — could not be commenced till 1816. By an ordinance of the former date, M. Beautemps-Beaupré was named hydrographic enginecr-in-chief* and joint keeper of the general depot of the charts, plans, and journals of the marine. The condition of French hydrography at that time was an anomaly result- ing from circumstances. The administration of Louis XIV had occupied itself — with the hydrography of the coasts of France, and the engineer Lavoye had executed, about 1670, charts of the coasts of Brittany which were quite passa- ble, or at least very much. superior to those which represented the parts of the coast comprised between the mouth of the Loire and the shores of Spain. A century afterwards, in 1776, the government ordered a hydrographical recon- naissance of the coasts of France under the superintendence of la Brettonniere, captain in the navy, and Mechain, astronomer for the marine and member of the Academy of Sciences; but it would seem that those distinguished person- ages were rather charged with the collection of materials for rectifying the errors of the old charts, than with the execution of such a detailed and com- plete survey as might meet the wants of the service under al! circumstances. There remain in the archives of the depot of marine but few documents rela- ting to their operations, which extended, however, from Dunkirk to the Bay of Cancale. . Since that time geography had made in France important advances with which hydrography had by no means kept pace. Before the close of the eighteenth century there were geographic charts of a great part of the globe, com- petent to convey a general and sutfiiciently precise idea of the continents and seas. France particularly had been enriched with the map of Cassini, known also by the name of the map of the Academy, a work of great merit for that time in point of execution, and of great utility. it may be said, however, with truth, that towards the end of the last and in the first years of the present cen- tury, the art of constructing geographical charts received improvements by which it was essentially revolutionized. This amelioration was consequent upon the establishment of the metric system, which had necessitated the meas- urement of the meridian of France, from Dunkirk to Barcelona, and afterwards to Formentera. To the chain of triangles established in the execution of this measurement a comprehensive triangulation was subsequently attached, ex- tending over the whole of France, and in the sequel over considerable portions of Spain, of Italy, and of Great Britain. In the prosecution of these vast and difficult labors several members of the Academy have borne a conspicuous part: MM. Delambre, Mechain, Biot, Arago, Mathieu, Puissant, in conjune- tion with most of the members of the corps of topographical engineers and sundry officers of the military staff. On the triangles of the meridian has been based the trigonometric system of the new map of France, published by the depot of war. In England, savants of the highest merit, Colonels Mudge, Roy, Sabine, and the most distinguished officers of the ordnance corps, have * Tt may occasion surprise that M. Beautemps-Beaupré, employed and appreciated as he was by the Emperor Napoleon I, should have retained till 1824 the title of ingenieur-hydro- graphe ordinaire; but this will be more easily understood from the following letter written July 20, 1819, by M. le due Decrés, who had been minister of the marine under the empire: ** All the world appreciates the services rendered by M. Beautemps-Beaupré with a zeal, per severance, and talent above all praise; but I, who have maintained ciose relations with him for many years, cannot but regard him with sincere attachment, and owe him many thanks for the proofs of friendship which he has always given me. There are persons who, without the least claim, are always soliciting; these are numerous. There are others, forming but a small minority, who, with the most incontestable claims, never solicit anything. The fact is, that during the eighteen years of my official relations with M. Beautemps-Beaupré, he ceased not to occupy my attention by his labors, but never once invoked it by a solicitation. Since. he forgets himself, it is but right that justice and friendship should remember him,” ois 130 MEMOIR OF CG. F. BEAUTEMPS-BEAUPRE. combined their operations with those of our own countrymen, and have com- menced the publication of a magnificent chart of England, designated by the name of the Ordnance Map. To place French hydrography on a level with geography, while rescuing it from the momentary abandonment which war had necessitated, was now the object of interest. ‘The instructions which M. Beautemps-Beaupré received for this purpose were framed by Admiral Rosily, chief of the marine depot, and M. de Rossel, who had become one of its joint directors, after having aided in the hydrographical labors of the expedition of d’Entrecasteaux. 'T' hese in- structions indicated the west coast of France as first claiming attention, since among all those to whose hydrography navigators had need of daily recur- rence, this was most noted for its defect of exploration. It was to Brest, therefore, that M. Beautemps-Beaupré repaired, and here two schooners had been built for him, whose names, /a Recherche and 7’ Astrolabe, gratefully re- called the memory of la Perouse and d’Entrecasteaux. To these were joined the light vessels necessary for the accomplishment of his mission. In indicating the objects proposed for his attainment, he was left at liberty to adopt that mode of operating which long experience in labors of this nature might induce him to select. He thus found himself authorized either to unite all the means placed at his disposal on a small extent of coast, in order to pro- educe promptly a description of it, or to distribute them over several points.at the same time. The first was the mode on which he determined; as well because he had already proved, as he himself tells us,* its efficiency under various cireum- stances, as because it was the only one which would enable the depot of marine to publish in succession the collective results of each campaign. By concen- trating the operations of the engineers successively on small extents of coast, it was in his power to verify in some measure daily the labors of each of his as- sistants. ‘hus, for instance, when an engineer, in sounding, encountered some obstruction which had escaped former researches, he gave notice of it, and M, Beautemps-Beaupié was in a position to make a personal investigation imme- diately. To this mode of operating he owed the advantage of being able to combine all his means at the same moment on a dangerous position, when the weather was favorable. In this way he has often succeeded in terminating in a single day, or even a few hours, the examination of dangers situated far in the offing, the description of which would have. required the employment ‘of an isolated engineer during a whole season; of this kind were the reconnaissances of the western extremity of the bank noe race of Sein, the flats of Roche- Bonne, &c. The years 1816, 1817, 1818, were exclusively devoted to the survey of the maritime position of Brest, and ite results, forming the first part of the Pdlote Frangais, were published in 1822. The operations of 1819, 1820, 1821, and of the first part of 1822, sate the survey of that part of the western coast of France comprised between the point of Penmarch (Finisterre) and the isle of Yeu, (Vendée,) and furnished’ the materials of the second part of the above work, published in 1829. From 1822 to 1826 the survey was extended to that part of the coast comprised between the isle of Yeu and Spain, and its results appeared as the third part in 1832. In 1839 the fourth part was given to the world, representing the labors of five years from 1829 to 1833, and embracing a description of the coast between the isle of Brehat and Bar- fleur. In 1834, 1835, and 1836, the operations were extended from the latter point to Dunkirk. Finally, in 1837 and 1838, the survey was made of that portion of coast comprised between the isle of Brehat and the * Exposé des Travaur Relatifs a la Reconnaissance Hydrographique des Cétes Occidentalis de France, par M, Beautemps-Beaupre, p. 3. ~ MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. 131 northern rocks of the Passage du Four, (Finisterre,) where operations had stopped in 1818, and thus were completed the materials for the fifth and sixth parts of the Pi/ote Frangais, which appeared in 1842 and 1844. The six atlases contain twenty-one general charts, sixty-five special charts, thirty-one plaus of double elephant size, fifteen of half elephant, and fourteen of quarter elephant size, two hundred and seventy-nine tables of surveys taken of the principal dangers of the west and north coasts of France, and one hundred and eighty-four tables of high and low water observed during the progress of the twenty seasons spent upon the same coasts. The account (/’ Exposé, &c.) of these hydrographical labors, executed under his orders, was so drawn up by M. Beautemps-Beaupré as to serve as the complement to the second chapter of the appendix attached to the first volume of the voyage of d’Entrecasteaux. In justifying this form of composition, he pleads that, when that appendix was ublished, his practical knowledge of the best means for reconnoitring maritime Be rections could not be so positive as that acquired during his first ten cam- paigns (1817 to 1827) on the coasts of France. It is certain, nevertheless, that in everything essential his method was definitely fixed at the time of the pub- lication of d’Entrecasteaux’s voyage in 1808; and in the preface to that work it is thus spoken of by M. de Rossel, an authority of undoubted competency : “ Navigators will in general find in this appendix hydrographic instructions of a far more complete nature than any heretofore published. M. Beautemps; Beaupré has here given also several expeditious methods for sounding a coast and marking the depths on the chart. These methods, of which he availed himself for his operations conducted on the coast of France, (before 1808,) by order of the minister of marine, are so useful that it would be unjust to with- hold them from navigators, as well as those of which he made use during the campaign.” From these judicious observations of one of the masters of hydrographic science, it will readily be inferred that the operations which M. Beautemps- Beaupré conducted on the coasts of France differ in several essential particulars from those with which he was habitually occupied in the voyage ot d’Entre- casteaux. In the latter, which pertain generally to what is called surveying under sail, the end principally in view was to fix the position of the remarkable objects seen on the land, capes, mountains, &c., by means of observations directed towards those objects from certain points in the course of the ship, de- termined with especial care. The operations on the coasts of France, within an extent generally less wide and with much less rapidity, had in view to fix various points of the sea, rocks, places of sounding, &c., with reference toi cer- tain objects determined on land, mountains, steeples, semaphores, and other signals. ‘This was almost an inverse operation to the preceding; yet this also required numerous admeasurements of angles, which were obtained with the same reflecting circle, and the geometric constructions were derived essentially from the same trigonometric principles, although the proposition of the “ problem of three points”? was here more frequently employed. As the bearings taken from the sea were directed upon all the remarkable objects of the land, it was necessary that the position of these should be deter- mined by geodetic measurements made ashore with all the precision attainable by science. For this reason a triangulation was executed on land embracing all the points of the coast. This was effected for the western coasts of Irance, from Brest to Saint Jean de Luz, by M. Daussy, and for the northern and southern coasts by M. Bégat, both members of the corps of hydrographical engineers of the marine. ‘These triangulations have been connected with the grand triangulation which serves as a base for the new chart of I'rance pub- lished by the corps of the e¢at-major, and have been found so exact that they have been finally incorporated in that fundamental system. MM. Daussy and Bégat have deduced from their trigonometric labors a complete table of the 132 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. positions of all the remarkable objects of the coasts of France which can be seen from the sea; and it was by bearings directed upon these points, rigor- ously determined, that M. Beautemps-Beaupré and his assistants fixed the posi- tions of the points of the sea which were to be marked on the charts and plaas. The bearings were invariably taken with the reflecting circle, in the managt- ment of which valuable and delicate instrament M. Beautemps-Beaupré had acquired great dexterity. Nor was he less expert in constructing graphically on the first rough draught of his chart the points observed by his method, founded on the geometrical principle of the “problem of three points.” He was master in a surprising degree of the varied constructions deducible from this principle, and applied them, as the case might require, with the utmost readi- ness and sagacity. It is usually by means of the circumferences of circles described with the ob- served distances that the points of station are obtained; but when this construc- tion presents some difficulty by reason of the length of the radius of the circle, the nearness of centres, &c., it is practicable to substitute one of those somewhat. numerous and generally quite simple constructions which elementary geometry deduces from the same fundamental theorem. ‘Thus, in many circumstances, calculation may be used to find the radii and centres of the circles to be described. M. Beautemps-Beaupré recommends for these constructions, combined with ‘ealculation, the employment of the tables of natural tangents and sines. The seale adopted by the hydrographic engineers for the first reduction of labors was six lines for 100 toises, or zq455 equal to six times that of the che. of Cassini. 'The charts, and even plans, however, have been generally published on a scale much smaller, but M. Beautemps-Beaupré soon recognized the propriety of not only collecting the materials requisite for the execution of the new charts of the coasts of France, but of exerting himself, moreover, to bring together in the archives of the depot of marine all the documents which might be useful in the sequel for forming a judgment of any projects relating to navigation. He suffered himself to be deterred neither by the difficulties nor magnitude of the work, and the depot found itself eventually in possession of a collection of five hundred and twenty-seven quarto volumes, containing the documents requisite to execute at need, on the largest scale, the plan of all parts of the western and northern coasts of France to which the attention of govern- ment might be called. One of the most essential and useful parts of marine charts is the indication of the depths of the sea at different points obtained by the sounding line and denoted by figures on the chart. M. Beautemps-Beaupré was equally skilled in making and in marking the positions of soundings, and it is with the authority of a practised master that he recapitulates in the Exposé des Travauz, &c., the rules of the difficult art of submarine topography. It was seldom that an obstruction or peril escaped him, though he seems to take pleasure in citing, for the instrue- tion of his successors, instances in which his researches were bafiled for years in succession. One day notice was given him that a vessel had touched upon a rock at a point where none was known to exist. He sought for it a long time without success, but at last his line fell upon it. The rock was simply a peak whose diameter scarcely exceeded that of.the lead of the sounding line. It is necessary to take account in soundings of the constant variations of the level of the sea by reason of the tides. “'The first thing to be done,” says our hydrographer, “at the commencement of a campaign, on a coast where the water through this cause continually changes its level, is to place a certain number of scales, divided into feet and inches, on which those changes shall be observed, since it is by means of observations of this kind that we are enabled, in giving the chart its definite form, to reduce to the lowest water’ level the soundings made at all hours of the day and tide. ‘To reduce the soundings is to subtract from the depths found on different days and at all hours of the tide, for every MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. P38 / point of the coast sounded, the suitable number of feet, in order to transfer to the plan only the depths of water found at each point at the precise instant of lowest depression. ‘the tables of high and low tide, at many principal points on the coasts of France, are extracts frem the large body of observations which served for the reduction of the soundings.” (Ezposé des Travaux, &c., p. 10.) As M. Beautemps-Beaupré has more than once remarked, the soundings in many parts of the sea are far from being necessarily unchangeable. It is readily conceived that they must vary as well from the effect of deposits produced at some points as of erosions which take place at others. He had said, as early as 1804, in his nautical description of the coast of the North sea: « We forewarn navigators that our work must not be regarded as everywhere authoritative, ex- cept for a limited time, on account of the changes which are in progress in the shoals upon these shores.’”’ ‘To the same effect he observes with reference to the western and southern coasts of France: ‘* All banks of sand and ooze un- dergo changes of position and of depth of which navigators should ever be dis- trustful, since the best charts can only give, as regards dangers of this kind, insufficient information when some time has intervened since their construction. And this applies especially to such banks when they obstruct the mouths of rivers. Hence the necessity of sounding annually the principal channels, and, indeed, of frequently renewing the charts of the entrances of rivers.” It may be added that the comparison of the successive charts of the same region will some day furnish valuable data respecting the accumulation of sub-marine alluviums. It was to the class of researches just spoken of that our colleague dedicated his last hydrographic labor. He had not taken final leave of the sea in closing, in 1839, his survey of the northern coast of France. In 1841, at the age of seventy-five, he cheerfully complied with the invitation of Admiral Baudin to join him in an investigation of the changes produced in the system of bars at the mouth of the Seine within the seven preceding years. It was then that for the first time he had at his disposal a vessel moved by steam, and the superior facilities thus furnished for hydrographic enterprises drew from him the remark, “That he would gladly recommence his career if it were only for the pleasure of prosecuting hydrography with such advantages.” Though he cheerfully acknowledged that the marine had done in his behalf all that was practicable, yet he had never, during his operations on the coasts of France, possessed other resources for transportation than those supplied by the sail and oar. He had generally at his command a company of eight or ten hydrographical engineers and officers of marine, and from this school of prac- tical hydrography have proceeded many of each class who have since been in- trusted with the most important labors in remote as well as neighboring seas. Among them have appeared at different times our present colleagues, M. Daussy, Admiral du Petit Thouars, and M. Dortet de Tessan; MM. Givry and Gressier, to whom was intrusted, under our distinguished and regretted colleague, Admi- ral Roussin, the hydrography of the coasts of Brazil; MM. Monnier and Le Bourguignon Duperré, who have furnished us a magnificent chart of our colony of Martinique, and have commenced the hydrographic survey of our Mediter- ranean coasts, and those of Italy; MM. Begat, Keller, Chazallon, Lisusson, Delamarche, de la Roche-Poncié, now actively prosecuting the grand hydro- graphic enterprises of the depot of marine; MM. Darondeau and Vincendon Dumoulin, who have so honorably associated their names with our great voy- ages of circumnavigation and other important labors; MM. Le Saulnier de Vauhello, Lapierre, Jehenne, De Villeneuve, who, as officers of our marine, have in different quarters of the world rendered signal services to hydrography. Familiar with all the hazards of the sea, M. Beautemps-Beaupré exercised a consummate prudence in the employment of his assistants, and was justified in saying to the Academy, when he presented it with the sixth and last volume of 134 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE. the Pilote de France: “It completes the satisfaction I feel at having brought to a successful close so considerable a work as that which I now submit to the Academy, that never in the course of twenty campaigns, amidst the innumerable dangers which beset our coasts, hi ve I had to deplore the loss of one of my Gomiades by any accident of the sea.’ Nor was he less emphatic i in acknowl. edging the zeal and science of those te had taken part in his labors, and we feel rh it it was with equal pride and pleasure that he took another oecasion to say: “ Practical knowledge may advance, and methods be hereafter improved, but we believe ourselves fully justified in affirming, that under no circumstances can greater zeal be exerted than has been displayed by all our fellow-laborers.” Hence, when Louis Philippe, in 1844, named him grand officer of the legion of honor, the entire cor ps of hy drographic: ul engineers felt themselves recompensed in the person of their v enerable chief. Kindness of disposition did not preclude, in the case of our colleague, great firmness of character, as was abundantly manifested amidst the vex aati in- separable from labors like his; especially was his constancy of purpose proved by a circumstance which would have discouraged most others. Although he embarked young, and at the outset was tossed fur two successive years on the most stormy seas, he ceased not at any time to be subject to sea-sickness, and it was amidst sufferings from this malady, which so completely subdues the stoutest spirits, that for fifty years it devolved on him to measure angles with the nicest precision, and note the details of soundings, while exposed on slight vessels to the waves which often swept over himself and his draw ings; yet “hie paid no attention to these things, and disliked to have his infirmity observed by others. ‘lo his assistants, Wow even his sufferings could not be unknown, and must have contributed to the sympathetic ee with which he was regarded by those, whether officers or mariners, with whom his labors brought him into contact. Jt was indeed natural that, with such a character as his, M. Beautemps- Beaupré should be loved by all who approached him, and it may be readily imagined that the 25th September, 1848, which witnessed his official retirement, was, for the depot of marine and the whole corps of hydrographic engineers, a day of undissembled regret. Equally may we conclude that it was a day of festivity when, February 2, 1853, M. Ducos, minister of marine, came, in the name of the Emperor and in the presence of the corps of engineers, to inaugurate the bust of our colleague in the grand gallery of the depot, whose iny aluable documents have in great part been collected by himself or under his orders, or at least by the methods with which he has endowed hydrography. On this interesting occasion, Admiral Mathieu, the worthy and learned director of the depot, pronounced a discourse, from which I must content myself with trans- cribing the following passage: “In having constantly before our eyes the ven- erable: features of him who was once our chies, and who has created that admi- rable hydrographic science which is the torch of navigation, we shall recall without ceasing his vast and conscientious labors, his useful counsels, his devo- tion to duty, his rigid probity, and at every moment of the day, so to speak, we shall pay him the abate of respect and gratitude due to him by so many titles.”’ ‘To this address M. Ducos cordially responde d: “This bust,” he said, in closing his remarks, “is entitled to our respect, for it is that of M. Beautemps- -Beaupré, so much endeared to the navigators of all nations and of every sea. In dedi- eating this efiigy of the man of science, whom you justly consider the founder of the depot of marine, in the place which has been the witness of the labors of his long career, it would seem to be no strained metaphor which should liken this tribute of your regard and veneration to one of those beacons ereeted by his counsels and exertions by which you would ingeniously recall to his sue- cessors the modest point of departure, and the glorious point of success which they too may realize.” The bust is perfect in its resemblance, faithfully repro- 2 MEMOIR OF C. F. BEAUTEMPS-BEAUPRE.” 135 ducing the noble features, the kindliness, united with penetration. which charac- terized the original. Under a physiognomy impressed with so much goodness, we are easily persuaded that we see one of those ancient savants of the primitive type whose renown is the property of ages. ‘To the skilful statuary (M. Desprez) who executed it, the more honor should accrue, inasmuch as M. Beau- temps-Beaupré had reached the age of eighty-six without having ever permitted any one to take his portrait. After the ceremony, the minister, the admiral, and the whole body of assistants proceeded to the modest residence of M. Beautemps-Beaupré, in the street des Sacnts-Peres, there to render to the illus- trious old man in person, and amidst the applause of all present, an homage which must have sensibly touched his heart. Nor were the scientific bodies, to which he belonged by more than one title, less conscientious in their acknowledgments. In 1824 he had been named member of the bureau of longitudes, and assiduously attended the meetings whenever he was in Paris. His advice in all that regarded navigation was here listened to with invariable deference. He had been also named one of the commission of light-houses from the commencement in 1826, and was especially intrusted with the suitable location of those invaluable aids to navigation. The active and influential part which he took in the deliberations of the board was warmly acknowledged at his funeral by M. Leonece Reynaud, the skilful con- structor of the light-house of Brehat, the site of which was fixed by M. Beau- temps-Beaupré himself, after the difficult and dangerous exploration of the Roches-Douvres at the entrance of the British channel. His character, his long experience of the sea, his solicitude for the public good, conspired, with the intrinsic wisdom of his counsels, to secure their constant adoption. Even on his death-bed his thoughts were still occupied with the interests and dangers of maritime enterprise; and if he manifested a sensibility, it was to the assur- ance that the member of the commission of light-houses had completed the work of the hydrographer, and that thenceforward all important questions bearing on the lighting of our sea-coast were resolved. Whatever related to the sea interested him to the last. In 1853 a commission was appointed to investigate, under the direction of M. Dumas, certain ques- tions touching the existence of the ¢angwe, a product of marine origin which the sea throws up at the entrances of certain rivers of Normandy and Brittany. Agriculture dreaded the disappearance of this fertilizer. The commission, de- sirous of consulting M. Beautemps-Beaupré on this production of shores which he had so thoroughly explored, repaired in a body to his residence. The aged navigator recovered all his animation im speaking of places which he had so often visited: “We know not,” he said, “how the tangue is reproduced at those points; it is the fowl which lays golden eggs; it must not be interfered with.” In the presence of the great spectacles of nature, M. Beautemps-Beaupré had contracted a taste for natural history. If he did not cultivate it himself, he zealously aided those who did. In the expedition of d’Entrecasteaux he had formed intimate relations with its botanist, M. de la Billardicre, and it was he who brought to France the beautiful nautilus vitré now in the Museum of Natural History which was bequeathed to the government by M. de Kermadee, captain of the Lsperance, on his death in New Caledonia. Many of our col- leagues recall with sensibility the cordial and obliging reception extended to them on our coasts by M. Beautemps-Beaupré while prosecuting his own arduous hydrographic labors. Reared among the savants of the close of the eighteenth century, he had pre- served that almost religious respect for science which was one of their dis- tinctive characteristics. Hence the dignity, united with friendliness, which per- vaded all his relations. ‘He was,” said the Marchioness de Laplace, whose remembrance is itself a eulogy, ‘a man of an antique character.” He possessed 136 MEMOIR OF CG. F. BEAUTEMPS-BEAUPRE. ‘ that elevation of sentiment which Plutarch so well knew how to paint. Reverses — of fortune, which would have overwhelmed another, were encountered by him — with stoic firmness. Involved at an advanced age in the failure of a banker,* he lost by that event the savings of his whole life; but he contented himself with saying affectionately to Madame Beautemps-Beaupré, “'This event, my love, makes us younger by thirty years,’”’ an expression which supposed in her an elevation of sentiment equal to his own. Few marriages, indeed, have been so happy as that which he contracted, in 1804, with Madame Fayolle, widow of a commissary general of marine. Both were nearly eighty when death sepa- rated them by the removal of the w ife; it was the first cloud which had dark- ened their union. M. Fayolle, issue of the first marriage of Madame Beautemps-Beaupré, found in our colleague a second father, and, as hydrographical engineer, was for many years one of fine most distinguished and useful assistants. M. Beautemps-Beaupré had always had a weakness of the breast; at the age of eighteen some physicians had even augured an early decline. W hen he embarked to take part in the expedition of d’Entrecasteaux, it was generally thought that he would never again see France. ‘This prognostic was fortu- nately falsified; but an penne cough attended his whole life, and in later years subjected him to much annoyance. It will scarcely be forgotten among ourselves that, at our sessions, he was a model of punctuality. He signed our record the 23d of October, 1853, but thenceforward was forced to renounce his attendance. 'This privation, and the sufferings which occasioned it, he bore with a resignation full of cheerfulness. One of our colleagues having called to see him, and expressing the hope that a strong constitution would again restore him to us, he replied with a smile, “I am duly sensible of your kindness, but I shall soon be eighty-eight.” Firm in | a Christian faith, M. Beautemps-Beaupré accepted death without a murmur. “Let us not repine,” said Admiral Baudin at his grave, “that, in subjecting him for several months to the supreme trial of excessive suffering, God afforded him the opportunity of setting an example of resignation and unalterable serenity.” He expired March 16, 1854, surrounded by a devoted family, which numbers two inheritors of his distinguished name—M. Pierre Beautemps-Beaupré, presi- dent of the Chamber of Commerce of Grandville, and M. Charles Beautemps- Beaupré, imperial procurator at Mantes. In this Academy he succeeded M. de - Fleurieu, his master and friend, and has himself been succeeded by M. Daussy, who, from 1811, had been his most constant collaborator, and who efliciently contributed to secure to the hydrographic survey of the coasts of France geodetic bases of irreproachable precision. * The banker, who was his relative, might have been prosecuted for fraudulent bank- tuptcy. M. Be autemps- -Beaupre threw in “the fire the only paper which could have pro- cured his condemnation, saying, ‘‘1t is not I who will ever be instrumental in disgracing a relative.” * OUTLINE OF THE ORIGIN AND HISTORY Ps OF THE BOvAL. SOCLETY. O02 «L0N DON PREPARED FOR THE SMITHSONIAN INSTITUTION BY C. A. ALEXANDER, “The principal advantage of academies consists in the philosophical spirit naturally en- gendered by them, which spreads itself throughout society, and extends to all objects. The isolated inquirer may resign himself without fear to the spirit of system; he only hears afar off the contradiction which he incurs. But in a learned society the conflict of systematic opinions soon results in their overthrow ; and the desire of being mutually satisfied necessarily establishes between the members anagreement to admit nothing but the results of observation and calculation. Hence, as experience hus shown, true philosophy has been generally dif- -fused since the rise of academies. by setting the example of subjecting everything to the examination of a rigorous analysis, they have dissipated the prejudices which had too long tyrannized in the sciences, and in which the best intellects of preceding ages had shared. Their useful influence over opinion has, in our day, dispelled errors which had been received with an enthusiasm that in other times would have perpetuated them. Equally exempt from the credulity which would admit everything, and the prejudice which disposes to the rejection of whatever departs from received ideas, these enlightened bodies have always, in difficult questions, and with reference to extraordinary phenomena, wisely awaited the answers of ob- servation and experiment, which they have at the same time solicited by prizes and by their own labors. Proportioning their appreciation, as well to the magnitude and difficulty of a discovery as to its immediate utility, and convinced by many examples that the most sterile in appearance may some day lead to important consequences, they have encouraged the re- search for truth in regard to all objects, with the exclusion of those only which the limits of man’s understanding render forever inaccessible. Finally, it is from their bosom that those great theories have arisen whose generality places them beyond the common reaeh, and which, spreading themselves by numerous applications over nature and the arts, have become inex- haustible sources of light and fruition. Wise governments, convinced of the utility of such societies, and considering them as one of the principal foundations of the glory and prosperity of empires, have not only instituted them, but attached them to their own service, that they might derive from them that knowledge which has often proved of the highest public’ advan- tage.” —(Laplace, Precis de l’ Histoire de l’ Astronomie, p. 99.) “The development and advancement of science,” it has been remarked, “are signally indebted to three among modern associations: the Accademia del Cimento at Florence, which endured, however, but for a short time; the Royal Society of London; and the Academy of Sciences at Paris.” The first of these was established in 1657, under the patronage of the Grand Duke Ferdinand II, acting upon the advice of Viviani, the great geometrician. ‘The name adopted by this society implies as its object the investigation of truth by experiment alone, and its members, whose number was unlimited and included the distin- guished names of Castellio and Torricelli, were held to no other obligation but an abjuration of all authority and a resolution to inquire after truth, without regard to the doctrines of any previous system of philosophy. Nor did the Academy pass away without leaving a record of its labors. A volume, con- taining reports of the experiments made under its auspices, was printed in 1666, including, with many others, those on the supposed incompressibility of water, the universal gravity of bodies, and the property of electric substances. For England, after Italy, is claimed a priority in the formal inauguration of a similar and purely scientific association, and the date of the establishment of 138 ORIGIN AND HISTORY OF THE the Royal Society, which is referred to 1660, certainly preceded by six years that of its French rival. But, independently of the consideration that the period had arrived when the state of experimental science urgently demanded the realization of those splendid visions of associated activity which had long before kindled the imagination of Bacon, * the chronological origin of the illus- trious bodies in question is involved in some obscurity in consequence of their previous existence as private and spontaneous reunions of certain learned men of the age. Ilence the title of the “ Invisible College,” which we find applied by Boyle to the future Royal Society, while as yet it existed only in this in- choate state, a period of which the following passageg convey to us some inter- ene notices ; és About the year 1645,” says Dr. Wallis, “while I lived in London, (at a time when, by our civil wars, academical studies were much interrupted in both our universities,) besides the conversation of divers eminent divines as to matters theological, | had the opportunity of being acquainted with divers worthy persons inquisitiye into natural philosophy and other parts of human learning, and particularly of what hath been called the New Philosophy, or Experimental Philosophy. We did, by agreement, divers of us, meet weekly in London on a certain day, to treat and discourse of such matters. Our, busi- ness was (precluding matters of theology and state affairs) to discourse and con- sider of philosophical inquiries, and such as related thereunto, as physic, anatomy, geometry, astronomy, navigation, statics, magnetics, chymics, me- chanics, and natural experiments, w ith the state of these studies as then culti- vated at home and abroad. We oe discoursed of the circulation of the blood, the valves im the veins, the vene lactea, the lymphatic vessels, the Copernican hypothesis, the nature of comets and new stars, the satellites of Jupiter, the oval shape (as was then supposed ) of Saturn, the spots on the sun and its turning on ats own axis, the inequalities and sclenography of the moon, the several phases of Venus and Mercury, the improvement of telescopes and grinding of glasses for that purpose, the weight of air, the possibility or impossibility of vacuities and nature’s abhorrence thereof, the Torricellian experiment in quicksilver, the descent of heavy bodies and the degrees of acceleration therein, and divers other things of like nature, some of which were then but new discoveries, and others not so generally known and embraced as now they are.’ “For such a candid and impassionate company as that was,” says Dr. Sprat, in his History of the Royal Society, “and for such a gloomy season, what could have been a better subject to pitch upon than natural philosophy? To have been always tossing about some theological question would have been to make that their private diversion, the excess of which they themselves disliked in the public; to have been eternally musing on civil business and the distresses of their country was too melancholy a reflection. It was mature alone which could pleasantly entertain them in that estate. Their meetings were as frequent as their affairs permitted; their proceedings, rather by action than discourse, chiefly attending some particular trials in chemistry or mechanics. They had no rules nor method fixed; their intention was more to communicate to each other their discoveries, which they could make in so narrow a compass, than an united, constant, or regular inquisition. Thus they continued, without any great intermissions, till about the fatal year 1658, when the continuance of their meetings might have made them run the hazard of the fate of Archimedes; for then the place of their meeting (Gresham College) was made a quarter for soldiers.” “There arose at this time,” says Dr. Whewell, alluding to the period ante- oO cedent to the epoch of Newton, “a group of philosophers who began to knock *See the ‘‘New Atlantis,” of Lord Bacon. ROYAL SOCIETY OF LONDON. 139 at the door where truth was to be found, although it was left for Newton to force itopen. These were the founders of the Royal Society.” «* The men who formed the Royal Society,” says Bishop Burnet, “were Sir Robert Moray, Lord Brouncker, a profound mathematician, and Dr. Ward, a man of great re- search, and so dexterous that his sincerity was much questioned. But he who labored most, at the greatest charge, and with the most success at experiments, was the Hon. Robert Boyle, a devout Christian, humble and modest almost to a fault.” Among other names connected with the Society in its earlier stage, or at the period of its formal organization, and still memorable in science, literature, or the arts, may be distinguished those of Bishop Wilkins, Sir Kenelm Digby, Evelyn, Denham, Clarke, Cowley, Willis, Wren, Ashmole, &c. « The first journal book of the Society, a plain unpretending volume, bound in basil, yet destined to receive great names and to be the record of important scientific experiments,” opens with the date of November 28, 1660, and with the proceedings of a meeting which may be regarded as organic in relation to the form and permanence of the Society. Here it was determined that mect- ings should be regularly held every Wednesday during term time; that a con- tribution of ten shillings on admission, and of one shilling weekly, should be levied on each member, whether present or absent, as long as he should please to maintain his connexion with the association, and a list was formed of the names of such persons, known to those present, as were judged willing and fit to unite with them in their design. Ata subsequent meeting a committee of three or more (as occasion might permit) was empowered to frame a constitu- tion, which was submitted and adopted at a general meeting on the 12th of December following. By this, the standing officers of the Society were declared to be three: a president or director, a qrensuidr: and a register; the first to be chosen monthly, the two latter annually. An amanuensis and operator are styled “servants belonging to the Society,” and receive salaries, the former 40, the latter 4 pounds per annum. The stated number of members was fixed at fifty-five, with permission that all persons of the degrees of baron or above might, at their choice, be admitted as supernumeraries. It was provided that no candidate should be elected the same day he was proposed, and that at least twenty-one members should be present at each election. Tor such election, the amanuensis, it is ordered, shall provide “several little scrolls of paper of equal length and breadth, in number double to the Society present. One-half of them shall be marked with a cross, and being rolled up shall be laid in a heap on the table; the other half shall be marked with ciphers, and being rolled up shall be laid in another heap. Every person coming in his order shall take from each heap a roll, and throw which he please privately into an urn, and the other into a box. ‘Then the director. and two others of the Society, openly numbering the crossed rolls in the urn, shall accordingly pro- nounce the election.”” ‘'wo-thirds of those voting were necessary to a choice. The Society having included, as we have seen, two poets, Denham and Cowley, among its members, was fairly entitled to a greeting from the muse. This it received through the ingenious pen of Cowley, in verses whose philoso- phical truth as well as originality of illustration may perhaps still justify quotation. After deploring the fate of philosophy, which for three or four thousand years had been kept by unwise or dishonest tutors in a state of nonage, he tells us: Bacon, at last, a mighty man! arose, Whom a wise king and Nature chose Lord chancellor of both their laws, And boldly undertook the injur’d pupil’s cause. * * * From the long errors of the way, In which our wandering predecessors went, And, like the old Hebrews, many years did stray i 140 ORIGIN AND HISTORY OF THE In deserts, but of small extent, Bacon! like Moses, led us forth at last The barren wilderness he pass’d— Did on the very border stand Of the bless’d promis’d land, And from the mountain’s top of his exalted wit, Saw it himself, and show’d us it. If the poet has somewhat overstated the claims of Lord Bacon as the herald of experimental philosophy, he seems to have been gifted with a clearer vision | of the future achievements of the Society, which he thus apostrophises : From you, great champions! we expect to get Those spacious countries but discover’d yet ; Countries where vet, instead of Nature, we Her image and her idols worship’d see. * * ~ * * * * * New scenes of heaven already we espy, And crowds of golden worlds on high, Which from the spacious plains of earth and sea Could never yet discover’d be By sailor’s or Chaldean’s watchful eye. Nature’s great works no distance can ubscure, No smallness her near objects can secure: Ye’ave taught the curious sight to press Into the privatest recess Of her imperceptible littleness ; Ye’ave learn’d to read her smallest hand, And well begun her deepest sense to understand. Cowley possessed other claims than merely literary ones to scientific fellow- ship; he had taken a degree in medicine and written, elegantly at least, on plants and trees. He had besides, as Dr. Sprat assures us, accelerated the foundation of the Royal Society by the publication of a proposition for the ad- vancement of experimental philosophy, which is still found among his works, and though the form of his proposed “ college’? was not adopted, it cannot be denied that he has comprehensively, if quaintly, stated the objects to which such an institution would necessarily be destined: “'To weigh, examine, and prove all things of nature, and detect, explode, and strike a censure through all false moneys, with which the world has been paid and cheated so long, and (as I may say) set the mark of the college upon all true coins, that they may pass hereafter without any further trial. Secondly, it will recover the lost in- ventions, and, as it were, drowned lands of the ancients. ‘Thirdly, it will im- prove all arts which we now have, and, lastly, discover others which we yet have not.” It cannot but afford a curious insight into the state of natural knowledge at this early stage of the labors of the Society, if we glance at the manner in which it proceeded to deal with the currency of which Cowley speaks, in order to explode what was spurious and accredit what was genuine. With this view a few entries from the journal are here given: “Dr Clarke was entreated to lay before the Society Mr. Pellin’s relation of the production of young vipers from the powder of the liver and lungs of vipers. “*Sir Gilbert Talbot promised to bring in what he knew of sympatheticall cures. Those that had any powder of sympathy were desired to bring some of it at the next meeting. “The Duke of Buckingham promised to cause charcoal to be distill’d by his chymist, and to bring into the Society a piece of unicorne’s horn. “Sir Kenelm Digby related that the calcined powder of toads reverberated, applyed in bagges upon the stomach of a pestiferate body, cures it by several applications. [Digby delighted in the marvellous, and is said to have fed his wife on capons fattened with the flesh of vipers, in order to preserve her beauty. ] “* A circle was made with powder of unicorne’s horne and a spider set in the middle of it, bat it immediately ran out severall times repeated. The spider once made some stay upon the powder. on letter was introduced treating of a petrified city and its inhabitants.” &c., &c. ROYAL SOCIETY OF LONDON. 141 ' Other entries there are undoubtedly, and in greater number, which show that the spirit of inquiry was rapidly finding its true direction: Investigations of the mechanical properties of the air, by Boyle; experiments with the pendu- lum, by Sir Christopher Wren, who is said to have first suggested its oscilla- tions as a standard of measure; observations on the ‘“ anatomy of trees,” by Evelyn; instructions for the guidance of curious observers “in the remotest parts of the world.” Even what now seem Indicrous tentatives with the pow- der of toads and vipers, or frivolous inquiries respecting the witch-hazel and still more wonderful Lepas anatifcra,* itis more just to regard as obligatory and conscientious efforts to bring the questionable opinions of the day, however trivial, to the assay of direct experiment. The time will probably not soon come when science can claim absolute exemption from like humble labors ; not, at least, “ While,” to borrow the words of Sir Thomas Brown, “ the spirit of delusion, though expelled from his oracles and more solemn temples, still runs into corners, exercising minor trumperies, and acting his deceits in inferior seducers.”’ The Restoration, in diffusing a general sense of permanenceand security, was highly favorable to the objects of the association, and Charles II had enough of curiosity, perhaps of wisdom, to look with a patronising eye on inquiries which threatened to interfere neither with his indolence nor pleasures. He held sundry communications with the philosophers, and even proposed subjects for investi- gation, before proceeding to what has been uncharitably called the only wise act of his reign—the incorporation of the Royal Society. In the instrument by which this was effected, the King, after protesting his zeal for all learning, especially for those studies which aim by solid experiments to strike out something new in philosophy, or bring to perfection what already exists, (novam extundere philosophiam aut expolire veterem,) declares himself founder and patron of the Socicty, conferring on it the name of the Royal Society of Loudon pro scientia naturali promovenda.t Its government is deposited in the hands of a president and council, to the number, including the president, of twenty-one, all of whom were, in the first instance, nominated by the crown. For the succession, it is provided that an election shall annually take place on St. Andrew’s day, in which a president shall be chosen from among the members of the existing council, and ten of this latter body shall be removed, and their places supplied by others; on which occasion not less than thirty-one members of the Society shall be present, (the president or his deputy being always one of them,) and a majority of that num- ber shall determine the choice in each instance. Other officers of the Society are a treasurer, two secretaries, two or more curators of experiments, one clerk, besides two mace-bearers to attend on occasion upon the president. Power is given to the president and council to make from time to time such laws and ordinances as shall seem to them useful and necessary for the better government and regulation of the Society; and grants of certain pieces and parcels (pecios et parcellos) of land, of no great extent, are made to the learned body, to be held of the crown by the tenure of free and common soceage. A somewhat singular concession is that which authorizes the Society to demand the bodies of such executed criminals as may be desired for dissection—a circumstance * Sir Robert Moray, first president of the Royal Society, signalized the meeting at which he was elected by presenting a paper relating to barnacles, in which he affirmed that he had him- self seen, in the western isles of Scotland, trees to which were attached multitudes of shells, each containing a small but perfectly shaped sea-fowl, or solan-goose. He candidly confesses, however, that he did not see the products of these extraordinary limpets alive. t ‘The epithet natural,” says Dr. Paris, in his Life of Sir Humphrey Davy, ‘‘ was here intended to imply a meaning of which few persons are probably aware. At the period of the establishment of the Society, the arts of witchcraft and divination were very extensively en- couraged, and the word natural was therefore introduced in contradistinction to supernatural.” 142 ORIGIN AND HISTORY OF THE pointing perhaps to the large proportion of medical men which entered at that time into the association. Finally, it is provided that if abuses should occur or dissensions arise, the Archbishop of Canterbury and certain high officers of state shall be invested with powers for removing such abuses and deciding such controversies.* The first president of the Society, after the incorporation, was Lord Brouacker; the secretaries, Dr. Wilkins and Henry Oldenburg; all appointed by the crown, “Some idea may be formed of the activity of the Society at this period by the following list of eight committees appointed on the 30th March, 1664: 1. Mechanical, consisting of sixty-nine members. 2. Astronomical and optical, fifteen members. 3. Anatomical, consisting of Boyle, Hooke, Dr. Wilkins, and all the physicians of the Society. 4. Chymical, comprising all the physicians of the Society, and seven other Fellows. 5. Georgical, consisting of thirty-two members. 6. For histories of trades, consisting of thirty-five members. 7. For collecting all the phenomena of nature hitherto observed, and all experiments made and recorded, consisting of twenty-one members. 8. or correspondence, consisting of twenty members.” Oldenburg, about this time, received, as he tells Boyle, the agreeable assurance from his correspondents in Paris, that ‘‘the English philosophers were doing more for science than all the other nations of Europe, as well in curious and detached particulars as in the great works given to the public.” The labors of the Society were destined to be soon interrupted by the plague of 1665, which drove the members very generally from London. Oldenburg, however, remained at his post, and continued his correspondence on scientific matters during the whole period of the pestilence. When the meetings of the Society were resumed, the sources of the late calamity became naturally a sub- ject of investigation, and on this occasion the animalcular origin of the epidemie was suggested. But “the vermination of the air as the cause of the plague” was supposed to have received its strongest confirmation in Italy, where Dr., Bacon, who had long practiced physic at Rome, was said to have observed that «there was a kind of insect in the air which laid eggs hardly discernible with- out a microscope; which eggs being, for an experiment, given to be snuffed up by a dog, the animal fell into a distemper accompanied with all the symptoms of the plague.”” Hooke, however, had observed that, during the summer in question, there was, in London at least, a very great scarcity of flies and insects. A second interruption of the meetings was occasioned by the “great fire” of the following year, for, though the apartments of the Society in Gresham Col- lege escaped, that edifice was required for the purposes of the corporation of London. A removal of the meetings to Arundel House, at the invitation of its owner, led in the sequel to a donation of his valuable library, which thus became the nucleus of that of the Society. The collection consisted -of 3,287 printed books, chiefly first editions after the invention of printing, besides 544 volumes of Hebrew, Greek, Latin, Turkish, and other rare manuscripts, of which the greater part, of both-classes, had been purchased in Vienna by an ~ ancestor of the noble house, and comprised the curious and costly collection formed by the celebrated Matthias Corvinus, King of Hungary. About this time also the foundations of a museum, or “collection of natural things,” was formed, which, it will not surprise us to be told, comprised, among other articles, ‘the stones taken out of Lord Balearres’s heart, a bottle full of stag’s tears, a petrified fish, the skin of an antelope which died in St. James’s park, a petrified fcetus,’”’ and other equally extraordinary objects, which the language of the age not unaptly termed “rarities.” ‘The rival museum of the Tradescants already contained “two feathers of the phoenix tayle” and “a natural dragon!” * The charters and statutes of the Society may be seen at large in the appendix to WELD’S HisToRY OF THE ROYAL Socrery, a learned and interesting work, on whose statements the present brief account is founded. ROYAL SOCIETY OF LONDON. 143 A subject which at this time attracted general attention was the transfusion f blood trom the veins of one animal to those of another as a means of restoring health or prolonging life. As usual, the most extravagant expectations were indulged by the unreflecting in regard to the eflicacy of this process, and the Society, rightly judging the verification of its virtues to fall within their domain, after trying with impunity the experiment of transfusion on that customary victim of scientific curiosity, the dog, set themselves in quest of a human sub- ject for further investigation. It was first proposed to try the practice upon “some mad person in Bedlam,” probably with a view to test the effects upon the mental as well as bodily sanity, but the physician in charge of the hospital re- fused his assent. A poor student was, however, soon found, who, for the price of a guinea, consented to undergo the operation, and indicated a sheep as the animal whose blood he was willing to receive. ‘The experiment was conducted at Arundel House, in the presence of the Society and of other distinguished in- dividuals, and was attended with such encouraging circumstances as to lead to its repetition some wecks afterwards, on which occasion eight owaces of human blood were taken, and about fourteen ounces of sheep’s blood injected. ‘The patient, we are told, was ‘well and merry”’ after the operation, his pulse and appetite being better than before, but respecting the permanence of these good results we are Icit somewhat in the dark. 'The condition of the patient’s mind, as well before as after the experiment, may be judged of from the mystical reason he assigned, when questioned why he had elected to. have the blood of a sheep transfused rather than that of some other creature: Sanguis ovis sym- bolicam quandan faculiatem habet cum sanguine Christi, quia Christus est Agnus Dei. The Society had thus far met with better fortune than some of the cotemporary inquirers in both Germany and France, where death had in more than one instance been the result of similar proceedings, exposing those who conducted them to the danger of prosecution for manslaughter. ‘Tidings of these disasters at once turned the current of public opinion in England, and led to the abandonment of further investigation on the part of the savants. There can be no doubt that the inquisitive spirit of the Society, though often directed to subjects which no longer appear either dignified or important, had already exercised the happiest influence on the course and habits of public thought. Inquiry was propagated, and a salutary scepticism everywhere man- ifested its encroachments on the domain of popular delusion. Under this point of view, the iustorian of the Society is justified in signalizing the fact that although “during the civil wars upwards of eighty individuals were executed in Sufiolk alone for supposed witchcraft, there were but two witches executed in England after the Royal Society published their Transactions.’ A body which at once prosecuted researches on the theory of eclipses, the nature of comets, and the causes of pestilence, could afford but little countenance to the wide- spread delusion which associated the last of these phenomena in some myste- rious concomitance with the two former. When even the scrupulous Boyle had thought fit to give to one of his scientific treatises the title of The Sceptical Chemist, there could be not much hope for alchemy and its attendant frauds. In other fields, too, the habits of philosophical speculation which, if the Royal Society did not introduce it; at least effectually promoted by influence and ex- ample, gave rise to reforms which, as Buckle remarks,* rendered the reign of the mean and spiritless voluptuary Charles II one of the brightest epochs in the na- tional annals, with reference to laws then passed and principles then established. The zeal of the Society for furthering and stimulating experimental inquiry was manifested at an early period by the adoption of a resolution “that such of the Fellows as regarded the welfare of the Society should be desired to oblige *History of Civilization in England, vol. I, p. 275. 7 144 ORIGIN AND HISTORY OF THE x themselves to entertain it, once a year at least, with a philosophical discourse, grounded upon experiments made or to be made; and in case of failure, to for- feit €5.” ‘This voluntary engagement on the part of Fellows, deemed “able and likely’’ to furnish such discourses, was at the same time made an imperative — obligation on each member of the existing council. For one, the indefatigable Hooke is recorded in the journal-book as having produced new experiments and inventions at almost every meeting. An agent was salaried to traverse England and Scotland in search of zoological and botanical specimens, and this at a time when a default on the part of many members in the payment of the weekly subseription had so crippled the resources of the Society as to render even its existence precarious. An active foreign correspondence had contributed to secure to it an influence abroad searcely inferior to that which it enjoyed at home, as was testified by the learned of Europe, among others by Leibnitz, Malpighi, and Leuwenhoeck, in the dedication of their works to the Society, or a submission of their labors to its judgment. It is a coincidence not unworthy, perhaps, of notice, that about the time when “one Mr. Leuwenhoeck,” as we find him ealled in the correspondence, recommended to the notice of the Society his improved microscope, by the assiduous use of which he eventually arrived at the distinction of being esteemed ‘the father of microscopical discoveries,” a “poor Cambridge student,’? named Isaac Newton, presented to it his reflecting telescope, “ the first perfect reflector known, and made by the hands of Newton himself.’* ‘Thus science was simultaneously endowed with the perfected means of realizing both terms of Cowley’s poetical prophecy—the penetration alike “of the crowds of golden worlds on high,” and “ the recesses of nature’s imper- ceptible littleness.’”” The presentation of the telescope was soon followed by the adoption of the inventor into the Society, the year 1671 being the date of the accession of the great philosopher, destined, in the eloquent language of Dr. Young, “to advance with one gigantic stride from the regions of twilight into the noonday of science.” From this period the history of the Royal Society becomes so thoroughly interwoven with the general history of science that it is manifestly impossible, in a sketch necessarily confined within the narrow limits of the present, to do more than touch upon a few prominent points illustrative either of the progress of the Society or of the knowledge which it has cultivated. On the 8th of February, 1671-’72, Newton communicated to the Society his investigations respecting “light, refractions, and colors, importing light to be not a similar, but a heterogeneous thing, consisting of difform rays.” For these discoveries the author received the “solemn thanks” of the Society, at whose re- . quest they were published in the Philosophical Transactions, being the first of Newton’s productions which saw the light. His experiments had been made in 1666, when he was only twenty-three years of age. No sooner, however, was his theory of light given to the world than it was vehemently attacked, both as regarded his conclusions and the accuracy of the experiments from which they had been deduced; Hooke and Huyghens appearing among the number of his assailants. So true is it, as Biot has remarked, that “by un- veiling himself Newton cbtained glory but at the price of his repose.” * Newton’s telescope, says Weld, was the first reflecting telescope directed to the heavens, though James Gregory had previously (1663) described the manner of constructing one with two concave specula. Newton perceived so great disadvantages in Gregory’s plan, that, ac- cording to his own statement, ‘‘he found it necessary to alter the design, and place the eye glass at the side of the tube, rather than at the middle.”’ Newton’s mechanical labors led to | his being sometimes regarded abroad as a maker of telescopes, and we find him styled in a | book of that period, Artefex quidam anglus nomine Newton. It is suggestive to consider into | what gigantic proportions the instrument constructed by the Cambridge student has been developed under the hands of Herschel and Rosse. Newton’s first telescope is nine inches jong; the length of Lord Rosse’s six-feet reflector is sixty feet. | ROYAL SOCIETY OF LONDON. 145 Tn 1686 the MS. of Newton’s immortal work, Philosophie Naturalis Pron- cipia Mathematica, was presented to the Society; and being accepted with thanks, it was ordered ‘that the printing of the book be referred to the con- sideration of the council, and that it be put into the hands of Mr. Halley to make a report thereof.” The council, duly sensible of the slenderness of the Society’s finances at that time, were glad to devolve upon Halley, who agreed to accept it, the “ business of looking after and printing the work at his own charge.’”’ In the course of the preparations for that purpose, it became neces- sary for Halley to inform the author that Hooke claimed to have “some pre- tensions upon the invention of the rule of the decrease of gravity being recip- rocally as the squares of the distances from the centre,” though he admitted the demonstration of the curves generated thereby to belong wholly to Newton. When apprized of this claim, the illustrious geometer determined upon the sup- pression of the entire third book of the Principia. ‘“ Philosophy,” he said, ‘is such an impertinently litigious lady, that a man had as well be engaged in law- ‘suits as have to do with her. I found it so formerly, and now I am no sooner come near her again but she gives me warning.’ In the controversy relative to his optical discoveries he had written to Oldenburg: “I intend to be no further solicitous about matters of philosophy, and therefore I hope you will not take it ill if you find me never doing anything more in that kind.” It required much remonstrance and entreaty on the part of Halley to induce New- ton to abandon his intention of suppressing the third book, De Systemate Mundi, without which the celebrated work might have borne the title, De motu Cor- porum Libri duo. In view of all the circumstances it is difficult to deny the justice of the remark made in Regaud’s Essay on the First Publication of the Principia, that “it is hardly possible to form a suflicient estimate of the im- mense obligation which the world owes in this respect to Halley, without whose great zeal, able management, unwearied perseverance, scientific attainments, and disinterested generosity the Principia might never have been published.” Halley had been elected a Iellow of the Society in 1678, on his return from his voyage to St. Helena, made chiefly with a view to astronomical observa- tions, of which the fruit remains in his Catalogus stellarum australium, but rendered subservient also to the science of terrestrial magnetism, of which he is styled by a high authority the father and founder. “ ‘To him,” says Sir John Herschel, ‘ we owe the first appreciation of the real complexity of the subject of magnetism. It is wonderful, indeed, and a striking proof of the penetration and sagacity of this extraordinary man, that with his means of information he should have been able to draw such conclusions, and to take so large and com- prehensive a view of the subject as he appears to have done.” Halley’s com- munications to the Socicty on this subject consist of a chart, the first of its kind, showing the variation of the compass, based on the idea of employing eurves drawn through points of equal declination, and of papers published in the 180th and 195th numbers of the Philosophical Transactions. In the last of these occurs a striking passage, in which he expresses his belief “that he has put it past doubt that the globe of the earth is one great magnet, having four magnetical poles or points of attraction; near each pole of the equator two; magnetical poles, the needle is chiefly governed thereby, the nearest poles being always predominant over the more remote.” Amid the efforts which are now directed to this subject, it will not be uninteresting to observe with how much modesty this early explorer defers the solution of his difficult problem to later times. ‘The nice determination,” he says, “of this and of several other particulars in the magnetic system is reserved for remote posterity ; all that we can hope to do is to leave behind us observations that may be confided _ in, and to propose hypotheses which after ages may examine, amend, or refute.” And he proceeds to urge upon all navigators and lovers of natural truths to s ; | and that in those parts of the world which lie near adjacent to any one of those 146 ORIGIN AND HISTORY OF THE make or collect observations of this kind in all parts of the world, and to com. municate them to the Royal Society, “in order to leave as complete a history as may be to those that are hereafter to compare all together, and to complete and perfect this abstruse theory.” | Another science which at this era engaged the attention of the Society was | geology, or, as it was then termed, “the Natural History of the Earth;” the chief representatives of which, before the Society, appear to have been Dr,/ Lister and Dr. Woodward. Of the former, Lyell remarks : “ He was the first. who was aware of the continuity over large districts of the principal groups of strata in the British series, and who proposed the construction of regular. geological maps.’’ Woodward published an essay towards a Natural History; of the Earth, which attracted much attention and was elaborately reviewed ini the Transactions. Dr. Whewell, moreover, has noted as ‘one of the most re) markable occurrences in the progress of descriptive geology in England, the for-- mation of a geological museum by William Woodward as early as 1695.) This collection, formed with great labor, systematically arranged, and carefully; catalogued, he bequeathed to the University of Cambridge; founding and en-, dowing at the same time a professorship of the study of geology. The Wood-| wardian Museum still subsists, a monument of the sagacity with which its author so early saw the importance of such a collection.’”’* An official connexion of the Society with the progress of astronomical obser-: vations resulted from its relations to the observatory of Greenwich (founded: 1675,) of which, after having done much to sustain and advance it during the many years while it remained neglected by government, the Society finally: became the formal difectors or visitors by royal warrant. Under this authority: the Society are required to exact from the astronomer royal for, the time being an account of the annual observations made, to inspect the instruments of the observatory, and to superintend and, if deemed proper, to direct its operations. If, therefore, so eminent an authority as M. Struve has singled it out as a point) well worthy of remark and encomium, that the astronomers of this illustrious; observatory have maintained one unchanged system or plan in their labors: during the long period from the origin of the establishment to the present day, something of this uniformity may reasonably be aseribed to its connexion with and subordination to a fixed and self-perpetuating body like the Royal Society, The application of steam, which in our day has acquired so astonishing a development, did not fail to find among the early Fellows of the Society at least one curious inquirer, whose speculations and projects are preserved im the Transactions. Dr. Papin, inventor of the well-known digester for softening) bones, and whose “ philosophical supper’’ prepared upon that plan may still be enjoyed by the readers of Evelyn’s Diary, is noticed in 1690 as having in¥ vented a method of draining mines by the force of “ vapor,” in which, though much was wanting to the practical perfection of the engine, the philosophical, principle of the condensation as well as elastic force of steam is observed and) pointed out. Ata later period Dr. Papin communicated to the Society an ex4 tension of this principle to the propulsion of boats “to be rowed by oars moved with heat,” and had the honor of having his project referred to Sir Isaac Newton, from whom it received a conditional approval.t * Woodward, whatever his scientific merit, seems to have been of an irascible tempera- ment. He was expelled from the council of the Society for insulting Sir Hans Sloane an refusing to apologize. He fought a duel with Dr. Mead, occasioned by a dispute, as Voltaire says, sur la maniere de purger un malade. Woodward's foot slipped and he fell. ‘* Tak your life!”’ exclaimed Meade. ‘‘ Anything but your physie,”’ replied Woodward. +The better known project of Savery, whose engine was able, through the introduction of a vacuum, to perform double the work of that devised, at a sti!l earlier day, by the Marquis of Worcester, was exhibited before the Society (1699, ) and the certificate granted by that body) to the ingenious contriver, was the means of his obtaining a patent from the Crown for # manufacture of steam-engines.—W eld, I, 357. | | | : i ROYAL SOCIETY OF LONDON 147 While the Society was thus pursuing its diversified and prosperous career, Charles II, ‘founder and patron,” had died, having entertained no inter- course with the learned corporation during his later years, except to send it a receipt for the cure of hydrophobia, compounded, after the manner of that time, of as many simples (agrimony roots, dragon roots, star of the earth, &e., &c.) as could well be disposed of in one preparation. Lord Brouncker had resigned the presidency after fifteen years of acceptable service, and had been followed in succession by Sir Joseph Williamson, (1677,) Sir Christopher Wren, (1680,) Sir John Hoskins, (1682,) Sir Cyril Wyche, (1683,) Samuel Pepys, (1684,) Lord Carbery, (1686,) Lord Pembroke, (1689,) Sir Robert Southwell, (1690,) Lord Halifax, (1695,) and Lord Somers, (1698.) The Society was soon to remove from the precarious quarters which it had here- _ tofore oceupied to a house of its own in Crane Court, Strand, and, as appears by one of its statutes, had found reason to place some further restriction on the too indiscriminate and easy admission of Fellows. On the withdrawal of Lord Somers, in 1703, Sir Isaac Newton was elected to the presidency, the duties of which he continued to fulfil for 24 years with exemplary punctuality. His treatise on Optichs was now presented to the Society, a work prepared long before, but which he had decided to withhold from publication during the lifetime of Hooke. The remark suggested by the death of that able but morose and jealous man of science seems, therefore, to be fully justified: La Société y gagne plus que la geometric n'y perd ; but, as if the sensitiveness of Newton was doomed never to be freed from impor- tunate molestation, the dispute respecting the authorship of the Infinitesimal analysis soon supervened ; a dispute in which Newton, indeed, maintained his: usual reserve, but which his own partisans, equally with those of Leibnitz, con- ducted with so much asperity and prejudice that the contest might have seemed one of honor or interest between Germany and England.* At the instance of Leibnitz, a committee was appointed by the Royal Society, in March, 1712, to examine the evidence bearing on the matter in question, and, in April following, were submitted, in a report, the reasons which led the committee “to reckon Mr. Newton the first inventor.” ‘That this did not satisfy or silence the parti- sans of Leibnitz will be readily believed ; but at this distance of time we may acquiesce in the opinion pronounced by the historian of the Society, that Newton was the zmventor of Fluxions as early as 1666, but that Leibnitz has the merit of having first given full publicity to his discovery of the Differential Calculus in 1673. ‘ Had Newton done this,” says Mr. Weld, “a controversy, painful in its nature and unsatisfactory in its results, would have been avoided. But all admit that he labored more for the love of truth than of fame; and this is one of the reasons why Newton is the greatest of philosophers.” This great man died.on the 20th March, 1727, being, perhaps, the only one who has ever lived whose genius and virtues could sustain the exaltation of his epitaph: Svb: grantulentur mortales tale tantumque exstitisse humani generis. He was succeeded in the presidency of the Society by Sir Hans Sloane, who had long acted as secretary and vice-president, and whose merits as a botanist, habits of business and official assiduity, relieved the council of embarrassment in a choice, even after Newton. Martin Folkes, (elected 1741,) Earl of Macclesfield, (1752,) Earl of Morton, (1764,) James Burrow, (1768,) James West, (1768,) Sir John Pringle, (1772,) bring down the succession in the presidency to the protracted official term of Sir Joseph Banks, (1778—1820.) There are points of interest, however, in this long interval, upon which it is proper to touch even in so rapid a sketch as the present. *M. Arago seems to have been willing to make France a third party to this memorable competition, for, in his Notices Biographiques, vol. III, p. 522, he brings forward the claims of ‘his countryman, Fermat of Toulouse, as an earlier inventor of the Calculus than either Newton or Leibnitz. JAs ORIGIN AND HISTORY OF THE From an early date the Society seems to have labored under two especial causes of embarrassment: want of pecuniary means, arising chiefly from the failure of members to pay the stipulated contribution, and a constant tendency to extend. the honor of membership to persons whose pretensions were of doubt- ful validity. We learn with some surprise that, while a few were occasionally exempted from the payment of the small weekly contribution, (among whom at one time was Sir Isaac Newton,) there were many others of ample means who suffered their liabilities to accumulate until the Society, to which no doubt they prided themselves in belonging, was reduced almost to the point of inaction. Nor does it increase our respect for this class of delinquents to find that when, in 1728, the Attorney General had given his opinion that the Society was authorized to sue for such arrears, and steps were taken for that purpose, the liabilities were generally discharged and the Society placed in comparative ease.* The extent of the second inconvenience may be appreciated from a saying ascribed to D’Alembert, who, in allusion to the extreme prodi- gality with which the honors of the Fellowship were distributed, used “jocularly to ask any person going to England if he desired to be made a member of the Society, as he could easily obtain it for him, should he think it any honor.” The necessity, therefore, for some additional restriction being sensibly felt, the Society sought legal advice as to their powers in that regard, and were advised that, while their charter did not appear to authorize them to limit the Fellows to a certain number, it clearly empowered them to describe and ascertain the quali- fications of persons to be elected. A statute was thereupon enacted, which has since been steadily observed, by which it is required that all candidates, except peers and some other privileged persons, shall be proposed at a meeting of the Society by three or more members, and that a paper signed by them and set- ting forth specifically the qualifications of the candidate, “shall be fixed up in the meeting-room at ten several ordinary meetings before the said candidate shall be put to the ballot.’ It appears that candidates were also expected to send in a paper on the branch of science with which they were most conver- sant. Another but more occasional source of disquietude has been a jealousy sometimes manifested of undue influence or irregular procedures on the part of the presiding officer. ‘This exhibited itself to some extent even towards New- ton in the course of the preliminary steps for the removal of the Society’s quarters to Crane court; but it broke out with excessive violence against Sir Joseph Banks, in 1784, upon the alleged charge of improper interference with elections, and particularly of having favored the pretensions of naturalists in preference to those of mathematicians. Groundless as this charge is shown to have been,t and factious and overbearing as was the conduct of Dr. Horseley,— who, with very slender scientific pretensions, affected the leadership of the mathematical party, this schism not only disturbed the harmony of the Society, but seemed for a time to threaten its stability. The influential part borne by the Society in the introduction of the reformed ealendar into England may render an allusion to it in this place not irrelevant. — By this change, which took place on the 2d September, 1752, “ eleven nominal days were struck out, so that the last day of old style being the 2d, the first ¢ of new style (the next day) was called the 14th instead of the 3d. The same * Before the incorporation, ten shillings were required of members on the admission and a weekly payment of one shilling. By the statutes of 1663 the initiatory fee is advanced to forty shillings, the weekly payments remaining as before. In 1847 the former charge had become ten pounds, and the weekly contribution been converted into an annual one of four pounds, to be paid in advance, Liberty is given to compound for the whole by the payment, in some cases, of forty, in others of sixty pounds. ' t See Lord Brougham’s Lives of Philosophers, p. 363, ROYAL SOCIETY OF LONDON. 149 legislative enactment which established the Gregorian year in England in 1752, shortened the preceding year (1751) by a full quarter. Previously the eccle- siastical and legal year was held to begin with the 25th March, and the year A. D. 1751 did so accordingly; that year, however, was not suffered to run out, but was supplanted on the Ist of January by the year 1752, which it was enacted should commence on that day, as well as every subsequent year.’’* The attempt to retrace here, even in the most summary manner, the philo- sophical labors of the Society would suggest a starting contrast between the narrow limits allotted to this outline and the vast field which it would be neces- sary to traverse. How mere a catalogue of names and of terms would be the result of any attempt to recall those achievements in every department of natural science which have distanced imagination and rendered the fictions of poetry tame and spiritless in comparison! Especially would this be the case as we approached that wonderful era of discovery, the close of the eighteenth century, which suggested to Cuvier the imposing retrospect with which he opens the Eloge of Hatiy: “The laws of a geometry, as concise as compre- hensive, extended over the entire heavens; the boundaries of the universe en- larged, and its spaces peopled with unknown stars; the courses of celestial bodies determined more rigorously than ever, both in time and space; the earth weighed as in a balance; man soaring to the clouds or traversing the seas with- out the aid of winds; the intricate mysteries of chemistry referred to certain clear and simple facts ; the list of natural existencies increased tenfold in every species, and their relations irrevocably fixed by a survey as well of their in- ternal as external structure; the history of the earth, even in ages the most remote, explored by means of its own monuments, and shown to be not. less wonderful in fact than it might have appeared to the- wildest fancy: such is the grand and unparalleled spectacle which it has been our privilege to con- template!”} And in the realization of each and all of these surprising results the Royal Society of London has borne its effective part, yielding to none in the reflected lustre of its long line of brilliant names: its Herschels, Bradleys, Maskelynes, Youngs, Priestleys, Daltons, Watts, Wollastons, Davys, Buck- lands, Murchisons, Faradays, and Airys. For, as the illustrious savant just quoted has elsewhere said with equal force and generosity, ‘‘ The philosophers of England have taken as glorious a part as those of any nation whatever in the labors of the intellect which are the common heritage of the civilized world ; they have dared the ices of either pole, nor is there any nook of the two oceans which they have not visited; they have multiplied tenfold the catalogue of the kingdoms of nature; by them the heavens have been made populous with planets, satellites, and stupendous phenomena; they have counted, so to say, the stars of the galaxy; if chemistry has assumed a new face, the facts which they have furnished have essentially contributed to the transformation; to them we are indebted for inflammable air, pure air, phlogisticated air; they have dis- covered the decomposition of water; new metals in large number have sprung from their analyses; by them only has the nature of the fixed alkalies been demonstrated ; finally, at their voice, mechanics has become pregnant with miracles, and placed their country above all others in nearly every species of productive industry.” * Herschel’s Astronomy, p. 413. So great was the popular repugnance to the change of the style or calendar, that the mob pursued the minister in his carriage, clamoring for the days by which, as they supposed, their lives had been shortened; and the illness and death of the astronomer Bradley, who had assisted the government with his advice, was attributed toa judgment from heaven. It is also related that when the grandson of Lord Macclesfield, who ad likewise been prominent in effecting the change of style, was standing a contested elec- tion for Oxford, the mob insultingly called out to him, ‘‘Give us back, you rascal, those eleven days which your grandfather stole from us.’’—Weld. t See Smithsonian Report, 1860, Memoir of Haity. $ Cuvier, Eloge of Sir Joseph Banks. 150 ORIGIN AND HISTORY OF THE Among the incentives and rewards of scientific research employed by the Society are three medals, derived from funds bequeathed or granted for that yurpose. st. The Copley medal, the fruit of a legacy bequeathed in 1709 by Sir Godfrey Copley, and termed by Sir Humphrey Davy “the ancient olive- crown of the Royal Society,” being regarded as the most honorable within its gift. This has been annually awarded, with a few intervals, since 1736, in conformity with a resolution then adopted by the Society, “that the medal should be adjudged to the author of the most important scientific discovery or contribution to science, by experiment or otherwise.” It cannot but be peeu- liarly gratifying to an American to find that when, in 1753, on the d ath of the surviving trustee of the legacy, the adjudication devolved on the president and council for the time being, the first award of the medal was made to Dr. Franklin, On this occasion the Earl of Macclesfield, in his address as presi- dent, stated that the council, “keeping steadily in view the advancement of science and useful knowledge, and the honor of the Society, had never thought of confining the benefaction within the narrow limits of any particular country, much less of the Socicty itself.” The money value of this medal is five pounds, and it bears as a legend the motto of the Society, Nullius in verba. 2d. The Rumford medal, derived from the interest of a fund of £1,000, given by Count Rumford, in 1796, for the purpose of promoting discoveries in heat and light. This premium is duplicate, consisting of two pieces struck in the same die, the one of gold, the other of silver, and by the terms of the gift is to be awarded “once every second year.’ The device on this medal is a tripod with a flame upon it, and the inscription from Lueretius, Noscere gue vis et causa. It is gratifying to note that the first adjudication of this prize was justly made to the founder himself, “for his various discoveries respecting light and heat,” while the names of Malus, Fresnel, Melloni, and Biot, among later competitors, show that this, too, is freely accorded to foreign merit. 3d. 'The Royal medal, which, again, is duplicate, consisting of two gold medals of the value of fifty guineas each, a beneficence projected by George IV in 1825, though not actually realized till the reign of his successor. These medals, bearing on one side the likeness of the reigning monarch, and on the reverse the figure of Sir Isaae Newton, with emblematical accompaniments, are given for such papers only, on important and completed discoveries, as have been presented to the Royal Society, and inserted in their Transactions. Here, also, the distinguished names of Struve, Encke, Mitscherlich, and De Candolle, in the list of recipients, ap- prise us that this recompense has been liberally offered to the competition of all countries. The subjects for which these prizes have been awarded are almost too multi- farious for classification, and afford no indifferent criterion of the astonishing progress which has been made ‘since the day when the founders of the Royal Society went forth to collect May dew for its supposed cosmetic virtues, or with the Virgula divina in search of the hidden treasures of the earth.” Yet those early inquirers are perhaps not less entitled to honor for the fidelity and hero- ism (for heroism it was at that epoch) with which they adhered to experiment amidst the difficulties and obseurity which surrounded them, than those who, following them in the use of the same irresistible instrument, continued to press forward with firmer and more rapid steps in the pursuit of abstract science, as if conscious that in ¢iat and its applications rested the sole hope for mankind of any real and sustained progression. Nor ean cither of the two classes cited justly claim pre-eminence over the intrepid explorers of to-day, who, undeterred by the seemingly exhaustive research to which the heavens and the earth have been subjected, still lift their minds to new and mightier enterprises, and, having encircled the entire globe with observatories and observers, shrink not-from grappling with problems as subtle and inconstant as magnetism or the winds, and vast as the secular movements of suns and constellations. ROYAL SOCIETY OF LONDON. 151 ‘When we reflect,”’ says Mr. Weld, “on the benefits conferred on mankind by the discoveries of modern science, Englishmen must feel an honest pride in the fact that so large a proportion have emanated from the Fellows of the Royal Society. Mor will that pride be diminished, when it is remembered that from first to last the Society has received no annual pecuniary support from govern- ment, nor assistance of any kind, beyond the grant of Chelsea College, shortly after their incorporation, and more recently, the use of the apartments they now occupy in Somerset House.* While the members of the French Institute re- ceive a yearly stipend, the Fellows of the Royal Society pay an annual sum for the support of their institution and the advancement of science. It would be repugnant to the feelings of Englishmen to submit to the regulations of the Institute, which require official addresses, and the names of candidates for ad- mission into their body, to be approved by government before the first are delivered or the second elected. The French savans are, it is true, ennobled and decorated by orders, which the wiser among them, in common with true philosophers of any country, regard with indifference. Nobly did Fourier say of Laplace: ‘ Posterity, which has so many particulars to forget, will little care whether Laplace was for a short time minister of a great state. ‘The eternal truths which he has discovered, the immutable laws of the stability of the world, are of importance, and not the rank which he occupied.” As a consequence of this independence and self-support, it was necessary that the Royal Society should be numerous, and by a consequence not less necessary, as Cuvier remarks, “ that, as in all political associations where the participation of the citizens in the government is in inverse ratio to their number, those to whom the Society intrusts its administration should exercise over its labors, and to a certain extent over the course and progress of science, an influence more considerable than can be readily conceived of by the academies of the conti- nent.” ‘That the Society has been fortunate in the zeal and ability of those called to preside over it, will have been observed in the course of the preceding sketch. It remains to be added that, on the death of Sir Joseph Banks, in 1820, the chair was for a short time occupied by Dr. Wollaston,t followed in the same year by Sir Humphrey Davy; by Davies Gilbert, in 1827 ;f the Duke of Sus- sex, in 1830; the Marquis of Northampton, in 1838; Earl of Rosse, in 1849 ; Lord Wrottesley, in 1854; Sir Benjamin Brodie, in 1858; and General Sabine, in 1861. The latter still worthily occupies the chair. . As something has been said above of financial embarrassments at an earlier period of the Society, it is gratifying to state, on the authority of Mr. Weld, referring to the year 1848, that this condition of things is wholly changed; be- sides certain tracts of land, the Society then held in the public funds upwards of £33,000; its income:being derived from rents, dividends, annual subscriptions, admission fees, compositions, and sale of Transactions and Proceedings. The number of Fellows, at the same date, was 821, of whom thirteen were honorary and forty-seven foreign. ‘The library of the Society, then containing upwards of 40,000 volumes, is extremely rich in the best editions of scientific books. Fellows are allowed to borrow books under certain regulations, though still more use is made of the library for purposes of reference. ; The sessions of the Society commence in November and continue until June. At the ordinary meetings, after the usual preliminary business, one of the see- retaries announces the presents made to the Society, which are so numerous that * Whither the Society removed in 1780. tIn reference to the extraordinary tact and acuteness of Wollaston as a physicist, it was said by Magendie that ‘‘his hearing was so fine he might have been thought to be blind, and his sight so piercing he might have been supposed to be deaf.” tMr. Gilbert will be remembered by Americans as having pronounced the eulogy on Simith 50n, contained in the first Smithsonian Annual Report. 152 ORIGIN AND HISTORY OF THE ROYAL SOCIETY OF LONDON. ’ their titles fill, on an average, two folio pages weekly during the session. Certificates of candidates for election are then read, and next such paper or pa- pers as may have been communicated to the mecting. For these papers formal thanks are returned, and they become thenceforth the property of the Society. Discussion on the subject treated of in the paper follows, after which the meet- ing is adjourned, and the Fellows repair with their friends to the library where they partake of tea, a custom introduced, it is stated, by Sir Humphrey Davy. A conversazione ensues, which lasts until about eleven o’clock. The council meets monthly, or more frequently, if necessary. The scientific committees assemble as occasion requires. ‘Those annually appointed are: Mathematics, astronomy, physics, chemistry, geology, botany, zoology, and animal physiology. The number of members varies from fifteen to thirty, the latter number repre- senting that of physics which is the largest. The Philosophical Transactions are generally published in two parts, (June and November,) which form a vol- ume, though occasionally a third or even a fourth part appears. Besides the Transactions, abstracts of the papers and minutes are published monthly, and these, now extending to more than ten volumes, are entitled Proceedings of the Royal Society. Set BNR ace — Ba ih = Se pksscy A BRIEF SKETCH OF THE MODERN THEORY OF CHEMICAL TYPES, BY CHARLES M. WETHERILL, PH. D., M. D. Arter the electric current had been applied to the decomposition of inorganic bodies, and it had been discovered that hydrogen, the metals, and the bases appeared at the negative pole, while oxygen, chlorine, and the acids were mani- fested at the positive pole, the assumption that electrical attraction was the bond of union in chemical combinations was very natural, and the electro- chemical theory growing out of these experiments became speedily adopted by chemists. ‘The theory explained satisfactorily all known phenomena; it gained additional support from the discovery that the chemical elements and com- pounds were separated by electricity from their combinations in the ratio of their equivalents. In those days it was assumed, and at the present time it is manifest, that any theory not embracing organic as well as inorganie com- pounds would be untenable, and hence arose the radical theory, first applied to inorganic salts, but afterwards thoroughly studied and developed in respect to organic compounds. As the present sketch is intended less for chemists than for others who may be confused at the appearance of the formule of organic compounds given in modern chemical essays, the author may be pardoned in citing facts and formule trite to chemists. He would also take occasion here to aceredit to the Lehrbuch of Graham Otto many of the illustrations, as well as some of the arguments, employed in the present sketch. The nature of electrical attraction renders the idea of b¢nary compounds in chemistry imperative, if we assume that electricity is the bond of union in such compounds. Berzelius imagined the elementary atoms laden with electricity and with positive and negative poles, but so that in the atom of one element the positive electricity predominated, while in that of another element the negative elec- tricity was in excess. ‘This excess of (+ or —) electricity communicated its characters to the element, making it positive or negative. If two atoms of dif- ferent electrical character are brought sufficiently near to each other, they mutually attract each other, forming a compound atom, which is itself positive or negative according to the predominance of one kind or the other of its electricity. The new compound atom was, therefore, susceptible of further attraction by another compound atom of different electricity, and so on, the attraction becoming weaker,as the compound atom becomes more complex. Ampére imagined the atoms of positive elements to have positive nuclei with negative atmospheres or envelopes, and atoms of the negative elements to have negative nuclei and positive envelopes. Hence a positive and a negative atom upon coming together would mutually polarize each other; the + and — E of their nuclei would draw them together to form a compound, and the + E of 154 THE MODERN THEORY OF CHEMICAL TYPES. their respective envelopes would be driven off and combine to produce the electrical phenomena always attending chemical action.* . According to this view all chemical compounds are binary; they are capable of being decomposed by the electric current, which attracts the atoms from each other according to their character, the positive appearing at the negative pole, the negative at the positive pole. In writing formule the positive atom or atom group is placed BEFORE the t- +-— + — negative one, thus: KO; SO3; KO, 803.7 The most complex formule are constructed according to this binary method. In alum = KO SO, + Al, O; 3503 + 24HO the sulphate of potassa atom is positive, and united to an electro-negative atom of sulphate of alumina to form a still more complex atom of positive character, which is united to the negative group of atoms 24HO. When, however, the atom becomes so com- plicated, it is difficult to determine the electro-chemical character of its imme- a ee * Por views as to polarity in chemical compounds, see the excellent treatise upon the cata- lytic force, by T. L. Phipson, Smithsonian Report for 1862, page 395. ter the convenience of those whose memory may require refreshing as to chemical symbols and combining quantities, or atomic weights, we subjoin the following table. SYMBOLS AND PROPORTIONAL NUMBERS OF THE ELEMENTS. (From Odling’s Manual of Chemistry. ) I Ey OTO penis. os sete etme = 1 Mg | Magnesium Zn Pimie;: sls. AG ess SH Fl Wilmore: 4 Pes) sts) ae 19 Cady) |pCadmiumy. fet a ssaete Cl (OIMOMINGY. os 5 ne Som) see 35.5 Br SC OMMMGRee a atemce tselace 80 He | Mercury, (Hydrargyrum) .. 100 I odine Seah nerset seas 127 Pb Lead, ( Plumbum) ....------ 103.5 Ag Silver, (Argentum) ...---.- 108 OPP OXYGEN 2-2 co cesacece 16* Ss DGD NUe erate ee tee 32* Cr Chromiumy. 32 4se eee 26 Se Bcleaiumn ss 22 S928 so as 80* Mn | Macanese=-s.- 3 esac eee at T Wellunrum S30 hs. 322 128* Fe Tron, )|Chentum)) teseo eee 28 . Ni Nickél\....05-r5c¢ ga5eeaeueee 29 N AAO CDS seein ee cine orstn 14 Co Coballt*: 72.5 (2 aoe 30 it PHOSpHOUOUR mn | Ruthenitiatseeee se sea =e 52 Ca WRIOINM S-\5h.2.5..2. Sew< 20 Pa Palladian SH sosski 2 Zo5. 53 Sr PPODURDON 2 a) tS! dnc reme 44 Ba Laer eb 68.5 || Pt Platinum eee ee oe 98.5 Wek Ir [ridiammees steer a a cen 98.5 G Glucinum ......-......... 457 108" || Ossie oe as 99.5 yy Matias tease sk seck 32 Th SDH OL sats eects we ci 59.5 eee * These elements have had their equivalents doubled to conform to the type theory. THE MODERN THEORY OF CHEMICAL TYPES. 155 diate constituents. In the above example the 24HO may be drivenoff by heat, but not by electricity simply; and from other considerations it is impossible to decide from analysis alone whether water is an acid or a base, as it possesses, according to the substance with which it is combined, each of these characters ; in oil of vitriol it is a base HO SO ; in hydrate of potassa, an acid KO HO. There is still another method of imagining the grouping of. the atoms in a complex atom to form a binary compound. ‘This involves the essence of the radical theory. SO; does not redden litmus nor form salts with bases; its compound with HO (oil of vitriol) possesses this property. We may imagine this acid to be HO, SOs, according to the principles just laid down; or to be H SOx, a binary compound, in which His + and SO,is—. If for hydrogen we substitute potas- sium or any metal, we will have sulphate of potassa or the salt corresponding to _ themetal. SOy,is, therefore, a compound radical in the sense in which the word has been employed in chemistry, although it has not been isolated. When water and anhydrous sulphuric acid are brought together, this compound radical is generated by the decomposition of water in the manner illustrated above. It is, however, more particularly in the case of the bases that the theory of compound radicals has been developed. The example of ammonia illustrates an inorganic compound radical; if, in- deed, it may at present be called inorganic. The gas ammonia NH; (in a manner analogous to that of anhydrous sulphuric acid) acquires basic properties only by the action of water; NH3, HO—NH,O. NH, is the compound radical, ammonium. It has never been isolated ; it is an hypothetical group of atoms playing the part of a metal. The following table illustrates the parallelism existing between compound and simple inorganic radicals : Comp. radical ammonia. Simple radical potassa. = -- + = ire CO } Oxide. ( K+0 NH, + S Sulphide. J K+5 NH, + Cl Chloride. Ki Ol NH, + SO, { Sulphate. K + SO, When organic chemistry began to be developed, the compounds first studied were those containing different proportions of carbon, hydrogen, and oxygen, together with a few containing nitrogen. ‘These were studied in their analogies to inorganic compounds, and the assumption of a large number of organic radicals became imperative. For example, if ether (Cy H;O) were the oxide of a radical (Cy H;) called ethyl, the compounds of ether could be brought into comparison with those of oxides of the different metals, (Cy H;,) being a com- pound organic radical, which group of atoms plays the part of a metal, thus: EB 6s, 5c ca co arn pea a ect odes (CyH5) Ether CRS fa Ith NSE alates eke aie) Sal alls arare te ime) moka (CsH5)O PAU Gy ja) 5 ays a es eB olen area, (C,H;)O, HO Whlomde) of ethy le. seca cose -) 5,25 ae bale (CyH;)C1 Nitrate of the oxide jof,ethyle..-..-.....-...- (C,H;) O, NOs Acetate of the oxide of ethyle.......... (CyH;)O,(CsH3)O3 Sulphate of the oxide of ethyle......... (CyH5)O, SO3 POMPOM: ACI a oc sta ris pe 0.725 4, 42 Cio H ‘ m cee Faee Ee ks oe. eae 2 Oi His.-svaiase 0.741 4,91 The members of this series are subject to the “same law;’’ they advance from the lowest by an increment of C2 H». A general formula for the series would be C,, H(, + 2,) n being an even whole number. Their boiling points as well as their specific gravities in the liquid and in the vaporous condition rise gradually. We have, from its position in this series, an additional reason why amyle should have the formula Cy) Hy, and not Cy Hy. Indeed, as may be scen in the table, amyle is regarded as having (in combination) Cy) Hy, but, when 7 the free state, two of its atoms are joined together to form a compound atom Ox, Hy». ‘The following are additional illustrations of homology . | J. Hyprocansons. i II. Actps. as Oe Che Siihvlene wees. ee Geatligy |) Orme: aie git: fed he's ow Gs Hip, Propplete eee So... Os. He |. Acetic ... «pst beige oniee Cz, Hy Og Dutviciiew se: ). <2. >See Ge Hy. -| Propionic spe eeee wee ee Cg Hg Og Amy lene eae e wenn ene een eeee Cio Hy Butyric eo or oo Us H, Ox : PUBCTIO 5 GN cst win ets eee Cy Hy Valerianic..... ve we cls ore Cio Hy On Palmmitic . .» «tccagn sa Sete en Laan Stearic ...... a= Sewenese C35 Hog O4 THE MODERN THEORY OF CHEMICAL TYPES. 161 III. ALcouois IV. Basss. V. HypDROCARBONS. ©, E(w'42H03) Cy Ha _5N) umn Formylic .... C, H, O, | Aniline..... Cy.H, N | Benzole ....... Cy He Ethylic -.... C,H. ©: || "Voludine-..-) Cig ho iN, | Toluole 2 32.2 Cy, H, Propylic.... Cs; H; O, | Xylidine ... Cys Hi N | Xylole.......- Cig Hin mtyiie ..... Cs Hy O2 | Cumidine... CygHj3N | Cumole ....... Cig Hy memylic..... . Cio Hip O2 | Cymidine-..- Cy His N | Cymole ....... Coo Hig w-e e ee ee we ee ee ee es Aethalic .... C2 Hs, Oz The most remarkable phenomenon connected with homologous series is not the uniform law according to which the formule are developed; but that the successive increment of the atoms Cz Hy contributes to a certain regularity of physical and chemical character; thus, neighbors in the series have greater analogy to each other than to more distant members. The acids and alcohols quoted advance (at the normal temperature) by degrees from liquids to solids ; and chemically, formic and acetic acids on the one hand, and palmitic and ste- aric acids on the other are analogous. ‘The boiling points increase with regu- larity ; for example, in series II and III every addition of C, Hz adds 19° C. to the boiling point. Though this regularity of boiling point applies to other series, the difference is not the same for all; thus in series V every increment of C, H, adds 24° C. to the boiling point. It would create too great a diversion from the main object of the present article to enter further upon the nature of homologous series. ‘The curious law may, however, be cited with respect to certain series of acids, ethers, and alco- hols, viz: that if two of them have an equal number of hydrogen and oxygen atoms, and one has X more atoms of carbon, the latter will boil at X 14.5 degrees centigrade higher. For example: Benzoic acid, Cy, Hs Ox; boiling point, 253° Propionic acid, Cg Hg O4; a 137 Difference, Cg Soe eo 116° Angelica acid, Ci) Hg Oy; boiling point, 185° Butyric acid, Cs Hg O4; ee 156° Difference, Cy, 9 96 -14-5-=—=---29° On the other hand, if the number of atoms of carbon and oxygen is the same, and one compound contains X equivalents less of hydrogen, its boiling point will be X 5 C.° higher. Angelica acid, Cy Hs O4; boiling point, 185° Valerianic acid, Cyo Hy O,; ee 175° Difference, H, os oe 10° Not only are the members of the same series subjected to one and the same law, but some of the series are connected with each other. The importance of this fact is very great, since it enables a systematie grouping of chemical com pounds. From the character of well-studied bodies, and from the analogies alluded to, we are able to pronounce a judgment upon the chemical constitution, nature, and behav::: of new bodies. This connexion of the series is as follows: From alcohol C, Hg O2 we may obtain by the addition of oxygen, and by the subtraction of hydrogen, acetic acid, (Cy Hg Oz) + Oy = (Cy Hy Oy) + 2 HO. Hence, in general terms, if from the series (C, H (+42) Oz) we subtract Hp, and add O, = (C, H,, O4,) we obtain an acid analogous to acetic acid. Moreover, s 162 THE MODERN THEORY OF CHEMICAL TYPES. by subtracting 2 H O from (C, Ha+e) O,) we obtain C, H,, or the series of hydrecarbons (I.) Ethylene is thus actually obtained from alcohol. Again, from every acid of the series C, H,, O, we may obtain an amide C, i (n+1) N Op. The law of homology conduced strongly to the type theory by contributing a better knowledge of the chemical constitution of bodies. By its study, radi- cals containing oxygen were definitely accepted. Thus, (in series II,) acetic acid (Cy Hy O,) is not formed from ethylene (C, Hy) by the addition of O,, but from alcohol (Cy Hg Oz) by the addition of O., and by the subtraction of H2 in such manner that the radical (C4 H O2) is formed ; which makes acetic acid (C4 H, O,) = (Cy Hy Oz) H O,. As a proof of the existence of such a radical in acetic acid, we may obtain its compound with chlorine by the action of oxychlo- ride of phosphorus upon acetate of soda, and we may restore this chlorine com- pound to acetic acid by the action of water upon it.* (NO,) is another radical containing oxygen. By acting upon benzoie acid so as to substitute (NO,) for hydrogen, we have nitro-benzoic acid—that is, Cy, He, Oy, becomes Cis H; (NO,) Ox. These considerations have been leading us gradually to the ideas of modern chemical types. Such a type is a group of atoms of which the individuals bear a certain relation to each other, and forms a pattern for imagining all chemical compounds, between the atoms of which a similar relation is supposed to exist. It may be illustrated by certain blocks glued together, or by a cage of wire with compartments, in which the blocks may be placed, thus: THE TYPE—WATER. Examples of the type of water: Sulphuretted Hydrogen. Hydrate of Potassa. Acetic Acid. * See examples of reactions by the type method toward the close of this article. i THE MODERN THEORY OF CEEMICAL TYPES. 163 The four compounds represented above are supposed to be constituted after the pattern of water, which is the type. Thus, if the oxygen atoms of the type are replaced by sulphur atoms, we have sulphuretted hydrogen. If, in the type, we substitute for the hydrogen block, upon the left hand, a potassium block, the result is hydrate of potassa. If, on the other hand, we re- move a right-hand block of hydrogen, and substitute a block representing the radical acetyle, we have acetic acid. And if we replace each hydrogen block of the type, one with a potassium block and the other with an acetyle block, there results acetate of potassa. In the above illustration the compounded blocks are of one size, thus repre- senting a volume of four oxygen blocks, and conforming to the law of conden- sation of organic compounds to four volumes. We must bear in mind that the individual blocks may be larger than an oxygen block when outside of the type, though condensed to the size of such block in the compound. For ex- ample, 2 volumes of oxygen+4 volumes of hydrogen == 6 volumes, which are condensed, by combination of’ the gases, to 4 volumes of vapor of water. Hydrogen constitutes another type, thus: HYDROGEN TYPE. Benzole and Acetone examples of this type are represented thus: Benzole. Acetone. 164 THE MODBRN THHORY OF CHEMICAL TYPES. # * _ Ammonia gives another type, thus: AMMONIA TYPE. Ethylamine and Aniline are examples of this type, and are thus represented : Ethylamine. Aniline. ee E The sezes of these hydrogen and ammonia types are equal to that of the water type, viz: four volumes. With this preliminary illustration the following table (from Graham Otto’s Lehrbuch) may be quoted : 165 THE MODERN THEORY OF CHEMICAL TYPES. “OUI[LUB.YINT ‘oprmreznog ‘oprmeyooy | ‘oprure;Aueqd-;Aozueq-1q, | ‘ourmmeyAqyo-11y, | camrure,Aqyo-1q | ‘oururep Ay ‘onary H H Ort ip) | Ae 0 ~ Ft | H H H ‘N H ‘N H "N4 *O pee et ao ‘Ny “H *O AN a EL "N H ‘N H 0 °H MO 50 *H 0 | sry) | "HD "HO | 1'D (ON) "H "9 °H 9 | ' H "NS H—N‘°H VINOWNY dA], FHL OL ONIGUOONDVY SaNnodWog H | | “prow “poe ‘apAqo ‘op Ay | ‘m08 “aUILOTY atyooRLo[YA | omoppoorpAyy ‘aphyopty | jo epruekg | jo opnory9 *9T10]00V ‘op Aq ‘gjozueg | -orpAy op Ayjopr i a *H*O } H ; H ee ee ; ‘a Pes oe a9 ioe ‘9 10 10 10 0 °H 70 N°O | 10 *0 “H*O Ee | H H | = — 9 NGDOUGAPF, AdA YT, FHL OL ONIGUOOOY SANNOdWO/) "plone ‘prow ‘oT Aqq0 ‘ot Aq0 JO opt ofAq}o dia snorpAyuy | ooo snorpAyuy | Jooprxojooyeurdy | -xo Jooyryoovs0[q | Jooprxo jo SIS DY, ‘OTOL *IOT]O VSSv}OT “"ESSBI0g 04 STON “6 -e "HW *O “ i oe. “t y aH 7) “ $6 oH “ ae 9 “6 yn "90 “6 — oN ©? 0 'H "9 Ol ND Oot070 | Ort0 HD Ol 9 Ke ou OVs ‘op Ato ‘ar Aya jo ‘oy Ayyout “10T]}9 “TUN TTOUIUR ‘plow oyoovrI0[yO “plow ore0V | JO oprxo jo oyV.4IN | Oprxo Jo oywozueg | Jooprxo Jooywyooy | o[Aq}0 a ‘oyoory | Jo oprxo oyerpéTT 7) gL “ i 6 . 9 2 ; at 7) “% ; *H %0 “ eee WD “ es 0 “ a ©2 % tH 9 Or oH 9 ©? "on © 0 HD ©2*0 HD Ov Hr 9 ot Oy *PIO’ OLIN “plow OTUIIO iT ‘essnyjod oyRyINy ‘essvjod oynjooy | “eImouUR oR}OOW ‘qpouNy ‘yrds poo, | “essvjod oyerpApT ‘6 “ H se 9. “ ; w ‘ } HN So oO ‘ ee °0 te ; w of dh 0} colt 0} sn O2 OH "0 °° "HD Oe ai 2a ovr “of T= FT = UALVMA AdAT, AHL OL ONIGHODOW SaNaodWwoy 166 THE MODERN THEORY OF CHEMICAL TYPES. ° The table illustrates the method of writing the formule of bodies according to the types of water, hydrogen, and ammonia, to which they respectively belong. Determinations of the specific gravities of the vapor of water and of hydrogen show that the formule H O and H (O =8 and H = 1) agree to a condensation of ‘wo volumes. In order, therefore, to make types of these bodies, their formule must be doubled so as to correspond to a condensation of four volumes, which is the atomic volume of the greater part of organic compounds. The formula for ammonia N Hz already corresponds to four volumes, e. g., 2 vols. N+6 vols. H=8 vols. condensed to 4 vols. N H3. It will be observed that, in the table, compounds of a basic character are placed to the left hand, those of acid nature to the right hand, while salt or neutral bodies occupy positions in the middle of the table. It will be observed, further, that in the formule of the bodies according to the types a ; O, and . } the electro-negative elements are placed in the bracket to the left hand, and these are distinguished into a superior atom of hydrogen, capable of being replaced by chlorine, &c., or an acid radical, and an inferior atom of hydrogen susceptible of being exchanged for a metal or basic radical, while the electro-negative elements, oxygen, sulphur, &c., occupy positions to the right hand, outside of the bracket. The relations existing between anhydrous or hydrated acids or bases; the difference between hydrogen acids and oxygen acids ; the nature of acid, base, or salt, are more readily perceived by a close examination of the table than by the most extended description. It will be seen by this inspection how the ammonia salts are represented. ee \ O, is the acetate of ammonia. By adding H H to the type ammonia we have a new type : N, ammonium, which enables H the formation of salts, according to the ammonium theory, by introducing this new type into the type of water. Thus diethyle-methyle-amyle-ammonium would be CG. He H ) C, H; O2 CG, i: C, H; l C, Hs C. I. N. Its hydrated oxide C, H; N Oy». Its acetate C, H; N On. C. I. C. H; i C, H; : se Cy) Hy Cyo Hn The homologous series may thus be generalized by this system of nomencla- stag © H : ture—e. ¢., ordinary alcohol is ; Oz; bo is any alcohol, and é : C.Hs§~?? Cn Hayy f 2% t On alae Ye \ any corresponding acid of the same homologous series. Another principle, which has been adopted in the type method, consists in the assumption of radicals capable of replacing H, or H; in the types. Such radicals are diatomic when they replace Hy, and are represented thus, (/’,) and triatomic (’’’) when they replace H;; and the types of water, hydrogen, and ammonia are doubled or trebled to form new types by which bibasie or tribasic acids or salts may be represented. Thus: BIBASIC ACIDS, Type. Sulphuric acid. Succinie acid. Tartarie acid. H. S, O,' C3y 0, J o 11, | He $ O ey Oe mE TRIBASIC ACIDS, Type. Phosphoric. Meconic., Citric. i : P QO. mt G H O mt 1 i ty HY Oe Hy. } Os oF, Oh: ee ee * ¥ s a THE MODERN THEORY OF CHEMICAL TYPES. 167 i The following are examples of the duplication and triplication of the hydro- gen and ammonium types: : Type. Chloro-sulphuric acid. Chloride of succinyle. H, , S2 OF ; Cs Hy, Ou t Hy, Cl, 12 Type. . Succinimide. H, Cs Hy O24" H, No. + H, No. 2 Hp Type. Oxychloride of phosphorus. He P O,!/ H; Cl; Type. Citramide. H; C2 Hs On!” H; e Nd. Hi; N3. 3 Hy These derived types are connected with the primary types by the hypothesis that a “polyatomic” radical may replace several atoms of hydrogen in the primary type. Thus— Type. Anhydrous sulphuric acid. Anhydrous succinic acid. 11 f 02 S,0." 10, Co H.0." } 0, Tyne. Sulphurous acid. at 8, 04"} Type. | Succinimide. i N. Paar br H The following examples illustrate the use of the type method of expressing a chemical reaction—e. g., that of hydrochloric acid with hydrated oxide of ammonium. By the former method it would be— NH,0 +H Cl=NH,Cl1+ HO By the type method— H cly— Gl H yufOt uf=nuft Hye Again: by the action of oxychloride of phosphorus upon acetate of soda, chloride of acetyle is formed together with phosphate of soda, which reaction is represented. By the former method— iP OC, a 3 CN: 0; C, Hy; Os) == 3 N,O, P O; + 3 (C4 H, Oz) Cl. By the type method— P O,!" C, H; Oz ee Er O,!” ° C4 H; Oz Cl, Vis ( Na On) = Na bos +3 { Cl. Some regard the type method of imagining a body as essential in the nature of matter; to these the type of the same body is invariable, with which, if ¥ 168 THE MODERN THEORY OF CHEMICAL TYPES. e phenomena agree not, the reason is sought, and the correct type determined by experiment. ¢ é , But others employ this method as a means of comparing chemical reactions, and as suggestive of new experiments. Such write formuls sometimes according to the old nomenclature, and sometimes take great liberties with the types, | viewing the same body in different types; for example, taking aldehyde C, H3 O02 tH t (C, Hy Oz) according to the type es thus: or, according to the fa ; type : t Os, thus: 4 _ ; 5: A very serious defect, in-my opinion, in the type method is that it places the hydrogen acids and salts in a different type from the oxygen acids and salts; while the analogies existing between these acids and salts furnish urgent reason why they should have the same constitution, which similarity chemists have always labored to discover. Itis not fair to constitute a type ammonia founded on the chemical analogies of it and the compound ammonias, and at the same time place hydro-chloric and nitric acids in different types. And yet, by the present method, they cannot come in the same type, because, first, oxygen can- not come in the hydrogen type, ; 5 = ees Oe HO BLS tele Mine 20° #OVPTA. 2b alice ci 3° eee. Sto BOT tee, 20° tebe ee chs 35° APPA. 36 shi CLP toed ida ceive cic - RO° ti SG ee siti. ae 4$° LB sy oman tel! A030? eke waibicis 21° to RGE ice danaixs 4° QO sigs alee BU? to RBA? aise 2 21° to AGB veel sities 24° 30™™. 2... RL 40,269 4 ee 2-1 21° fo QBAO esc wee 14° * The thermometric indications are in degrees of Reaumur. ¥ ; THE PROPAGATION OF ELECTRICITY. 183 The following is the result of an experiment in which the duration of the passage of the current was prolonged beyond 2 minutes, through atmospheric air at a pressure of 5™™; Duration of passage. Positive thermometer. Negative thermometer. Difference. pee steep -34 « AS toss ace septs i 40! 26° scr :ctewee 5° os atin = 80:37? )\eee 228 — to 30$°......... 64° Seite e aap os =) HOMO: ass aaloe See | 12 stn eeeya 8° Pi cine. 36 == £0437 Wc) Su eesnis ==5s" (OG 7 FS fete Sie a MD a ereatate my ninie == ihO ABP ou ismian ad 2 Sn MOA 2 aid 2h. AP In proportion as the duration of the experiment increases and the absolute temperature rises, the differences: between the temperatures indicated by each of the two thermometers become proportionally less ; the indications of the two thermometers end by approximating, and even becoming the same after the lapse of a certain time. Hydrogen and nitrogen give the same results. The numbers which express the temperatures in the preceding tables cannot be given as being of perfect exactness; they vary, in effect, in their absolute values with the intensity of the electric stream; but they are sufficiently con- stant and exact to demonstrate: 1st, that there is a sensible elevation of tem- perature, which accompanies the propagation of the electric current in rarefied gases; 2d, that this elevation is sensibly less in the neighborhood of the negative electrode than near the positive, when once the gases are sufficiently rarefied for the discharge to pass easily and the electric light to be stratified ; 3d, that the absolute elevations of temperature at the two electrodes, and their differences, vary with the density and the nature of the gas. A fact which shows well all the calorific and luminous power of electricity, is, that hydrogen reduced to 14™™ of pressure can become luminous and be heated in a very sensible degree* by the passage of electricity, although at that pressure it has a density so inconsiderable that a cubie centimetre of the gas does not weigh more than barely => of a milligramme. When we sce matter so subtle as hydrogen reduced to one or two millimetres of pressure, becoming luminous under the influence of electricity, the temptation ean hardly be resisted of surmising an analogy with the matter at once so subtle and so luminous which constitutes the cometary bodies. This analogy becomes still more striking when we examine closely the appearance presented, in the tube which contains the rarefied hydrogen traversed by the electric current, by those species of luminous mists which manifest themselves at the moment when we introduce a little gas into the tube, and which we also sce in the obscure space when a certain degree of rarefaction has been attained. Undoubtedly the gaseous matter is there still more rarefied than it is in the rest of the mass where it is already extremely so, and it offers at the same time a remarkable resem- blance with the luminous matter which constitutes the comets. § IV.—INFLUENCE OF MAGNETISM ON ELECTRIC CURRENTS PROPAGATED IN HIGHLY RAREFIED GASEOUS MEDIUMS. This influence, whose existence I have shown under the form of a rotation communicated by the pole of a magnet to the electric currents which radiate from it, is, as might be expected, and, as M. Plucker has evinced by several re- markable experiments, general. The luminous filaments which display them-. selves in rarefied gases, traversed by the discharges of the Ruhmkorff apparatus, * The heating of the gas must in fact be very considerable to be capable, in two minutes, of raising by nearly 3° the temperature of a thermometer whose reservoir is a cylinder of mer- cury 2} millimetres in diameter by 3 centimetres in length. Besides, the single fact that the | gas is luminous well evinces its high temperature; for the light is evidently but the effect of its incandescence. 184 PHENOMENA ACCOMPANYING are attracted or repelled by magnets as electric currents circulating in metallic wires would be. In a word, this action is subject to all the laws of electro- dynamics, with this difference, that all the parts of the mobile conductor being independent of one another, instead of being united with one another, as they are in a rigid wire, they completely obey the forces which act upon them, and take the positions of equilibrium which result therefrom. Hence it is that the luminous filament takes the form of a magnetic curve; a necessary condition, in order that the equilibrium should take place, since the action of the magnet on the element of the current is then nothing, the direction of the action being per- pendicular to that clement when it is a tangent to the magnetic curve. I have verified in sundry cases the law just recited, and have even succeeded in showing that, conformably to the law of Ampcre, two electric streams having the same direction in a rarefied gas attract each other as two voltaic currents transmitted across movable metallic wires would do. I have not realized the repulsion of two electric streams passing in contrary directions, by reason of the practical difficulty which I have hitherto encountered in constructing an appa- ratus for the purpose. I do not, however, renounce the hope of being able to do so. I shall return to this subject in an article in which I propose to consider the mutual action of electric currents on one another. I restrict myself, for the present, to an investigation of the effects of magnetic action on those currents. My researches on this subject comprise two series of experiments : first, those in which the electro-magnet from which the electric action emanates is placed externally to the rarefied gas thrqugh which the electric stream is propagated; secondly, those in which the magnetized iron is situated in the gas itself. One of the most simple cases is that in which one of the tubes of which I have spoken in preceding experiments is placed either axially or equatorially in relation to the poles of a strong electro-magnet. The following is what is ob- served when care has been taken to rarefy well the gas which transmits the electric current. The portion of this current submitted to magnetic action is condensed towards the walls of the tube in the part nearest, or that most remote from, the magnetic poles, according to the direction of the current and that of the magnetization; the striae become much more compressed and more brilliant. If the portion of the tube placed in the neighborhood of the electro-magnet is that where the negative electrode happens to be, the obscure space is immedi- ately seen to become luminous, and to present close and brilliant striz as would be the case with the constantly luminous portion of the current which seems to advance. At the same time, the bluish photosphere which surrounds the neg- ative ball contracts to at least half its size, becoming more brilliant, and the sort of bluish sheath which surrounded the metallic rod, at the extremity of which is the negative electrode, completely disappears.. All that bluish atmosphere is concentrated on the ball. It seems that all the gaseous filaments, which may be considered as so many conductors of the discharge, instead of radiating from all points of the negative ball and rod, and being disseminated through the entire gascous mass as far as the positive electrode, radiate only, when the magnetic action is exerted on them, from the negative ball, becoming condensed towards the walls of the tube, on one side or the other, as far as that portion of their course at which, the action being no longer sensible, they resume their normal position. ‘his condensation explains why the part of the current which was obscure because the gas was there too much dilated, becomes luminous, and why that part which was already luminous becomes more slender and brilliant, with stratifications more closely compressed. The action of the magnet pro- duces the same effect which would be produced by a local augmentation of density in the rarefied gaseous matter. Further, it is not necessary that the action of the magnet should take place exactly on the obseure part in order to its becoming luminous; it equally becomes so, even when the magnetism acts THE PROPAGATION OF ELECTRICITY. 185 on another portion of the current, provided it be not too remote from the neg- ative electrode. The consequence of the explanation just given, and which it is easy to verify by experiment, is, that the portion of the gas which transmits the discharge must, when it is subjected to the action of the magnet, become a more imperfect conductor, and that consequently the electric current must, on the whole, en- counter a greater resistance in its passage along the interior of the tube when one part of the tube is approached by the electro-magnet than it encountered previously. Thus the tube of one metre being filled with rarefied hydrogen, and the ap- paratus of derivation placed in the circuit,* we obtain the following results : Pressure. Intensity of the derived current. Without magnetization. Magnetization at the Magnetization at the ; : positive electrode. negative electrode. EO Tk pcVs ist cr's ay vaveh ats Bebo, Seah ch eparee tune aie SOCK ata De ets 28 20g Smm. .....-. Syren ORLA elon ates ebctaets SOP Ss teertenve «SYS. 10° With the tube 50 centimetres in length, filled with nitrogen, we have: Pressure. Intensity of the derived current. Without magnetization. Magnetization at the Magnetization at the positive electrode. negative electrode, Gil Ts Se et ee EAI risen, SERN sae i. UD ASPAY s DA SOME T Area Unc be of 49° ee Pa sr. 2 ys Sie Lb aC Bie ert Sole Mt A ee 1 GUT Pad F deb S Goat | «aes 71 oe ee eee a BOS Sh Bae 129 The effects are more marked when the tubes are placed equatorially between two soft-iron armatures of the electro-magnet, which are immediately in contact with the walls of the tube, than when they are placed axially on the poles themselves. We see that there is a much greater increase of resistance when the magnetism acts on the portion of the current near the negative electrode than when it acts on the portion near the positive electrode. The reason of this difference is, that the first portion which, as we have seen in the preceding paragraph, is endued with a much greater share of conductibility, must natu- rally experience a more considerable diminution of that property by the con- densation of the gaseous matter produced by the action of the magnet, than is experienced by the second portion, where the gas is less rarefied. The direction of the magnetization has no influence on the results: it has no other effect than to elevate or depress the current, which, when the magnet does not act, is simply horizontal. Among the experiments which I have made regarding the influence exerted by the exterior action of magnetism on rarefied gases enclosed in tubes, I will further cite those in which the tube is convoluted into a flat spiral terminated by two prolongations perpendicular to the plane of the spiral which serve to in- troduce and rarefy the gas, as well as to give a passage to the discharges; the tube of the spiral and its prolongations is a little less than one centimetre in diameter, and its total development nearly eighty centimetres. It is necessary that the gas should be rarefied at least as much as 2™™ for the discharges to pass when nitrogen or atmospheric air is employed. With hydrogen, a press- ure of 5 or 6™™ suffices for their transmission. But whatever the gas or its degree of rarefaction, it is only after the lapse of some minutes from its being placed in the circuit that the discharge begins to pass. It is evidently neces- sary that it should be sometimes charged with static electricity for the resist- ance to the establishment of the continuous stream to be surmounted. But that *It should not be forgotten that here the derived current is proportional to the principal current, so that its intensity may be regarded as being quite approximately the measure of that of the discharge which traverses the tube. 186 PHENOMENA ACCOMPANYING Cc resistance once surmounted, we may interrupt the passage of the discharge with- out incurring the necessity of waiting more than an instant for the transmission to recommence, when we close the circuit anew, provided the interruption does not exceed an hour or two. The luminous current presents, with hydrogen under a pressure of 5 or 6™™, very neat and distinct striz of a rose color; ata pressure of 2™™, they become much larger and less distinct ; the color is also paler. The same occurs with air and with nitrogen, but the effects are more striking with hydrogen. A remarkable appearance presented by the current in the interior of the spiral is, that it seems to undergo a very distinct movement of rotation, in a direction which appears to vary with the direction of the dis- charge ; but this last result is not very constant, which has led me to think that the rotation is only apparent, and that it is the effect of the discontinuity of the discharges which constitute the current, a discontinuity which produces the illusion of a displacement. This point, however, deserves to be studied anew. In order to observe the action of magnetism on the spiral current, I place the spiral of glass between the two poles of the electro-magnet in such a way that - its plane shall be the same with that of the two polar surfaces, the two prolon- gations being thus rendered vertical, the one above, the other below, that plane. The magnetization, according to its direction, either condenses the current towards the interior walls of the spiral tube, or, on the contrary, repels it towards the exterior walls, rendering it very diffuse. In the first case, it becomes highly brilliant, and the stratifications are very distinct; in the second case, they are but slightly visible, and the current itself is much larger and quite dim. It appears to undergo, in even a more sensible manner, the movement of rotation, ot which we have spoken. A quite curious fact is, that in the vertical branch of the tube which is below the spiral, and consequently between the two branches of the electro-magnet, the current divides itself, under the influence of the magnetism, into two streams or filaments, which tend, respectively, to one and the other side of the tube. Of these two filaments, one is very small, and of little brilliancy, in comparison with the other. The cause of this separation consists, very probably, in the fact that the inductive current of the Ruhmkorff apparatus is really composed, as we have already taken occasion to say, of two successive and opposite inductive currents, one having much more tension, and passing almost exclusively through the gas, while the other is transmitted with much difficulty, but yet passes, in very small proportion, it is true, since the action of the magnet separates it from the principal current, which is the only one in general that it is requisite to consider in this kind of phenomena, because it is by much the strongest. I have sought to determine in the case of the spiral tube, as I had done with the large rectilinear tube, the influence of magnetization on the resistance of the gas to the transmission of the discharge, and I have obtained a rather curious result. ‘The two points of platina of the apparatus of derivation being at a dis- tance of ten millimetres from one another in the distilled water, I obtained a derivative current of 20°, the spiral tube being filled with hydrogen under the pressure of 2", The spiral was placed vertically between the two horizontal armatures of the electro-magnet which were exactly in contact with its two faces. As soon as the magnetization took place, the derivative current was re- duced to 15°, when the discharge was repelled, and driven towards the exterior walls of the spiral with an apparent movement of rotation, and it was raised, on the contrary, to 25°, when the discharge was condensed towards the interior walls of the spiral. Does this influence of the direction of the current or of the magnetization depend on the particular form given to the stream, or to the small diameter of the tube, in comparison with its development in length? It is a point for future elucidation. I pass now to the case where the magnetic pole is in the midst of the gas which transmits the discharge. I have first operated with a spherical globe, ) ’ , t | ! : ; THE PROPAGATION OF ELECTRICITY. 187 about fifteen centimetres in diameter, furnished with four tubulures situated at the respective extremities of two diameters of the globe, which intersect one another at right angles. ‘Two cylindrical rods of soft iron are fixed by means of two of these tubulures in the interior of the globe, in the direction of the same diameter, so that their interior extremities may be at a distance of about eight or ten centimetres from one another, while their exterior extremities project from the tubulure nearly two centimetres. It is these exterior extremi- ties which are to be placed in contact with the poles of a strong electro-magnet, in order that the interior extremities may thus become two magnetic poles. The two other tubulures serve to introduce into the interior of the globe two isolated metallic rods, terminated by balls which are at a distance of about ten centimetres from one another, and which serve as electrodes to the electric stream whose direction is thus equatorial, that is to say, perpendicular to the right line which joins the two magnetic poles. As long as the rods of soft iron are not magnetized, the electric stream remains perfectly rectilinear ; but so soon as magnetization takes place, the stream, which we will suppose to have a hori- zontal direction, takes the form of a half circumference of a circle situated either above or below the line which joins the magnetic poles, according to the direc- tion of the magnetization or that of the discharge. The form of the luminous are is that of a half ring much flattened, as well as widened. ‘The striz are strongly marked in it, more than they were in the rectilinear current, and its exterior part is much serrated, especially when the gas contains a little vapor of alcohol or ether. If the electric current, instead of being equatorial, is axial, that is to say, directed from one of the magnetic poles to the other, these two poles serving it as electrodes, it experiences no sensible modification under the influence of magnetization. If, however, the discharge is made to pass between a ball of brass and one of iron, placed at the extremity of an iron rod so as to be capable of being mag- netized, there is observed, at the moment of magnetization, a movement of de- pression, or of elevation in the luminous atmosphere which surrounds the ball of iron. This movement pertains evidently to the change of direction under- gone by the electric filaments which radiate from the ball. But the best mode of studying the action of magnetism in the cases where the magnetized bar is in the interior of the gas, is to make use of a bell or cylindrical jar sixteen centimetres in diameter by twenty centimetres in height, in the axis of which is placed a rod of soft iron having a diameter of about three centimetres, whose rounded end is situated at the middle of the axis of the cylinder. This rod is planted in a circular disc, which serves to close the jar. A metallic ring, about twelve centimetres in diameter, formed of wire from 3 to 4™™ in diameter, and having for its centre the top of the iron rod, is situated in a plane perpendicular to the axis of the jar. This ring communicates, by means of a rod covered with an isolating coat which is soldered to it, with one of the poles of the Ruhmkorff apparatus, while the other pole is placed in communication, outside the jar, with the extremity of the rod of soft iron, which, in the interior of the jar, is also covered with an isolating coat, except at its summit. It is between this summit and the ring of which it is the centre that the discharge takes place. In order to magnetize the rod of soft iron, it now suffices to place it in contact, by its exterior extremity, with the pole of an electro-magnet, taking care to place between the two a thin strip of caoutchouc to serve as an isolating layer, so that the whole apparatus shall be well isolated. The cylindrical jar is also closed at that one of its two extremities where the rod of soft iron is absent, and it is there furnished with two cocks, of which one serves to form a vacuum, and to introduce a gas which is more or less rarefied ; and the other, constructed in Gay Lussae’s manner, permits the introduction into the ball of a greater or less quantity of vapor of whatever nature. 188 . PHENOMENA ACCOMPANYING I have made many experiments with this jar by filling it successively with atmospheric air, with nitrogen, and with hydrogen, at different degrees of rare- faction, these gases being at times perfectly dry ; at others, containing a greater or less proportion of vapor, either of water or of alcohol. 5 / Atmospherie air and nitrogen, when both dry, give nearly identical results, with this difference, that the light is more vivid and clearer with nitrogen. If the soft iron be taken for the positive electrode, and the ring for the negative one, the luminous current is seen to form, at a certain degree of rarefaction, a sort of peach-red envelope around the top of the soft iron, and a sheath of a pale violet color along an are of a greater or less number of degrees around the ring. At avery weak pressure this sheath encompasses the whole ring, while the top of the soft iron is completely enveloped with a rose-colored aureole, from which issues a very short stream of the same shade, and presenting the form of a large virgule, or comma. ‘This virgule, when the iron is magnetized, is distinctly seen to turn in one or the other direction, with the aureole from which it emanates, according to the direction of the magnetization. The violet- colored sheath which surrounds the ring is also seen to turn in the same direc- tion with the rose-colored aureole, although they are separated by a space completely obseure. By changing the direction of the discharges, there will be seen at the negative electrode a violet-colored envelope, which only covers the whole surface of the top of the iron rod when the gas is very much rarefied, and at the positive electrode, brilliant points, separated from one another by a roseate glimmer which surrounds the entire ring, and whence emanate regular stratifi- cations, internally concentric to the ring. When the gas is not greatly rarefied, there is seen to issue from the ring a luminous jet which tends to the summit of the central rod of soft iron, being only separated from it by a small, black space, and which undergoes a movement of rotation in one direction or the other, like the hand of a watch, according to the direction of the magnetization. Tn this case there is but a portion of the top of the iron rod which is covered with the violet envelope, and this luminous segment turns with the brilliant jet. I have made a great number of experiments, under the conditions just indi- cated, with atmospheric air, with nitrogen, and with hydrogen, whether dry or more or less charged with vapors. I shall proceed to give a description of them in a Summary manner, first remarking, however, that, whatever be the gas and its degree of elasticity, whether it be dry or impregnated with vapor, the rapidity of rotation is always much greater when the ring serves as the positive than when it serves as negative electrode, and that this rotation, which increases in rapidity in proportion as the tension diminishes, ceases to be appreciable at a much less tension in the second case than in the first. In my earlier experiments I had made use of a large globe, twenty-five cen- timetres in diameter, in which the ring was twenty centimetres in diameter, and the central iron rod three. This globe was furnished with two tubulures, one serving to introduce the iron rod,,whose top reached the centre of the globe, and its lower extremity issuing from the tubulure, so as to be capable of resting on the polar surface of an electro-magnet. The other tubulure was closed by a cock, which served to introduce the gas and vapor, and from it there issued an isolated conductor, which supported the ring and admitted of its being placed in the circuit. The discharge thus passed between the summit of: the rod of soft iron and the metallic ring. This globe was filled with air rarefied to 4™, The discharge took place under the form of a stream which turned with a rapidity of sixty revolutions per minute when the ring was positive, and twenty when it was negative. At a pressure of 6™™ the velocity was only forty revolutions per second in the former case and twenty in the latter. With vapor of alcohol, at a pressure of 5", the velocity was respectively twenty-two and eleven revolutions per minute. THE PROPAGATION OF ELECTRICITY. 189 After these first experiments, which served as my introduction to this sort of researches, I resumed the study by availing myself of the jar of twenty by six- teen centimetres, described above. ‘The following are the results obtained with dry atmospheric air : Pressure. Number of revolutions in a minute. Ring, positive. Ring, negative. I SO a5) aha; of. ane che fs 2/25) aaa aN OE Pe eis) sis \aseys. ccs Avan eye age 3 IO ee os nays Be SleVewanarerg one SoU Mmm cesta ha. as ok a a 55 EINE oS ojo a iw oo oc ieee eey abies aie S Oe Ss ahsetape ree ale ye a 5 obs 63 REE Goo jhe cis ce d/Slosm ye wis See TS ON RAPP eM el So, bil, Soe 100 oe ier. Mek iio tt 3 ails Lite Me ne] ace 5 Men ae acter eet ciate a. oo ehaS 128 ee II os | cis ateieycra eke oe, nes SP ee Meet ete Aiea eee acts a a3 At 9™™, with the ring serving as a positive electrode, there is no longer a stream, but a dilatation of the discharge, forming a sector of from 30° to 45°; and this sector obeys the movement of rotation as the stream before obeyed it. But it enlarges, in proportion as the pressure diminishes, and at 6™™" forms a complete circular sheet, and it is then that the rotation, which, up to this point, had increased in rapidity, becomes no longer sensible. When the ring serves as a negative electrode it is covered with a violet sheath, whose size likewise increases in proportion as the pressure diminishes, but which occupies only half the circumference of the ring under a pressure of 4™™, It is seen to turn very rapidly, but at a pressure of 2™™ it occupies the whole circumference of the ring, and there is no longer any sensible rotation. At the summit of the mag- netized iron rod there is a roseate aureole, from which, as has been said, emanates at one point a very short jet in shape of a comma, which turns with the violet- colored sheath, from which it is separated by a very considerable obscure interval. It should be remarked that, at a pressure of 6, of 4, and sometimes of even 3mm, it most often happens, when the ring serves as positive electrode, that at the first moment of the circuit being formed there issues a stream which turns too rapidly to allow its velocity of rotation to be measured, but which quickly expands so as to form, for so ne instants, a sector which continues to revolve, and soon after a complete circular sheet, which no longer manifests any movement. It does not follow that the action of magnetism is annulled when the gas is too much rarefied for the continuance of a sensible rotation. ‘That action is manifested under another form, as is shown by experiments made under a pressure of from 3 to 2™™. Thus, if the ring serves as negative electrode, the violet sheath which surrounds the soft iron is seen, at the moment when this last is magnetized, to subside sensibly, and to rise at the instant of its being demagnetized. If, on the contrary, the ring serves as positive electrode, the rose-colored sheet which fills the interval between the ring and the summit of the central rod of iron is raised, as well as the violet sheet which issues from that summit, at the moment of magnetization, and depressed at the instant of demagnetization. The following is a more complete experiment with dry nitrogen, and shows that rotation begins to manifest itself at stronger pressures when the ring is positive than when it is negative: Pressure. Number of rotations in a minute. Ring, positive. Ring, negative. PAPER. ah. tas jx af tan af anne A ase cake fate aes tay = Serie ear 9 Bee Ee si). '5).=\ >, 2.013) eee Crilics 4 ia repo ters (Sp etsyer aye sare 3 Pe east onc! as 13) naomi Ae chai fae Seas 0 tape apcccteyt die’ aie 36 Nahe ad ia ta( hn: sink = cae Ole Seta Sen ag syheta) sh hence ays ol SE at a, 3a) 6 el Re eye ten aia outta ture e fay ai ahi ay 59 Be Nacale hic» 12)3[d1aspap sso oe DELS or ay bi sighspalaiaatorayaya, « ePokapae 70 BEE a a, 854) dhs rss a aval Seana east averaieis ahi odmralane bie pis 115 5mm PN eee hes catiacrasulneeane Man 190 PHENOMENA ACCOMPANYING At 4™™ the rotation is too rapid to allow its degree to be observed; at 3mm it appears completely to cease. The rose-colored aureole is very vivid when the summit of the rod of soft iron is positive. When there is no longer any rotation, there is observed, as with atmospheric air, a movement of depression and of ascension under the influence of magnetization. The presence of vapor modifies in some important particulars the results obtained with dry gases. The following is an experiment made with ordinary air subjected to a pressure of 2™™, into which vapor of water has been intro- duced in successive quantities, so as to increase that pressure solely by the effect of the presence of the vapor: Pressure. Number of rotations in a minute. Ring, positive. Ring, negative. PaO te Ors oi Sissi euandus aioe oabgt age aie! seit tetas o aieystej alos ce ie PP, I. Piva, cpaicigeian= ar aienetohe acute eid Sr yn) = nis eyatepetet aaa Fe eee = ihapnic aiatas ales ee ai aed ae 92 Rania = das sags- eusyctenaiaiahe mosis TAOS a ie ake ie piaeiaiee eye eevee 70 ee aka aid ee aie aie tein ee UD De eh ate, orca eae a eee a tarates See 52 ees ie is eyagaiteNeteve! = cene is aha ioKe QO be oe sya aucusss ad cya totais caarete 50 A ee cna ct unis A cgasede. SUsteeee SOR es sta cies eee eel oetae ies 48 We see that at an equal pressure the rapidity of rotation is greater with vapor of water than with dry air, which is attributable probably to the greater facility with which the electric discharge is transmitted. With the external air of a mean humidity, we have, with a pressure of 14™™, 72 revolutions instead of 80 when the ring is positive, and 44 instead of 48 when it is negative. But the most characteristic fact produced by the presence of watery vapor is the division, under the influence of magnetism, of the single current into several small distinct and equidistant currents, which turn like the radii of a wheel. ‘This division is only observed when the ring serves as a positive electrode. At a pressure of 6™™ the single current begins with turning, then expands, whereupon the rotation is no longer perceptible; but at the pressure of 8, of 10, and of 12™™ this current, from the commencement of its rotation under the action of magnetism, divides into five or six small streams which turn, as was just said, like the radii of a wheel; while, when the air is dry, the current never divides; but, under a weak pressure, it merely expands into a sector or a circle of which all the parts are continuous. When the ring is negative, and there is vapor present, it will be seen that the current which issues from the summit of the iron rod presents, where it is in contact with the iron and at the moment when this is magnetized, instead of a continuous surface, a series of small brilliant points, which seem points of emanation for as many small currents, too little distant from one another to become distinet. Here, then, this current, which does not divide into separate filaments, simply undergoes dilatation or expansion at the point where it is in contact with the iron. ‘The vapor of alcohol produces similar effects with the vapor of water. The single current is, in this case, much more brilliant than with dry air or with the vapor of water; it presents fine stratifications, which give it an appearance not unlike that of a caterpillar. Magnetization expands and divides it into several currents, sensibly larger than those observed with the vapor of water. If, however, the diameter of the ring is too large, greater, for instance, than fifteen centimetres, the subdivision of the current is not effected without difficulty, unless the intensity of the discharge and that of the magnetization be very considerable. The following is an experiment in which, the rarefied gas being hydrogen, different portions of alcoholic vapor were successively introduced. The pressure THE PROPAGATION OF ELECTRICITY. 191 of the dry and pure gas was in the commencement 5™™; at this pressure, as we shall forthwith see, the hydrogen transmits the discharge only under the form of a luminous sheet. The pressure was afterwards augmented solely by means of the vapor of alcohol, with the following results : Pressure. Nuniber of revolutions in a minute. Ring, positive. Ring, negative. TN Bo Tuminons sheet i... -..-..5 92 Dee i can oe bh ao) Pas, oc Oar oiete te, acs ne age .aiee Soe o2 ee a a faa a toate aE tam OA ae ere acena sss. dace es 48 Ei yc. 2 altos hata ia ks Be re ne ee ais eo et fa 38 {SRC 1 arene pore eaegee A ata eee ea eae ee hhh 32 i ood, al so Stems yo hai SO ey oop ere ere a inle awk, 5 3 20 aE ee ee Ne oes te a Ck Ps RE a a ee a 18 Pte Sls A aaa ra a DN a aa Sameer arc eee a ae) 10 Se eae aN ea a Pea So ese el Ae oe eee crane eet 10 The division into distinct currents, more or less numerous, was manifested when the ring was the positive electrode. When pure and dry hydrogen is adopted as the medium in which the dis- charges take effect, the phenomena of rotation are obtained with great difficulty. At rather strong pressures, such as that of 128™™, we have a number of currents, but these currents are too intermittent to allow of the magnet’s acting upon them. At 90" I have obtained a small stream under the form of a bluish-white filament, which, the ring being positive, turned at the rate of thirty-five times per minute; but, at the lapse of some instants, it became subdivided into a multitude of small, irregular streams, and rotation was no longer perceptible. As far as 40™™, the action of the magnet was indistinct. At 30™™, the negative ring was covered with small violet sheaths, at equal intervals, which seemed to experience, at the moment it was magnetized, a tendency to move in one direc- tion or the other, according to the direction of the magnetization. The same was the case with the small brilliant points, likewise distributed at minute in- tervals, with which the ring, when positive, is covered. At 5™™, and still more at three and at two, the ring is entirely covered, when it is negative, with a fine violet-colored sheath, which becomes contracted under the influence of the mag- net. ‘The top of the iron rod, which is then positive, is surrounded by a beau- tiful white aureole, slightly tinged with rose, three centimetres in breadth, and stratified in a very marked degree. Magnetization sensibly contracts this au- reole, and compresses its strize without diminishing their number, clevating it, and, at the same time, giving it the form of a pear resting with its base on the magnetic pole. When this pole is the negative electrode, there issues from it, as we have seen, a brilliant tuft of a violet color, which conforms itself to the action of the magnet. ‘ All the phenomena just described show, in a striking manner, the molecular differences which various elastic fluids present, as regards one another, even at an advanced degree of rarefaction. Thus.in hydrogen, although that gas is a very good conductor of electricity, electric currents can, with difficulty, and, indeed, scarcely at all, obey the action of the magnet, probably by reason of the slight density of the gas. In air, and in nitrogen, it is quite otherwise, and still more when these gases are humid. ‘The singular property possessed by the electric current of dividing itself into several small and distinct streams, instead of diffusing itself, under the influence of magnetization, when the medium which transmits it contains a more or less quantity of vapor, would seem to indicate in the vapor a greater cohesion than in the gases properly so called, if, indeed, we may employ the term cohesion when the question relates to elastic fluids so much rarefied. It might also be possible that this division into streamlets is * 192 PHENOMENA ACCOMPANYING PROPAGATION OF ELECTRICITY. the result of an optical illusion, due to a very rapid succession of jets emanating from different points, and which, in reality, are not simultaneous. This is a point for examination. However this may be, it is evident that the study of the stratification of elec- tric light, and of the action of the magnet on the discharges in different gaseous mediums, discloses differences between those mediums which can only result from their difference of molecular constitution. Density, in particular, would appear to have a great influence on this order of phenomena, since we see hy- drogen manifest them in so feeble a degree, while the vapors of water, and especially of aleohol and ether, present them in so decided a manner. The proper nature of elastic fluids, opposing more or less resistance to the transmis- sion of electricity, must, doubtless, also play its part. It might not be impos- sible then, that, in a more detailed and more exhaustive study of the phenomena with which our attention has been occupied, and more particularly of those re- lating to the action of the magnet on electric currents propagated in much rare- fied elastic fluids, we may be able to find the means of acquiring some new ideas on tke physical constitution of bodies, and on the manner in which the propa- gation of electricity is therein effected. REPORT ON THE PROCEEDINGS OF THE SOCIETY OF PHYSICS AND NATURAL HESTORY OF GENEVA, FROM JULY, 1862, TO JUNE, 1863. BY PROFESSOR MARCET, PRESIDENT. TRANSLATED FOR THE SMITHSONIAN INSTITUTION. « In proceeding, as has been the custom of my predecessors, to present an account of the labors of the society during the year just elapsed, it is but proper that I should acknowledge how greatly my task has been facilitated by the scrupulous exactness with which the reports of our several meetings have been drawn up by our secretary, M. Ed. Claparéde. Among the topies claiming my attention, many have been already communicated to the public, or are*about to be so, through the medium of scientific journals ; as regards these, therefore, I shall restrict myself to an indication of the titles, or a very summary analysis of the conclusions arrived at.. In the arrangement of subjects I cannot do better than adopt the division into two sections, that of the physical and that of the natural sciences, first proposed by M. de la Rive, and since observed by the greatcr part of the presidents who have succeeded him. I shall follow, more- over, the example of my immediate predecessor in touching very lightly on the discussions which have taken place cither on the occasion of original memoirs read before the society or of verbal.reports on recent discoveries made in other countries; not that these discussions have not often possessed a genuine interest, but because it is essential, if this valuab'e observance is to be retained by us, that the appreciation of the labors of others, the verbal communications in which one is sometimes led to enunciate ideas arising at the moment and perhaps not always sufficiently considered, should receive no greater publicity than that which results from the reading of the journal of our sittings. PHYSICAL SCIENCES. Our indefatigable colleague, Professor Gautier, has continued to keep the “society well informed of the discoveries made in astronomy. His communica- tions have been numerous and diversified; we must here limit ourselves to the mention of the most important. M. Gautier presented to the society, in the first place, a report on the observations of M. d’Arrest, of Copenhagen, relative to the number and to the variability in brightness of the nebula, as well as to certain points, still doubtful, which would tend to indicate a proper movement in some of those bodies; secondly, an account of a memoir of M. Lamon on the periods of the variations of magnetie declination, and the analysis of researches by M. Maine on the flattening of Mars, which he estimates at j4; thirdly, a report on some recent observations of M. Donati on the comets, and on a memoir of the same author relative to stellar spectra: M. Gautier announced on this 13s 194 PROCEEDINGS OF THE SOCIETY OF oceasion that Father Secchi also was occupied in the study of stellar spectra compared with the solar spectrum ; fourthly, M. Gautier presented lastly to the society a plate of I’ather Secchi, representing the different appearances of the nucleus of the comet of 1862, differences which, as M. Wartmann, sr., has pointed out, might result, at least in part, from the circumstance that the observations took place at different hours. Professor Plantamour announces that he has collated the series of observa- tions made for twenty years on the latitude of the observatory of Geneva. That latitude would be 46° 11/ 58.75, with a mean error of some hundredths of a second. : ‘ Meteorology and terrestrial physics establishing a natural bond between astronomy and physies properly so called, we shall first direct our attention to several communications which we owe to Professor Plantamour. Besides the annual meteorological summary for Geneva and Saint-Bernard, published, as usual, in the archives of the physical and natural sciences of the “ Bibliotheque Universelle,” M. Plantamour has communicated to the society an interesting memoir relative to observations made at Geneva, for thirty-five years, on the force and direction of the winds. He has found that in winter the number of northeast and that of southwest winds balance each other; the northeast pre- dominates in spring and in autumn, the southwest in summer. ‘The general ~ resultant is a little west of north, which proceeds from the fact that the mean | direction of northeast winds more nearly approximates to north than does the mean direction of southwest winds to south. ‘The above results are somewhat modified if the origin of the winds be taken into account and if local are dis- tinguished from general winds. 'The former depend chiefly on the vicinity of the lake and the variation of temperature in the twenty-four hours, giving rise to a regular breeze morning and evening, analogous to breezes of the land and sea. ‘lhe memoir of M. Plantamour has been lately published in his extensive — work on the climate of Geneva. (See page 14, et sequent.) The same savant read to the socicty a memoir on the diurnal variations: of the atmospheric pressure, a memoir likewise published in the work just men- tioned. After having passed in review and combated as insufficient the theories proposed by MM. Krail and Dové, M. Plantamour coneludes in favor of that proposed by M. Lamon, according to which the phenomenon of the diurnal variation would depend on two distinct influences, one resulting from the tem- perature properly so called, the other from a kind of electric attraction, whose nature is as yet completely unknown, but owing probably to the action of the sun. M. Plantamour founds his preference for this theory over the preceding on the consideration that it furnishes the means of explaining the double diurnal oscillation which is observed in the barometer, while the influence of the tem- perature, it would appear, ought to produce but a single one. The author presents, in support of his opinion, a comparative table of the:diurnal variation of the temperature and of the barometer for Geneva and Saint-Bernard. To complete our analysis of what relates to terrestrial physics and meteor- ology, I have still to notice two communications, one from Professor de la Rive, relative to an aurora borealis observed in the month of December, in which the rotation of the arch from east to west was perfectly evident, and another from M. Louis Soret, who has presented to the Society an apparatus constructed according to his directions in the workshop of M. Schwerdt, an apparatus de- signed for the measurement of heights by a determination of the temperature of the ebullition of water. In the construction of this instrument, the chief object of M. Soret has been to attain a perfect precision in thermometrical indications, — a condition which has heretofore been wanting. He has sueceeded, on the one hand, by surrounding the ball of the thermometer with two envelopes of vapor instead of one, in abating the variations of temperature proceeding from with- out; and, on the other hand, he prevents the effect of an ebullition often too PHYSICS AND NATURAL HISTORY OF GENEVA. 195 much precipitated, by immersing the bottom of the lamp of alcohol, by the flame of which the water is to be made to boil, in a bath of cold water. The sole, yet somewhat grave objection which has been advanced against this apparatus, is, that in astill greater degree perhaps than the barometer, it requires to be observed with scrupulous care, and demands precautions which can searcely be ex- pected on the part of observers who are not physicists. If we pass now to physics properly socalled, we shall see that, as in the past, it is electricity which has played the principal part in the communications made to the Society during the year under review. Our colleague, M. de la Rive, has communicated to us, at two consecutive meetings, the results of his researches on the phenomena which characterize and accompany the propagation of electricity in highly rarefied elastic fluids. In the classification of his ap- paratus, M. de la Rive insists more particularly on the means which he has em- ployed to measure the intensity of the discharges or transmitted currents, by availing himself of a derived current taken by means of two small sounds of platina, in the distilled water placed in the circuit of the principal current. He also describes a manometer which enables him to appreciate to nearly the fiftieth part of a millimetre, and, for practiced eyes, even to the hundredth part, the tension of the elastic fluid submitted to experiment. 'The researches of M. de la Rive have been directed to atmospheric air, nitrogen, and hydrogen. He has studied, in the case of each of these gases, the influence of the dimen- sions and form of the gaseous mass, as well as of the pressure, on its capacity for transmitting electricity. He has described the successive appearances which the electric light assumes, in proportion as the pressure of the gas dimin- -ishes, and particularly the variable form and size of the stratifications of that light, together with the formation of a violet-colored photosphere around the ball serving as a negative electrode, and of a black space, from five to ten centi- metres in length, which separates that photosphere from the stratified luminous column. He has satisfied himself, in the course of a great number of ex- periments, that these appearances of electric light in rarefied gases are due to a mechanical effect produced by the transmission of electricity, an idea which had already been advanced by M. Riess. M. de la Rive has suc- ceeded in showing, by direct experiments, that the mechanical effect in ques- tion consists in a considerable dilatation of the gaseous matter near the negative electrode, followed by alternate contractions and dilatations in the column up to the positive electrode. First. He was easily able to verify, by means of the manometer, the existence of the oscillatory movement in the gaseous column, and the variations in its intensity, which depends, as he has shown, on the nature, degree of tension, and dimensions of the gaseous mass in question. Secondly. Hehas demonstrated experimentally thatif, by means of small sounds of platina suitably arranged, derived currents are taken in different parts of the luminous column, all traversed by the same discharge, great differences will be found in the intensity of these currents, differences which prove that the ob- scure parts possess a greater conducting capacity, and are consequently the most dilated. With hydrogen, the best conductor of the gases, no derived current is obtained in the obscure part of the column. Thirdly. M. de la Rive points out that the indications of the thermometer placed in different parts of the stratified column conduct us to the same results, by evincing great differences between the temperatures of those different parts ; the more obscure parts being sensibly less warm than the luminous, which proves that the former are better conductors. The author has obtained a great number of numerical results, in- dicating the differences of temperature, at different pressures of various portions of the gaseous column traversed by the discharges. M. de la Rive completed his communication at a subsequent session, by ex- plaining to the Society the modifications produced in the phenomena relative to the propagation of electricity, through highly rarefied mediums, by the action of 196 PROCEEDINGS OF THE SOCIETY OF a strong magnetic power. This action tends to augment the resistance of the gascous substance (o the transmission of electricity, by condensing the gaseous filaments, and has in particular the effect of rendering luminous the obscure part of the column, by contracting the previously too much dilated gas which oceurs there. Lastly, the attention of M. de la Rive was especially drawn to the rotatory and expansive action of magnetism on the electric discharge. THe has succeeded in obtaining, in regard to this point, certain very constant facts, such as those relative to the duration of the rotatory movement of the discharge, which varies with the direction of the current, the nature of the gas, and its degree of density. He has also remarked the very great difference which the phenomenon presents, according as the rarefied gas is dry or contains vapor of water or of alcohol. In the first ease, the luminous discharge expands under the influence of magnetism into a sheet which forms the surface of a sector, or even that of a full circle when the gas is very much rarefied. In the case in which vapor is present in the rarefied gas, the discharge, instead of expanding, divides into a greater or less number of small partial jets at equal interspaces, forming, as it were, a star animated by a movement of rotation around its centre. These phenomena, and others of the same kind, have led M. de la Rive to establish a difference between permanent gases and vapors, in reference to the point of cohesion, or rather their molecular constitution. The author termi- nated the reading of his memoir with some general considerations on this exten- ‘sive subject; announcing that, for the present, conclusions too absolute would be premature, and that he abstains from presenting them until he shall have completed his researches by extending them to a greater number of gaseous substances. : If we have enlarged a little more than is usual in an analysis of the memoir of M. de la Rive, we find a justification, not only in the importance of the sub- ject, but in the circumstance that the results which he obtained have been here- tofore published only in fragments. ‘The entire memoir is about to appear in the seventeenth volume of the Memoirs of the Society, now in the press.* It should be added, that we owe to M. de la Rive the model of a new system of Grove’s apparatus. ‘lhe modification which he has introduced into the bat- tery of that physicist is essentially calculated to render its management more commodious and prompt. Lis instrument, which is extremely manageable, and is furnished with conductors of alumina, possesses the advantage of requiring little manipulation, and of rendering superfluous the removal of the nitric acid; the same acid suffices for the service of several days.and many experi- ments. With the help of a single pair of this battery, M. de la Rive has been able to repeat all the principal experiments of the clectro-dynamics of Ampére— experiments which usually require five or six pairs of Grove or of Bunsen. Besides some verbal communications by Professor Wartmann relative to electrical phenomena, particularly to the limit of pressure which permits a spark to pass through a gascous medium, as well as to the influence which the state of tension of a gascous medium exercises on the passage of a current, the savant just named cugaged the attention of the society by an account of some of the principal subjects diseussed in the last reunion of the British Association at Cambridge, at which he was present. Among the communications made on that occasion, M. Wartmann cites more particularly the observations of M. Nasmith relative to the structure of the sun. ‘lo avoid the inconvenience of a too great light, M. Nasmith, instead of introducing the solar rays dircetly into the eye,*places near the object glass a lens which is plane on the side next the eye, but concave on the opposite side, so as to disperse the luminous rays and allow the study of only the quantity of light reflected by the plane surface. Lhe author has thus been able to ascertain that towards the hour of noonday A full translation of this interesting memoir is given in this report.—See page PHYSICS AND NATURAL HISTORY OF GENEVA. 197 the luminous envelope of the sun presents a great number of spindle-shaped images, which might be compared to willow leaves strewn confusedly over its surface. Of these M. Wartmann has presented to the Society a photograph taken from the original designs of M. Nasmith. These images seem to be dis- placed one by another, sometimes parallel to their axis, sometimes by an angu- lar movement. The preceeding observations have been confirmed by M. Prit- chard, who announces that they may be repeated with a good telescope of from three to four inches. M. Wartmann also gave an account of experiments in telegraphic electricity by M. Wheatstone, which he witnessed, and by which it is practicable to obtain despatches written with extraordinary rapidity. The same physicist communicated to the Society a note relative to an clee- trical phenomenon observed by M. Alizier, teacher at Geneva, July 24, 1856, on the summit of the Oldenhorn. Of a sudden the staves borne by M. Alizier and the persons who accompanied him began to sound in the manner of the posts of the telegraph. In a few moments a heavy storm of hail descended. Professor de la Rive, on his return, in May, 1863, from a sojourn in Paris, reported to the Society several new scientific facts which he had gathered. He drew attention, in particular, to an investigation of M. Helmholtz, by which that savant had arrived, simultaneously with M. W. Thompson, at the conclusion that the earth cannot be liquid in its interior. He also thinks himself entitled to affirm that it is not necessary to recur to the hypothesis of aerolites falling continually into the sun, in order to explain the persistence of the high tem- perature of that body. It suffices to admit that the sun, having become heated by an undetermined cause, is now growing cold with extreme slowness; for, according to M. I[elmholtz, the calculations heretofore made greatly exag- gerated the rapidity of refrigeration in regard to that body, because they neglected to take account of an important element, namely, that the sun diminishes in volume as it grows cooler, and that this contraction must de- velop new heat. M. de la Rive presented to the Socicty, in the name of his son, M. Lucien de la Rive, a memoir on the number of independent equations in the solution of a system of linear currents. his memoir, being wholly mathematical, is not adapted to analysis. Professor Marcet has continued to impart to the Society many facts relative to nocturnal radiation; among others, to an altogether abnormal refrigeration of the surface of the ground, and of the stratum of air in immediate contact with it, which he has remarked during the first days of March in localities turned towards the north, not only at the hour of sunset, but even during the warmest hours of the day. The author attributes this extraordinary cooling of the surface to the concurrence of several atmospheric circumstances, but more especially to the extreme dryness which had prevailed for some time, and which, as Tyndall has proved, peculiarly facilitates the radiation of terrestrial heat.* M. Mareet has taken advantage of the residence of his son in Australia, to induce him to repeat at Queensland, under the 22d degree of south latitude, the experiments on nocturnal radiation, which have been recently made in our temperate climates. It would seem to result from these experiments that the phenomenon of the inerease of temperature at certain periods of the day, when we ascend some fect above the surface of the earth—a phenomenon so well authenticated in our temperate climates—is not remarked in the regions of the torrid zone either at the rising or setting of the san; or if it takes place, it is in a degree seareely sensible, hardly ever execeding 0°.4 Cent. M. Lucien de la Rive has recently made some observations in Egypt, on the banks of the Nile, which would appear to lead to an analogous result. M. Marcet explains * See Archives des Sciences Physiques et Naturelles, April, 1863, 198 PROCEEDINGS OF THE SOCIETY OF this apparent anomaly by attributing it to several causes, but more particu- larly to the great quantity of water, under the form of elastic vapor, held by the atmosphere in tropical regions, especially in countries but little remote from the sea—vapor which, it is known, possesses the property of intercepting in a high degree the dark heat emitted by the ground, and which would thus contribute to render so much less apparent the effects produced by the nocturnal radiation. Communications on chemistry proper have this year been less numerous than usual. We have scarcely anything to cite but some remarkable researches of Professor Marignac on the tungstates, the fluo-tungstates, and the fluo- borates. The subject, although of great importance, and treated in a masterly manner, is too special to allow of my presenting here even a summary analysis. We may, besides, direct the reader for a detailed extract of the memoir to the comptes rendus of the Academy of Sciences, in anticipation of its appearance in extenso in early numbers of the Annales de Chimie et de Physique. Dr. W. Marcet has drawn the attention of the Society to investigations made by him on the digestion of fats, particularly on the mode in which the emulsion of those substances is effected by means of the bile, and prebably also of the phosphates, which occur abundantly in animal food. 'The same chemist also communicates experiments, which he has recently undertaken, on the compo- sition of the gastric juice, and on the changes which it undergoes as to the degree of acidity during the act of digestion. NATURAL SCIENCES. The natural sciences, and more especially geology and paleontology, have this year had a large share in the labors of the Society. We should mention, in the first place, several important communications of Professor A. Favre; and, first, his geological chart of portions of Savoy, Piedmont, and Switzerland, in the neighborhood of Mont-Blane—a chart drawn on a scale of zzg5g9> and which is the result of persevering and conscientious labors pursued since 1840. M. Favre has also presented us with the geological chart of the Jura mountains pertainmg to Basle—the first published at the expense of the confederation, under the care and direction of M. Miiller. It is designed on a seale of s54355- There is reason to fear, however, that the enterprise cannot be continued in such wide proportions, and that it will be necessary to return to the scale of yooo00: Lhe chart is accompanied by a publication in two series—one for the Jura, the other for the Alps. M. Favre also read to the Society a memoir containing a detailed description of the mountain of the Voirons, of which he has determined the succession of the different strata. This memoir will soon appear in the text which will ac- company the chart of Savoy. The same geologist read to the Society a critical analysis of MM. Koechlin- Schlumberger and Schimper on the transition deposit of the Vosges—a deposit referred at present to the old carboniferous series. He also presented, in the name of M. Studer, a geological memoir on the Balligstock and the Béatenberg, situated on the borders of the Lake of Thounc—a memoir which has been pub- lished in the Archives of the Physical and Natural Sciences. Professor Pictet read to thé Society a note containing critical observations on the subject of a new stratum, which M. Coquand proposes to introduce into the series of cretaceous formations—a stratum already known under the name of “alpine neocomian,”’ and to which he proposes to give that of “ barémian,” considering it as the equivalent of the yellow stone of Neuchatel. M. Pictet, without disputing the propriety of a new name, does not admit, between the a and the yellow stone of Neuchatel, so precise and restricted a paral- elism. PHYSICS AND NATURAL HISTORY OF GENEVA. 199 The same savant called the attention of the Society to an alleged reptile with feathers, found in the jurassic of Solenhofer, and described by M. Wagner as possessing at once the tail of a reptile and the feathers and feet of a bird. This fossil has been acquired for the British Museum by M. Owen, who will soon publish a detailed description of it. . The Society has continued to keep itself informed of the facts relative to the «fossil man.” Its interest has been particularly excited by the discovery of the human jaw-bone of Moulin-Quignon, near Abbeville. M. Pictet, who took occasion very recently to study, at Paris, this bone, and the hatchets which ac- companied it, has set forth to the Society the reasons which seemed to him to render the authenticity of those objects incontestable, notwithstanding the doubts at first expressed on this subject by eminent paleontologists. More recently we have learned with much interest that a sort of scientifie congress had been con- voked at Paris, and the authenticity admitted with unanimity. It remains to solve the question of antiquity—that is to say, to decide what place the deposit of Moulin-Quignon should occupy in the series of quaternary and modern formations. . «M. Renevier has communicated to us a photographic view of the Diablerets, geologically colored, and has, at the same time, given to the Society an account of some recent geological excursions in the vaudese Alps. He has been enabled to complete the series of jurassic formations in this district by the discovery, in the Diablerets, of a stratum of bajocian, (inferior oolite,) and of a stratum of bathonian, (greater oolite,) the first being characterized by a gigantic fucoid. Finally, M. Renevier announces grains of “chara”? in the nummulitic of the Diablerets. We arrive now at organic natural history, and it remains to speak of botany and zoilogy. Botany.—Professor De Candolle has presented to the Society several in- teresting communications relative to vegetable physiology and to botany proper; particularly a paper on a new character observed in the fruit of oaks, and on the best division to adopt for the genus “ Quercus ;”’ a memoir entitled Studies on species, occasioned by a revision of the family of Cupulifere, in which the author discusses the system of Darwin, and the theory, applied to the vegetable kingdom, of a succession of forms proceeding from the deviations of an anterior form. Both these memoirs having been published in the archives of the physical and natural sciences of the Bibliotheque Universelle we shall here content ourselves with indicating them to savants who are interested in questions of this kind. Besides the original memoirs just cited, M. de Candolle brought to the notice of the Society some interesting results of observations made by M. Schubler “on plants cultivated in Norway.’ The author has shown us in what degree the deficiency of heat, in northern regions, appears to be compensated by the prolonged action of the light due to the length of the days; to such an extent that, in proportion as we advance towards the north, the coloration and sapidity of plants seem to increase rather than diminish in intensity. M. de Candolle has also drawn attention to two memoirs of Dr. Hooker. The first relates to a plant discovered on the African continent, opposite Fernando-Po, to which he has given the name of Welwitschia. This plant, whose trunk is a cone of little height, surmounted by a torous (dosselé ) table attaining a diameter of six feet, presents the singular character of having but two leaves, which are indeciduous cotyledons. It is the only vegetable known whose cotyledons are not caducous. The second memoir of M. Hooker relates to the celebrated group of cedars of Lebanon, which is found to be established on the moraine of an ancient glacier, and which this botanist visited in 1860. M. Hooker is inclined to think that, in the present circumstances of climate, this tree could, with difficulty, establish itself on the mountain where it is found, and pronounces 200 PROCEEDINGS OF THE SOCIETY OF the opinion that the old cedars which now exist there are but the remains of — an ancient forest, dating from an epoch more favorable to the development of the species. It is certain, in the mean time, that the cedar of Lebanon, that of the Himalaya, and that of the Atlas present varieties which it is difficult to distinguish from one another, Hence M. Ilooker is disposed to admit that they all descend from one primitive form, which has spread itself over a vast region when the climate was more temperate than it is at present. To Rev. M. Duby we are indebted for a note relative to observations made at Bombay, on a champignon or fungus which attacks the feet of the natives, and produces a malady known in the country under the name of * podeleoma mycetoma.”’ The bones of the foot and lower leg are gradually perforated through and through, and the champignon, which bears spores very similar to those of the oidium, lodges in the cavities thus formed, under the shape of a — spongy mass. M. Duby has also occupied our attention with the very ingenious observations of M. Darwin on “the mode of fecundation of the red flax.” The same botanist’also announces that he has observed in the Cadlistachys linearis a very remarkable movement of the inferior leaves which, at the decline of day embrace the stem, while the superior leaves embrace the ear. Zoblogy and Physiology.—Dr. Dor called the attention of the Society to a new theory of Daltonism, or rather to an old theory of Young, to which there seems to be a tendency to recur at the present time. Agreeably to this theory 7 there exist in the retina three descriptions of nervous fibres; the first sensitive — to red, the second to green, the third to violet. Daltonists, then, would be those ii whom one of these orders of, fibres: is completely paralyzed. M. Dor has also proposed a new scale of characters for measuring the distinctness of vision. M. Victor Fatio presented to the Society a specimen of a lizard of the Alps ealled “ Lacerta nigra,’ regarded by some authors as constituting a particular species. M. Fatio is rather disposed to consider it as being but a simple variety of the “ Lacerta vivipara,’”’ and he adduecs the reasons which lead him to hold this opinion. The same physiologist read to the Society a note on the habits of the “ pléo- bate cultripede,” of the coasts of Brittany. Te has ascertained that this batra- chian is a nocturnal animal, which buries itself during the day in the sand, and remains there till night in a state of complete immobility. M. Fatio has also communicated to us a plan of geographical distribution, designed to form the basis of an extensive work, which he has undertaken with the view of making a complete catalogue of the vertebrata of Switzerland. To complete what we have to say on organic natural history, we should mention an interesting notice by M. Muller, relative to the recent modifications which the theory of cellular organization has undergone through the influence of the labors of MM. Briicke and Max. Schultze; and a communication of M. Claparede, in which that physiologist renders an account of some epidemie Instances of “trichinus spiralis” lately authenticated in Germany, and more especially in Saxony. It is now known that the larva of this parasite continues to live in the flesh of the hog when iusufiiciently smoked. Now, a single pair of these animalcules, arriving at maturity in the human intestine, suffice to infect with larvae all the muscles of the body, and to occasion the gravest con- Bequences, sometimes even death. The danger of such an infection is now so fully realized that the inhabitants of Planen, in Saxony, have established at _ their slaughter-house an official, provided with a microscope, and have prohibited the sale of hogs whose flesh has uot been previously examined with the help of that instrument.* eae 2s ON NERC eet EN! * Por an appendix to this part of the report see the end of this article. | PHYSICS AND NATURAL HISTORY OF GENEVA. 201 Dr. Gosse has communicated to the Society a note of M. Campbell relative to the frequency of goitre, in the districts near the foot of the Himalaya—a malady with which also goats and sheep are frequently infected when they de- seend from the mountain Lastly, Dr. Lombard has read to us a detailed extract of observations publishe1 by M. Jordannet, a French physician, on the climate of Mexico, considered in a medical point of vie Having thus presented a cursory review of our proceedings during the past year, my task unfortunately is still incomplete ; for, notwithstanding the re- stricted number of our members, scarcely a year passes in which your presiding officer, in his annual report, is not called on to deplore the loss of one or more of them. This year has removed two from among us: one of them, M. Le Royer, a retired member, of advanced age; the other, M. Etienne Melly, a member in ordinary, whose years authorized us to hope that we might long re- tain him. I must not close this report without briefly recalling the titles they possessed to the esteem of the learned world and the affection of their colleagues. Etienne Melly, born at Geneva, in 1807, early evinced a decided taste for the physical sciences. After successfully pursuing the course of our Academy, he went to Paris to complete his scientific studies, and on his return to his country was attached to the Industrial school of this city as a teacher of physics and chemistry, the study of which he may be said to have created in the establish- ment in question, and from the superintendence of which he never desisted until the infirm state of his health made it impossible for him to give to his duties the care and attention which his scrupulous conscience exacted. While thus employed he prosecuted divers physico-chemical researches of great interest, only a part of which, owing to his characteristic diffidence, have been commu- nicated to the public. His two principal publications appeared, the first, in 1839, in the Bibliotheque Universelle, the second, in 1841, in the first volume of the Archives de V Electricité. ‘The former treats of certain felicitous attempts which he had made to apply platina to other metals by means of pressure so as to obtain.a very solid plate, and be thus: able to substitute, in certain chemical processes, for utensils of platina, utensils of platinized copper. This mode of platinizing offers greater assurance than that by electricity ; in that it better resists the action of chemical agents. The second publication of M. Melly, and that of most importance, embraces two distinct parts: the first, relating to a more economical construction of the battery of!'Grove, then just invented, and to the study of the chemical effects of electricity by means of that apparatus. ‘The second part has for its object the study of the chemical effects of the electric spark, whether produced by Grove’s battery or by currents of induction. M Melly sets forth in his memoir the numerous experiments by which he had succeeded in decomposing, by means of that spark, not only distilled water, but the most isolating substances, such . as oils, ethers, alcohol, &e. He establishes, by a well-sustained analysis of the results he had obtained, the difference which exists between this mode of de- composition and electro-chemical decomposition properly so called, and he shows that it is an effect, not of electricity itself, but of the intense heat developed by the electric spark. ; We know that this decomposing power of heat, carried to a high degree, has been since demonstrated in a direct manner upon water, without the interven- tion of electricity, by M. Grove, and has been exfended upon a wide seale to a multitude of substances by M. Deville, who has called it, “the dissociation of bodies by heat.’ Still, there will remain to M. Melly the honor of having first, by his ingenious experiments, called the attention of the learned world to this important subject. Independently of what he has made known by his publi- 202 PROCEEDINGS OF THE SOCIETY OF cations, Melly, who knew no remission of labor, often obtained interesting results which he kept to himself, or communicated but to a few of his friends. The distressing state of his health having compelled him, many years since, to abandon his laboratory, he did not give way to discouragement, but continued to devote himself with the same ardor to the microscopic investigations which constituted the scientific interest of his latter days. Of these he has left but few written notices; their results are contained in his collections, especially in that of the Diatomez, of which he has left more than fifty boxes, containing as well the Diatomeee of the environs of Geneva, as those of foreign lands and those of types determined by known authors. As to the microscopes of which he availed himself, it may be affirmed that never have the Alge of our country: been studied with the help of instruments so perfect. Melly, besides, brought an extreme carefulness to the preparation of microscopic objects; we may judge of it by the following fact reported by Professor Thury in the interesting notice which he read of his friend: The collection of Diatomee was twice resumed | entirely anew by Melly, because the distilled water and alcohol which he had employed were found to be not absolutely pure. Of a conversation as frank as amiable, Melly had, moreover, that devotedness for others, whose character is the most complete self-abnegation. Happy in the success and welfare of his friends, every feeling of envy and jealousy was so alien from his nature, that he would not even admit the existence of these evil sentiments in another. Having suffered in his dearest affections by the loss of a beloved consort, he remained thenceforward completely isolated. But this isolation, far from rendering him egoistic, had still more enlarged his heart. His gratitude, for the cares and attentions of which he was the object on the part of his friends was as touching as amiable. The religious sentiments which sustained him in the midst of trials so various and afflicting were always united in him with a perfect tolerance in regard to those who did not share his opinions. It was the fruit of an elevated and disinterested nature, such as is rarely witnessed. He sank, February 4, 1863, after long and acute sufferings. Auguste Le Royer sprung from an honorable family, and whose ancestors had been pharmaceutists from father to son ; was born at Geneva, in 1793. After pursuing his earlier studies in his native city, he went in 1811 to Strasburg, where he passed eighteen months of preparafion in studying pharmacy, his future vocation. In 1813 he returned to Geneva, took an active part in the political events of the time, and in 1817 was admitted a pharmaceutist after an honorable examination. 'Thenceforward Le Royer zealously occupied himself in scientific labors related to his profession. It was in 1818 that the illustrious Dumas, then ten years of age, entered himself as a clerk with Le Royer, and subsequently became his principal assistant. Besides these friendly connexions with Dumas, Le Royer contracted others with Dr. Prevost, taking part in many of the physiological researches of the latter in their chemical bearing. In 1821 he was adopted as a member of this Society and of the Helvetic Society of natural sciences. 'The departure of M. Dumas for Paris, in 1823, compelled Le Royer to occupy himself almost exclusively with pharmacy, and I know not that he has published anything since 1824. Nevertheless, he preserved a taste for study, and always encouraged the scientific labors of those who approached him. Like Etienne Melly, with whom he had more than one trait of conformity, an extreme modesty pushed almost to timidity, joined to delicate health, pre- vented Le Royer from making that mark in science to which he might have pretended: 'The following is a list of the articles which he published jointly with Dr. Prevost : 1. Note on the free acid contained in the stomach of the herbivoré, (Memoirs of the Society of Physics and Natural History, vol. IIT, 2d part.) 2. A memoir on digestion in the ruminants, (Bibliotheque Universelle for 1824, vol. XX VIL.) PHYSICS AND NATURAL HISTORY. OF GENEVA. 203 3. Observations on the contents of the digestive canal in the foetus of the vertebrates, ( Bibliotheque Universelle, vol. X XIX.) Lastly, he published alone in the Bibliotheque Universelle, vol. XXVI, a memoir on the active principle contained in the “ purple digitalis.” Having become a valetudinarian in 1850, in consequence of rheumatic affee- tions, Le Royer was struck, in 1860, with cerebral apoplexy, which kept him riveted to his chair till the moment of his death, a few weeks since, without any notable abatement of his intellectual faculties. APPENDIX ON THE TRICHINIASIS. We annex the following additional information in respect to Trichiniasis, mentioned in the preceding article: A few months ago there was a festive celebration in Hettstadt, a small coun- try town near the Hartz Mountains, in Germany. Upwards of a hundred per- sons set down to an excellent dinner, and having enjoyed themselves more majorum, separated, and went to their homes. Of these one hundred and three persons, mostly men in the prime of life, eighty-three are now in their graves ; the majority of the twenty survivors lin- ger with a fearful malady; and a few only walk apparently unscathed among the living, but in hourly fear of an outbreak of the disease which has carried away such numbers of their fellow-diners. They had all eaten of a poison at that festive board, the virulence of which far surpasses the reported effects of agua tophana, or of the more tangible agents described in toxicological text-books. It was not a poison dug out of the earth, extracted from plants, or prepared in the laboratory of the chemist. It was not a poison administered by design or negligence. But it was a poison unknown to all concerned; and was eaten with the meat in which it was con- tained, and of which it formed a living constituent. When the festival at Hettstidt had been finally determined upon, and the dinner had been ordered at the hotel, the keeper of the tavern arranged his bill of fare. ‘The introduction of the third course, it was settled, should consist, as usual in those parts of the country, of Rostewurst und Gemiise. The Roste- wurst was, therefore, ordered at the butcher’s the necessary number of days beforehand, in order to allow of its being properly smoked. 'The butcher, on his part, went expressly to a neighboring proprictor, and bought one of two pigs from the steward, who had been commissioned with the transaction by his master. It appears, however, that the steward, unfortunately, sold the pig which the master had not intended to sell, as he did not deem it sufficiently fat or well-conditioned. ‘Thus the wrpng pig was sold, carried on a barrow to the butcher, killed and worked up into sausages. ‘The sausages were duly smoked and delivered at the hotel. ‘There they were fricd and served to the guests. at the dinner table. On the day after the festival, several persons who had participated in the dinner were attacked with irritation of the intestines, loss of appetite, great prostration and fever. 'Vhe number of persons attacked rapidly increased ; and great alarm was excited in the first instance by the apprehension of an impend- ing epidemic of typhus fever or continued fever, with which the symptoms ob- served showed great similarity. But when, in some of the cases treated by the same physician, the features of the illness began to indicate at first, acute peri- tonitis, then pneumonia of a circumscribed character, next paralysis of the inter- costal muscles and the muscles in front of the neck, the hypothesis of septic fever, though sustained in other cases, had to be abandoned with respect to these particular cases. Some unknown poison was now assumed to be at the bottom 204 PROCEEDINGS OF THE SOCIETY OF " of the outbreak ; and an active inquiry into all the cireumstances of the dinner was instituted. Every article of food and material was subjected to a most rigid examination, without any result in the first instance. But when the symp- tons in some of the cases invaded the muscles of the leg, particularly the calves of some of the sufferers, the description which Zenker had given of a fatal case of trichinous disease was remembered. ‘The remnants of sausage, and of pork employed in its manufacture, were examined with the microscope, and found to be literally swarming with encapsuled trichine. From the suffering muscles of several of the victims small pieces were excised, and under the microscope found charged with embryonic trichinée in all stages of development. It could not be doubted any longer, that as many of the one hundred and three as had had partaken of Rosfewurst Lad been infested with trichinous disease by eating of trichinous pork, the parasites of which had, at least in part, escaped the effects of smoking and frying. This awful catastrophe awakened sympathy and fear throughout the whole of Germany. Most of the leading physicians were consulted in the interest of the sufferers, and some visited the neighborhood where most of the afilicted patients remained. But none could bring relief or cure. With an obstinacy unsurpassed by any other infectious or parasitic disease, trichiniasis carried its victims to the grave. Many anthelmintics were arrayed to destroy, if not the worms already in the flesh, at least those yet remaining in the intestinal canal. Picric acid was employed until its use seemed as dangerous as the disease; benzole, which had promised well in experiments upon animals, was tried, but was unavailing. As patient after patient died off, and the dissection of each proved the parasites to have been quite unaffected by the agents employed, the conviction was impressed upon every mind that a man afflicted with flesh-worm is doomed to die the slow death of exhaustion from nervous irritation, fever, and loss of muscular power in parts of the system essential to existence. But medical science had only just unravelled a mystery ; and if it could not save the victiins, it was determined at least to turn the occasion to the next best account. ‘The cases were therefore observed with care and chronicled with skill. All the multifarious features of the parasitic disease were registered in such a manner that there can hereafter be no difliculty in the diagnosis of this disorder. A valuable diagnostic feature was repeatedly observed, namely, the appearance of the flesh-worm under the thin mucous membrane on the lower side of the tongue. The natural history of trichina in man was found to be the same as that in animals. All observations led to the conviction that the trichina encapsuled in the flesh is in the condition of puberty. Brought into the stomach, the calcareous capsule is digested with the flesh, and the trichina is set free. It probably feeds upon the walls of the intestines themselves, for the irritation of the intes- tines begins before the bringing forth or*young trichine has taken place. Copulation is immediately effected ; and within a few hours, or a short portion of days, from sixty to eighty live embryos leave the female, and begin then own career of destruction. This consists, in the first instance, in an attempt to pierce the walls of the intestinal canal. Great inflammation of the entire surface ensues, ending not rarcly in death of the villous or mucous membrane, or in the formation of masses of pus on its surface. Sometimes there are bloody stools. But these severe symptoms only ensue when much trichinous meat has been eaten; when less has been consumed, pain and uneasiness in the abdomen are produced, accom- panied, however, in all instances by wasting fever and prostration. The embryos actually pierce the intestines, and are found free in the effusion, sometimes serous, sometimes purulent, which is always poured out into the abdominal cavity. ‘Thence they again proceed towards ,the periphery of the body, pierce the peritoncum, causing great irritation, and sometimes peritonitis, PHYSICS AND NATURAL HISTORY OF GENEVA. 205 ‘ to the extent of gluing the intestines together to a coherent mass. They next roceed to the muscles nearest to the abdomen; arrived at the elementary muscular fibres, which, under the microscope, appear as long cylinders with many transverse strie, they pierce the membranes, enter the fibres, eat and destroy their striated contents, consume a great part of the granular detritus, moving up and down in the fibres until grown to the size necessary for passing into the quiescent state. ‘They then roll up in spiral or other irregular windings, the bags of the muscular fibres collapse, and only where the trichine lie a cal- careous matter is deposited, perhaps by the trichinz themselves, which hardens into perfect capsules round the parasites. A muscular fibre may harbor one or several parasites ; but every fibre invaded by a single parasite loses its character entirely, and becomes a bag of detritus from one end to the other. If it be remembered that one ounce of meat filled with trichine may form the stock from which in a few days three millions of worms may be bred, and that these worms will destroy in the course of a few weeks not less than two millions of striated muscular fibres, an idea of the extent of destruction produced by these parasites can be formed. We are not in a position to say to what propor- tion of the fifty or sixty pounds of muscle required for the performances of the human body these two millions of elementary fibres actually amount. In the muscles nearest to the abdomen the destruction is sometimes so complete that not a fibre free from parasites can be found. ‘This amounts to complete paralysis. But death is not always produced by the paralysis; it is mosily the result of paralysis, peritonitis, and irritative fever combined. No case is known in which trichiniasis, after having declared itself, became arrested. All persons affected have either died, or are in such a state of prostration that their death is very probable. Most educated people in Germany have, in consequence of the Hettstadt tragedy, adopted the law of Moses, and avoid pork in any form. ‘To some of the large pig-breeders in Westphalia, who keep as many as two thousand pigs, the falling of the price of pork has been a ruinous—at the least a serious—loss. In the dining-rooms of the hotels in the neighborhood of Hettstadt notices are hung up announcing that pork will not be served in any form in these estab- lishments. ‘'I'o counteract this panic, the farmers’ club of the Hettstadt district gave a dinner, at which no other meat but pork was eaten. But it has had no appreciable effect. The raw ham and sausages of Germany are doomed to extinction; the smoked and fried sausages must necessarily be avoided. * * In the south of Germany some people now say that it is the Hungarian pigs which are most frequently affected with trichine. This rumor, like the famous pork dinner of the farmers’ club, may, however, have been set up with the inten- tion of quieting apprehension about the native pigs. We have already mentioned the accident which befell the crew of a merchant vessel. They shipped a pig at Valparaiso, aud killed it a few days before their arrival at Hamburg. Most of the sailors ate of the pork in one form or another. Several were affected with trichinsze and died. Of those whose fate could be inquired into, only one seems to have escaped the parasites. Another outbreak in Saxony has carried away twelve persons. / 208 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS But the difference of the two forces is still more strikingly exhibited by the difference of their spheres of attraction. ht the case of gravitation every atom, for example, of the earth attracts every other atom of the whole mass, eaclf conspiring with all the others to produce the spherical form. While under the influence of molecular attraction the atoms of a liquid globule only acts upon the other atoms which are immediately around them; and hence the atoms in the interior of a globule are, as it were, in a neutral condition, attracted equally in every direction. ‘The only atoms, therefore, which are active in producing the globular forms and in giving rise to the phenomena deseribed in this memoir, are those at the surface of the liquid, since these are only attracted on one side, and are, therefore, free to exert their energy towards the mass, and their tendency to bring this into the smallest compass, namely, that of a sphere. According to this view a globule of water may be considered an assemblage of atoms, without attraction, compressed into the spherical form by a contractile film, within which the atoms are enclosed. ‘The amount of contractile foree of such a film will depend on the energy of the attraction between the con- tiguous atoms and the degrees of curvature. To illustrate this, let us suppose a slip of India-rubber to be stretched horizontally between two supports. If to the middle of this we attach a small weight, the slip will sag downwards, and the point to which the weight is attached will descend until there is an equi- librium between the weight and the contractile force. If an additional weight be attached, the descent will be inereased until a new equilibrium is attained, and so on, the contractile foree will increase with the degree of bending. A similar force is exerted at the free surface of all liquids. If this surface is hori- zontal, the attraction will be equal in every direction in the horizontal plane; but if at any point we press the surface so as to bend it out of this plane, the contractile force will be called forth, tending to bring the point back into its former position. It is this surface contractile force which causes a small globule of water or mercury, when flattened, to spring back into the spherical form when the compressing foree is removed. ‘Lhe more the globule is compressed, or the greater the curvature at the circumference, the greater will be the resist- ance. Ience, also, the smaller the bubble the greater will be the contractile power of its surfaces, and the more energetically will it assume the spherical form. ‘This is converse of the action of gravity, the tendency of which to produce the globular form will be the greater in proportion to the greater size, and consequently less curvature of the surface. These remarks will enable the reader to comprehend more definitely the nature of the phenomena exhibited in the following paper. J. FIRST SERIES. 1. Liquids, being gifted with an extreme molecular mobility, yield with facility to the action of forces which tend to modify their exterior form. But amongst these forees there is one which predominates so much over the rest that it almost entirely masks their action. This foree is gravity; this it is which czuses liquids to assume the form of vessels which contain them; and it is this, also, which makes smooth and horizontal the portion of their surface which remains free. We can scarcely recognize, along the contour of this free surface, a slight curve which reveals the action of the combined forces of the attraction of the liquid for itself, and of its adherence for the solid matter of the vesscl. Jt is only by observing very small liquid masses, upon which the rela- tive action of gravity is thus weakened, that we can see the influence of other forces upon the figure of these masses manifested in a very forcible manner. ‘Thus the small drops of liquid, placed upon surfaces which they cannot moisten, ‘ WITHDRAWN FROM THE ACTION OF GRAVITY. 209 assume a spherical form more or less perfect. Leaving these minute quantities, if we wish to observe liquid masses which have freely taken a certain form, we must quit the earth, or rather consider the terrestrial globe itself and the other planets as having been primitively fluid, and having adapted their exterior form to the combined action of gravitation and centrifugal force. Theory then indi- cates that these masses ought to take the form of spheroids more or less flattened in the direction of their axis of rotation, and observation confirms these deduc- tions of theory. Observation shows us, also, around Saturn, a body of annular form, and theory finds, in the combined actions of gravity and centrifugal force, means of satisfying the equilibrium of that singular form. If, however, we could, by some means, withdraw from the action of gravity one of the liquid masses upon which we have to operate, at the same time leaving it free to be acted upon by other forces which might tend to modify its form, and if our process allowed of giving to this mass sufficiently large dimen- sions, would it not be very curious to see it take a determinate figure, and to see this figure vary in a thousand ways with the forces on which it depends? Now I have succeeded, by an extremely simple means, in submitting to the above conditions a considerable liquid mass. 2. Fat oils are, it is known, less dense than water, and more dense than aleco- hol. Accordingly, we may make a mixture of water and alcohol having a den- sity precisely equal to that of a given oil—of olive oil, for example. Now, if any quantity of olive oil is introduced into the mixture thus formed, it is evident that the action of gravity upon this mass of oil will be completely annihilated ; for, in virtue of the equality of density, the oil will only hold the place of an equal mass of the ambient liquid. On the other hand, the fat oils do not mix with a liquor composed of alcohol and water. The mass of oil must therefore remain sus- pended and isolated in the midst of the surrounding liquid, and it will be per- fectly free to take the exterior form which the forces that may act upon it will give to it. This being supposed, if the molecular attractions of the oil for itself, those of the alcoholic mixture for itself, and those of this mixture for the oil were identi- cal, there would be no reason that the mass of oil left in the midst of the ambient liquid should take spontaneously one form more than another, since, relatively. to all the forces acting upon it, it would be exactly in the same position as an equal mass of alcoholic nixture whose place it would occupy. But it is evident that this identity between the different attractive forces does not exist, and that the attraction of the oil for itself greatly exceeds the two others. The mass of oil, therefore, ought to obey this excess of its own attractive forces. We thus come to this conclusion, that our mass of oil may be perfectly as- similated to a liquid mass without weight, suspended freely in space, and sub- mitted to its own proper molecular attractions. Now, it is clear that such a mass must take the spherical form. Well, experiment confirms all this in a complete manner. The mass of oil, whatever its volume, remains, in fact, suspended in the midst of the alcoholic liquid, and takes the form of a perfect sphere. 3. In order to obtain this singular result with facility, it is necessary to take certain precautions, which I will describe. The first concern the formation of the alcoholic mixture. The density of this mixture necessarily varies with the kind of oil which is used. For the olive oil which I employed, and for the purity of which I cannot vouch, the proper mixture marked twenty-two degrees on the areometer of Beaumé. If, therefore, any one wishes to use olive oil, he may always consider the above vulue as a first approx- imation, and, by successive attempts, will bring the liquor at length to the exact _ point which it ought to reach. ‘To accomplish this, a test tube is filled with ° the liquor, into which a little oil is afterwards poured by means of’a long-necked funnel, which reaches about half way down the test tube. The oil, on reaching 14s ' soe 910 ‘THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS the liquor, forms a globule, to which a diameter of about two centimetres * must be given, and which a little shake will detach from the mouth of the funnel if it does not detach itself. Then, accordingly as this globule falls to the bottom of the liquor or rises to its surface, we conclude that the quantity of alcohol of the mixture is too great or too small; we therefore add to this a little water or alcohol, taking care to stir it well, and recommence the experiment of the test tube. ‘Ihe same operations are repeated until the globule of oil remains sus- pended in the liquor, without appearing to have a tendency either to fall or rise. The mixture may then be considered as approaching very nearly the desired point. I say very nearly, for the globule of oil of the test tube, being of small dimensions, has more difficulty in moving in the liquor than spheres of a large diameter, and it may seem to be in equilibrium of density with the surrounding liquid, whilst for a larger volume of oil this equilibrium does not exist. 4. When the alcoholic mixture, which I presuppose to be contained in a large glass flask of the ordinary form, has attained this point of approximation, the next thing is to introduce the mass of oil. or this purpose the long-necked funnel which has been mentioned above must be again used, and this must reach to a certain depth in the liquor contained in the flask. Letting the funnel - rest on the neck of the latter, we pour the oil slowly. Then, if the alcoholic mixture is by chance exactly in the requisite proportions, the oil forms, at the extremity of the neck of the funnel, a sphere, the volume of which increases gradually in proportion as we add this last liquid. When the sphere has at- tained the volume we desire, the neck of the funnel is withdrawn with caution; the sphere which adheres to it rises with it toward the surface of the liquor, and the oil which it still contains is added to-the preceding. Lastly, when the sphere has nearly reached the surface of the alcoholic mixture, a little shake detaches it from the funnel. Ordinarily, however, the mixture has not so exactly the desired density. We then see, in general, several successive spheres of oil formed, which, detaching themselves one after another from the mouth of the funnel, fall slowly to the bottom of the flask, or rise to the surface of the alco- holic liquor. In this case all these spheres should, in the first place, be unitea into one, which is easily done by the following means. We introduce into one of them the end of an iron wire. The adherence which the oil contracts with “this metal then allows the sphere in question to be easily conducted in the am- bient liquid, and to be led to join with a second sphere.t By continuing this treatment, we soon succeed in uniting all. Then, according as the whole sphere shall remain at the bottom or on the surface of the liquor, add cautiously to the latter a certain quantity of water or of alcohol; and, after having corked the flask, we next turn it several times slowly, and so as not to disunite the sphere of oil, until the mixture is well effected, which will take place when we no longer perceive any striz in the liquor on looking through it at a window. Lastly, the same operation is to be repeated until the sphere of oil is perfectly in equilibrium in the surrounding liquor. 5. If the experiment has been made, as I have supposed, in a flask of the ordinary form, that is to say cylindrical, the mass of oil does not, however, ap- pear exactly spherical; it is widened in the horizontal direction. But this is only an optical illusion, attributable to the form of the flask. The latter, with the liquor which it contains, acts in the manner of a cylindrical lens whose axis ’ * See table of measures at the end of this volume. tIn order thus to compel two spheres to unite, it does not suffice to put them in contact with one another. They might touch for a long time without mingling into one; one would say that they are enveloped in a resisting pellicule which opposes their union. It is also necessary, therefore, to introduce the extremity of the metallic wire into the second sphere, as if we wished to break the partition which separates the two masses. The union is then effected immediately. I’shall revert to these phenomena hereafter. a i a ie WITHDRAWN FROM THE ACTION OF GRAVITY. 211 would be vertical, and enlarges in appearance the horizontal dimensions of the object. . In order entirely to avoid this illusion, we must use a vessel of plane smooth sides, formed of plates of glass set in a metal frame, (§ 8.) We then have, ina complete manner, the curious spectacle of a considerable mass of liquid present- ing the form of a perfect sphere, and imitating, in some measure, a planet sus- pended in space. ‘ Instead, also, of the above vessel, a glass balloon may be used, which is more imple and less expensive. In this case, indeed, the mass of oil only appears in its real figure when it occupies the centre of the balloon; but the apparent distortion is small, as long as the sphere is not moved considerably from this centre. A vessel of this kind is very convenient for most of the experiments which I shall describe in this part of the memoir; but it would not serve for those which I shall have to make known subsequently? 6. Now, having obtained, by means of the process above detailed, a fine sphere of oil well suspended, and presenting, I will suppose, a diameter of six to seven centimetres, we shall observe the following circumstances, which it is important to notice before we proceed further : in the first place, the equilibrium, previously well established, is soon dis- turbed of itself. At the end of a few minutes we see the sphere quit its place, and rise with extreme slowness towards the upper part of the ambient. liquid. If a little aleohol be then added to restore the equilibrium, on treating the mix- ture by the process of § 4, this equilibrium is again broken in the same manner at the end of a certain time. In fine, it is only by continuing for some days to - maintain it by the successive addition of small quantities of aleohol that we come to obtain a permanent equilibrium, which is then no further: disturbed, except by an accidental cause, of which we shall speak in the following. para- _ graph. If the temperature does not fall below 18° centigr., the above phenomena are the only ones observed; but sometimes, if the temperature remains below that limit, and always, if it is below 15°, another effect is manifested, namely, a diminution in the transparency of the oil. These phenomena are owing to a gradual chemical action which takes place between the oil and the alcoholic mixture. The first of these would be very inconvenient in most of the experiments; but, happily, it may be obvi- ated. This can evidently be effected by employing the two liquids only when they have already exerted upon one another all the action of which they are capable. The oil and the aleoholic mixture which I -used are now inert with regard to one another, because, having been employed a great number of times, they have bad time to exercise the whole of their mutual action. Besides, it is easy, in a short time, to bring the two liquids to that state of relative neu- trality, by agitating them together in order to divide the oil, and thus to aceélerate the action, then separating them by a suitable process. ‘This opera- tion requires some precautions, which we shall examine in § 24, in order not to interrupt the course of the memoir by details which are not now indispensable. In all that follows we shall always suppose that two liquids thus prepared are employed. 7. Another cause disturbs the equilibrium between the sphere of oil and the ambient liquid. his is the variations of temperature, which alter the equality _of the two densities; and the degree of sensibility of such a system in this re- spect would hardly be conceived. For example, when the vessel is carried into a room a little warmer or colder than that in which it had been before, the sphere soon falls in the first case and rises in the second. On the mere appli- cation of the hands to the outside of the vessel, it will be seen, after a few see- . onds, that the sphere begins to fall. We must be continually on our guard against these effects of temperature ; otherwise, they disturb the experiments. The following is a recent instance 212 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS « which oceurred to me. The oil and the alcoholic liquor were enclosed in dif. — ferent flasks, and the latter contained a very slight excess of aleohol. Having, — by chance, carried these two flasks into a room warmer than that in which they — had been, I first introduced into the mixture a certain quantity of oil, which, by reason of the slight excess of alcohol, descended slowly to the bottom of the — flask. A short time afterwards I poured in another quantity of oil, and I was’ © surprised to see this, on the contrary, rise towards the upper part of the mix- ture. The reason of the singular difference was this: the alcoholic mixture inclosed in one of the flasks was very considerable in quantity relatively to the oil which the other contained. Now, at the first moment the liquids, not having sensibly changed their temperature, ntaintained between them the same relation of density ; but after a short time the oil, by reason of its small volume, having become warmer than the alcoholic mixture, had thus become relatively lighter. The warmth of the hand which held the flask in pouring out the oil must have also contributed to the effect in question. 8. Now let us suppose a fine sphere of oil in permanent equilibrium in the surrounding liquid, and let us endeavor to submit it to other forces than its own attractions. The first idea which presents itself is to try the action of centrifugal force. For this purpose it is necessary to impress on the sphere of oil a movement of rotation around one of its diameters, and which is effected by introducing into this sphere a small metallic disc, which is made to turn upon itself by means of an axis which traverses it perpendicularly. ‘This dise carries the oil with it by its adherence, and the whole mass of this liquid takes a movement of rotation. Before explaining the effects which result from this movement, I shall deseribe in detail the apparatus I have employed—an apparatus by the aid of which all the experiments succeeded perfectly and with the greatest facility. It is rep- resented in fig. 1. Fig. 1. The vessel is with plane sides, formed of rectangular plates of glass set in an iron frame; the sides are each 25 centimetres broad and 20 high. The » small dise and its axis are also of iron, a metal whose prolonged contact with oil does not stain it as copper does. The diameter of the dise is about 35 milli- metres, and the axis is formed of an iron wire about 14 millimetre thick. This aR -- WITHDRAWN FROM THE ACTION OF GRAVITY. males axis is fixed by its lower end into a hole pierced in the middle of the plate of glass which forms the bottom of the vessel. This hole is closed below by a | small plate of iron cemented to the glass. The upper end of the axis is screwed ' to a larger wire, which forms the prolongation of it, and which, held with a moderate degree of friction, [a frottement douz,]in apiece of which I shall speak hereafter, receives at its other extremity the handle by means of which the dise is turned. When the whole system is in place the dise ought to be half way up the vessel. ‘The square plate of glass which closes the vessel above is pieced with two openings, each furnished with an iron neck, which is closed with a stopper of the same metal. One of these openings is in the middle of the plate, and its diameter is 55 millimetres. It is through the stopper which closes it that the rod passes, @ frottement doux, which receives on the one side the axis of the disc, and on the other the handle. (See figure 2.) The other \ ‘ , N opening is smaller, and is placed near one of the angles of the plate. It serves for introducing into the vessel either the metallic wire, by the aid of which we unite the partial masses of oil, or additional portions of alcohol, or of mixture at another degree, (§ 9,) &c., when these operations are to be performed without removing the disc from its place. Lastly, this same plate is cemented into an iron frame, which is turned up all round, so as to fit upon a vessel as a lid upon abox. The upper edges of the vessel have been ground with emery all to- -gether, after their being placed in the frame, so that the upper plate of glass fits exactly upon them; and by rubbing these edges and the metallic steppers with a little oil, the vessel, when the plate and stoppers have been placed, may be considered as perfectly closed and keeping the mixture without evaporation of alcohol. In my apparatus the plates of glass are fixed to the metallic framing by a resinous cement, and this is slightly attacked by the alcoholic mixture. It would perhaps be better to use some glazier’s putty; for the alcoholic mixture, being prepared so as not to act any more upon the oil, (§§ 6 and 24,) this latter cement would probably not suffer any alteration. However, the resinous mastie resists to such a degree, that I have been able to leave the alcoholic liquor, without inconvenience, in the vessel for whole months. The apparatus which I have just described is the best suited for obtaining, in all their beauty, the phenomena, which are the objects of these experiments; but, as I have said above, a hollow sphere of glass of pretty large dimensions might be used with less cost, and without too much disadvantage, at least for the experiments treated of in this part of the memoir. This ought to be fur- nished with two tubular openings, one of which would serve for introducing the system of the disc, and the other would effect the same object as the second opening of which we have spoken above. I shall, however, in what follows, suppose all along that the plane-sided ves- _ sel above described is the one employed. : * iD 214 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS : 9. The apparatus being properly arranged, the next thing is to operate so as _ to cause a sphere of oil to surround the dise in such manner that their two centres are sensibly coincident. ‘To attain this point, let us first endeavor, be- fore introducing the dise into the vessel, to bring the centre of the sphere to — remain at the height at which that of the dise should be. It would be extremely difficult to accomplish this by suspending a sphere in a homogeneous alcoholic i mixture, as we have hitherto supposed; for then there is no reason why the — sphere should not stand higher or lower; and, if even by chance it were placed — exactly at the desired height, the movements which would be produced on in- © troducing the disc would very probably change this height. It is, therefore, necessary to employ a more sure. process, and the following succeeded perfectly. We begin by causing the alcoholic mixture to contain a small excess of alcohol. Then, the vessel being furnished with its lid, and the stopper which closes the central opening being lifted up, the mixture is introduced by this opening in such quantity that the vessel be not completely filled. A certain quantity of a mixture, less charged with alcohol, and marking only 16° on the areometer of Beaumé, is then cautiously added. This, from its excess of density, falls to the bottom of the vessel, where it spreads itself in a horizontal layer. The oil is then introduced, which, by reason of the small excess of aleohol contained in the upper mixture, descends through the latter till it rests upon the denser layer of the lower mixture, either in a single mass or in several partial masses (§ 4.) This being so, we unite, if the case requires it, the isolated spheres into a sin- — gle one; then we stir the liquor cautiously with a glass rod, so as to mix im-. perfectly the layer at the bottom with the higher layers, but without dividing — the mass of oil, and the system is then left to rest. It will be seen that there ~ must hence result in the alcoholic liquor a state of density increasing from the — upper layers of less density to the lower of greater density than that of the " oil; and that, in consequence, the mass of oil will necessarily remain in stable — equilibrium with respect to the vertical direction, in a certain layer whose mean ~ density is equal to its own. Now, in performing the operation with the neces- sary precautions—that is to say by stirring the liquid only a very little, then — leaving it to rest to observe the effect which results, again stirring it and leaving — it to rest, and so on; lastly adding, if necessary, a small portion of mixture at — 16°, or of pure alcohol, according to circumstances, we easily succeed in causing the mass of oil to remain exactly at the desired height, and, as we have seen, without tendency to a change of position in the vertical direction.* In geome- trical strictness, truly, this mass of oil cannot then be any longer perfectly — spherical; it must be flattened a little in the vertical direction; but, if we have — operated so that the increase of the densities is very feeble at the height at ~ which the oil stands—and we easily obtain that result by suitable trials—the flattening in question is completely insensible to the eye, and the mass appears — exactly spherical. : a For the experiments which we have to deseribe, the most convenient diameter — to give to the sphere of oil is about 6 centimetres. We easily accomplish this by first forming a less sphere, and adding successively fresh portions’ of oil, © which we unite with the first. The next thing is to place the dise. This being attached by its axis to the © rod which passes through the metallic stopper, (§ 8,) we begin by oiling it as — well as the axis, then introduce it slowly into the alcoholic liquid, and cause it to penetrate by its edge into the sphere of oil. As the dise has previously © been oiled, the sphere envelopes it without difficulty, and, what is remarkable, 2 | * The different liquid layers thus superposed tend of themselves, it is true, to mix; but, as they are placed in the order of their densities, this spontaneous mixture proceeds only with extreme slowness, and it requires a great many days for the liquor to become homogeneous. No inconvenience therefore results from this for the experiments } 4 , WITHDRAWN FROM THE ACTION OF GRAVITY. 215 & gradually of itself. assumes such a position that the axis of the dise traverses it diametrically. This effect is evidently owing to the attractive action of this axis, or rather of the coating of oil with which it has been moistened—an action which tends to operate in a symmetrical manner all around it, and thus brings the entire sphere of oil into a position symmetrical with respect to this same axis. Now it will be seen that the centre of the sphere tending, on the one hand, to remain at the height of that of the disc, on aecount of the super- position of the alcohelic layers of unequal density, and, on the other hand, to place itself in the axis of the disc, on account of the symmetry of the attractive actions exerted by the latter upon the oil, the centre of the sphere and that of the disc will coincide, and will thus remain in a fixed position. Only the sphere will then be slightly elongated in the vertical direction by the attraction of the axis of the disc; but this elongation is very trifling if the sphere present, as we have supposed, a diameter of 6 centimetres. 10. The sphere of oil being thus suitably placed, we slowly turn the handle. We then presently see the sphere flatten at its poles and swell out at its equator, and we thus realize on a small scale an effect which is admitted to have taken place in the planets. However, although the results may be of the same nature in the case of the great planetary masses and in that of our little masses of oil, I must not omit to remark here that there is an essential difference between the forces which are in play in the two cases. In the first, the foree which tends to give to the great planetary mass a spherical figure, and against which the centrifugal force acts, is universal attraction ; in the second, the force which acts the same part with regard to the small mass of oil, is molecular attraction, which is subject to different laws. But as, on either hand, the aggregate of the actions reduces itself to a contest between centrifugal force and another force tending to pre- serve the spherical form of the liquid mass, it appears that the results must be analogous, if not identical, with respect to the figure which that mass assumes. [This, we do not think, is quite correct. The forces which produce the equi- librium of the ring are as follows: First. The centrifugal force which tends to throw the atoms from the centre of motion. Second. The force developed by the external and internal horizontal curvatures, the direction of which is to- wards the centre. Third. The force developed by the external and internal vertical curvatures, one of which acts towards the centre, and the other from the centre. The roundness of the ring is caused by the combined action of the external and internal curvatures, which, under no circumstances of velocity of rotation, would produce a flattened ring —J. H.] In order to observe, in all its beauty, the phenomenon on which we are en- ' gaged, the handle must, at first, be turned with very little velocity—a tum in five or six seconds. The effects are even then very decided. If we after- wards apply a somewhat greater velocity—for example, a turn in four seconds— the flattening at the axis, and the swelling at the equator, are seen to be more considerable, and they are further augmented by increasing the velocity of the handle to one turn in three seconds. Before proceeding further we may remark that, in these experiments, the handle must not be turned too long, for the mass of oil which, in the first moments, presents exactly a figure of revolution, eventually loses this form. At each fresh trial, therefore, the system must be left to repose. ‘The oil then resumes its spherical form, and slowly, of itself, replaces itself in the proper position. ‘The change of form which supervenes when too many turns are given to the disc occasions results of a particular kind, and which are not without interest. I shall speak of them by-and-by, (§ 22.) 11. Now, if instead of moving the handle slowly a considerable velocity is given to it, as two or three turns in a second, new, and very curious, phe- . 216 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS nomena are manifested. The liquid sphere first takes rapidly its maximum Fig. 3. of flattening, then becomes hollow above and below around the axis of rotation, stretching out continually in a horizontal direction, and, finally abandoning the disc, is transformed into a perfectly regular ring, (fig. 3.) . ‘This ring is rounded transversely, and appears to have a circle for its generatrix. At the moment of its form- ation its diameter increases rapidly up to a certain limit; when this is reached the movement of the dise must be stopped. The ring now remains for some seconds in the same state. ‘Then, the resistance of the ambient liquid weakening its movement of rotation, it returns upon itself and changes back into a sphere around the dise and its axis. The velocity of the handle most suitable for producing a beautiful ring, is about three turns per second. The ring thus obtained has a mean diameter of 9 to 10 centimetres. 1 12. Whef, at the instant of the formation of the ring, the mass of oil which constitutes it separates from the disc, a singular circumstance is observable ; the ring remains united to the disc by an extremely thin pellicle or film of oil, which fills all the space between them. But at the instant that, the ring havin reached its greatest extent, we stop the motion of the disc, this pellicle breaks and disappears of itself, and the ring then remains perfectly isolated. It may be conceived that this pellicle is not a circumstance essential to the , phenomenon of the formation of the ring; and we shall see, in another part of these experiments, that it is probably. connected with an order of faets wholly different. 13. The heavens exhibit to us also a body of a form analogous to our liquid ring. I allude to Saturn’s ring. That, indeed, is flattened, whilst the trans- verse contour of ours appears altogether round ; but Ido not think that this dif- ference is so great as it appears at first. In fact, the centrifugal force, which goes on increasing from the inner cir- cumference of the ring of oil up to its outer circumference, necessarily tends to stretch this ring in the direction of its breadth, or, in other words, to flatten it. But the flattening must be of very small amount; for, on account of the in- considerable dimensions of the ring, and the slowness of its angular movement, the kind of traction wHich results from the variation of centrifugal force must be very trifling in comparison with the forces developed by molecular attrae- tion. ; 14. It appears to me, then, that we may reasonably admit that our ring of oil is in reality slightly flattened, and that in consequence it only differs from that of Saturn, with regard to general form, in the less quantity of flattening.* But further, in the system of Saturn, the flattening of the ring is in part deter- mined by the attraction of the central planet. Now, at the first moment of the formation of the ring of oil, the latter is submitted to a particular force, which plays a part analogous to that of the above attraction. In fact, this attraction acts with the greatest intensity At the inner cireumference of Saturn’s ring, and thence decreases rapidly in the rest of this body. Now, at the first moment of the formation of the ring of oil, we have seen (§ 12) that the latter remains united to the dise by a thin film of the same liquid, and we may con- vince ourselves that this film exerts, on the inner circumference of the ring, a considerable force of traction. In fact, if we stop the movement of the disc a little too soon, that is to say a little before the ring has reached its maximum * I leave out of the question here the subdivision of the ring of Saturn. This subdivision, as is known, is not essentially connected with the conditions of equilibrium of the ring. q | ey WITHDRAWN FROM THE ACTION OF GRAVITY. zp of diameter, the film of oil does not break, and the ring then returns upon itself (§ 11) with a much greater rapidity than when the film of oil is broken, and the ring remains isolated. ‘The traction which the film of oil exerts on the imner circumference of the ring ought therefore to produce an effect analogous to that of the attraction of Saturn, that is to say, contribute to increase the flattening. Well, the ring of oil before the rupture of the film presents a very marked flattening. In order to obtain it perfectly, care must be taken that the sphere be well centred in relation to the dise, before beginning the experiment; and it is useful to turn the handle with a velocity somewhat less than that indicated at § 11 ; the most suitable velocity has appeared to me to be about two turns ina second. As soon as the film of. oil breaks the flattening disappears, and the generatrix of the ring becomes, as Wwe have seen, sensibly cireular.* _ 15. Geometricians, who have investigated the figure of equilibrium of a liquid mass in rotation, have only regarded the case in which the attraction which counteracts the centrifugal force is that of universal gravitation, and they have demonstrated that elliptical figures in that case satisfy this equilibrium. Are we thence to conclude that the annular form developed by the rotation of our mass of oil results from the different law which governs molecular attraction, (§ 10,) and that, in the instance of the heavenly bodics, the figure of an iso- lated ring could not be produced by the sole combination of centrifugal force and of the mutual attractions of the different parts of the mass? I am not of that opinion, and I think it, on the contrary, very probable that if calculation could approach the general solution of this great problem, and lead directly to the determination of all the possible figures of equilibrium, the annular figure would be included among them. This general and direct solution presenting very great difficulties, geometricians have contented themselves with trying whether elliptical figures could satisfy the equilibrium, and with proving that they in fact do satisfy it; but they leave the question in doubt, whether other figures would not fulfil the same conditions. In truth, M. Liouville, in his last researches on this subject,t appears at first view to have nearly solved the question, by introducing the consideration of the stability of the figure of equilibrium, and showing that for each value of the moment of rotation, or, in other words, for any initial movement, whatever, of the mass, there is always an elliptical figure, either of revolution or of three unequal axes, according to *T had thought that it would be possible to obtain rings isolated and greatly flattened by operating upon larger masses of oil, for then, the ring having a larger volume, the influence of the molecular attraction should be less. But I have found that, in operating on larger masses, it was necessary, in order to obtain the ring in a regular manner, to employ a more feeble velocity of rotation, so that, if the influence of the molecular attraction was diminished, that of the centrifugal force was so equally. The flattening, then, did not become more sensi- ble; or, if I have sometimes imagined that I observed any, I have not been able to reproduce it at will. I have operated thus on spheres which were, successively, about 10, 11, 12, and 14 centimetres in diameter, with discs of a diameter of from seven to nine centimetres, and in a vessel with plane surfaces, having a bottom 35 centimetres square, and a depth of 25 centi- metres. The effects, however, thus obtained re very beautiful. The rings are magnificent; present a considerable diameter, and remain souci.nes for eight to ten seconds before return- ing on themselves. With a sphere of ten centimetres diameter, a disc of seven, and a velocity a little less than one turn of the dise per second, we obtain, in a very beautiful and very marked manner, the flattening resulting from the traction of the film of oil. These experiments, however, are inconvenient and difficult, on account of the large dimen- sions of the vessel, and the great quantity of alcoholic liquid necessary to fill it. It may be conceived, moreover, why a larger mass of oil requires a less velocity of rotation to produce a regular ring. It is precisely because the molecular attraction has less influence; whence, it resuits that, if we attempt to employ the same velocity of rotation which would give a beautiful ring with a less quantity of oil, the mass disunites, and is scattered into spherules. + The memoir of M. Liouville was communicated to the Academy of Sciences in the sitting of the 13th of February in this year. An analysis of it may be found in the Journal L’In- stitut, No. 477. 218 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS the cireumstances, which constitutes a form of stable equilibrium. It appears, — in effect, natural to admit that, for a given disturbance of a liquid mass, there is _ but one single final state admissible; and, in this case, this state must necessa- — rily possess stability. However, I do not deem the conclusion which may be drawn from these results so general as it appears at first sight. Without doubt, — for a primitive disturbance given, there is only one final state possible, and that — state must be stable. But the condition of stability of a found figure of equi- — librium does not necessarily involve the consequence that this figure will con stitute the final state in question, for it may happen that several figures of equi- librium, corresponding to the same primitive disturbance, might equally possess stability, and that the choice of the mass for one of these figures may have been — determined by other circumstances; for example, by the modifications which — its movement experiences in the first moments of rotation. In fact, it is by © examining these modifications, to which the attention of geometricians has not — been directed, that I shall attempt to arrive at the mode of generation of annular ~ figures. 16. When the mass begins to revolve upon itself, the angular velocity of the portions remote from the axis, which are carried off by their centrifugal foree, necessarily goes on diminishing. This diminution is esvecially apparent on the equator of the mass, and it is the more considerable in proportion as the initial movement of rotation was more rapid. It thence results that, in the first instants of a sufficiently rapid rotation, there will bea great difference of angular 4 velocity between the portions which are near the axis and those which are near the equator. Nevertheless, if we admit for a moment that, in virtue of the adherence of the liquid for itself, and of the friction of its several parts, the portions which turn most rapidly communicate by degrees a part of their ve- locity to the others, so that in the end the result is a mean angular velocity, corresponding to the same moment of rotation, and equal in all the points of the mass, this may take an ellipsoidal figure. But long before the feeble forces, of which we have just spoken, can bring about this mean result, another order of phenomena would be manifested, which may impede the development of the elliptical figure and give rise to an annular form. . In fact, it follows necessarily from the preceding considerations that, in the first instants of a rotation sufficiently rapid, the centrifugal force at the equator of the mass will be much less than that which would correspond to the above mean velocity ; and that, on the other hand, the centrifugal force of the portions near the axis will be by much superior to that which would correspond to the same mcan velocity. ‘The liquid next the axis will, therefore, be driven towards the liquid of the equator, whence there will necessarily result the formation of a sort of circular cushion, (dowrrelet,) more or less marked. In other words, — the mass will soon become hollow in the middle, and will swell out all around. Now as soon as this phenomenon takes place, it will be conceived that the at- traction exerted by this bourre/et on the liquid remaining around the axis must _ be an addition to the action of the centrifugal force, and contribute to increase — the volume of the bourrelet at the expense of the central liquid. Hence, there- fore, it may evidently result that all the liquid will leave the axis for the bour- relet, and the latter become in a manner a veritable ring. This generation of the annular figures would therefore be independent of the law which the attraction follows, and would be, in consequence, the same in the ease of universal attraction and in that of molecular attraction. 17. It is easy to verify this mode of generation upon our mass of oil, or at least to assure ourselves that during the formation of the dourrelet and of the ring, the angular velocity is much less at the equator of the mass than towards the axis. For this purpose I shall first point’ out that when a certain number of experiments have been performed upon the same mass of oil, and this has been several times disunited and reformed into a single sphere and into a ring, te a * = a —— jee - WITHDRAWN FROM THE ACTION OF GRAVITY. 219 it always holds within it a multitude of small bubbles of alcoholic liquor, which borne along by the oil that surrounds them, render the movements of the differ- ent points of the mass perfectly observable. Now, if the experiments which we have described be repeated with the aid of a sphere of oil thus filled with alcoholic bubbles, the following results are observed. So long as we give to the disc such slight velocities only as are sufficient to produce a simple flatten- ing, there is not a great difference of angular velocity between the portions next to the axis and the portions adjoining the equator; but this difference becomes very considerable when the dise turns more rapidly, and the bourrelet and the ring are developed. ' We may thus prove, by means of the small alcoholic bubbles, that the mean angular velocity is established in the ring once formed, and that all the points of the latter perform their revolutions in the same time. Furthermore, in our experiments upon the masses of oil, there are two foreign fotces which act, in addition to the causes which we have noticed, to facilitate the development of the dourrelet and of the ring. One is the resistance of the ambient liquid, which contributes to weaken the angular velocity of the equa- tor of the mass; the other is the action of the hand which keeps up the motion of rotation of the disc, and consequently hinders the central portions of the mass from participating gradually in the slackening of the’equatorial portions. But that which is produced by these two foreign forces would be equally pro-_ duced by a greater initial velocity of rotation if we could annul them. 18. When, by the aid of a moderate velocity of the disc, we limit ourselves to producing the flattening of the mass, the two foreign forces of which we have just spoken necessarily hinder the latter from attaining an angular velocity equal in all its points, even though we keep turning the disc. The result is, that the mass cannot take exactly the figure which would correspond to that equality of angular velocity. ‘That which it adopts is a figure of revolution; but on placing the eye at the height of the centre of the mass, it is easily recog- nized that it is not an ellipsoid. The curvature at the equator is too small, and this is the more evident in proportion as the flattening is more consider- able. Now, is this difference between the figure thus produced and that which would correspond to the case of universal gravitation solely the result of the action of the two foreign forces in question, or is it in part caused by the difference of the laws which the two kinds of attraction follow? In other words, if we could _ eliminate or render insensible the differences of angular velocity of the several _ parts of the mass of oil, would the figure produced be an ellipsoid or not? Now, we should render these differences of angular velocity insensible if we could impress a movement of rotation on a mass of oil suspended in an isolated man- ner, without interior system, in the alcoholic liquid, and then leave it to itself. In this case the resistance of the ambient liquid would be exercised, indeed, on the exterior of the mass; but nothing maintaining the constancy of velocity of the central parts, these, by virtue of the strong self-adherence of the oil, would participate eventually in the slackening of the exterior portions, and we might consider the mass as having each instant an angular velocity equal throughout. Now, it is very easy to realize the above by availing ourselves of the fact that, when the ring of oil is formed, it returns, after some time, upon itself, (§ 11.) _ At the instant when the ring is well developed, and when we have just stopped the disc, we lift the latter cautiously by means of the metallic stopper which bears its axis. Then the mass of oil, which is again formed by the return of the ring upon itself, continues still to regolve for some time, completely isolated the ambient liquid. Its figure is then, as well as the eye can judge of it, a perfect ellipsoid of revolution, which gradually approximates to a sphere in 220 THE FIGURES OF EQUILIBRIUM OF A LIQUID’ MASS proportion as the rotatory motion becomes weaker.* ‘Thus, the difference of the laws which govern the two sorts of attraction appears not to influence the nature of the figure taken by the mass that turns upon itself. é 19. A liquid mass can only assume and preserve an annular form under the influence of a sufficient centrifugal force. ‘Thus, as we have seen, when the resistance of the alcoholic liquid-has diminished below a certain limit the velocity of rotation of the ring of oil, the latter, obeying the preponderating action of the molecular attraction, returns upon itself, loses its annular form, and reconstitutes itself into an entire mass, first ellipsoidal and then spherical. But if, by a method which I shall describe, we prevent the ring from agglomerating thus, and still leave the action of its centrifugal force to diminish, we then witness the appearance of other phenomena well meriting interest. In order to produce them perfectly, in place of the dise of 35 millimetres, a dise of about 5 centime * T had expected to be able to obtain a revolving isolated mass by means of another process, viz: by forming a splexre of oil in the middle of a cylindrical flask so arranged as to be able to turn upon its axis; then causing this flask thus to turn with rapidity, until all the liquid within, aleoholic mixture and mass of oil, had taken the same motion; then suddenly stop- ping the flask. In effect, it seems that then the alcoholic liquor being the first to lose its rotatory motion by the friction against the stationary sides of the flask, a moment must occur when the mass of oil maintains an excess of angular velocity over the ambient liquid, and that then the effects of centrifugal force upon that mass may manifest themselves. But the experiment gives few results. First, it is extremely difficult to keep a mass of oil in the middle of the flask. We keep it tolerably in the axis of the latter, because, if we have suc- ceeded in placing it so that its centre is little removed from that axis, the rotation of the am- bient liquid brings it there, and then retains it there very well. But it is not the same in the direction of the height of the flask. If a homogeneous alcoholic mixture be employed, and the sphere of oil is placed, before turning the flask, a little higher or lower than-the middle of the height of the latter, it quits its place when the flask turns to ascend, in the first case, or to descend, in the second, until it comes to be dispersed against one of the two bases of the flask. This effect is attributable, I think, to the fact that the two bases exercising upon the sections of liquid which touch them a motive action much greater than that to which the parallel sections of the interior of the mass are subjected, there ensues near these bases, at the commencement of the rotation, an excess of centrifugal force which determines a ten- dency upwards and downwards of the liquid near the axis. It is therefore necessary to en- deavor to place the sphere of oil in a position very near to the middle of the height of the , vessel. Unfortunately we cannot use for this purpose the process of superposition of the al- coholic layers of unequal density, (§ 9;) for then, in the rotation of the flask, the denser in- ferior layers come necessarily, by the excess of centrifugal force which results from their ex- cess of density, to rise against the sides, causing the less dense liquid to occupy the axis; and in this movement the mass of oil is drawn downwards, and is also dispersed upon the bottom of the vessel. By employing a homogeneous alcoholic mixture and a sphere of oil of only about three centimetres diameter, I however succeeded several times, by dint of patience, in giving to this sphere a sufficiently exact position in the flask to be able to keep it at the same height ’ until it had itself taken the rotatory movement of the whole system. But then, when I stopped the flask, a violent internal agitation was produced, which almost always dispersed the oil in innumerable spherules throughout the alcoholic liquid, or at least destroyed its form in a completely irregular manner. I attribute these effects to the following cause. When the flask is stopped, the portions of the alcoholic liquid which touch the sides and bases, losing first their centrifugal force, the more internal portions, which still retain theirs, make their way through them, dividing them, and this confusion is soon propagated to the axis, where it gives rise either to the dispersion or to the irregular disfiguring of the mass of oil. In the cases in which I have been able to give a suitable position to the sphere of oil, I ‘have observed a curious effect; namely, that in the first instance of the rotation of the vessel the mass of oil quits the spherical form, and becomes elongated in the direction of the axis of rotation. This elongation is easy explained: the movement of rotation is communicated to the portions of the mixture which are nearest the axis above and below the mass of oil, before being able to communicate itself with the same intensity to the latter: hence, in the different points of this mass, there must result a less centrifugal force than in the points of the alcoholic mixture situated at the same distances from the axis of rotation. Thence a rush of the oil to the axis, and an elongation of the mass of the latter in the direction of this same axis. But, on continuing the rotation, the 4l comes to receive the same movement as the surrounding liquid, and it also resumes gradually the spherical form. On stopping the flask, not suddenly, but in a rather rapid manner, I succeeded once in obtaining a result sufficiently regular, and I observed, as I expected, the sphere become flat- tened considerably in the direction of the axis of rotation. , t WITHDRAWN FROM THE ACTION OF GRAVITY. 224 tres was substituted *, which renders necessary, in order to form the ring well, a less velocity of rotation than with the preceding disc, (the most suitable ap- pears to me to be a little less than two turns in a second.) Now, instead of stopping the movement of the disc at the instant when the ring has attained its greatest development, we must continue to move the handle. The film of oil will then break in a little time, as if the dise had been stopped; but, the latter continuing to revolve in the alcoholic liquor, the portions of that liquor which are in contact with it will themselves assume a rotatory movement, and the centrifugal foree which results from it will drive them continually towards the ring, so that the latter'will not be able to return upon itself. Now, ia these circumstances, we soon see the ring lose its regularity, then divide into several isolated masses, each of which immediately takes the spherical form. Thus the ring, when it cannot preserve its figure on account of the decrease of its cen- trifugal force, and an obstacle prevents its reforming itself into a single sphere, resolved itself into several isolated spheres. As soon as the separation begins to take place, the movement of the dise must be stopped. This is not all: one or more of these spheres are then almost always seen to assume, at the instant of their formation, a movement of rotation upon them- selves—a movement which constantly takes place in the same direction as that of the ring. Moreover, as the ring, at the instant of its rupture, had still a re- mainder of velocity, the spheres to which it has given birth. tend to’fly off at a tangent; but as, on the other side, the disc, turning in the alcoholic liquor, has impressed on this a movement of rotation, the spheres are especially carried along by this last movement, and revolve for some time around the dise. Those which revolve at the same time upon themselves consequently then present the curious spectacle of planets revolving at the same time on themselves and in their orbit. The movement of rotation of these masses is, however, too slow, in relation to their diameter, to cause any sensible flattening. Finally, another very curious effect is also manifested in these circumstances. Besides three or four large spheres into which the ring resolves itself, there are almost always produced one or two very small ones, which may thus be compared to satellites. The experiment which we have just described, presents, as we see, an image in miniature of the formation of the planets, according te the hypothesis of Laplace, by the rupture of the cosmical rings attributable to the condensation of the solar atmosphere. 20. When some oil is introduced into a mixture containing a little excess of alcohol, a phenomenon is observable, which is connected with that of the reso- lution of the ring into isolated spheres. If the oil be poured in with sufficient rapidity it forms a long cylindrical train, extending from the beak of the funnel to the bottom of the vessel, where the mass gathers. Now, this kind of tail, which connects the mass of oil with the beak of the funnel, remains as long as the oil which forms it has a sufficiently rapid movement of translation—that is to say, as long as we continue to pour; bunt, as soon as we cease to pour out, and the movement of translation is slackened, the train of oil is instantly re- solved into several isolated spherules. 21. The formation of a ring analogous to that of Saturn naturally inspires the desire to carry further the resemblance to the system of that planet, and to seek, whether, by some modification of our experiment, it would not be possible to contrive so that a sphere of oil should remain in the middle of thering. Now, I have succeeded in producing this effect, by means of a process which I shall proceed to describe; only that this experiment must be regarded merely as a scien- tific sport, for the circumstances which give rise to the result have evidently no anal- ogy with those which can have occasioned the configuration of the system of Saturn. * This substitution is accomplished by detaching the upper end of the axis of the first dise from the large wire which passes through the metallic stopper (§ 8,) and screwing in its place the end of the axis of the new disc. 222 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS It is first necessary to be able to give to the dise a considerable velocity of — rotation. ‘To do this, we adapt to the upper part of the vessel a system of two pulleys—one small, and fixed on to the prolongation of the axis of the dise at — the place of the handle, which is taken away; the other larger, and to the axis of which the same handle is attached. In my apparatus the diameters of the two pulleys are, respectively, 12 and 75 millimetres. In the second place, the diameter of the sphere being always nearly six centimetres, that of the dise © should be only two centimetres. Lastly, the dise should not have, as in the preceeding experiments, its centre coinciding with that of thesphere. It should be placed lower, toward the inferior part of the latter. Matters being thus arranged, the handle is turned with a velocity which ex- perience soon enables us to determine. In my apparatus this velocity ought to be about two turns and a half per second, which nearly corresponds to fifteen turns of the dise in the same time. We then see, in general, a ring rapidly formed, which extends itself, leaving in its centre a mass of oil, to which it remains united by a thin pellicle. At the instant when the ring has attained a sufficient development, (and by habit alone can this be correctly learned,) the rotation is suddenly stopped. The pellicle then breaks, the ring remains completely iso- lated, and the central mass forms into a sphere. We have thus, during some instants, a curious representation of the system of Saturn, except the flattening of the ring. The ring returns rapidly, afterwards, upon itself, and is again — united to the central sphere. This experiment does not offer any great diff- culties. It requires, however, some skill to succeed perfectly.* 4 22. In describing (§ 10) the experiment in which the flattening of the sphere is — effected by the immediate action of the dise, I have remarked that the movement’ — of the latter should not be continued too long, because the mass of oil then — comes to lose its form. Now, if we continue, nevertheless, to turn the handle, with a view to observe the results of this disfigurement, we see manifested new and very capricious effects. : p The sphere being well centred with relation to the disc, if we give velocities of one turn in six, five or four seconds to the latter, we begin, after seven or — eight turns, to see the mass of oil elongate itself horizontally in one direction, taking a form which*resembles much an ellipsoid of three axes; and, what is more singular, this kind of ellipsoid is placed in an eccentric manner with rela- tion to the axis of rotation. Figure 4 represents, for a velocity of a turn in. Fig. 4. i four seconds, the mass viewed from three different sides; that is to say, from above and in the two lateral directions of the smallest and of the largest hori- zontal axis: the dotted parts indicate the positions of the dise and of the axis of rotation. The aspect of the mass seen fromabove shows thatitis slightly bentin one direction; but this effect is evidently owing to the resistance of the ambient liquid. When once the mass has taken this form, it preserves it indefinitely as long as the movement of the dise continues; it continues to revolve eccentrically * On communicating this very experiment to the academy, in the sitting of April, 1842, (see the Bulletins, ) I stated that it was necessary to vary the velocity of rotation. I have since found that, having adopted a convenient velocity, it was best to keep it uniform, vel id . | 7 / Ni } WITHDRAWN FROM THE ACTION OF GRAVITY. 220 round the latter, and with a velocity much less than that of this dise. This inferior velocity, I may add, evidently also proceeds from the resistance of the ambient liquid. If a greater velocity is given to the disc without, however, passing a certain limit—if, for example, we give it one turn in three seconds, the phenomena are still of the same kind; only the mass is more elongated, the flexure due to the resistance of the ambient liquid is more decided, and the Fie. 5 form is more removed from an ellipsoid. Figure 5repre- % ~~ | sents the mass viewed on the side, and showing to the eye i its greatest length. If the velocity of the disc is increased to a turn in two seconds, the phenomena become less constant and less y regular. We should say that there is, for this velocity, a } transition from one order of phenomena to another, and that the mass hesitates between the two. In fact, with a velocity still alittle greater, namely, about one turn in a second and a half, the phenomena begin again to be regular and constant, but they are different from the first. ‘They are exhibited in all their beauty when the velocity is increased to a turn ina second. ‘The mass then is at first deeply hollowed around the axis, as if the ring was on the point of being developed ; and it re- mains under this form of a circular bourrelet during sixteen to eighteen turns of ‘the disc; we then see it elongate gradually according to a horizontal diameter, but no longer eccentrically, so that; seen from above, it presents an elliptic figure sometimes very perfect, of which the disc occupies the centre, (fig. 6.) ‘This ellipse then lengthens more and more, rather rapidly, and begins to bend Fig. 6. Fig. 7. by the resistance of the ambient liquid, (fig. 7.) Lastly, on a sudden the mass becomes strongly inflected from both sides, and its form Fie. 8 seen from above is then as represented in fig. 8. The ee mass afterwards preserves this last form in a perfectly fixed manner, as long as the movement of the dise con- tinues. ; 23. However capricious these phenomena may appear, chance, or accidental causes, have still no part in them. I have repeated a great number of times the experiments detailed above, and the effects have aways been identically the same for the same velocities. After having seen the stable figures which the mass takes in these cireum- stances, we cannot help making a comparison between these figures and the ellipsoids of three axes of MM. Jacobi and Liouville, (§15,)—ellipsoids which are also always, as the latter of these geometricians has shown, figures of stable equilibrium. Would the identity of the phenomena in the case of universal éravitation and in that of molecular attraction hold good so far? Doubtless the singular figures which we have just described are not ellipsoids ; but their aspect admits of our attributing the difference to the resistance of the ambient liquid, which on one side determines the flexures of which we have spoken, and on the other maintains a permanent inequality of angular velocity between the portions adjoining the disc and the more distant portions. Calculation alone could inform us up to what point the above comparison is well founded; the complete solution of the problem, for the case of molecular attraction, would per- haps not present difficulties so insurmountable as for that of universal attraction. { ) 2 224 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS 24. In all the experiments which I have described in this mémoir, I have supposed that the oil and the alcoholic mixture were rendered chemically inert with regard to each other, and I have said (§ 6) that it was easy in a short space of time to obtain two such liquids. I proceed now to detail the process by means of which this object is attained. We begin by making a mixture of alcohol and distilled water, containing a certain excess of alcohol, so that when submitted to the trial of the test tube (§ 3) it lets the small sphere of oil fall to the bottom rather rapidly. After having formed the mixture in quantity more than sufficient to fill the vessel which is to serve for the experiments, we introduce into this same mixturea quantity of oil about double what is considered necessary for these experi- ments.* Ifa flask is not at hand large enough to contain the whole, we divide the masses among several separate flasks: but care must then be taken that each one may contain the same proportions of water, alcohol, and oil. After this we invert these flasks rapidly a great number of times, but without shaking them, until the oil has been divided into spherules of the size of a pin’s head ; the whole is then left to rest. Then if the alcohol of the mixture is in proper quantity, the spherules should sink with extreme slowness, so as to take about a quarter of an hour for the greater part to collect at the bottom of the flasks. If it is otherwise, water or alcohol is to be added, as may be required; the con- tents to be mixed by inverting the flasks several times, as above, then left again to settle, and the operation thus to be recommenced until the result is obtained which I have described. When this point is obtained the whole is thrown upon filters, care being taken to cover the funnels containing these. last with plates of glass. This precaution is necessary in order to prevent, as much as possible, the evaporation of the alcohol, and for another reason, of which we shall speak hereafter. 'The alcoholic liquor passes the first through the filters, ordinarily carrying with it a certain number of very minute spherules of oil. When the greater part has thus passed, the spherules become more numerous. What still remains in the first filters, namely, the oil, anda residue of alcoholic liquor, is then thrown into a single filter placed on a new flask. This last filtration takes place much more slowly than the first, on account of the viscosity of the oil. It is considerably accelerated by renewing the filter once or twive during the operation. If the funnel has been covered with suffi- cient care the oil will collect into a single mass at the bottom of the flask, under a layer of alcoholic liquor. The preceding operations have thus given us the following results: On the one hand, the inert alcoholic mixture, still holding a small, excess of alcohol, and containing a certain number of small spherules of oil; on the other hand, the oil equally inert, and covered with a little of this same aleoholic liquid. Now, a second filtration completely clears the first from the spherules which it holds. With respect to the oil, it is extracted from below the alcoholic layer by means of a small siphon, armed with a lateral tube, and received into a dry flask, which is to be perfectly corked. In this manner we have the two liquids separate and inactive, with regard to each other. .When it is desired to use them, if we perceive that the alcoholic liquid is a little too dense, we correct it with pure alcohol; and if, on the contrary, there is too little density, we correct it with alcohol at 16 degrees. In this latter case we must not use pure waters because this, when it mixes with the prepared alcoholic liquor, produces in it a cloudiness more or less decided. The various trials I have made relatively to the above process, have led me to ascertain that the two liquids, when they have not been submitted to this preparation, are both modified by their mutual contact. The alcoholic liquid “ It is indispensable to have the two liquids thus in excess, on account of the quantities which are necessarily lost during the different operations which we shall describe, and in the preparation of the experiments. ne pee oer Seen eae ee # WITHDRAWN FROM THE ACTION OF GRAVITY. 225 |} dissolves some oil, and this in its turn probably dissolves someyalevhol. It is | especially from the modification which the oil undergoes that its great diminu- ~ tion of relative density results, (§ 6.) Now, when the oil thus modified remains | exposed to the air, it passes again gradually to the state of fresh oil, and resumes | its former density. It is partly to avoid this that [ have recommended the fun- nels which enclose the filters to be kept constantly covered, and the oil to be kept in a flask perfectly corked. As for the alcoholic mixture, it is evident that this last. precaution is equally necessary. - 25. Before I conclude, I must forewarn those persons who may wish to repeat my experiments of two effects which sometimes occur, and which cause disturb- -ance in the operations if the experimenter does not know the means of pre- venting or destroying them. When some oil is introduced into a mixture containing an excess of alcohol, it happens sometimes that the mass which has sunk to the bottom of the vessel contracts adherence with this bottom and spreads itself out more or less on its surface. There is then no means of removing it entire; but the spreading of the adhesion may be prevented by contriving that the bottom of the vessel should be occupied by a layer of a mixture more dense than the oil, (§ 9.) The second effect to which [ allude is presented in the inverse case—that is | to say, when the sphere of oil, instead of reaching the bottom of the vessel, rises, _ on the contrary, to the surface of the alcoholic liquor, either because this liquor | contains too little alcohol, or on account of a lowering of temperature, or because | we have not been able to use prepared oil. When this happens the mass flat- tens at first, more or less, at the surface of the mixture, as it this last opposed ‘aresistance to it. Then, after some time, it makes its way through, and then pre- _ sents a portion of plane surface, more or less extended, on the level with that of the _aleoholic liquor. But what occasions trouble is, that then, so to speak, it has - contracted an adherence with this same surface, from which it is not detached _ without great difficulty. It is, at first, easy to prevent the production of this effect by pouring on the surface of the liquor a small layer of pure alcohol; and this same means will serve also to destroy the effect in question, if it is already produced. In this latter case we may again invert the vessel with caution. The movement thus imparted to the ambient liquor suflices, ordinarily, to detach the mass of oil, with the exception of a small portion, which almost always re- mains adhering to the surface. t 26. Lastly, I have already mentioned the fact that, after a certain number of experiments, the oil becomes filled with small spherules of alcoholic liquor. Now, reciprocally, the ambient alcoholic liquor is also often’ sprinkled with a multitude of small spherules of oil. It is scarcely necessary to remark that, when all these spherules have become too numerous, and we desire to restore the liquids to their original transparency, this is easily accomplished by filtra- tions similar to those of which I have spoken above, (§ 24.) 27. We have been hitherto engaged with the figures assumed by a liquid mass abstracted from the action of gravity and submitted to the attraction of its molecules, either when this mass is at rest, or when a movement of rotation upon itself is imparted to it. Notwithstanding the difference of the laws which the attractive forces follow in this case and in that of the large planetary masses, we have seen produced, on a small scale, a striking representation of the _ majority of the phenomena of configuration relative to the celestial bodies. In _ the second part of this investigation we shall submit our liquid masses to new forces, and we shall then see developed a series of phenomena quite as curious _ but of a different class. dents ain, Sek Ag « ¥ > “ _ Nore.—Professor Faraday, who has repeated many of M. Plateau’s remarkable and beau- _ tiful experiments, coloured his oil green, for the purpose of rendering it more distinctly visible _in‘the spirit, by dissolving in it a little oxide of copper. This, he states, is easily done by _ heating a little oil with the oxide, and then mingling that with the rest. a 15s % : 996 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS SECOND SERIES. PREFACE. AT the period when attacked by the disease which has entirely deprived me of sight, I had terminated the greater part of the experiments relating to this series, as well as the following. M. Duprez, correspondent of the Brussels Academy, and M. Donny, had the kindness to undertake those which were still wanting. I constantly directed their execution; nearly all were made in my presence, and I followed all the details. I shave therefore considered myself justified, in order to simplify the description, in expressing myself in the course of. this investigation as if I had made the experiments. With respect to the theoretical portions, I am indebted to the able assistance of one of my colleagues, M. Lamar!e, who has most kindly devoted many long hours to listening to the details of my investigations, and to aiding me in the explanation of several difficult points, I am also indebted to another of my colleagues, M. Manderlier, for the execution of a part of the caleulations. May I be permitted to express in this place my gratitude to these devoted friends? Thanks to their generous help, science is still an open field for me: notwithstanding the infirmity with which I am afilicted, I am able to put in order the materials I have collected, and even to undertake fresh researches. ; in . Preliminary considerations and theoretical principles. General condition to be satisfied by the free surface of a liquid mass withdrawn from the action of gravity, and in a state of equilibrium. Liquid sphere. 1. The process described in the previous memoir enabled us to destroy the action of gravity upon a liquid mass of considerable volume, leaving the mass completely at liberty to assume the figure assigned to it by the other forces to which it is subject. This process consists essentially in introducing a mass of oil into a mixture of water and alcohol, the density of which is exactly equal to that of the oil employed. The mass thengremains suspended in the sur- rounding liquid, and behaves as if withdrawn from gravity. By this means we have studied a series of phenomena of configuration, dependent either simply upon the proper molecular attraction of the mass, or upon the combination of this foree with the centrifugal force. We shall now abandon the latter force, and introduce another of a different kind, the molecular. attraction exerted be- tween liquids and solids; in other words, we shall cause the liquid mass to adhere to solid systems, and study the various forms assumed under these cir- cumstances by those portions of the surface which remain free. In this way we shall have the curious spectacle presented by the figures of equilibrium ap- pertaining to a liquid mass, absolutely devoid of gravity and adherent to a given solid system. But the figures which we shall obtain present another kind of interest. The free portions of their surface belong, as we shall show, to more extended figures, which may be conceived by the imagination, and which, in the same condition of total absence of gravity, would belong to a perfectly free liquid mass; thus our processes will partially realize the figures of equilibrium of a mass of this kind. ‘Phe latter are far from being confined to the sphere; but among them the sphere alone is capable of being completely formed, the others presenting either infinite dimensions in certain directions, or other peculiarities which we shall point out, and which equally render their realization in the complete. state impossible. Moreover, the results at which we shall arrive will constitute so many new and unexpected confirmations of the theory of the pressures exerted by liquids upon themselves in virtue of the mutual attraction of their molecules, a theory” upon which the explanation of the phenomena of capillarity is based. Lastly, in our liquid figures we shall discover remarkable properties, which. will lead us to some important applications. Ere LL ee eS Ll ae he eae: ow See. WITHDRAWN FROM THE-ACTION OF GRAVITY. 227 2. In order to guide us in our experiments, and also to enable us to com- prehend their bearing, we shall first consider the question in a purely theoretic point of view. The action of gravity being eliminated and the liquid mass being at rest, the only forces upon which the figure of equilibrium will depend will be the molecular attraction of the liquid for itself, and that exerted between the liquid and the solid system to which we cause it to adhere. The action of the latter force ceases at an excessively minute distance from the solid ; hence, in regard to any point of the surface of the liquid situated at a sensible distance from the solid, we have only to consider the first of the two above forces, 2. e., the molecular attraction of the liquid for itself. The general effect of the adhesive force exerted between the liquid and the solid is to oblige the surface of the former to pass certain lines; for instance, if a liquid mass of suitable volume be caused to adhere to an elliptic plate, the surface of the mass will pass the elliptic outline of the plate. At every point of this surface, situated ‘at a sensible distance from this margin, the molecular attraction of the liquid for itself alone is in action. Let us now examine into the fundamental condition which all points of the -free surface of the mass must satisfy, in virtue of the latter force. The determination of this condition and its analytical expression are com- prised in the beautiful theories upon which the explanation of the phenomena of capillarity is based, although geometricians have not specially studied the problem of the figure of a liquid mass void of gravity adherent to a given solid system. We shall, therefore, now resume the principles and the results of the theories in question, at least those which relate directly to our subject. 3. Within the interior of a liquid mass, at any notable distance from its sur- face, each molecule is equally attracted in every direction; but this is not the case at or very near the surface. In fact, let us consider a molecule situated at a distance from the surface less than the radius of the sphere of sensible activity of the molecular attraction, and let us imagine this molecule to be the centre of a small sphere having this same radius. It is evident that one por- tion of this sphere being outside the liquid, the central molecule is no longer equally attracted in every direction, and that a preponderating attraction is directed towards the interior of the mass. If we now imagine a rectilinear canal, the diameter of which is very minute, to exist in the liquid, commencing at some point of the surface in a direction perpendicular to the latter, and ex- tending to a depth equal to the above radius of activity, the molecules con- tained in this minute canal, in accordance with what we have stated, will be attracted towards the interior of the mass, and the sum of all these actions» will constitute a pressure in the same direction. Now, the intensity of this pressure depends upon the curves of the surface at that point at which the minute canal commences. In fact, let us first suppose the surface to be concave, and let us pass a tangent plane through the point in question. All the molecules situated externally to this plane, and which are sufficiently near the minute canal for the latter to penetrate within their sphere of activity, will evidently attract the line of molecules which it contains from the interior towards the exterior of the mass. If, therefore, we suppressed that portion of the liquid situated ex- ternally to the plane, the pressure exerted by the line would be augmented. Hence it follows that the pressure corresponding to a concave surface is less than that which corresponds to a plane surface, and we may conceive that it will be less in proportion as the concavity is more marked. If the surface is convex, the pressure is, on the contrary, greater than when the surface is plane. To render this evident, let us again draw a tangent plane at that point at which the line of molecules commences, and let us imagine for a moment that the space included between the convex surface and this plane is filled with liquid. Let us then consider a molecule, m, of this space sufficiently near, and from this point let fall a perpendicular upon the minute canal. The 228 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS action of the molecule m upon the portion of the line comprised between the base of the perpendicular and the surface will attract this portion towards the interior of the mass. If afterwards we take a portion of the line equal to the former from the other side of the perpendicular, and commencing at the base of the latter, the action of the molecule m upon this second portion will be equal and opposite to that. which it exerted upon the first; so that these two portions conjointly would neither be attracted towards the interior nor the exterior of the mass; if beyond these two same portions another part of the line is com- prised within the sphere of activity of m, this part will evidently be attracted towards the exterior. The definitive action of m upon the line will then be in the latter direction. Hence it follows that all the molecules of the space com- prised between the surface and the tangent plane which are sufficiently near the line to exert an effective action upon it, will attract it towards the exterior of the mass. If, then, we suppress this portion of the liquid so as to reproduce. . the convex surface, the result will be an augmentation of the pressure on the part of the line. Thus the pressure corresponding to a convex surface is greater than that corresponding to a plane surface, and its amount will evidently be greater in proportion as the convexity is more marked. 4. If the surface has a spherical curvature, it may be demonstrated that, rep- resenting the pressure corresponding to a plane surface by P, the radius of the sphere to which the surface belongs by 7, and by A a constant, the pressure exerted by a line of molecules, and reduced to unity of the surface, will have the following value : Po A eT eran eee ee (1.) r r being positive in the case of a convex, and negative in that of a concave surface. Whatever be the form of the surface, let us imagine two spheres, the radii of which are those of greatest and least curvature at the point under consideration. It is evident that the pressure exerted by the line will be intermediate between those corresponding to these two spheres, and calculation shows that it is ex- actly their mean. Denoting the two radii in question by R and R’, the press- ure exerted by the line, referred to the unity of surface, would be AKU RT ' Pee a Se oe ld ee ene a : +Hatw): (2) The radii R and R’ are positive when they belong to convex curves, or, in other terms, when they are directed to the interior of the mass; whilst they are nega- tive when they belong to concave curves, @. e., when they are directed towards the exterior. 5. From the preceding details we can now easily deduce the condition of equilibrium relative to the free surface of the mass. The pressures exerted by the lines of molecules which commence at the dif- ferent points of the surface are transmitted to the whole mass ; consequently, for the existence of equilibrium in the latter, all the pressures must be equal to each other. In fact, let us imagine a minute canal running perpendicularly from some point of the surface, and subsequently becoming recurved so as to terminate perpendicularly at a second point of this same surfaze, it is evident that equilibrium can only exist in this minute canal when the pressures exerted by the lines which occupy its two extremities are equal; and if this equality exists, equilibrium will necessarily exist also. Now, the pressures exerted by the different lines depend upon the curves of the surface at the point at which they commence; these curves must therefore be such, at the various points of the free surface of the mass, as to determine everywhere the same pressure. Such is the condition which it was our object to arrive at, and to which in cach case the free surface of the mass must be subject. WITHDRAWN FROM THE ACTION OF GRAVITY. 229 The analytical expression of this condition is directly deducible from the general value of the pressure given in the preceding paragraph; we only require to equalize this value to a constant, and, as the quantities P and A are them- ‘selves constant, it is in fact sufficient to make 1 1 ‘ R yO SA tapch iets sy ee 2) SS ets Peak diced sic (3.) the quantity © being constant for the same figure of equilibrium. This equation is the same as those which are given by geometricians for ea- pillary surfaces, when, in the latter equations; the quantity representing gravity is supposed to be O. R and R’ may be replaced by their analytical values; we are thus led to a complicated differential equation, which only appears susceptible of integration in particular cases. Yet the equation (3) will be useful to us in the above sim- ple form. Now we know that the normal plane sections which correspond to the greatest and the least curvature at the same point of any surface form a right angle with each other. Geometricians have shown, moreover, that if any two other rectangular planes be made to pass through the same normal, the radii of curvature, p and p’, corresponding to the two sections thus deter- 5 ; sth able ds ST aes 5 mined, will be such that the quantity —-+ — will be equal to the quantity pp 1 if ROR Hence the first of these two quantities may be substituted for the second; and, consequently, the equation of equilibrium, in its most general expression, will be a kites teas Q ft ee ee wee eee ee ee ee ee (4.) p in which equation p and p' denote the radii of curvature of any two rectangular sections passing through the same normal. 6. These geometric properties lead to another signification of the equation (4.) We know that unity divided by the radius of curvature corresponding to _. any point of a curve is the measure of the curvature at this point. The quantity 1 1 — + — represents, then, the sum of the curvatures of two normal rectangular pp | sections at the point of the surface under consideration. This being admitted, if we imagine that the system of the two planes occupies successively different positions in turning around the same normal, a sum of curvatures ‘1 eer ns 1 p i p" pl! ele per pry _and, according to the property noticed in the preceding paragraph, all these sums will have the same value. Consequently, if we add them together, and let m denote the number of positions of the system of the two planes, the total sum will be equal to x times the value of one of the partial sums, 1 F ae + —, &ce., will correspond to each of these positions ; P or to 7 C oe =) Now, this total sum is that of all the curvatures pp a ie a, —., &e., in number 2z, corresponding to all the sections determined p p! me pe y the two planes. If, then, we divide the above equivalent quantity by 2z, the result = G ee aa ) will represent the mean of all these curvatures. Now, ee as this result is independent of the value of x, or of the number of positions occupied by the system of the two planes, it will be eaually true if we suppose > 930 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS this number to be infinitely great, or, in other words, if the successive positions — of the system of the two planes are infinitely approximated, and consequently if this same system turns around the normal in such a manner as to determine all the curvatures which belong to the surface around the point in question. The quantity 3G + 7) represents, then, the mean of all the curvatures of =P P the surface at the same point, or the mean curvature at this point. Now if, in enh : assing from one point of the surface to another, the quantity — + — retains Pp 8 pa i i : the same value, ¢. ¢., if for the whole surface we have — + ——Q, this sur- Pei Pea face is such that its mean curvature is constant. Considered in this purely mathematical point of view, the equation (4) has formed the object of the researches of several geometricians, and we shalb profit by these researches in the subsequent parts of this memoir. Thus our liquid surfaces should satisfy this condition, that the mean curve must be the same everywhere. We can understand that if this occurs, the mean effect of the curvatures at each point upon the pressure corresponding to this point also remains the same, and that this gives rise to equilibrium. Hence we now see more clearly the nature of the surfaces we shall have to consider, and why they constitute surfaces of equilibrium. 6*. We must now call attention to an immediate consequence of the theo- retical principles which have led us to the general condition of equilibrium. According to these principles, each of the lines of molecules exerting upon the mass the pressures upon which its form depends, commences at the surface and terminates at a depth equal to the radius of the sensible activity of the mole- cular attraction, so that these lines collectively constitute a superficial layer, the thickness of which is equal to the radius itself, and we know that this is of extreme minuteness. It results from this that the formative forces exerted by the liquid upon itself emanate solely from an excessively thin superficial layer. We shall denominate this consequence the principle of the superficial layer. all the curvatures in it are the same at each point; also when our mass is per- fectly free, 7. e., when it is not adherent to any solid which obliges its surtace to assume some other curve, it in fact takes the form of the sphere, as shown in the preceding memoir. 8. Before proceeding further, we ought to elucidate one point of great im- portance in regard to the experimental part of-our investigations. The liquid mass in our experiments being immersed in another liquid, the question may | be asked whether the molecular actions exerted by the latter exert no influence . upon the figure produced; or, in other words, whether the figure of equilibrium of a liquid mass adherent to a solid system, and withdrawn from the action of gravity by its immersion in another liquid of the same density as itself, is exactly the same as if the mass adherent to the solid. system were really de- prived of gravity and were placed in vacuo. Now, we shall show ithat this really is the case. ‘The molecular actions resulting from the presence of the surrounding liquid are of two kinds, viz., those resulting from the attraction of this liquid for itself, and those resulting from the mutual attraction of the two liquids. Let us first consider the former, imagining for an instant that the others do not exist. The surrounding liquid being applied to the free surface of the immersed mass, the former presents iz intaglio the same figure as the latter mass presents in relief. Those molecules of this same liquid which are near the common surface of the two media must then exert pressures of the same 7. A spherical surface evidently satisfies the condition of equilibrium, because - i in, i. WITHDRAWN FROM THE ACTION OF GRAVITY. 231 nature as those which we have considered throughout the preceding details, towards the interior of the liquid to which they belong, and these pressures must consequently also impart a figure of equilibrium to the surface in intaglio ; so that if the immersed mass of itself had no tendency to assume any one figure rather than another, the surrounding liquid would give it a determinate one, by compelling it to mould itself in the above hollow figure. This is why a bubble of air in a liquid assumes the globular form, solely in consequence of the pres- sures exerted by the liquid upon it. Now let us suppose that the immersed mass has assumed that figure which it would acquire 7 vacuo if really deprived of gravity; the analytical condition of paragraph 5 would then be satisfied as regards this mass. Now at each point of the common surface of the two media, the radii of curvature p and p’ have the same absolute values, both in the case of the immersed mass and of the hollow figure of the surrounding liquid, except . that their signs are contrary, according as they are considered as referring to one or the other of the two liquids. ‘To pass from one of the two figures to the other, we need therefore only change the signs p and p’, or, what comes to the same thing, change the sign of the constant C. Changing the sign does not destroy the condition of equilibrium; and consequently, if the immersed mass is in equilibrium as regards its own molecular attractions, the same will hold good in the case of the hollow figure of the surrounding liquid. The pressures of the latter liquid cannot, therefore, by themselves produce any modification in the figure of equilibrium of the immersed mass. Let us now introduce the second kind of molecular actions, 7. e., the mutual attraction of the two liquids, and see what will be its effects. Let us imagine, for an instant, that the immersed mass, or, for the sake of fixing the ideas, the mass of oil in our experiments is replaced by the same kind of liquid as that which surrounds it, z. e., by the alcoholic mixture. In other words, supposing the vessel to contain only the alcoholic mixture and the solid system, let us limit, in the imagination, a portion within the liquid of the same figure and dimensions, and situated in the same manner as the preceding mass of oil. It is then clear that the molecules of the mass near its surface being, like those of the interior, completely surrounded by the same kind of liquid beyond their sphere of activity, these molecules will no longer exert any pressure upon the mass; consequently, the pressures which would exist if this mass could be isolated must be considered as destroyed by the attractions emanating from the surrounding liquid. The latter forces are, therefore, all equal and opposite to the pressures in question. Now, as these are all equal to each other in ac- cordance with the figure which we have attributed to the imaginary surface of the mass, the attractions emanating from the surrounding liquid will also all be equal to each other. If we now replace the mass of oil, the attractions emanating from the surrounding liquid may certainly alter in absolute value, but it is evi- dent that they will retain their directions, and that they will remain equal to each other. We therefore see that they will only diminish, by the same quan- tity, all the pressures exerted by the mass of oil upon itself; consequently, as all the differences remain equal to each other, the condition of equilibrium will sti!l be satisfied as regards that mass. It is evident that the same mode of reasoning may be applied to the pressures exerted by the surrounding liquid upon itself—pressures which will retain their directions, all of which will only be diminished to the same extent by the attractions emanating from the oil, so that the condition of equilibrium will still be satisfied as regards the hollow figure of the surrounding liquid. ‘Thus the whole of the molecular actions due to the presence of the surrounding liquid will not tend in any way to modify the figure of equilibrium of the immersed mass, which figure will, consequently, be idettically the same as if that mass were really void of gravity and were placed i vacuo. We can, therefore, leave the surrounding liquid completely 232 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS out of the question, its sole function being to neutralize the action of gravit upon the mass forming the object of the experiments. 9. We shall now pass to the experimental part. And first, to avoid useless repetition, we shall say a few words relative to the apparatus to be used. As the liquid always consists of a mass of oil immersed in an alcoholic mixture of the same density as itself, our solid systems will all consist of iron, and this for the following reasons: In ordinary circumstances oil contracts, I believe, per- fect adhesion with all solids; but this is not exactly the case when the same oil is plunged into a mixture of water and alcohol ; for then, in the case of cer- tain solids, as, e.g., glass, the phenomena of adhesion sometimes undergo modi- fications which give rise to trouble In the experiments. We shall meet with an instance of this in the subsequent parts of this memoir. Now, the metals do not present this inconvenience ; moreover, the form which we have given to most of our solid systems would render their construction of any other sub- stance besides a metal difficult. Now, among metals we prefer iron, not copper, because oil removes nothing from iron, whilst by prolonged contact with copper it slightly attacks it, acquires a green color, and increases in density, which is a great inconvenience.* When we wish to use one of these solid systems of iron, before introducing it into the vessel, it must be completely moistened with oil; and for this pur- pose it is not suflicient simply to immerse it in this liquid, but it must be eare- tully rubbed with the finger. The presence of this coating facilitates the adherence of the liquid mass. We shall continue to make use of the vessel with plane walls, described in the preceding memoir, § 8;+ a common-shaped bottle, and the flask previously mentioned (§§ 5 and 8) in the same memoir, are not well adapted, because they do.not exhibit the true figure of the mass. When the solid system is composed of a single piece, it is supported by a vertical iron wire, which is screwed to the lower end of the axis traversing the metallic stopper; but for certain experiments the solid system is formed of two . isolated parts, and then only one of them is attached to the axis, as I have stated; the other is supported by small feet which rest upon the bottom of the vessel. It need not be mentioned that those liquids only which are prepared in such a manner as to-be incapable of exerting any chemical action upon each other can be employed, (§§ 6 and 24 of the preceding memoir.) In addition to the little funnel for introducing the mass of oil into the vessel, the iron wire which serves for uniting the isolated spheres, &c., of which I have spoken in the preceding memoir, the experiments require some other accessory instruments, as, In the first place, a small glass syringe, the point of which is elongated and slightly bent. It is used as a sucking-pump, to remove, for in- * In a letter which Dr. Faraday did me the honor of sending to me, regarding the pre- ceding memoir, he informed me that, when about to repeat my experiments before a numerous audience, wishing to produce a still greater difference in the aspect of the two liquids, he dissolved intentionally a little oxide of copper in the oil, so as to render the latter of a green color. The compound haying thus been made beforehand, and rendered perfectly homoge- neous, and the alcoholic mixture having been regulated according to the density of the modi- fied oil, the presence of the copper in solution could not produce any inconvenience ; but in this case also the solid systems should unquestionably be made of iron. tIn making the experiments rela.ing to the present memoir, I found that it was requisite slightly to modify the apparatus in question. The second perforation in the plate forming the lid of the vessel should be but little smaller than the centrat aperture ; its neck should be less elevated; and, lastly, it should be placed near the other; if left as preyiously described and figured, the employment of the accessory instruments which we sha!l describe would be impossible. Moreover, the neck of the central aperture should be furnished with a slight rin, so that it may be easily taken hold of when we wish to remove the lid, as, e. g.,, when it is required to attach a solid system which is too large to pass through this same aperture to the axis which traverses the stopper. Lastly, the vessel should be furmished with a stop cock at its lower part, so that it may be easily emptied. WITHDRAWN FROM THE ACTION OF GRAVITY. 233 stance, a portion of the oil composing the liquid mass, whes it is required to diminish the volume of the latter, or to withdraw the entire mass of oil from the vessel, an operation which is sometimes required, &c. In the second place, two wooden spatulas, one being slightly bent, the other straight, covered with fine linen or cotton stuff. When these spatulas are introduced into the vessel , and the cloth with which they are furnished is thoroughly impregnated with the alcoholic liquid, the mass of oil does not adhere to them. Hence, by means of one or the other of these spatulas, the mass can be moved in the surrounding liquid, and conducted to the place which it is required to occupy in the interior of the vessel without any of it remaining upon the spatula. This is the pur- pose for which these instruments are intended. After they have been used, care must always be taken to agitate them in pure alcohol before allowing them to dry. If this precaution ‘be omitted, the alcoholic mixture with which they are impregnated, on evaporating, would leave the small quantity of oil which it held in solution upon their surface; and when the same instruments are used again, the mass of oil would adhere to it. In the third place, an iron spatula, the uses of which we shall point out in the proper place. Lastly, as it is necessary, in all the experiments which we shall relate, that the alcoholic liquid should be homogeneous, the process indicated in the preceding memoir (§ 25) cannot be used to prevent the mass of oil from becoming occasionally adherent to the bottom of the vessel; but the same result is obtained by cover- ing the bottom with a panesS piece of linen. New experiments in support of the theoretical principles brought forward in the preceding observations. Figures of equilibrium terminated by surfaces of spherical curvature.. New principle relating to layers of liquids. 10. The facts which we shall first describe may be considered as constituting the experimental demonstration of the principle of the superficial layer, (§ 6, dzs.) Let us imagine any solid system to be immersed in the liquid mass, and let us give to this mass such a volume that it may constitute a sphere which com- pletely envelops the solid system without the latter reaching the surface at any point. ‘Then, if the above principle be true, the presence of the solid system will exert no influence upon the figure of equilibrium, because, under these circumstances, the superficial layer, from which the configuring actions emanate, remains perfectly free; whilst if these actions emanated from all points of the mass, any unsymmetrical modification occurring in the internal parts of the latter would necessarily produce one in the external form. ‘This is confirmed by experiment. ‘The condition of a solid system completely enveloped by the mass of oil would be somewhat difficult to realize; but it must be remembered that, in the experiments relating to the preceding memoir, the system of the disk, by means of which the mass was made to revolve, was very nearly in this con- dition, because it did not reach the external surface of the mass excepting at the two very small spaces which gave passage to its axis. But we then saw (§ 9 of the preceding memoir) that when the mass was at rest, its sphericity was only very slightly altered by the presence of this system. 'The theoretical condition may be more nearly approached by taking a very fine metallic wire for the axis of this same system; in this case the alteration in form is quite imperceptible. ‘The axis being supposed to be vertical, the disk may, moreover, be placed so that its centre coincides with that of the mass of oil, or is situated above or below the latter without producing any diiference. I shall relate another fact of an analogous nature. In the course of the experiments, it some- times happens that portions of the alcoholic liquid become imprisoned in the interior of the mass of oil, forming so many isolated spheres. Now, however these spheres may be situated in the interior of the mass, not the least alteration __ is produced in the figure of the latter. 934 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS 11. Again, let us cause some kind of solid system to penetrate the liquid — mass; but now let the'mass be of too small a volume to: be capable of com-_ pletely enveloping this system. The latter will then necessarily reach the superficial layer ; and, if the principle in question be true, the figure of the _ liquid mass will be modified, or, in other words, will cease to remain spherical. _ This does really oecur, as we might have expected ; the liquid mass becomes i) extended at those portions of the solid system which project externally from — its surface ; it finally either occupies the whole of these portions, or only a part — of their extent, according to the form and the dimensions of the solid system, and thus assumes a new figure of equilibrium. We shall meet with examples fp of this hereafter, (§§ 14, 15, 17.) é. 12. Instead of causing the solid system to penetrate the interior of the liquid _ mass, let it simply be placed in contact with the external surface of the latter. x An action being then established at a point of the superficial layer, equilibrium _ must be destroyed, and the figure of the liquid mass ought again to be modified. This really occurs; the mass becomes extended upon the surface presented to it, and consequently acquires a different shape. This result might also have been anticipated from what occurs under ordinary circumstances, when a dro of water is placed upon a previously moistened solid surface. “One might be ; induced to believe that, as regards the actual result, this case is referable to — that of the preceding paragraph or that in paragraph 10; for it appears that — the liquid mass, becoming extended upon the solid system so as to obtain the — new figure of equilibrium, should ultimately occupy or envelop this system in the same manner as if the latter had been made to penetrate its interior directly. _ Under certain circumstances this must occur; but the experiments which are about to be related will show that under other circumstances the result is totally different. t 13. Let us take for the solid system a thin circular plate,* attached by its centre to the iron-wire which supports it, (Fig. 1,) and let us produce the “i. Steel ee Fig 1. Fig. 2. adhesion of its lower surface to the upper part of the mass of oil.t Directly contact is completely established, the oil extends rapidly over the surface pre- * The diameter of that which I have used is 4 centimetres. I mention this diameter for the sake of being definite. Jt is evident that in our experiments the dimensions of the appa- ratus are completely arbitrary, except that if these dimensions exceed certain limits, the operations will become embarrassing in consequence of the large quantities of liquid which would be required. + In order that this operation may be effected with facility, the sphere of oil must first yemain in the surrounding liquid beneath the central aperture in the lid; the plate being then introduced into the vessel, we have merely to lower it by means of the axis traversing the stopper to bring it towards the liquid mass. If the latter does not occupy the position in question, it must be previously placed there by means of a spatula covered with lincn, (§ 9) It must be remarked here, that true contact between the plate and the sphere of oil does not usually ensue immediately; a certain resistance has to be overcome, analogous to that treated of in the note to paragraph 4 of the preceding memoir; but to overcome this, the liquid sphere need only be gently moved by means of the plate. The slight resulting pressure soun causes the rupture of the obstacle and the production of adhesion. oy UeweaAs ze Ine iq ale eee ge BEN DOE poor me de WITHDRAWN FROM THE ACTION OF GRAVITY. 235 _ sented to it; but, what is remarkable, although the precaution has been taken _ of rubbing the whole of the system, (§ 9,) that is, the two faces of the plate as _ well as its rim, with oil, the oil terminates abruptly at this rim without passing to the other side of the plate, and thus presents a sudden interruption in the curvature of its surface. In the case in question, the new figure acquired by the mass is a portion of a sphere. This portion will be as much larger in pro- rtion to the complete sphere as the volume of oil is greater; but the curvature will always terminate abruptly at the margin of the plate. (See Fig. 2, which _ represents a section of the solid system and the adherent mass in the ease of three different volumes of the latter.) The cause of this singular interruption of continuity is readily understood. The rim of the plate reaching to the superficial layer, it is natural that some- thing peculiar should occur along this margin, and that the continuity of form _ should cease at that point where a foreign attractive action is exerted without transition on the superficial layer. 14. Let us again make use of the above plate; but instead of presenting one of its faces to the exterior of the sphere of oil, let us insert the plate edgewise into the interior of this sphere.* The liquid will necessarily extend over both faces of the solid; and if the diameter of the primitive sphere were less than that of the plate, the oil will be seen to form two spherical segments upon the two faces in question, the curvatures of which will still terminate abruptly at the margin of the plate. These two segments may be either equal or unequal, according as the edge of the plate has been introduced into the liquid sphere in such a manner that the plane of the plate passes through the centre of the sphere or not. ‘The upper segment will be slightly deformed by the action of the suspending wire; but this effect will be less sensible in proportion to the thinness of the wire in question. Fig. 3 represents the result of the experiment with two unequal segments. The discontinuity of the curvatures is a very general fact, which we shall frequently find to recur in the course of our experiments; it will hereafter lead us to very important consequences. Fig. 3. Pig. 8. 15. I have repeated the same experiment, substituting a plate of an elliptic form for the circular plate. In this, as in the preceding case, the oil extends over both faces of the solid, so as entirely to cover them; and, if the volume of * This operation is performed as follows: The stopper to which the system of the plate is attached is kept at some distance above the neck of the central aperture, in such a manner, however, that the latter is immersed to a sufficient depth in the alcoholic mixture. The plate can then be moved with tolerable freedom, and it is conducted towards the liquid mass For this purpose the latter ought previously to occupy a suitable position. Imme- diately the liquid mass is cut, the piate is kept still until the action is termimaicd, after which the stopper is carefully placed in the neck. A process the reverse to the preceding may also be made use of. The liquid mass is first made to occupy a position near the second aperture, and a sufficient distance from the axis which passes through the centre of the cen- _ tral aperture; then, having fixed the solid system firmly in the position which it is to occupy, move the liquid mass towards it, and when this has been cut, allow the action to continue aninterruptedly. These processes are also employed in other experiments, and it is enough to have pointed them out once. In some cases the second is the only practicable one. This. may be easily decided upon in making the experiments. 936 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS the liquid mass is not too great, the curvatures again terminate abruptly aléng_ the rim of the plate. By gradually augmenting the volume of the primitive sphere of oil, without, however, rendering it sufficiently large to allow of the mass completely enveloping the plate so as to retain the spherical form, a limit is attained at which the edge of the plate ceases to reach the superficial layer of the new figure of equilibrium except at the two summits of the ellipse. The discontinuity in the curvatures then only occurs at these two places. Figs. 4 and 5 exhibit the result of the experiment in this case. In Fig. 4 the long axis of the ellipse is presented to view, in Fig. 5 its short axis. 16. All the facts which we have hitherto detailed show that so long as the interior of the mass is modified its external shape undergoes no alteration ; but that directly the superficial layer is acted upon, the mass acquires a different form. ‘I'o complete the proof, by experiment alone, that the configuring actions’ exerted by the liquid upon itself emanate solely from the superficial layer, the only point would then be the possibility of reducing a liquid mass to its super- ficial layer, or at least to a thin pellicle, and to see if in this state it would assume the same figure of equilibrium as a complete mass. Now this is com- pletely realized in soap-bubbles; for these bubbles, when detached from the tube in which they have been made, assume, as is well known, a spherical form, i. e., the same figure as that which we find a complete mass acquires in our apparatus when withdrawn from the action of gravity and perfectly free. When the mass adheres to a solid system, which modifies its figure, it is clear that the entire ‘configurative action is composed of two parts, one of which belongs to the solid system; and we find that this system only exerts if when acting upon the superficial layer; the other belongs to the liquid, and emanates directly from the free portion of this same superficial layer. The facts which we have related show clearly what is the seat of this second part of the whole configurative action, but they do not make us acquainted with the nature of the forces of which it consists. On referring to theory, we find that these forees consist in pressures exerted upon the mass by all the elements of the superficia! layer, pressures the intensity of which depend upon the curvatures of the surface at the points to which they correspoud. Hence it follows. that the mass is pressed upon by every part of its superficial layer, with an intensity depending in the same manner upon the curvatures of the surface. For instance, a mass the free surface of which presents a convex spherical curvature, will be pressed upon by the whole of the superficial layer belonging to this free surface, with a greater intensity than if this surface had been plane; and this intensity will be more considerable in proportion as the curvature is greater, or as the radius of the sphere to which the surface belongs is less. Let us see whether experiment will lead us to the same conclusions. 17. The solid system which we shall employ is a cireular perforated plate, (Fig. 6.) It is placed vertically, and attached by a point of its circumference to the iron wire which supports it. Let the diameter of the sphere of oil be less than that of the plate, and let the latter be made to penetrate the mass by its edge in a direction which does not pass through the centre of the sphere. At first, as in the experiment at paragraph 14, the oil will form two unequal spherical segments ; but matters do not remain in this state. 'The most convex segment is seen to diminish gradually in volume, consequently in curvature, whilst the other increases, until they have both become exactly equal. One part of the oil then passes through the aperture in the plate, so as to be trans- ferred from one of the segments towards the other, until the above equality is attained. Let us now examine into the consequences deducible from this experiment, judging from the preceding ones, and independently of all theoretical considera- tions. When the oil has once become extended over both surfaces of the plate, in such a manner that the superficial layer is applied to every part of the ’ WITHDRAWN FROM THE ACTION OF GRAVITY. aan margin of the latter, the action of the solid system is completed; and the move- ments which subsequently ensue in the liquid mass, to attain the figure of equilibrium, can only then be due to an action emanating from the free part of the superficial layer. It is, therefore, the latter which compels the liquid to pass through the aperture in the plate; and the phenomenon must necessarily result either from a pressure exerted by that portion of the superficial layer which belongs to the most convex segment, or by a traction produced by the portion of this same layer belonging to the other segment. Our experiment not being alone capable of determining our choice between these two methods of explaining the effect in question, let us provisionally adopt the first, ¢. e., that which attributes it to pressure.+ In our experiment, this pressure emanates from the superficial layer of the most curved segment; but it is easy to see that the superficial layer of the other segment also exerts a pressure which, alone, is less than the pre- ceding. In fact, if for the most curved segment a segment less curved than the other were substituted, the oil would then be driven in the opposite direction. Hence it follows that the entire superficial layer of the mass exerts a pressure upon the liquid which it encloses, and that the intensity of this pressure depends upon the curvatures of the free surface. Moreover, as the liquid proceeds from the most curved segment to that which is least so, it is evident that in the case of a convex surface, the curvature of which is spherical, the pressure is greater in proportion as the curvature is more marked, or as the radius of the sphere to which the surface belongs is smaller. Lastly, since a plane surface may be considered as belonging to a sphere, the radius of which is infinitely great, it is evident that the pressure corresponding to a convex surface, the curvature of which is spherical, is superior to that which would correspond to a plane surface. All these results were announced by theory. They pertectly verify, then, that part of the latter to which they refer, and this concordance ought now.to decide in favor of the hypothesis of pressure. This same part of the theory was already verified, in its application to liquids submitted to the action of gravity, by the phenomenon of the depression presented by liquids in capillary tubes, the walls of which they do not moisten; but the series of our experiments, setting out with the elements of the theory, and following it step by step, yields far more diréct and complete verification. Our last experiment leads us to still further consequences. The liquid passing from one of its segments to the other, so long as their curvatures have not become identical, and the pressures corre- sponding to the two portions of the superficial layer becoming equal to each other simultaneously with the two curvatures, it follows that the mass only attains its figure of equilibrium when this equality of pressure is established. We thus have a primary verification of the general theory of equilibrium which governs our liquid figures, a condition in virtue of which the pressures exerted by the superficial layer ought to be everywhere the same. Moréover, it is evident that if a superficial layer, having a spherical curvature, exerts by itself a pressure, this principle must be true, however small the extent of this layer may be supposed to be. It follows, therefore, that an extremely minute por- _tion of the superficial layer of our mass, taken from any part of either of the two segments, ought itself to be the seat of a slight pressure; consequently, that the total pressure exerted by the superficial layer is the result of individual pressures emanating from all the elements of this layer. This was also shown by theory. Further, following the same train of reasoning, we see that the intensity of each of the minute individual pressures ought to depend upon the curvature of the corresponding element of the layer, which is also in contormity with theory. Lastly, as in a state of equilibrium the two segments belong to spheres of equal radii, the curvature is the same in all points of the surface of the mass; whence it follows that all the minute elementary pressures are equal to each other. The general condition of equilibrium (§ 5) is, therefore, perfectly verified in the instance of our experiment. 238 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS 18. The principle of the superficial layer, applied to the preceding expéri- ment, allows of the latter being modified in such a manner as to obtain a very remarkable result. When the figure of equilibrium is once attained, the per- forated plate acts upon the superficial layer by its external border only. ‘The whole of the remainder of this plate then exerts no influence upon the figure in question. Hence it follows that this figure would still be the same if the aper- ture were enlarged, only the greater the diameter of the latter the less time is required for the establishment of the equality between the two curvatures. Lastly, we ought to be able to enlarge the aperture nearly to the margin of the plate without changing the figure of equilibrium ; or, in other words, to reduce the solid system to a simple ring of thm iron wire. Now, this is confirmed by experiment; but, to put it in execution, we cannot confine ourselves, as before, to making the solid system penetrate a sphere of oil of less diameter than that of this same system, and subsequently to allow the molecular forces to act, be- cause the metallic wire, on account of its small extent of surface, would not exert a suflicient action upon the superficial layer to cause the liquid to extend so as to adhere to the entire surface of the ring. The mass would then remain traversed by part of the latter, and its spherical form would not be sensibly altered if the metallic wire were small; the liquid surface would merely be slightly raised upon the wire in the two small spaces at which it issued from the mass. ‘To speak more exactly, under the circumstances in question two figures of equilibrium are possible. One of these differs but very slightly from the sphere; it is not symmetrical with regard to the ring, one part of which traverses it whilst the other part remains free. The second figure is perfectly symmetrical as regards the ring, and completely embraces its margin; its surface is composed of two equal spherical curves, the margins of which rest upon the ring; in other words, it constitutes a true doubly convex lens of equal curva- tures. This is the figure which it is our object to obtain. For this purpose we first give the sphere of oil a diameter slightly greater than that of the metallic ring; we then introduce the latter into the mass so that it is com- pletely enveloped; lastly, by means of the small giass syringe, (§ 9,) some of the liquid is gradually removed from the mass.* As this diminishes in volume, its surface is soon applied to every part of the margin of the ring, and the volume continuing to diminish, the lenticular form becomes manifest. After- wards, by withdrawing more of the liquid, the curvatures of the two surfaces may be reduced to that degree which is considered suitable. In this way a beautiful double convex lens is obtained, which is entirely liquid except at its circumference. Moreover, in consequence of the index of refraction of the olive oil being much greater than that of the alcoholic mixture, the lens in question possesses all the properties of converging lenses; thus, it magnifjes objects seer through it, and this magnifying power may be varied at pleasure by removing some of the liquid from, or adding more to, the mass. Our figure, therefore, realizes that which could not be obtained with glass lenses, 7. e., it forms a lens, the curvature and magnifying power of which are variable. The diameter of that which I formed was 7 centimetres, and the thickness of the metallic wire was about $a millimetre. A much finer wire might have been used with the same success; but the apparatus would then become inconve- nient on account of the facility with which it would be put out of shape. By operating with care, the curvatures of the lens may be diminished so as almost to make them vanish; thus I have been enabled to reduce the lens which I formed, and the diameter of which, as I have stated, was 7 centimetres, to such an extent that it was only 2 or 3 millimetres in thickness. Hence we might presume that it would be possible to obtain, by a proper mode of pro- * The point of the instrument is introduced into the vessel through the second aperture in the lid. WITHDRAWN FROM THE ACTION OF GRAVITY. 239 ceeding, a layer of oil with plane faces. This is, in fact, confirmed by expe- rience, as we shall see further on. 19. 'T’o render the curvatures of the liquid lens very slight, the point of the *syringe must naturally be applied to the middle of the lens, because the maxi- mum of thickness exists there. Now, when a certain limit has been attained, the mass suddenly becomes divided at that point, and a curious phenomenon is produced. The liquid rapidly retires in every direction towards the metallic circumference, and forms a beautiful liquid ring along the latter; but this ring does not last for more than one or two seconds, after which it spontaneously resolves itself into several small, almost spherical masses, adhering to various parts of the ring of iron wire, which passes through them like the beads of a necklace. 20. The reasoning which led us, at the commencement of paragraph 18, to reduce the primitive solid system to a simple metallic wire representing the line in the direction of which this system is met*by the superficial layer belonging to the new figure of equilibrium, may be generalized. We may conclude that whenever a solid system introduced into the mass is not met by the superficial layer of the figure produced, excepting in the direction of small lines only, sim- ple iron wires, representing the lines in question, may be substituted for the solid system employed. But if the volume of the primitive solid system were considerable, it would evidently be requisite to add to the mass of oil an equiva- lent volume of this liquid, to occupy the place of the solid parts suppressed. There is, however, an exception to this principle ; it occurs when the solid system separates the entire mass into isolated portions, as in the experiment of paragraph 14; for then these portions assume figures independent of each other, and which may correspond to different pressures. In this case the suppression of one portion of the solid system would place the figures primitively isolated in communication, and the inequality of the pressures would necessarily induce ~ achange in the whole figure. Excluding this exception, the principle is gen- eral, and the result of it is that well-developed effects of configuration may be obtained on employing simple iron wires instead of solid systems. The experi- ment of the biconvex lens furnishes one instance of this, and we shall meet with a great many others hereafter. Nevertheless, to be enabled to comprehend the influence of a simple metallic wire upon the configuration of the liquid mass, it is not requisite to consider this wire as substituted for a complete solid system; it may also be considered by itself. It is, in fact, clear that the solid wire acting by attraction upon the superficial layer of the mass, the curvatures of the two portions of the surface resting upon it ought not to have any further relation of continuity with each other. The metallic wire may, therefore, de- termine a sudden transition between these two portions of the surface, the eurv- atures of which will terminate abruptly at the limit which it places to them. The principles which we have established ought undoubtedly to be considered , as among the most remarkable and curious consequences of the prineiple of the _ superficial layer, and one cannot avoid being astonished when we see the liquid maintained in such different forms by an action ex- 7 7 erted upon the extremely minute parts of the superficial layer of the mass. 21. We have experimentally studied the influence of convex surfaces of spherical curvature; let us now ascertain what experi- ment is able to teach us in regard to plane surfaces and concave surfaces of spherical curvature. Let us take for the solid system a large strip of iron, curved circularly so as to form a hollow cylinder, and attached to the suspending iron wire by some point on its outer surface, (Fig.7.) To prevent the production of accessory phenomena in the experiment, we shall suppose that the breadth of the metallic band is less than the diaieter of the cylinder formed by the same band, or that it isat least equal to it. Make the mass of oil adhere to the internal surface of this » w 940 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS ~ system, and let us suppose that the liquid is in sufficient quantity then to project outside the cylinder. In this case the mass will present on each side a convex surface of spherical curvature, and the curvatures of these two surfaces will be equal. This figure is a consequence of what we have previously seen; and we must not stop here, for it will serve us as a starting point in obtaining other figures which we require. Apply the point of the syringe to one of the above convex surfaces, and gradually withdraw some of the liquid; the curvatures of the two surfaces will then gradually diminish, and with care they may be ren- dered perfectly plane. It follows from this first result that a plane surface is also a surface of equilibrium, which is evidently in conformity with theory. Let us now apply the end of the syringe to one of these plane surfaces, and again remove a small quantity of liquid. The two surfaces will then become simul- taneously hollow, and will form two concave surfaces of spherical curvature, the margins of which rest upon the metallic band, and the curvatures of which are the same. Finally, by the further removal of the liquid, the curvatures of the two surfaces become greater and greater, always remaining equal to each other. Hence it results, first, that concave surfaces of spherical curvature are still surfaces of equilibrium, which is also in accordance with theory. Moreover, as the plane surface left free sinks spontaneously as soon as that to which the in- strument is applied becomes concave, it must be concluded that the superficial layer belonging to the former exerts a pressure which is counterbalanced by an equal force emanating from the opposite superficial plane layer, but which ceases to be so, and which drives away the liquid as soon as this opposite layer com- mences to become concave. Again, as further abstraction of the liquid deter- mines a new rupture of equilibrium, so that the concave surface opposite to that upon which we directly act exhibits a new spontaneous depression when the curvature of the other surface increases, it follows that the concave superficial layer belonging to the former still exerted a pressure, which at first was neutral- ized by an equal pressure arising from the other concave layer, but which be- comes preponderant, and again drives away the liquid, when the curvature of this other layer is increased. Hence it follows, first, that a plane surface produees a pressure upon the liquid; second, that a concave surface of spherical curvature also produces a pressure; third, that the latter is inferior to that corresponding to a plane surface; fourth, that it is less in proportion as the concavity is greater, or that the radius of the sphere to which the surface belongs is smaller. These results were also pointed out by theory, and had already been verified in the application of the latter. to liquids submitted to the action of gravity, by the phenomenon of the elevation of a liquid column in a capillary tube, the walls of which are moistened by it. Reasoning upon these facts, as we have done at the end of paragraph 17 in regard to convex surfaces of spherical curvature, we shall arrive at the conclu- sion that the entire pressure exerted by a concave superficial layer of spherical curvature is the result of minute individual pressures arising from all the elements of this layer, and that the intensity of each of these minute pressures depends upon the curvature of that element of the layer from which it emanates. Our last experiment, therefore, perfectly verifies that part of the theory which relates to plane and convex surfaces of spherical curvature. Lastly, in the state of equilibrium of our liquid figure, the curvature being the same at all points of each of the two coneave surfaces, it is again evident that all the minute elementary pressures are equal to cach other, which gives a new complete verification of the general condition of equilibrium. 22. The figure we have just obtained constitutes a biconcave lens of equal curvatures, and possesses all the properties of diverging lenses, z. e., it dimin- ishes objects seen through it, &c. Moredver, as the curvature of the two sur- faces may be increased or diminished by as small degrees as is wished, it follows 5 So png nena ce aman ee aL eR in IE eae ” “ - WITHDRAWN FROM THE ACTION OF GRAVITY. DAY that we thus obtain a diverging lens, the curvature and action of which are variable. ° 23. Now let us suppose that we have increased the curvatures of the lens until the two surfaces nearly touch each other by their summits.* We might presume that if the removal of the liquid were continued, the mass would be- come disunited at that point at which this contact took place, and that the oil would recede in every direction towards the metallic band. ‘This is, however, not the case; we then observe in the centre of the figure the formation of a small sharply defined circular space, through which objects no “longer appear diminished, and we easily recognize that this minute space is occupied by a layer of oil with plane faces. If the removal of the liquid be gradually con-° tinued, this layer increases more and more in diameter, and may thus be ex- tended to within a tolerably short distance of the solid surface. In my experi- ment, the diameter of the metallic cylinder was seven centimetres, and I have been enabled to increase the size of the layer until its circumference was not more than about five millimetres from the solid surface; but at this instant it broke, and the liquid of which it consisted rapidly receded towards that which still adhered to the metallic band. The fact which we have just described is very remarkable, both in itself and in the singular theoretical consequences to which it leads. In fact, that part of the mass to which the layer adheres by its margin presgnts concave surfaces, whilst those of the layer are plane; now the existence of such a system of surfaces in a continuous liquid mass seems in op-’ position to theory, since it appears evident that the pressures cannot be equal _ inthis case. But let us investigate the question more minutely. |. 24. According to theory, the pressure corresponding to any point of -the sur- face of a liquid mass, as we have seen, (§ 3,) is the integral of the pressures _ exerted by each of the molecules composing a rectilinear line perpendicular to | the surface at that point, and equal in length to the radius of the sphere of activity of the molecular attraction. The analytical expression of this integral contains no other variables than the radii of the greatest and of the least curva- ture at the point under consideration, (§ 4,) consequently the pressure in _ question varies only. with the curvatures of the surface at the same point. This is rigorously true when the liquid is of any notable thickness; but we shall show that in the case of an extremely thin layer of liquid there is another element which exerts an influence upon the pressure. Let us conceive a liquid layer, the thickness of which is less than twice the radius of the sphere of sen- sible activity of the molecular attraction. Let each molecule be conceived to be the centre of a small sphere with this same radius, (§ 3,) and let us first consider a molecule situated in the middle of the thickness of the layer. The little sphere, the centre of which is occupied by this molecule, will be intersected _ by the two surfaces of the layer, consequently it will not be entirely full of liquid; but the segments suppressed on the outside of the two surfaces being equal, the molecule will not be more attracted perpendicularly in one direction than in the other. Now let a small right line, normal to and terminating at the two surfaces, pass through this same molecule, and let us consider a second molecule situated at some other point of this.right line. The little sphere which belongs to the second molecule in question may again be intersected by the two surfaces of the layer; but then the two suppressed segments will be unequal; the molecule will consequently be subjected to a preponderating at- | traction, evidlently directed towards the thickness of the layer. The molecule _ will then exert a pressure in this direction, and it must be remarked that this pressure will be less than if the liquid had any notabie thickness, the molecule * To effect this operation, the point of the syringe must not be placed in the middle of the figure, as in the case of the doubly convex lens; but, on the contrary, near the metallic band, as this is now the point where the greatest thickness of the liquid exists. 168 " 7 i 242 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS © being situated at the same distance from the surface ; for in the latter case the little sphere would only be eut on one side, and its opposite part would be per- fectly full of liquid. It might also happen that the little sphere belonging to the molecule in question in the thin layer is only cut on one side ; the molecule will then still exert a pressure in the same direction, but its intensity will then be as great as in the case of a thick mass. It is easy to see that if the thick- ness of the layer is less than the simple length of the radius of the molecular attraction, the little spheres will all be eut on both sides; whilst if the thickness in question issecomprised between the length of the above radius and twice this same length, a portion of the minute spheres will be cut on one side only. In both cases the pressure exerted by any molecule being always directed towards the middle of the thickness of the layer, it is evident that the integral pressure corresponding to any point of either of the two surfaces will be the result of the pressures individually exerted by each of those molecules, which, commencing at the point in question, are arranged upon half the length of the small perpen- dicular. Now each of the two halves of the small perpendicular being less than the radius of the sphere of activity of the molecular attraction, it follows that the number of molecules composing the line which exerts the integral pressure is less than in the case of a thick mass. Thus, on the one hand, the intensities of part or the whole of the elementary pressures composing the integral pres- sure will be less than in the case of a thick mass, and, on the other hand, the number of these elementary pressures will be less; from this it evidently follows that the integral pressure will be inferivr to that which would occur in the case of a thick mass. P always denoting the pressure corresponding to any point of a plane surface belonging to a thick mass, (§ 4,) the pressure corresponding to any point of either of the surfaces of an extremely thin plane layer will there- fore be less than P. Moreover, this pressure will be less in proportion as the layer is thinner, and it may thus diminish indefinitely ; for it is clear that it would be reduced to zero if we supposed that the thickness of the layer was equal to no more than that of a simple molecule. We can obtain liquid layers with curved surfaces; soap-bubbles furnish an example of these, and we shall meet with others in the progress of this investi- gation. Now by supposing the thickness of such a layer to be less than twice the radius of the molecular attraction, we should thus evidently arrive at the conclusion that the corresponding pressures at either of its two surfaces would be inferior in intensity to those given by paragraph 4, and that, moreover, these intensities are less in proportion as the layer is smaller. We thus arrive at the following new principle : In the case of every liquid layer, the thickness of which is less than twice the radius of the sphere of activity of the molecular attraction, the pressure will not depend solely upon the curvatures of the surfaces, but will vary with the thick- ness of the layer. 25. We thus see that an extremely thin plane liquid layer, adhering by its edge to a thick mass the surfaces of which are concave, may form with this mass a system in a state of equilibrium; for we may always suppose the thickness of the layer to be of such value that the pressure corresponding to the plane surfaces of this layer is equal to that corresponding to the concave surfaces of the thick mass. Such a system is also very remarkable in respect to its form, inasmuch as surfaces of different nature, as concave and plane surfaces, sue ceed each other. This heterogeneity of form is, moreover, a natural consequence of the change which the law of pressures undergoes in passing ff)m the thick to the thin part. . 26. As we have already seen, theory demonstrates the possibility of the ex- istence of such a system in a state of equilibrium. As regards the experiment which has led us to these considerations, although the result presented by it | tends to realize in an absolute manner the theoretical result, there is one circum- + . ~ WITHDRAWN FROM THE ACTION OF GRAVIT 943 stance which is unfavorable to the completion of this realization. We can un- derstand that the relative mobility of the molecules of oil is not sufficiently great to occasion the immediate formation of the liquid layer with that excessive tenuity which is requisite for equilibrium ; the thickness of this layer, although very minute, absolutely speaking, is undoubtedly, during the first moments, a considerable multiple of the theoretical thickness. If, then, we produce the layer without extending it to that limit to which it is capable of increasing during the operation, and afterwards leave it to itself, the pressure correspond- ing to its plane surfaces will still exceed that corresponding to the concave surfaces of the remainder of the liquid system. Hence it follows that the oil within the layer will be driven towards this other part of*the system, and that the thickness of the layer will progressively diminish. The equilibrium of the figure will then be apparent only, and the layer will in reality be the seat of continual movements. The diminution in thickness, however, will be effected slowly, because in so confined a space the movements of the liquid are neces- sarily restrained; this is why, as in the experiment in paragraph 17, the mass only acquires its figure of equilibrium slowly, because there is a cause which impedes the movements of the liquid. The thickness of the layer gradually approximates to the theoretical value, from which the equilibrium of the system would result; but unfortunately it always happens that before attaining this point the layer breaks spontaneously. This effect depends, without doubt, upon the internal movements of which I have spoken above. We can imagine, in fact, that when the layer has become of extreme thinness, the slightest cause is sufficient to determine its rupture. The exact figure which corresponds to the equilibrium is therefore a limit towards which the figure produced tends; this limit the latter approaches very nearly, and would attain if it were not itself previously destroyed by an extraneous cause. Our experiment has led us to modify the results of theory in one particular instance; but we now see that, far from weakening the principles of this theory, it furnishes, on the contrary, incomplete as it is, a new and striking verification of it. The conversion of the doubly concave lens into a system comprising a thin layer is connected with an order of general facts: we shall see that a large number of our liquid figures become transformed, by the gradually produced diminution of the mass of which they are composed, into systems consisting of layers, or into the composition of which layers enter. 27. If by some modification of our last experiment we could succeed in ob- taining the equilibrium of the liquid system, we might be able to deduce from it a result of great interest—an indication of the value of the radius of the sphere of activity of the molecular attraction. In fact, we might perhaps find out some method of determining, the thickness of the layers; these might, for instance, then exhibit colors, the tint of which would lead us to this determina- tion. Now we have seen that in the state of equilibrium of the figures, half the thickness of the layer would be less than the radius in question; hence we should then have a limit above which the value of this same radius would exist. In other words, we should know that the molecular attraction produces sensible effects, even at a distance from its centre of action beyond this limit. Our experiment, although insufficient, may thus be considered as the first step towards the determination of the distance of sensible activity of the molecular attraction, of which distance at present we know nothing, except that it is of extreme minuteness. 28. Let us now return to the consideration of thick masses. It follows from the experiments related in paragraphs 13, 14, 17, 18, and 21, that when a con- tinuous portion of the surface of such a mass rests upon a circular periphery, this surface is always either of spherical curvature or plane. But to admit this principle in all its generality, we must be able to deduce it from theory. We shall do this in the following series, at least on the supposition that the portion 944 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS of the surface in question is a surface of revolution. We shall then see that this same principle is of great importance. We may remark here that in the experiment in paragraph 23 the layer commences to appear as soon as the surfaces can no longer constitute spherical segments. Now we shall again find - that in the other eases, when a full figure is converted, by the gradual with- drawal of the liquid, into a system composed of layers, or into the composition | of which layers enter, the latter begin to be formed when the fig. &. figure of equilibrium, which the ordinary law of pressures would determine, ceases to be possible. 'The mass then assumes, or tends to assume, another figure, compatible with a modification of this law. Such is the general principle of the formation of layers under the circumstances in question. 29. After having formed a converging and a diverging liquid lens, it appeared to me curious to combine these two kinds of lens, so as to form a liquid telescope. For this purpose, I first substi- tuted for the ring of iron wire, in paragraph 18, a circular plate ~—< / of the same diameter, perforated by a large aperture. (Fig. 8.) bal This plate having been turned in a lathe, I was certain of its being perfectly circular, which would be a very difficult condition to fulfil in the case of a simple curved iron wire. In the second place, I took for the solid part of the doubly concave lens a band of about twoycentimetres in breadth, and curved into a cylinder three and a half centimetres in diameter. ‘These two systems were arranged as in Fig. 9, in such a manner that the entire apparatus being suspended vertically in the alcoholic mixture by the iron wire a, and the two liguid lenses being formed, their two centres Were at the same height, and ten centimetres distant from each other. In this arrangement the telescope cannot be adjusted by altering the distance between the objective and the eye-piece ; but this end is attained by varying the curvatures of these two lenses. With the aid of a few preliminary experiments, I easily managed to obtain an excel- lent Galilean telescope, magnifying distant objects about twice, like a common opera-glass, and giving perfectly distinct images with very little irisation. 8. o which represents a section of the system, shows the two lenses com- ined. Figures of equilibrium terminated by plane surfaces. Liquid polyhedra. Laminar figures of equilibrium. 30. In the experiment detailed at paragraph 21, we obtained a figure pre- senting plane surfaces. ‘These were two in number, parallel, and bounded by circular peripheries; but it is evident that these conditions are not necessary WITHDRAWN FROM THE ACTION OF GRAVITY. QA5 in order to allow plane surfaces to belong to a liquid mass in equilibrium. We can understand that the forms of the solid contours might be indifferent, pro- vided they constitute plane figures. We can, moreover, understand that the number and the relative directions of the plane surfaces may be a matter of indifference, because these circumstances exert no influence upon the pressures which correspond to these surfaces, pressures which will always remain equal to each other. Lastly, it follows from the principle at which we arrived at the end of paragraph 20, relative to the influence of solid wires, that for the estab- lishment of the transition between a plane and any other surface, a metallic thread representing the edge of the angle of intersection of these two surfaces will be sufficient. We are thus led to the curious result, that we ought to be able to form polyhedra, which are entirely liquid excepting at their edges. Now, this is completely verified by experiment. If for the solid system we take a framework of iron wire representing all the edges of any polyhedron, and we cause a mass of oil of the proper volume to adhere to this framework, we obtain, in fact, in a perfect manner, the polyhedron in question; and the curious spectacle is thus obtained of parallelopipedons, prisms, &c., composed of oil, and the only solid part of which is their edges. To produce the adhesion of the liquid mass to the entire framework, a volume is first given to the mass slightly larger than that of the polyhedron which it is to form; it is then placed in the framework; and, lastly, by means of the iron spatula, (§ 9,) which must be introduced by the second aperture of the lid of the vessel, and which is made to penetrate the mass, the latter is readily made to attach itself successively to the entire length of each of the solid edges. ‘The excess of oil is then gradually removed with the syringe, and all the surfaces thus become simultaneously exactly plane. But that this end may be attained in a complete mannez, it is clearly requisite that the equilibrium of density between the oil and the alcoholic mixture should be perfectly established ; and the slightest difference in this respect, is sufficient to alter the surfaces sensibly. It should also be borne in mind that the manipu- lation with the spatula sometimes occasions the introduc- tion of alcoholic bubbles into the interior of the mass of oil. These are, however, easily removed by means of the syringe. 31. Now, having formed a polyhedron, let us see what will happen if we gradually remove some of the liquid. Let us take, for instance, the cube, the solid framework of which, with its suspending wire, is represented at Fig. 11.* Let the point of the syringe be applied near the middle of one of the faces, and let a small quantity of the oil be drawn up. All the faces will immediately become depressed simul- taneously and to the same extent, so that the super- ~ ficial square contours will form the bases of six similar hollow figures. We _ should have imagined this to have been the case for the maintenance of equality between the pressures. If fresh portions of the liquid are removed, the faces will become more and more hollowed; but to understand what happens when this manipulation is continued, we must here enunciate a preliminary proposition. Suppose that a square plate of iron, the sides of which are of the same length as the edges of the metallic frame, is introduced into the vessel, and that a mass of oil equal in volume to that which is lost by one of the faces of the cube is placed in con- tact with one of the faces of this plate; I say that the liquid, after having become extended upon the plate, will present in relief the same figure as the * The edges of all the frames which I used were 7 centimetres in length. 246 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS face of the modified cube presents in intaglio. Then, in fact, in passing from the hollow surface to that in relief, the radii of curvature corresponding to each point will only change their signs without changing in absolute value; conse- quently, (§ 8,) since the condition of equilibrium is satisfied as regards the first of these surfaces, it will be equally so with regard to the second. Now, let us imagine a plane passing through one side of the plate, and tan- gentially to the surface of the liquid which adheres to it at that point. As ‘Jong as this liquid is in small quantity, we should imagine—and experiment bears us out—that the plane in question will be strongly inclined towards the plate; but if we gradually increase the quantity of liquid, the angle comprised between the plane and the plate will also continue to increase, and instead of being acute, as before, will become obtuse. Now, so long as this angle is less than 45°, the convex surface of the liquid adhering to the plate will remain identical with the coneave surfaces of the mass attached to the metallic frame, and suitably diminished ; but beyond this limit, the coexistence in the frame of the six hollow identical surfaces with the surface in relief becomes evidently impossible, for these surfaces must mutually intersect each other. Thus, when the withdrawal of the liquid from the mass forming the cube is continued, a point is attained at which the figure of equilibrium ceases to be realizable in accordance with the ordinary law of pressures. We then meet with a new verification of the principle enunciated in § 28, 2. e., that the formation of layers commences. These layers are plane; they commence at each of the wires of the frame, and connect the remainder of the mass to the latter, which continues to present six concave surfaces. In fact, we can, imagine that, by this modification of the liquid figure, the existence of the whole of this in the metallic frame again becomes possible, as also the equilibrium of the system ; for there is then no further impediment to the concave surfaces assuming that form which accords with the ordinary law of pressures ; and, on the other hand, in supposing the layers to be suffi- ciently thin, the pressure belonging to them might be equal to that which corresponds to these same concave sur- faces, (§ 25.) On removing still further portions of the liquid, the layer will continue to enlarge, whilst the full mass which oc- cupies the middle of the figure will diminish in volume, and this mass can thus be reduced to very minute dimen- sions: Fig. 12 represents the entire system in this latter state. It is even possible to make the little central mass disappear entirely, and thus to obtain a complete laminar system; but for this purpose certain precautions must be taken, which I shall now point out. When the central mass has become sufliciently small, the point of the syringe must first be thoroughly wiped; otherwise the oil adheres to its exterior to a certain height, and this attraction keeps a cer- tain quantity of oil around it, which the instrument cannot absorb into its interior. In the second place, the point of the syringe must be depressed to such an extent that it nearly touches the inferior surface of the little mass. During the suction this surface is then seen to become raised, so as to touch the orifice of the instrument, and the latter then absorbs as much of the alco- | holic mixture as of the oil; but this is of no consequence, and the minute mass is seen to diminish by degrees, so as at last completely to disappear. The system, then, consists of twelve triangular layers, each of which commences at one of the wires of the frame, and all the summits of which unite at the centre of the figure; it is represented in Fig. 13. But this system is only formed during the action of the syringe. If, when this is complete, the point of the instrument is slowly withdrawn, an additional lamina of a square form is seen WITHDRAWN FROM THE ACTION OF GRAVITY. DAT to be developed in the centre of the figure, (Fig.14.) This, then, is the defini- tive laminar system to which the liquid cube is reduced by the gradual diminu- tion of its mass. Fig 13 Bly. 4. 32. In the preceding experiment, as in that of paragraph 23, the thickness of the layers is at first greater than that which would correspond to equilibrium. If, then, the system were left to itself whilst it still contains a central mass, we should imagine that one portion of the liquid of the layers would be slowly driven towards this mass, and that the layers would gradually become thinner. Moreover, it always happens that one or the other of the latter increases after some time, undoubtedly for the reason which we have already pointed out, (§ 26.) Hence, for the perfect success of the transformation of the cube into the laminar system, one precaution, which has not yet been spoken of, must be attended to. It consists in the circumstance that, from the instant at which the layers arise, the exhaustion of the liquid must be continued as quickly as possible until the central mass has attained a certain degree of minuteness. In fact, as soon as the formation of the layers commences, their tendency to become thinner also begins to be developed; and if the operation is effected too slowly, the system might break before it was completed. When the central mass is sufficiently redueed—and experience soon teaches us to judge of the suitable point—the action of the syringe must be gradually slackened, and at last the other precautions which we have mentioned must be taken. We are able, then, to explain the rupture of the layers so long.as there is a large or small central mass; but when the laminar system is complete, we do not at the first glance see the reason why the thickness of the layers diminishes, and consequently why destruction of the system takes place. Nevertheless the rupture ultimately takes place in this as in the other case, and the time during which the system persists rarely extends to half an hour. In ascertaining the cause of this phenomenon, it must be remarked that the intersections of the different layers cannot occur suddenly, or be reduced to simple lines: it is evident that the free transition between two liquid surfaces could not be thus established in a discontinuous manner. ‘These transitions must, therefore, be effected through the intermedium of minute concave surfaces, and with a little attention we can recognize that, in fact, this really takes place. We can then understand that the oil of the layers ought also to be driven towards the places of junction of the latter; and consequently the absence of the little central mass does not prevent the gradual attenuation of the layers, and the final destruction of the system. 33. If, during the action of the syringe, when the system shown in Fig. 13 has been attained, instead of slowly withdrawing the instrument, it is suddenly detached by a slight shake in a vertical direction, the additional layer is not developed; but the little mass in Fig. 12 is seen to be reproduced very rapidly. This fact confirms in a remarkable manner the explanation which we have given in the preceding paragraph. In fact, at the moment at which the point of the instrument is separated from the system, the latter may be considered as composed of hollow pyramids. Now it also follows, from causes relating to . 248 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS their continuity, that the summits of these pyramids should not constitute sim- ple points, but little concave surfaces. But as the curvatures of these minute surfaces are very great in every direction, they would give rise to still far less pressure than those which establish the transitions between each pair of sur- faces of the layers; for in the latter there is no curvature in one direction. The oil of the layers will, therefore, be driven with much greater force towards the centre of the figure than towards the other parts of, the junctions of these layers. Again, the twelve layers terminating in this same centre, the oil flows there simultaneously from a large number of sources. ‘These two concurrent causes ought then, in conformity with experiment, to produce the rapid reappearance of the small central mass; and we can understand why it is impossible to obtain the complete system of the pyramids otherwise than during the action of the syringe. 34. All the other polyhedric liquids become transformed, like the cube, into laminar systems when the mass of which they are composed is gradually diminished. Among these systems some are complete; the others still contain very small masses, which cannot be made*to disappear entirely. Analogous considerations to those which we applied with regard to the cube would show, in each case, that the formation of layers commences as soon as the hollow surfaces which would correspond to the ordinary law of pressures cease to be able to coexist in the solid frame. Figs. 15, 16, 17, and 18 represent the Pay 15. Fig. 18 laminar systems resulting from the triangular prism, the hexahedral prism, the tetrahedron and the pyramid with a square base, these systems being supposed to be complete. They are all formed of plane layers, commencing at each of the metallic wires; and that of the hexahedral prism, as is ‘shown, contains an additional layer in the centre of the figure. Fig, 9. Fig. 20. a RET TI 33. The system arising from the regular octohedron presents a singular exception, which I have not been able to explain. The layers of which this system is composed are curved, and form a fantastical group, of which it is difficult to give an exact idea by graphic representations, Fig. 19 exhibits WITHDRAWN FROM THE ACTION OF GRAVITY. 249 ~~ them projected upon two rectangular vertical planes; and it is seen that the aspects of the system observed upon two adjacent sides are inverse as regards each other. The formation of this system presents a curious peculiarity. At the commencement of the operation all the faces of the octohedron become simultaneously hollow; the layers in progress of formation are plane, and arranged symmetrically, so that the system tends towards the form represented at Fig. 20. But when a certain limit is attained, a sudden change occurs, the layers become curved, and the system tends to assume the singular form which we have mentioned. I have several times repeated the experiment, varying the circumstances as much as possible, and the same effects are always pro- - duced. In the course of this memoir I shall point out another process for obtaining laminar systems; it is an extremely simple one, and has moreover the advan- tage of producing all the systems in a complete state. 36. In concluding our observations upon polyhedric liquids, I shall remark that the triangular prism may be employed to produce the phenomena of dis- persion. In this way a beautiful solar spectrum may be obtained by means of a prism with liquid faces. But as the effect only depends upon the excess of the refracting action of the oil above that of the alcoholic liquid, to obtain a considerably extended spectrum the angle of refraction of the prism must be obtuse; an angle of 110° gives a very good result. Moreover, it is evidently requisite that the faces of the prism should be perfectly plane, which is obtained by using a carefully made frame; by establishing exact equilibrium between the density of the liquids; and, lastly, by arresting the action of the syringe exactly at the proper point. 950 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS Other figures of Revolution besides the Sphere. Liquid Cylinder. 37. Let us now endeavor to form some new liquid figures. Those best _ adapted to theoretical considerations would be figures terminated by surfaces of revolution other than the sphere and lenticular figures, which we have already studied. Surfaces of revolution enjoy simple properties in regard to the radii of the greatest and least curvature at every point; we know that one of these two radii is the radius of curvature of the meridional line, and that the other is re that portion of the normal to this line which is included between the point under — consideration and the axis of revolution. We shall now endeavor to obtain figures of this nature. 38. Let our solid system be composed of two rings of iron Fig. 20% wire, equal, parallel, and placed opposite to each other. One of these rings rests upon the base of the vessel by three feet composed of iron wire; the other is attached, by means of an intermediate piece, to the axis traversing the central stopper, so that it may be approximated to or removed from the former by depressing or elevating this axis.* The system formed by these two rings is represented in Plate VII, Fig. 20 dis; the diameter of those which I employed was 7 centimeters. After having raised the upper ring as much as possible, let a sphere of oil, of a slightly larger diameter than that of the rings, be formed, and conducted towards the lower ring in such a manner as to make it adhere to the entire circum- ference of the latter; then depress the upper ring until it comes into contact with the liquid mass, and the latter is uniformly attached to it. When the mass has thus become adherent to the system of the two rings, let the upper ring be slowly raised; when the two rings are Fig. 24. at a proper distance apart, the liquid will then assume the form the vertical projection of which is represented in Fig. 21, in which the lines a 4 and ¢ d are the projections of the rings. ‘The two portions of the surface which are respect- _ ively applied to each of the rings are convex spherical seg- ments; and the portion ineluded between the two rings con- stitutes a figure of revolution, the meridional curve of which, as is shown, is convex externally. We shall recur, in the following series, to this part of the liquid figure. If we now continue gradually to raise the upper ring, the curvature of the two extremities and the meridional curvature of the intermediate portion will be diminished; and if there is exact equilibrium be- tween the density of the oil and the surrounding liquid, the Lig. XZ. surface included between the two rings will be seen to assume a perfectly cylindrical form, (Fig. 22.) The two bases of the = liquid figure are still convex spherical segments, but their cur- —, vature is less than in the preceding figure. If the interval _____ between the rings be still further increased, it is evident that - = the surface included between them would lose the cylindrical form, and that a new figure would result. This is what occurs; but the consideration of the figure thus produced must be deferred. Instead, then, of immediately increasing the distance between the rings, let us commence by adding a certain quantity of oil to the mass, which will again _,. In the experiments which we are now about to describe, the short axis represented in Fig. 2 of the preceding memoir, and which has hitherto answered our purpose, must be replaced by another of about 15 centimeters in length. WITHDRAWN FROM THE ACTION OF GRAVITY. 251 render the surface included between the rings convex. Let us then gradually elevate the upper ring, and we shall produce a cylinder of greater height than Fig, 22. Fig, 24. the first. If we repeat the same manipulation a suitable number of times, we shall ultimately obtain the cylinder of the greatest height which our apparatus permits. I have in this manner obtained a perfectly cylindrical mass 7 cen- timeters in diameter, and about 14 centimeters in height, (Fig. 23.) To allow of the cylinder of this considerable height being perfect, it is requisite that per- fect equality be established between the densities of the oil and the alcoholic liquid. As a very slight difference in either direction tends to make the mass ascend or descend, the latter assumes, to a more or less marked extent, one of the two forms represented in Fig. 24. Even when the cylindric form has been obtained by the proper addition of alcohol of 16°, or absolute alcohol, as ocea- sion may require, (§ 24 of the preceding memoir,) slight changes in tempera- ture are sufficient to alter and reproduce one of the above two forms. 39. Let us now examine the results of these experiments in a theoretical point of view. First, it is evident that a cylindrical surface satisfies the generat condition of equilibrium of liquid figures, because the curvatures in it are the same at every point. Moreover, such a surface being convex in every direction except in that of the meridional line, where there is no curvature, the pressure corresponding to it ought to be greater than that corresponding to a plane sur- face. The same conclusions are deducible from the general formule (2) and (3) of paragraphs 4 and 5. In fact, as we have already stated in paragraph 37, one of the quantities R and R’ is the radius of curvature of the meridional line, and the other is the portion of the normal to this line included between the point under consideration and the axis of revolution. Now, in the case of the cylinder, the meridional line being a right line,/its radius of curvature is every- where infinitely great; and, on the other hand, this same right line being parallel to the axis of revolution, that portion of the normal which constitutes the second radius of curvature is nothing more than the radius itself of the 1 1 cylinder. Hence it follows that one of the terms of the quantity Rt PR dis- appears, and that the other is constant; this same quantity is, therefore, con- stant, and consequently the condition of equilibrium is satisfied. Now, if we denote by 2 the radius of the cylinder, the general value of the pressure for this surface would become . P Al st tad. Now 2 being positive because it is directed towards the interior of the liquid, (§ 4,) the above value is greater than P, z. e., than that which would correspond 252 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS to a plane surface. It is, therefore, evident that the bases of our liquid cylinder must necessarily be convex, as is shown to be the case by experiment; for as equilibrium requires that the pressures should be the same throughout the whole extent of the figure, these bases must produce a greater pressure than e that which corresponds to a plane surface. Our plane figure, then, fully satisfies theory; but verification may be urged | still further. Theory allows us to determine with facility the radius of those spheres of which the bases form a part. In fact, if we represent this radius by. z, the formula (1) of paragraph 4 will give, for the pressure corresponding to the spheres in question, fl P+A.-—. Zz Now, as this pressure must be equal to that corresponding to the cylindrical surface, we shall have se ‘ Se yee ae from which we may deduce = 2A, Thus the radius of the curvature of the spherical segments constituting the bases is equal to the diameter of the cylinder. ‘ Hence, as we know the diameter, which is the same as that of the solid rings, we may calculate the height of the spherical segments; and if by any process we afterwards measure this height in the liquid figure, we shall thus have a verification of theory even as regards the numbers. We shall now investigate this subject. 40. If we imagine the liquid figure to be intersected by a meridional plane, the section of each of the segments will be an are belonging to a circle, the radius of which will be equal to 24, according to what we have already stated, and the versed sine of half this are will be the height of the segment. If we suppose the metallic filaments forming the rings to be infinitely small, so that each of the segments rests upon the exact circumference of the cylinder, the chord of the above are will also be equal to 24; and if we denote the height of the segments by #, we shall have h=i(2— V3) =0.268. 2. Now, the exact external diameter of my rings, or the value of 22, correspond- ing with my experiments, was 71.4 millimeters, which gives 49.57 millime- ters. But as the metallic wires have a certain thickness, and the segments do not rest upon the external circumference of the rings, it follows that the chord of the meridional arc is a little less than 2A, and that, consequently, the true theoretical height of the segments is a little less than that given by the pre- ceding formula. ‘To determine it exactly, let us denote the chord by 2c, which will give A=22— V4? —c*. Now, let us remark that the meridional plane intersects each of the rings in two small circles to which the meridional are pf the spherical segment is tan- gential, and upon each of which the chord of this are intercepts a small circular segment. he meridional are being tangential to the sections of the wire, it follows that the above small circular segments are similar to that of the spheri- cal segment; and as the chord of the latter differs but very slightly from the radius of the circle to which the are belongs, the chords of the small circular segments may be considered as equal to the radius of the small sections, which radius we shall denote by 7. It is moreover evident that the excess of the ex-- ternal radius of the ring over half the chord ¢ is nothing more than the excess WITHDRAWN FROM THE ACTION OF GRAVITY. 253 of the radius 7 over half the chord of the small circular segments, which half . 3 Y 1 chord, in accordance with what we have stated, is equal to 37° Thence we 1 1 »geta Sao 5 whence c == ay and we have only to substitute this value ~ inthe preceding formula to obtain the true theoretical value of 4. The thick- ness of the wire forming my rings is 0.74 millimeters; hence a7 = 0.18 milli- meters, which gives as the true theoretical height of the segments under these } circumstances, . h=9.46 millimeters. I may remark that it is difficult to distinguish in the liquid figure the precise limit of the segments, @. e., the circumferences of contact of their surfaces with those of the rings. To get rid of this inconvenience, I measured the height of the segments, commencing only at the external planes of the rings; 7. e., in the ease of each segment, commencing at a plane perpendicular to the axis of revo- lution, and resting upon the surface of the ring on that side which is opposite the summit of the segment. The quantity thus measured is evidently equal to the total height minus the versed sine of the small cireular segments which we have considered above ; consequently these small circular segments being simi- lar to that of the spherical segment, we obtain for the determination of this versed sine, which we shall denote by f the proportion “=~, which in the 2” ease of our liquid figure gives f—=0.05 millimeters, whence h—f=9.41 millimeters. This, then, is definitively the theoretical value of the quantity which was required to be measured. 41. Before pointing out the process which I employed for this purpose, and communicating the result of the operation, I must preface a few important remarks. If the densities of the alcoholic mixture and of the oil are not rigor- ously equal, the mass has a slight tendency to rise or descend, and the height of one of the segments is then a little too great, whilst that of the other is a little too small; but we can understand that if their difference is very small, an exact result may still be obtained by taking the mean of these two heights. We thus avoid part of those preliminary experiments which the establishment of perfect equality between the two densities requires. But one’ circumstance which requires the greatest attention is the perfect homogeneity of each of the two liquids. If this condition be not fulfilled with regard to the alcoholic mix- ture, 2. e., if the upper part of this mixture be left containing a slightly greater proportion of alcohol than the lower portion, the liquid figure may appear regular and present equal segments; all that is required for this is, that the mean density of that part of the mixture, which is at the same level as the mass, must be equal to the density of the oil; but under these circumstances _ the level of the two segments is too low. In fact, the oil forming the upper | segment is then in contact with a less dense liquid than itself, and, conse- quently, has a tendency to descend, whilst the opposite applies to the oil form- ing the inferior segment.* Heterogeneity of the liquid produces an opposite effect, 2. e., it renders the height of the segments too great. In fact, the least dense portions rising to the upper part of the mass tend to lift it up, whilst the most dense portions descend to the lower part, and tend to depress it. Now, —— * By intentionally producing very great heterogeneity in the alcoholic mixture, (§ 9 of the preceding memoir, ) and employing suitable precautions, a perfectly regular cylinder may be formed, the bases of which are absolutely plane. 954 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS the quantities of pure alcohol, and that at 16° added to the alcoholic mixture «to balance the mass, necessarily produce an alteration in the homogeneity of the oil; for, in the first place, the oil during these operations being in contact with mixtures which are sometimes more, sometimes less charged with alcohol, must absorb or lose some of this by its surface; in the second place, these same additions of alcohol to the mixture diminish the saturation of the latter with the oil, so that it removes some of it from the mass; and this action is undoubt- edly not equally exerted upon the two principles of which the oil is composed. Hence, before taking the measures, the different parts of the oil must be inti- mately mixed together, which may be effected by introducing an iron spatula into the mass, moving it about in it in all directions, and this for a long time, because the mixture of the oil can only be perfectly effected with great diffi- culty on account of its viscidity. ; T'o avoid the influence of the reactions which render the oil heterogeneous, the operations must be conducted in the following manner: The mass being introduced into the vessel and attached to the two rings, and the equality of the densities being perfectly established, allow the mass to remain in the aleo- holic liquid for two or three days, re-establishing from time to time the equi- librium of the densities altered by the chemical reactions and the variations of temperature. Afterwards remove the two rings from the vessel, so that the mass remains free; remove almost the whole of this, by means of a siphon, into a bottle, which is to be carefully corked; withdraw with the syringe the small portion of oil which is left in the vessel, and reject this portion. Next replace the two rings, and mix the alcoholic liquid perfectly ; then again introduce the oil into the vessel, taking the precaution of enveloping the bottle containing it with a cloth several times folded, so that the temperature may not be sensibly altered by the heat of the hand.* Then attach the mass to the lower ring only, the upper ring being raised as much as possible; mix the oil intimately, as we have said above; then depress the upper ring, cause the mass to adhere to it, elevate it so as to form an exact cylinder, and proceed immediately to the measurement. * The following is the reason why the oil must be removed from the vessel before employ- ing it for the experiment. After having remained a considerable time in the alcoholic liquid, the oil becomes enveloped by a kind of thin pellicle; or, more strictly speaking, the super- ficial layer of the mass has lost part of its liquidity, an effect which undoubtedly arises from the unequal action of the alcohol, upon the principles of which the oil is composed. The necessary result of this is, that the mass loses at the same time part of its tendency to assume a determinate figure of equilibrium, which tendency must, therefore, be completely restored to it. This is why the oil is withdrawn by the siphon. In fact, the pellicle does not pene- trate the interior of the latter, and during its contraction continues to envelop the small por- tion remaining; so that after the latter has been removed by the syringe, which ultimately absorbs the pellicle itself, we get completely rid of the latter. Before using the siphon, the thickness and consistence of the pellicle are too slight to enable us distinctly to perceive its presence; but when the operation of the siphon is nearly terminated, and the mass is thus considerably reduced, we find that the surface of the latter forms folds, hence implying the existence of an envelope. Moreover, when the siphon is removed, the small residuary mass, which then remains freely suspended in the alcoholic liquid, no longer assumes a spherical form, but retains an irregular aspect, appearing to have no tendency to assume any regular form. This indifference to assume figures of equilibrium, arising from a diminution in the liquidity of the superficial layer, constitutes a new and curious proof of the fundamental principle relating to this layer, (§§ 6 bis and 10 to 16.) M. Hagen (Mémoire sur la Surface des Liquides, in the Memoirs of the Academy of Berlin, 1845) has observed a remarkable fact, to which the preceding appears to be related. It consists in this, that the surface of water, left to itself for some time, undergoes a peculiar modification, in consequence of which the water then rises in capillary spaces to elevations which are very distinctly less than is the case when its surface is exempt or freed from this alteration. This fact might, perhaps, * be explained by admitting that the water dissolves a small proportion of the substance of the solid with which it is in contact, and that the external air acts chemically at the surface of the Iquid upon the substance dissolved, thus giving rise to the formation of a slight pellicle which modities the effects of the molecular forces. WITHDRAWN FROM THE ACTION OF GRAVITY. 255 42. The instrument best suited for effecting the latter operations in an exact manner is undoubtedly that which has received the name of cathetometer, and which, as is well known, consists of a horizontal telescope moving along a ver-— tical divided rule. The distance comprised between the summits of the two segments is first measured by the aid of this instrument; the distance included between the external planes of the two rings (§ 40) is then measured by the same means. ‘The difference between the first and the second result evidently gives the sum of the two heights, the mean of which must be taken; and, con- sequently, this mean, or the quantity sought, 2 —f, is equal to half the differ- ence in question. _ The determination of the distance between the external planes of the rings requires peculiar precautions. First, as the points of the rings at which we must look are not exactly at the external surface of the figure, the oil inter- osed between these points and the eye must produce some effects of refraction, which would introduce a slight error into the value obtained. 'To avoid this inconvenience, we need only expose the rings by allowing the liquids,to escape from the vessel by the stop-cock, (note 2 to § 9,) then remove the minute portions of the liquid which remain adherent to the rings by passing lightly over their surface a small strip of paper, which must be introduced into the vessel through the second aperture. The drops of alcoholic liquid remaining attached to the inner surface of the interior side of the vessel must also be absorbed in the same manner. In the second place, as it would be difficult for the rings to be rigorously parallel, their distance must be measured from two opposite sides of the system, and the mean of the two valves thus found taken. The follow- ing are the results which J obtained: The mensuration of the distance between the summits gave first, in four successive operations, the values 76.77, 76.80, 76.85, and 76.75 millimeters, the mean of which is 76.79 millimeters. But after the alcoholic liquid had been again agitated for some time, to render its homo- geneity more certain, two new measurements taken immediately afterwards gave 77.05 and 77.00 millimeters, or a mean of 77.02 millimeters. The distance between the external planes of the rings was found, on the one hand, by two observations, which agreed exactly, to be 57.73 millimeters; on the other hand, two observations furnished the values 57.87 and 57.85 millimeters, or as the mean 57.86 millimeters. Taking, then, the mean of these two results, we get 57.79 millimeters as the value of the distance between the centres of the ex- ternal planes. Hence, if we assume the first of the two values obtained for the distance of the summits, 76.79 millimeters, we find h—f= te Eee = 9.50 millimeters ; and if from the second result, 77.02 millimeters, we find 77.02 — 57.79 h—f=——_o = 9.61 millimeters. These two elevations evidently differ but little from 9.41 millimeters, the altitude deduced from theory, (§ 40;) in the first case the difference does not amount to the ;4,th part of this theoretical value, and in the second it hardly exceeds ;2;ths. These differences undoubtedly arise from slight remains of heterogeneity in the liquids; it is probable that in the first case neither of the two liquids was absolutely homogeneous, and that the two contrary effects which thence resulted (§ 41) partly neutralized each other, whilst in the second case, the alcoholic liquid being rendered perfectly homogeneous, the effect of the slight heterogeneity of the oil exerted its full influence. However this may be, these differences in each case are so small that we may consider experiment as in accord- ance with theory, of which it evidently presents a very remarkable confirmation. 43. Mathematically considered, a cylindrical surface extends indefinitely in the direction of the axis of revolution. Hence it follows that the cylinder 956 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS figure of equilibrium. Hence also, if the liquid mass were free, it could not assume the cylindrical form as the figure of equilibrium; for the volume of this mass being limited, it would be necessary that the cylinder should be termi- nated on both sides by portions of the surface presenting other curvatures, which would not admit of the law of continuity. But this heterogeneity of curvature, which is impossible when the mass is free, becomes realizable, as our experi- ments show, through the medium of solid rings. As each of these renders the curvatures of the portions of the surface resting upon it (§ 20) independent of each other, the surface comprised between the two rings may then be of cylin- drical curvature, whilst the two bases of the figure may present spherical curvatures. We therefore arrive at the very remarkable result, that with a liquid mass of a limited volume we may obtain isolated portions of figures of equilibrium, which in their complete state would be extended indefinitely. 44. With the view of obtaining a cylinder in which the proportion between the height and the diameter was still greater than that in Fig. 23, I replaced the rings previously employed by two others, the diameter of which was only 2 centimeters. I first tried to make a cylinder 6 centimeters in height, 7. e., the height of which was thrice the diameter; and in this operation 1 adopted a slightly different process from that of paragraph 38. The uniformity in the ~ density of the two liquids being accurately established, I first gave the mass of oil a somewhat larger volume than that which the cylinder would contain; having then attached the mass to the two rings, I-elevated the upper ring until it was at a distance of 6 centimeters from the other; this distance was measured by a scale introduced into the vessel and kept in a vertical position by the side of the liquid figure. In consequence of the excess of oil, the meridional line of the figure was convex externally; and as there was still a slight difference between the densities, this convexity was not symmetrical in regard to the two rings. I corrected this irregularity by successive additions of pure alcohol and alcohol of 16°, an operation which requires great circumspection, and towards the end of which these liquids could only be added in single Pig. 23. drops. ‘The figure being at last perfectly symmetrical, 1 carefully re- moved the excess of oil by applying the point of the syringe to a point at the equator of the mass, and in this manner I obtained a perfect cylinder. Subsequently, after having added some oil to the mass, I increased the distance between the rings until it was equal to 8 centi- meters, 2, €., to four times their diameter. The oil was in sufficient quantity to allow of the meridional line of the figure being convex ex- ternally ; but the curvature was not perfectly symmetrical, and I en- countered still greater difficulties in regulating it than in the preceding case. ‘The defect in the symmetry being ultimately corrected, the meri- dional convexity presented a versed sine of about 8 millimeters, (Fig. 25.) I then proceeded to the removal of the excess of oil; but before the versed sine was reduced to 2 millimeters, the figure appeared to have a tendency to become thin at its lower part and to swell out at the upper part, as if the oil - had suddenly become slightly increased in density. At this moment I . withdrew the syringe, so as to be enabled to observe the effect in ques- \ tion better; the change in form then became more and more pronounced; 4 the lower part of the figure soon presented a true strangulation, the neck of which was situated nearly at a fourth part of the distance be- tween the rings, (Fig. 26;) the constricted portion continued to narrow gradually, whilst the upper part of the figure became swollen; finally, the liquid separated into two unequal masses, which remained respect- ively adherent to the two rings; the upper mass formed a complete sphere, and the lower mass a doubly convex lens. The whole of these phenomena lasted a very short time only. 7 included between the two rings constitutes one portion only of the complete — a - 7 WITHDRAWN FROM THE ACTION OF GRAVITY. 257 With a vicw to determine whether any particular cause had in reality pro- duced the alteration of the densities, I approximated the rings; then, after having reunited the two liquid masses, I again carefully raised the upper ring, ceasing at the height of 74 centimeters, so that the versed sine of the meridional convexity was slightly greater than when this was 8 centimeters. The figure was then found to be perfectly symmetrical, and it did not exhibit any tendency to deformity ; whence it follows that the uniformity in the densities had not experienced any appreciable alteration. I recommenced, with still more care, the experiment with that figure which was 8 centimeters in height; and I was enabled to approach the cylindrical form still more nearly; but before it was attained, the same phenomena again presented themselves, except that the alteration in form was effected in an inverted manner, @. e., the figure became narrow at the upper part: and dilated at the base; so that after the separation into two masses, the perfect sphere existed in the lower ring and the lens in the upper ring. On subsequently uniting, as before, the two masses, and placing the rings at a distance of 74 centimeters apart, the figure was again obtained in a regular and permanent form. ‘Thus when we try to obtain between two solid rings a liquid cylinder the height of which is four times the diameter, the figure always breaks up spontaneously, without any apparent cause, even before it has attained the exactly cylindrical form. Now as the cylinder is necessarily a figure of equilibrium, whatever may be the proportion of the height to the diameter, we must conclude that the equilibrium of a cylinder the height -of which is four times the diameter is unstable. As the shorter cylinders which I had obtained did not present analogous effects, I was anxious to satisfy myself whether the cylinders were really stable. I therefore again formed a cylinder’ 6 centimeters in height with the same rings; but this, when left to itself for a full half hour, presented a trace only of alteration in form, and this trace ap- peared about a quarter of an hour after the formation of the cylinder, and did not subsequently increase, which shows that it was due to some slight accidental cause. The above facts lead us then to the following conclusions: 1st, that the cyl- inder constitutes a figure the equilibrium of which is stable when the proportion between its height and its diameter is equal to 3, and with still greater reason when this proportion is less than 3; 2d, the cylinder constitutes a figure the equilibrium of which is unstable when the proportion of its height to its diameter is equal to 4, and with still greater reason when it exceeds 4; 3d, consequently there exists an intermediate relation, which corresponds to the passage from stability to instability. We shall denominate this latter proportion the Limit of the stability of the cylinder. 45. These conclusions, however, are liable to a well-founded objection. Our liquid figure is complex, because its entire surface’ is composed of a cylindrical - portion and of two portions which present a spherical curvature. Now we can- not affirm that these latter portions exert no influence upon the stability or the instability of the intermediate portion, and consequently upon the value of the proportion which constitutes the limit between these two states. To allow of the preceding conclusions being rigorously applicable to the cylinder, it would be requisite that the figure should present no other free surface than the cylin- drical surface, which is easily managed by replacing the rings by entire disks. I effected this substitution by employing disks of the same diameter as the pre- ceding rings, but the results were not changed; the cylinder, 6 centimeters in height, was well formed, and was found to be stable; whilst the figure.8 centi- meters in height began to change before becoming perfectly cylindrical, and was rapidly destroyed. The final result of this destruction did not, however, consist, as in the case of the rings, of a perfect sphere and a double convex lens, but, as evidently ought to have been the case, of two unequal portions of spheres, 17s . 258 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS ¢ respectively adherent to the two opposite solid surfaces. The limit of the stability of the cylinder, therefore, really lies between 3 and 4. The experiments which we have just related are very delicate, and require some skill. In this, as in all other cases of measurements, the ‘oil must be allowed to remain in the alcoholic mixture for two or three days, then the pel- licle must be removed from it, (note to p. 254;) afterwards, when the mass, after having been again introduced into the vessel, has been attached to the two solid disks, some time must be allowed to elapse in order that the two liquids may be exactly at the same temperature; moreover, it must be understood that the experiments should be made in an apartment the temperature of which remains as constant as possible. Lastly, it is scarcely necessary to add, that when the alcoholic liquid is mixed, after having added small quantities of pure alcohol or alcohol at 16°, the movements of the spatula should be very slow, so as to avoid the communication of too much agitation to the mass of oil; we are’ even sometimes compelled momentarily to depress the upper disk, so as to give greater stability to the mass, and thus to prevent the movements in question from producing the disunion. a 46. It might be asked whether the want of symmetry, which ‘3 constantly seen in the spontaneous modification of the above unstable figures, is the result of a law which governs these figures ; or whether it simply arises, as we should be led to believe at first sight, from imperceptible differences still existing be- tween the densities of the two liquids, which differences acting upon unstable figures might produce this want of symmetry, notwithstanding their extreme minuteness After having concluded the preceding experiments, I imagined that to solve the question in point, all that would be requisite would be to arrange matters so that the axis of the figure, instead of being vertical, as in the above experiments, should have a horizontal direction. In fact, in the latter case, the slightest difference between the densities ought to have the effect of slightly curving the figure, but evidently cannot give the liquid any tendency to move in greater quantity towards one extremity of the figure than the other; whence it follows, that if the spontaneous alteration of the figure still occurs unsymmetrically, this can only be owing to a peculiar law. On the other hand, if the figure really tends of itself to change its form un- symmetrically, it is clear that, in the case of the vertical position of the axis, the effect of a trace of difference between the densities ought to concur with that of the instability, and thus to accelerate the moment at which the figure com- mences to alter spontaneously. Consequently, on avoiding this extraneous cause by the horizontal direction of the axis of the figure, we may hope to approximate more nearly to the cylindrical form, or even to attain it exactly; we can, moreover, understand that the difficulty in the operations will be found to be considerably diminished. I therefore constructed a solid system, presenting two vertical disks of the same diameter, placed parallel with each other, at the same height, and opposite each other. Each of these disks is sup- ported by an iron wire fixed normally to its centre, then bent vertically down- wards, and the lower extremities of these two wires are attached to a hori- zontal axis furnished with four small feet. This system is represented in perspective in Fig. 27. ‘The diameter of the disks is 30 millimeters, but the distance which separates them is not ara four times this diameter. I thought that by approximating the figure more to the limit of stability, the operations WITHDRAWN FROM THE ACTION OF GRAVITY. 259 would require still less trouble; the distance in question is only 108 millime- ters, so that the relation between the length and the diameter of the liquid eylinder which would extend between the two disks would be equal to 3.6. We shall now detail the results obtained by the employment of this system. In the first place, the operations were much more easily performed.* In the second place, the figure still had a tendency to deformity before it had been rendered perfectly cylindrical ; but this tendency always exhibited itself unsym- metrically, as in the vertical figures; from which circumstance alone we might _ conclude that the unsymmetrical nature of the phenomenon is not occasioned by a difference between the densities of the two liquids. In the third place, by a little management, I have pursued the experiment further, and succeeded in forming an exact cylinder.t ‘This lasted for a moment; it then began to be narrowed at one part of its length, becoming dilated at the other, like the verti- eal figures; and the phenomenon of disunion was completed in the same manne, giving rise ultimately to two masses of different volumes. I repeated the experiment several times, and always with the same results, except that the separation occurred sometimes on.one, sometimes on the other side of the middle of the length of the figure. However, although the phe- nomenon is produced in an unsymmetrical manner with regard to the middle of the length of the figure, whether horizontal or vertical, on the contrary there is always symmetry with regard to the axis; in other words, throughout the dura- tion of the phenomenon the figure remains constantly a figure of revolution. We may add here, that in the horizontal figure the respective lengths of the constricted and dilated portions appear to be equal; we shall show, in the fol- lowing series, that this equality is rigorously exact, at least at the commencement of the phenomenon. It is now evident that the alteration in the form of these cylinders is really the result of a property which is inherent in them. We shall hereafter deduce this property as a necessary consequence of the laws which govern a more general phenomenon. It moreover results from the above experiment that the proportion 3.6 is still greater than the limit of stability, so that the exact value of the latter must lie between the numbers 3 and 3.6. It is obvious that this method of experimént might be employed to obtain a closely approximative determination of the value in question; I propose doing this hereafter, and I shall give an account of the result in the following series, when I shall have to return to the question of the limit of stability of the cylinder. 47. In the unstable cylinders which we have just formed, the proportion of the length to the diameter was inconsiderable ; but what would be the case if we were to obtain cylinders of great length relatively to their diameter? Now, under certain circumstances, figures of this kind, more or less exactly cylindri- eal, may be realized, and we shall proceed to see what the results of the spon- taneous rupture of equilibrium are. * The two disks ‘in this solid system being placed at an invariable distance from each other, it is necessary, in making a mass of oil, the volume of’ which is not too great, adhere to them, to employ an extra piece consisting of a ring of iron wire of the same diameter as the disks, supported by a straight wire of the same metal, the free extremity of which is held in the hand. By means of this ring the mass, which has been previously attached to one of the disks, is drawn out until it is equally attached to the other; tho ring is then removed. The latter removes a small portion of the nfass at the same time; but on leaving the vessel it leaves this portion in the alcoholic liquid. It is then removed by means of the syringe. + To effect this the following proceeding must be adopted for the removal of the excess of oil. The operation is at first carried on with a suitable rapidity until the figure begins to alter in form; the end of the point of the syringe is then drawn gently along the upper part of the mass, proceeding from the thickest to the other portion. This slight action is sufficient to move a minute quantity of oil towards the latter, and thus to re-establish the symmetry of the figure; a new absorption is then made, the figure again regulated, and these proceed- ings are continued until the exactly cylindrical form is attained. 260 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS A fact which I described in paragraph 20 of the preceding memoir, and which I shall now describe more in detail, affords us the means of obtaining a cylinder of this kind, and of observing its spontaneous destruction. Wheti some oil is introduced by means of a small funnel into an alcoholic mixture containing a slight excess of alcohol, and the oil is poured in sufficiently quick to keep the funnel full, the liquid forms, between the point of the funnel and the bottom of the vessel where the mass collects, a long train, the diameter of which continues toyincrease slightly from the upper to the lower part, so as to form a kind of very elongated cone, which does not differ much from.a cylinder.* ‘This nearly cylindrical figure, the height of which is considerable in proportion to the diameter, _ remains without undergoing any perceptible alteration so long as the oil of which it consists has suflicient rapidity of transference; but when the oil is no longer poured into the funnel, and-consequently the motion of transference is retarded, the cylinder is soon seen to resolve itself rapidly into a series of spheres, which are perfectly equal in diameter, equally distributed, and with their centres arranged upon the right line forming the axis of the cylinder. To obtain perfect success, the elements of the experiment should be in certain proportions. The orifice of the funnel which I used was about 3 millimeters in diameter, and 11 centimeters in height. It rested upon the neck of a large bottle containing the alcoholic mixture, and its orifice was plunged a few milli- meters only beneath the surface of the liquid. Lastly, the length of the cylinder of oil, or the distance between the orifice and the lower mass, was nearly 20 centimeters. Under these circumstances, three spheres were constantly formed, the upper of which remained adherent to the point of the funnel; the latter was therefore incomplete. We may add, that the excess of alcohol contained in the mixture should neither be too great nor too small; the proper quantity is found by means of a few preliminary trials. 48. The constancy and regularity of the result of this experiment complete then the proof that the phenomena to which the spontaneous rupture of equilib- rium of an unstable liquid cylinder gives rise are governed by determinate laws. In this same experiment, the transformation ensues too rapidly to allow of its phases being well observed; but the phenomena presented to us by larger and less elongated cylinders, 7. e., the formation of a dilatation and constriction in juxtaposition, and equal or nearly so in length, the gradual increase in thickness of the dilated portion and the simultaneous narrowing of the constricted portion, &e., authorize us to conclude that in the case of a cylinder the length of which is considerable in proportion to the diameter, the following order of things takes place: the figure becomes at first so modified as to present a regular and uniform succession of dilated. portions, separated by constricted portions of the same length as the former, or nearly so. ‘This alteration, the indications of which are very slight, gradually becomes more and more marked, the constricted por- tions gradually becoming narrower, whilst the dilated portions increase in thick- ness, the figure remaining a figure of revolution ; at last the constrictions break, and each of the various parts of the figure, which are thus completely isolated from each other, acquire the spherical form. We must add, that the termination of the phenomenon is accompanied by a remarkable peculiarity, of which we have not yet spoken; but as it only constitutes, so to speak, an accessory por- tion of the general phenomenon, we shall transfer the description of it to a subsequent part of this memoir, (see § 62.) ; 49. It might be asked why, in the experiment which we have last described, the cylinder is only resolved into spheres when the rapidity of the transference of liquid of which it is composed is diminished. In fact, we cannot understand how a motion of transference could give stability to a liquid figure which in a ST * The slight increase in diameter depends upon the retardation which the resistance of the surrounding liquid occasions in the movement of the oil. ot WITHDRAWN FROM THE ACTION OF GRAVITY. 261 state of repose was unstable. In explaining this apparent peculiarity, we must remark that, as the spontaneous transformation of an unstable cylinder is effected under the action of continued forces, the rapidity with which the phenomenon occurs ought to be accelerated ; this may be, moreover, casily verified in experi- ments relating to larger and less elongated cylinders; this same rapidity ought, _ therefore, always to be very minute at the commencement of the phenomenon. Now, in the case in question, as the changes in figure occur in the liquid of the cylinder whilst this liquid is animated by a movement of transference, it is evident, from what we have stated, that if this movement of transferenee is sufficiently rapid, the changes of form could only acquire a very slightly marked development during the passage of the point of the funnel to the mass accumu- lated at the bottom of the vessel; so that, the liquid being continually renewed, there will be no time for any alteration in form to become very perceptible to the eye. Hence, so long as the rapidity of the flow is sufficiently great, the liquid figure will appear to retain its almost cylindrical form, although its length is considerable in comparison with its diameter. On the other hand, when the velocity of the transference is sufficiently small, there will be time for the alterations in form to take place in a perfect manner, and we shall be able to see the cylinder resolve itself into spheres throughout the whole of its length. 50. We shall now describe another method of experimenting, which allows us to observe the result of the transformation under less restrained and more regular conditions in some respects than those of the preceding experiment, and which will, moreover, lead us to new consequences as regards the laws of the phenomenon. We shall first succinctly describe the apparatus and the opera- tions, and afterwards add the necessary details. The principal parts of which the apparatus consists are: Ist, a rectangular plate of plate-glass, 25 centimeters in length, and 20 in breadth; 2d, two strips of the same glass, 13 centimeters in length, and * millimeters in thickness, perfectly prepared and polished at the edges; 3d, two ends of copper wire, about 1 millimeter in thickness, and 5 centimeters in length; these wires should be perfectly straight, and one extremity of each of them should be cut very accurately, then carefully amalgamated. The plate being placed horizontally, the two strips are laid flat upon its surface and parallel with its long sides, so as to leave an interval of about a centimeter between them; the two copper wires are then introduced into this, placing them in a right line in the direction of the length of the strips, and in such a manner that the amalgamated extremi- ties are opposite to, and a few centimeters distant from, each other. A globule of very pure mercury, from 5 to 6 centimeters in diameter, is next placed be- tween the same extremities; the two strips of glass are then approximated until they touch the wires, so as only to leave between them an interval equal in width to the diameter of these wires. The little mass of mercury, being thus compressed laterally, necessarily becomes elongated, and extends on both sides towards the amalgamated surfaces. If it does not reach them, the wires are made to slide towards them until contact and adhesion are established. The wires are then moved in opposite directions, so as to separate them from each other, which again produces elongation of the little liquid mass and dimi- nution of its vertical dimensions. By proceeding carefully, and accompanying the operation with slight blows given with the finger upon the apparatus to facilitate the movements of the mercury, we succeed in extending the little mass until its vertical thickness is everywhere equal to its horizontal thickness, i. é., to that of the copper wires. Thus the mercury forms a liquid wire of the same diameter as the solid wires to which it is attached, and from 8 to 10 cen- timeters in length. This wire, considering the small size of its diameter, which renders the action of gravitation insensible in comparison with that of molecular attraction, may be considered as exactly cylindrical; so that in this manner we obtain a liquid cylinder, the length of which is from 80 to 100 times its diame- 262 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS ter, and attached by its extremities to solid parts, which cylinder preserves its form so long as it remains imprisoned between the strips of glass. Weights are next placed upon the parts of the two copper wires which project beyond the extremities of the bands, so as to maintain these wixes in firm positions ; lastly, by means which we shall point out presently, the two strips of glass are raised vertically. At the same instant, the liquid cylinder, being liberated from its shackles, becomes transformed into a numerous series of isolated spheres, ar- . ranged in a straight line in the direction of the cylinder from which they origi- nated.* Ordinarily the regularity of the system of spheres thus obtained is not perfect; the spheres present differences in their respective diameters and in the distances which separate them; this undoubtedly arises from slight acci- dental causes, dependent upon the method of operation; but the differences are sometimes so small that the regularity may be considered ds perfect. As regards the number of spheres corresponding to a cylinder of determinate length, it varies in different experiments; but these variations, which are also due to slight accidental causes, are comprised within very small limits. 51. Let us now complete the description of the apparatus, and add some details regarding the operations. As the plate of glass requirés to be placed in a perfectly horizontal position, it is supported for this purpose upon four feet with screws. A small transverse strip of thin paper is glued to each of the extremities of the lower surface of the strips of glass, in su¢h a manner that the strips of glass resting upon the plate through the medium of these small pieces, of paper, their lower surface is not in contact with the surface of the plate. Without this precaution, the strips of glass might contract a certain adhesion to the plate, which would introduce an obstacle when the strips are raised vertically. Moreover, the latter are furnished, on their upper surface and at a distance of 6 millimeters from each of their extremities, with a small screw placed vertically in the glass with the point upwards, firmly fixed to it with mastic, and rising 8 - millimeters above its surface. These four screws are for the purpose of receiving the nuts which fix the strips to the system by means of which they are elevated. This system is made of iron; it consists, in the first place, of two rectangular plates, 55 millimeters in length, 12 in breadth, and 3 in thickness. Each of them is pierced, perpendicularly to its large surfaces, by two holes, so situated, that on placing each of these plates transversely upon the extremities of the two strips of glass, the screws with which the latter are furnished fit into these four holes. ‘The screws being long enough to project above the holes, nuts may then be adapted to them, so that on screwing them the strips of glass become fixed in an invariable position with regard to each other. The holes are of an elongated form in the direction of the length of the iron plates; hence, after having loosened the nuts, the distance between the two strips of glass may be increased or diminished without the necessity of removing the plates. A vertical axis, 5 centimeters in height, is implanted upon the middle of the upper surface of each of the plates; and the upper extremities of these two axes are connected by a horizontal axis, at the middle of which a third vertical axis commences ; this is directed upwards, and is 15 centimeters in length. The section of the latter axis is square, and it is 5 millimeters in thickness. When the nuts are screwed up, it is evident that the strips of glass, the iron plates, and the kind of fork which connects them, constitute an invariable system. The long vertical axis serves to direct the movement of this system; with this view, it passes with very slight friction through an aperture of the same section as itself, and 5 centimeters in length, pierced in a piece which is fixed very firmly by a suitable support 10 centimeters above the plate of glass. Lastly, the perforated piece is provided laterally with a thumb-screw, which allows the axis to be screwed ete te ER ed oe * We may remark that the conversion of a metallic wire into globules by the electric dis- charge must undoubtedly be referred to the same order of phenomena. - WITHDRAWN FROM THE ACTION OF GRAVITY. 263 into the tube. By this arrangement, if all parts of the apparatus have been carefully finished, when once the little nuts have been screwed up, the two strips of glass can only move simultaneously in a parallel direction to each other, and always identically in the same direction perpendicular to the plate of glass. When the liquid cylinder is well formed, and the weights are placed upon the free portions of the copper wires, the finger is passed under the hori- zontal branch of the fork, and the movable system is raised to a suitable dis- tancé above the plate of glass; it is then maintained at this height by means of the thumb-screw, so as to allow the result of the transformation of the cylin- der to be observed. As the amalgamation of the copper wires always extends slightly upon their convex surface, the latter is coated with varnish, so that the amalgamation only occurs upon the small plane section. It would be almost impossible to judge by simple inspection of the exact point at which the separation of the copper wires from each other, to allow of the liquid attaining a cylindrical form, should be discontinued. ‘To avoid this difficulty, the length of the cylinder is given beforehand, and this length is marked by two faint _ seratches upon the lateral surface of one of the strips of glass; the weight of the globule of mercury, which is to form a cylinder of this diameter and of the length required, is then determined by calculation from the known diameter of the wire; lastly, by means of a delicate balance, the globule to be used in the experiment is made exactly of this weight. All that then remains to be done is to extend the little mass until the extremities of the copper wires between which it is included have reached the marks traced upon the glass. Lastly, in making a series of experiments, the same mercury may be used several times if the isolated spheres are united into a single mass at the end of each observa- tion. However, after a certain number of experiments, the mercury appears to lose its fluidity, and the mass always becomes disunited at some point, in spite of all possible precautions, before it has become extended to the desired length, which phenomena arise from the solid wires imparting a small quantity of cop- per to the mercury. The latter must then be removed, the plates of glass and the strips cleaned, and a new globule taken. ‘The amalgamation of the wires also sometimes requires to be renewed. 52. By means of the above apparatus and methods, I have made a series of experiments upon the transformation of the cylinders; but before relating the _results, it is requisite for their interpretation that we should examine the phe- nomenon a little more closely. Let us imagine a liquid cylinder of considerable length in proportion to its diameter, and attached by its extremities to two solid bases; let us suppose that it is effecting its transformation, and let us consider the figure at a period of the phenomenon anterior to the separation of the masses, 7. e., when this figure is still composed of dilatations alternating with constrictions. As the surfaces of the dilatations project externally from the primitive cylindrical sur- face, and those of the constrictions on the contrary are internal to this same surface, we can imagine in the figure a series of plane sections perpendicular to the axis, and all having a diameter equal to that of the cylinder; these sections will evidently constitute the limits which separate the dilated from the con- stricted portion, so that each portion, whether constricted or dilated, will be terminated by two of them; moreover, as the two solid bases are necessarily part of the sections in questiou, each of these bases should occupy the very extremity of a constricted or dilated portion. This being granted, three hypo- theses present themselves in regard to these two portions of the figure, 7. e., to those which rest respectively upon each of the solid bases. In the first place, we may suppose that both of the portions are expanded. In this case each of the constrictions will transfer the liquid which it loses to the two dilatations immediately adjacent to it; the movements of transport of the liquid will take place in the same manner throughout the whole extent of the figure, and the 264 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS : transformation will take place with perfect regularity, giving rise to isolated spheres exactly equal in diameter, and at equal distances apart. ‘This regu- larity will not, however, extend to the two extreme dilatations; for as each of these is terminated on one side by a solid surface, it will only receive liquid from the constriction which is situated on the other side, and will, therefore, acquire less development than, the intermediate dilatations. Under these cir- cumstances, then, after the termination of the phenomenon, we ought to find two portions of spheres respectively adherent to two solid bases, each present- ing a slightly less diameter than that of the isolated spheres arranged between _ them. In the second place, we may admit that the terminal portions of the figure are, one a constriction and the other a dilatation. ‘The liquid lost by the first, not being then able to traverse the solid base, will necessarily all be driven into the adjacent dilatation; so that, as the latter receives all the liquid necessary to its development on one side only, it will receive none from the opposite side ; consequently all the liquid lost by the second constriction will flow in the same manner into the second dilatation, and so on up to the last dilatation. The distribution of the movements of transport will, therefore, still. be regular throughout the figure, and the transformation will ensue in a perfectly regular manner. This regularity will evidently extend even to the two terminal por- tions, at least so long as the constrictions have not attained their greatest depth; but beyond that point this will not exactly be the case, for independ- ence being then established between the masses, each of the dilatations, except- ing that which rests upon the solid base, will enlarge simultaneously on both sides, so as to pass into the condition of the isolated sphere, by appropriating to itself the two adjacent semi-constrictions, whilst the extreme dilatation can enlarge on one side. Consequently, after the termination of the phenomenon, we should find, at one of the soild bases, a portion of a sphere of but little less diameter than that of the isolated spheres, and at the other base a much smaller portion of a sphere, arising from the semi-constriction which has remained attached to it. : Lastly, in the third place, let us suppose that the terminal portions of the figure were both constrictions, in which case, after the termination of the phe- nomenon, a portion of a sphere equal to the smallest of the two above would be left to each of the solid bases. In this case, to be more definite, let us start from one of these terminal constrictions ; for instance, that of the left. All the liquid lost by this first constriction being driven into the contiguous dilata- tion, and being sufficient for-its development, let us admit that all the liquid lost by the second constriction also passes into the second dilatation, and so | - on; then all the dilatations, excepting the last on the right, will simply acquire their normal development; but the right dilatation, which, like each of the others, receives from that part of the constriction which precedes it the quan- tity of liquid necessary for its development, receives in addition the same quantity of liquid from that part of the constriction which is applied to the adjacent solid, so that it will be moré voluminous than the others. Hence it is evident, in the case in point, that the opposed actions of the two terminal con- strictions introduce an excess of liquid into the rest of the figure. Now, what- ever other hypothesis may be made respecting the distribution of the move- ments of transport,-it must always happen either that the excess of volume is simultaneously distributed over all the dilatations, or that it only augments the dimensions of one or two of them; but the former of these suppositions is evidently inadmissible, on account of the complication which it would require in the movements of transport; hence we must admit the second, and then the isolated spheres will not all be equal. Thus this third mode of transformation would necessarily of itself induce a cause of irregularity; and, moreover, it would not allow of a uniform distribution of the movements of transport, be- Se WITHDRAWN FROM THE ACTION OF GRAVITY. 265 _ cause there would be opposition in regard to these movements, at least in the terminal constrictions. It may, therefore, be regarded as very probable that the transformation takes place according to one or the other of the two first methods, and never accord- ing to the third, 2. e., that things will be so arranged that the figure which is transformed may have for its terminal portions either two dilatations, or one constriction and one dilatation, but not two constrictions. In the former case, as we have seen, the movement of the liquid of all the constrictions would ensue on both sides simultaneously; and in the second this movement would occur in all in one and the same direction. If this is really the natural arrange- ment of the phenomenon, we can also understand how it will be preserved even when it is disturbed in its regularity by slight extraneous causes. Now, this, as we shail see, is confirmed by the experiments relating to the mercurial cylinder. Although the transformation of this cylinder has rarely yielded a perfectly regular system of spheres, | have found in the great majority of the results either that each of the soild bases was occupied by a mass little less in diameter than the isolated spheres, or that one of the bases was occupied by a mass of this kind and the other by a much smaller mass. 53. For the sake of brevity, let us denominate divisions of the cylinder those portions of the figure each of which furnishes a sphere, whether we consider these portions in the imagination as in the cylinder itself, before the com- mencement of the transformation, or whether we take them during the accom- plishment of the phenomenon, 7. e.,during the modifications which they undergo in arriving at the spherical form. The length of a division is evidently that distance which, during the transformation, is comprised between the necks of two adjacent constrictions; consequently it is equal to the sum of the lengths of a dilatation and two semi-constrictions. Let us, therefore, see how the length in question, z. e., that of a division, may be deduced from the result of an experiment. Let us suppose the transformation to be perfectly regular, and let A be the length of a division, / that of the cylinder, and m the number of isolated spheres found after the termination of the phenomenon. Each of these spheres being furnished by a complete division, and each of the two terminal masses by part of a division, the length 7 will consist cf » times A, plus two fractions of 4. To estimate the values of these fractions, we must recollect that the length of a constriction is exactly or apparently equal to that of a dila- tation, (§ 46 ;) now, in the first of the two normal cases, (§ 52,) 7. e., when the masses remaining adherent to the bases after the termination of the phenomenon are both of the large kind, each of them evidently arises from a dilatation plus half a constriction, therefore three-fourths of a division; the sum of the lengths of the two portions of the cylinder which have furnished these masses is, there- fore, equal to once and a half 2, and we shall have in this case 7 ==(m + 1.5) 4, whence A ra ieee In the second case, 2. e., when the terminal masses con- n fa sist of one of the large and the other of the small kind, the latter arises from a semi-constriction, or a fourth of a division, so that the sum of the lengths of the portions of the cylinder corresponding to these two masses is equal to 2; con- sequently we shall have 4— Sere As the respective denominators of these two expressions represent the num- ber of divisions contained in the total length of the cylinder, it follows that this number will always be either simply a whole number, or a whole number . and a half. On the other hand, as the phenomenon is governed by determinate laws, we can understand that for a cylinder of given diameter composed of a given liquid, and placed under given circumstances, there exists a normal length which the divisions tend to assume, and which they would rigorously assume if the total length of the cylinder were infinite. If. then, it happens 266 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS that the total length of the cylinder, although limited, is equal to the product of the normal length of the divisions by a whole number, or rather a whole number plus a half, nothing will prevent the divisions from exactly assuming this normal length. If, on the other hand, which is generally the case, the total length of the cylinder fulfils neither of the preceding conditions, we should think that the divisions would assume the nearest possible to the normal length; and then, all other things being equal, the difference will evidently be as much ‘less as the divisions are more numerous, or, in other words, as the cylinder is longer. We should also believe that the transformation would adopt that of the two methods which is best adapted to diminish the difference in question, and this is also confirmed by experiment, as we shall see presently. Hence, although, as I have already stated, the transformation of the cylinder of mer- cury almost always ensues in one of the two normal methods, the result is rarely very regular; we must, therefore, admit that slight accidental disturbing causes. in general render the divisions formed in any one experiment unequal in length; but then the expressions of 2 obtained above evidently give in each experiment the mean length of these divisions, or, in other words, the common length which the divisions would have taken if the transformation had occurred in a perfectly regular manner, giving rise to the same number of isolated spheres and to the same state of the terminal masses. Lastly, since the third method of transformation presents itself, 2. e., since it sometimes happens that each of the bases is occupied by a mass of the small kind, if we would leave out of consideration the particular cause of irregularity inhe- rent in this method, (the preceeding paragraph,) and find the corresponding expression of A, it need only be remarked that each of the terminal masses then proceeds from a semi-constriction or the fourth of a division, which will l n+ 0.5 54. I shall now relate the results of the experiments. The diameter of the copper wires, consequently of the cylinder, was 1.05 millimeter. I first gave the cylinder a length of 90 millimeters, and repeated the experiment ten times, noting after each the number of isolated spheres produced, and the state of the masses adherent to the bases; I then calculated for each result the correspond- ing value of the length of a division, by means of that of the three formule of the preceding paragraph which refers to this same result, I afterwards made ten more experiments, giving the cylinder a length of 100 millimeters, and alo calculated the corresponding values of the length of a division. ‘Che table con- tains the results furnished by these cylinders, and the values deduced for the length ofadivision. I only obtained a pertectly regular result in one ease in each series; I have placed an * opposite the corresponding number of isolated spheres. evidently give 2 == Length of the cylinder 90 millimeters. Length of the cylinder 100 millimeters. Number of} Masses adherent to the bases. | Length |Number of] Masses adherent to the bases. Length isolated of a isolated ofa spheres. division. | spheres, ; division. millims. millims, UU ON AT OCS eon. oan alain en la 7.83 11 | One large and one small..| 8.u. m9 HAV OALT Osos oe |! 6.67 14 | Twowlateere sce t-oeea 6.45 er bworsmalbosos s ok! le! - 7,20 14° | "Dwotlanocde2: tse 6.45 i MEMO oes 220! stn 28 5,45 14). Rwodlanoees.:s\: aesinee 6.45 14} SOWOMBN OO. ji otss2 6 ok oe: 5.81 *14 | One large und one Hae Jhonson, Oe) ERO cts ie cian oni « 7.2 13 | One large and one sma!f..; 7.14 dt }| ‘Pwo latge.=+:.-..2 2... 7.20 11 | Pwo largest 4.2. YR 8.00 12 | One large and one small..| 6.92 14 | One large and one small..| 6.67 13 Two llatge sarah lie test 6.21 13 Two latgess 43 s-ceee. 6.90 AL s | Ra largees son aerate eas 7.20 10 8.69 TL WOUBI POs) cciiiees | ‘ WITHDRAWN FROM THE ACTION OF GRAVITY. 267 This table shows, in the first place, that the different values obtained for the length of a division are not so far removed from each other as to prevent our perceiving a constant value, the uniformity of which is only altered by the influence of slight accidental causes. In the second place, out of twenty ex- periments, it happened once only that the masses adherent to the bases were both of the small kind. In the third place, both the perfectly regular results have given identically the same value for the length of a division; this value, expressed approximatively to two decimal places, is 6.67 millimeters; but its exact expression is 63 millimeters; for the operation to be effected consists, in the case of the first series, in the division of 90 millimeters by 13.5, and, in the case of the second series, in the division of 100 millimeters by 15. As the two lengths given to the cylinder are considerable in proportion to the diameter, and consequently the numbers of division are tolerably large, this value, 6% milli- meters, ought very nearly, if not exactly, to constitute that of the normal length of the divisions. It is seen, moreover, that to give the divisions this closely approximative or exact value of the normal length, the transformation has chosen, iu one case the first, in the other case the second method. 55. Let us pursue our inquiry into the laws of the phenomenon with which we are engaged ;, we shail soon make an important application of them, and it will then be understood why so extensive a development is given to this part of our work. It might be regarded as evident @ priori that two cylinders formed of the same liquid and placed in the same circumstances, but differing in diameter, would tend to become divided in the same manner, 2. ¢., that the respective nor- mal lengths of the divisions would be to each other in the proportion of the diameters of these cylinders. In order to verify this law by experiment, I procured some copper wires, the diameter of which was exactly double that of the first, therefore equal to 2.1 millimeters, and I made with them a new series of ten experiments, giving the cylinder a length of 100 millimeters. This series also furnished me with only a single perfectly regular result, which I have denoted as before by an * placed opposite the corresponding number of isolated spheres. The following is the table relating to this series: Number / Masses adherent to the bases. Length isolated of a spheres, division. ame manoAy STN BLL.) ene te aap pales ria aoe ai atl aIaiPmc ein a Soe Su lziarss See SMRPOUBI OG. 56 2 iene Belctiaay cp anise 2-5 nae 4m Ses oe ENE cree Peleus Jarve and one small2o 2.2003 2-6 uses cue est 7c ee De omelarce and onolsmall) 22.0 22 2oi Sse Ses Sane oes wees Wade he oe Orem BIOL So 22282 SRS SB beri whem nim apele bien atm Sasi ania ae eee i WOMANS. 2 3.5 se em eepinaeee diene ae - mae ane pa —~ - ae inne emn inna an 6 | One jarge and one small.....-------. ----2- e+ 0~-- eee o-- oa == === === ©! ne laree and‘one mall’. —2 2222). 2. 2. cee eee ee eee rar SHiall 2... xls. Soetoro tang sisi eetobay Sotetten as aes dp te Se 6 | One large and one small -...--.----------.- gf Se eae ie Ses ala on ee By stopping at the second decimal place, we have, as is evident, 13.33 milli- meters for the value of the length of a division corresponding to the perfectly regular result; but as the operation which yields it consists in the division of 100 by 7.5, the value when perfectly expressed is 134 millimeters. This then is very nearly, if not exactly, the normal length of the divisions of this new cylinder; now this length, 13$ millimeters, is exactly twice the length, 63 millimeters, which belongs to the divisions of the cylinder of the preceding 268 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS. paragraph; these two lengths are therefore, in fact, in the proportion to each other of the diameters of the two cylinders. As the perfectly regular result of the above table has given a mass of the larger kind to each base, it follows, that to enable the divisions of the cylinder itself to assume their normal length, or the nearest possible length to this, the transformation has necessarily ensued according to the former method; whilst in regard to a cylinder the diameter of which is a half less, and the total length of which is the same, 00 millimeters, the transformation ensued according to the second method, (§ 54.) ; Here, also, the case in which there are two masses of the small kind to the solid bases is the least frequent, although it occurred twice. Lastly, the differ- ent values of the length of a division are more concordant than in the second series relating to the first diameter, and consequently show the tendency towards a constant value better; we also see that the normal length is that which is most frequently reproduced. 56. According to the law which we have just established, when the nature of the liquid and external circumstances do not change, the,normal length of the divisions is proportional to the diameter of the cylinder; or, in other words, the proportion of the normal length of the divisions to the diameter of the cylinder is constant. As we have seen, the diameter of the cylinder in paragraph 54 was 1.05 mil- limeters, and the normal length of its divisions was very little, less than 6.67 millimeters ; consequently, when the liquid used is mercury and the cylinder rests upon a plate of glass, the value of the constant proportion in question is 6.67 1.05 To ascertain whether the nature of the liquid and external circumstances exert any influence upon this proportion, we shall now determine the value of the latter in the case of a cylinder of oil formed in the aleoholic mixture, which may be effected, at least approximatively, with the aid of the result of the experiment in paragraph 47. 'To simplify the considerations, we shall suppose that the transformation docs not commence until the rapidity of transference has entirely ceased. he point of the funnel, on the one hand, and the section by which the imperfect liquid cylinder is in contact with the mass which collects at the bottom of the vessel, on the other hand, may then be regarded as playing the part of the two bases of the figure. Now it is evident that, as regards the second of these bases, the last portion of the figure which is transformed should be a constriction ; for if it constituted a dilatation, there would be discontinuity of the curvature at the junction of the respective surfaces of the latter andthe large mass, which is inadmissible. But the same reason does not apply to the other base; and experiment shows that. in this case a dilatation is formed, be- cause after the termination of the phenomenon we always find at the point of the funnel a mass comparable to the isolated spheres. Hence in this experiment the transformation ensues according to the second method. Therefore, asthe: whole length of the figure is about 200 millimeters, and as the transformation constantly yields two isolated spheres, the mean length of the divisions has : “ ‘ : 200i +h (§ 53) for its approximative value - millimeters = 66.7 millimeters; I say e —= 6.35, which approximates closely. the mean length, because, as the diameter of the figure increases slightly from the summit towards the base, the divisions are probably not exactly equal in length: It must be added here, that the transformation ensues under cireum- stances which are always identical, and consequently, in the absence of acci- dental disturbing causes, the above quantity ought to represent the normal length of the divisions, or the nearest possible length to the latter. Now, I WITHDRAWN FROM THE ACTION OF GRAVITY. 269 estimate the mean diameter of the figure before the transformation at about 4 7]: 66.7 millimeters; we should consequently have = 16.7 as the approximative value of the proportion between the normal length of the divisions and the diameter of the cylinder. This is, therefore, approximatively the constant pro- portion sought in the case of a cylinder of oil formed in the alcoholic mixture ; now this proportion, as is evident, is much greater than that which belongs to the case of a cylinder of mercury resting upon a plate of glass. In fact, the length 66.7 millimeters may differ somewhat materially from the normal length; for if, on the one hand, the whole length of the figure of oil is considerable in regard to its diameter, on the other hand, the number of divisions which form there is very small. Let us then see, for instance, what is the least value which the normal length of these divisions may have. We must in ihe first place remark, that in this case, notwithstanding the absence of disturbing causes, the third method of transfor:nation is possible; in fact, as the lower constriction is adherent to a liquid base, nothing can prevent the oil which it loses from traversing this base to reach the large mass, so that in the third method, also, the direttion of the movements of transport may be the same in regard to all the constrictions, (§ 52.) 'lhis granted, as the denominator of the expression which gives the length of one division can only vary by half units, (53,) and as the length which we have found resulted from the division of 200 millimeters by 3, it follows that the length immediately below would be © 5 millimeters — 57.1 millimeters, which would correspond to three isolated spheres and a transformation disposed according to the third method. But as. matters do not take place in this manner, since there are never more than two isolated spheres formed, and the transformation always ensues according to the second method, we must conclude that the’ normal length of the divisions approximates more closely to the length found, 66.7 millimeters, than the length 57.1 millimeters. If, then, the normal length is greater than the first of these two quantities, it must at least be more than their mean, 7. e.,61.9 millimeters ; consequently the relation of the normal length of the divisions and the diameter 61. of the cylinder is necessarily greater than ae ea 15.5; now this latter num- ber considerably exceeds the numbcr 6.35, which corresponds to the mercurial cylinder. Thus, the proportion of the normal length of the divisions to the diameter of the cylinder varies, sometimes according to the nature of the liquid, sometimes according to external circumstances, at others according to both these elements. 57. But I say that there is a limit below which this proportion caniot descend, and that this is exactly the limit of stability. Let us imagine a liquid cylinder of sufficient length in proportion to its diameter, comprised between two solid bases, and the transformation of which is taking place with perfect regularity. Suppose, for the sake of clearness, that the phenomenon ensucs according to the second method, or, in other words, that the terminal portions of the figure con- sist one of a constriction, the other of a dilatation; then, as we have seen. (§ 52,) the regularity of the transformation will extend to these latter portions; z. e., the terminal constriction and the dilatation will be respectively identical with the portions of the same kind of the rest of the figure. Let us then take the figure at that period of the phenomenon at which it still presents constrictions and dilatations, and let us again consider the sections, the diameter of which is equal to that of the cylinder, (§ 52.) Let us start from the terminal constricted por- tion ; the solid base upon which this rests, and which constitutes the first of the sections in question, will-occupy, as we have shown, the origin of the constric- 270 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS tion itself; we shall then have a second section at the origin of the first dilatation ; a third at the origin of the second constriction; a fourth at the origin of the second dilatation, and’so on; so that all the sections of the even series will occupy the origins of the dilatations, all those of the odd series the origins of — the constrictions. The interval comprised between two consecutive sections of the odd series will therefore include a constriction and a dilatation; and as the figure begins with a constriction and terminates with a dilatation, it is clear that its entire length will be divided into a whole number of similar intervals. In consequence of the exact regularity which we have supposed to exist in the transformation, all the intervals in question will be equal in length; and.as the moment at which we enter upon the consideration of the figure may be taken arbitrarily from the origin of the phenomenon to the maximum of the depth of the constrictions, it follows that the equality of length of the intervals subsists during the whole of this period, and that, consequently, the sections which terminate these intervals preserve during this period perfectly fixed positions. Besides the parts of the figure respectively contained in each of the intervals undergoing identically and simultaneously the same modifications, the volumes of all these parts remain equal to each other; and as thefr sum is always equal to the total volume of the liquid, it follows that, from the origin of the trans- formation to the maximum of depth of the constrictions, each of these partial volumes remains invariable, or, in other words, no portion of liquid passes from any one interval into the adjacent ones. Thus, at the instant at which we consider the figure, oh the one hand, the two sections which terminate any one interval will have preserved their primitive positions and their diameters ; and on the other hand these sections will not have been traversed by any por- tion of liquid. Matters will then have occurred in each interval in the same manner as if the two sections by which it is terminated had been solid disks. But the transformation cannot.ensue between two solid disks, if the proportion of the distance which separates the disks to the diameter of the cylinder is less than the limit of stability; the proportion of the length of our intervals and the diameter of the cylinder cannot then be less than this limit. Now, the length of an interval is evidently equal to that of a division; for the first, in .accord- ance with what we have seen above, is the sum of the lengths of a dilatation and a constriction ; and the second is the sum of the lengths of a dilatation and two semi-constrictions, (§ 53;) the proportion of the length of a division to the diameter of the cylinder cannot then be less than the limit of stability; and we may remark here that this conclusion is equally true, whether the divisions are able or not to assume exactly their normal length. 58. Let us now attempt to ascertain the influence of the nature of the liquid and that of external cireumstances, commencing with the latter. Our liquid cylinder of mercury, along the whole of the line at which it touches the plate of glass, must contract a sight adherence to this plate, which adherence must more or less impede the transformation. T’o discover whether this resistance exerted any influence upon the normal length of the divisions, consequently upon the proportion of the latter to the diameter of the cylinder, a simple means presented itself, viz., to augment this resistance. ‘To arrive at this result, | arranged the apparatus in such a manner as to remove only one of the strips of glass, so that the liquid figure then remained simultaneously in co tact with the plate and the other strip. I again repeated the experiment ten times, using copper wires 1.05 millimeters in diameter, and giving the cylinder a length of 100 millimeters. The following were the results : ey a: > WITHDRAWN FROM THE ACTION OF GRAVITY. avs Number o Masses adherent to the bases. Length isolated ofa spheres. division. emcmedanre and ono smalls .co8s oc ote See pee 710,00 Bae neuarce and-oneismall). 32.26 odes tosgeceeebet sss ccs ous eee 11.41 Suan wires and one Small. wia< 6 6s cemmmnin suuied cue ee Ste ae wide ow Baheurle 10.00 eperte Mare ANG ONG SHOAL ecb oe eels paw de pe baal win stm bon em cannon 11.11 ce) LSBU Ue ae aes SES ES ES gy pl lg a 8.69 Seecooarees and one smalls iie) eet ee I eo. 2 11.41 Sauonelarco god. one: small \ diac ieiay boo wataten Wee on ee 11.11 ret || Layne Se eR RE He ee mire o Bec OCS cs Pee eemetee See 10.53 aero tnree And ONG SNiall o-oo oto oie. a chpts pee tomes ae ees nae os 11.11 SNES ADE Sema ee sean ar cee ee ee ee ae eae eee ae scans 13.33 It is evident that the different values of the length of a division, with a sin- gle exception, are all obviously greater than all those which relate to a cylinder of the same diameter, the surface of which only touches the glass by a single line, (§ 54.) We must thence conclude that, all other things being the same, the length of the divisions increases with the external resistance; consequently, under the action of the same resistance, this length is necessarily greater than it would be if the convex surface of the cylinder had been perfectly free. In the above series neither of the results appears to be very regular; but we can readily understand that the mean of the values of the third column will approach the normal length of the divisions. This is, moreover, confirmed by the tables in §§ 54 and 55. If we take in the former the respective means of the values of the two series, we find for one 6.77 millimeters, and for the other 7.17 millimeters, quantities, the first of which is nearly equal to the length 6.67 millimeters, which may be considered as the normal length, and from which the second does not differ much; and if likewise we take the relative mean in the following table, we find 13.15 millimeters, a quantity very near the length 13.33 millimeters, which in the case of the second table may also be regarded as the normal length. Now, the corresponding mean in the above table is 10.81 millimeters ; consequently, in the case of two lines of contact we have — == 10.29 as the approximate value of the proportion of the normal 1.0 length of the divisions to the diameter of the cylinder, whilst in the case of a single line of contact we found only 6.35. Hence the proportion between the normal length of the divisions and the diameter of the cylinder increases by the effect of an external resistance. 59. Let us proceed to the influence of the nature of the liquid. All liquids are more or less viscid; 7.¢., their molecules do not enjoy perfect mobility with regard to each other. Now, this gives rise to an internal resistance, which must also render the transformation less easy; and as external resistances increase the length of the divisions, we can understand that the viscidity will act in the same manner; consequently, all other things being equal, the propor- tion now under consideration will inerease with this viscidity. But, on the other hand, with equal curvatures, the intensities of the forces which produce the transformation vary with the nature of the liquid; for these intensities depend, in the case of each liquid, upon that of the mutual attraction of the molecules. Now, it is clear that the viscidity will exert so much more influence upon the length of the divisions as the intensities of the forces in question are less. Thus, leaving external resistances out of the question, the proportions of the -normal length of the divisions to the diameters will be greater in proportion to the viscidity of the liquid and the feebleness of the configuring forces. 272 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS The intensities of the configuring forces corresponding to different liquids ‘may be compared numerically for the same curvatures. In fact, let us first bear in mind that the pressure corresponding to one element of the superficial layer, and reduced to unity of the surface, is expressed by (§ 4,) A fl T eo a(atw)y Now, the value of the part P of this pressure being the same for all the elements of the superficial layer, and the pressures being transmitted throughout the mass, this part P will always be destroyed, whether equilibrium exists in the liquid figure or not; so that the active part of the pressure (that which consti- tutes the configuring force) will have for its measure simply = G J nv) Hence it is evident that when the curvatures are equal, the intensity of the configuring force arising from one element of the superficial layer is propor- tional to the coeflicient A. Now, this coefficient is the same as that which enters into the known expression of the elevation or depression of a liquid in a capillary tube: consequently the measures relating to this elevation or depres- sion will give us, in the case of each liquid, the value of the coefficient in ques- tion. Hence we may also say that the proportion of the normal length of the divisions to the diameter of the cylinder will be greater as the liquid is more viscid and as the value of A which corresponds to the latter diminishes. For instance, oil is much more viscid than mereury; on the other hand, it would be easy to show that the value of A is much less for the first than for the second of these two liquids; lastly, this value must be much diminished in regard to our figure of oil by the presence of the surrounding alcoholic liquid, — | the mutual attraction of the molecules of the two liquids in contact diminishing the intensities of the pressures, (§ 8.) This is why the proportion belonging to a cylinder of oil formed in the alcoholic mixture considerably exceeds that be- longing to a cylinder of mercury resting upon a plate of glass, notwithstanding the slight external resistance to which the latter is subjected. 60. 1t follows from this discussion concerning the resistances that the smallest value which the proportion of the normal length of the divisions to the diameter of the cylinder could be supposed to have corresponds to that case in which there is simultaneously complete absence of external resistance and of viscidity; and, after the demonstration given in § 57, this least value will be at least equal to the limit of stability. Now, as all liquids are more or less viscid, it follows that, even on the hypothesis of the annihilation of all ex- ternal resistance, the proportion in question will always exceed the limit of stability; and since this is more than 3, this proportion will, @ fortiori, be always more than 3. Jt is conceivable that the least value considered above, 2. e., that which the proportion would have in the case. of complete absence of resistance, both internal as well as external, would be equal to the limit of stability itself, or would very slightly exceed it. In fact, on the one hand, the proportion ap- proximates to this limit as the resistances diminish, and on the other hand, if it exceeds it, the transformation becomes possible, (§ 57;) hence we see no reason why it should differ sensibly from it if the’ resistances were absolutely null. The results of our experiments, moreover, tend to confirm this view. First,. since the proportion belonging to our cylinder of mercury descends from 10.29 to 6.35, passing from that case in which the cylinder touches the glass at two lines to that where it touches it at a single one only, (§ 58,) it is clear that if this latter contact itself could be suppressed, which would leave the influence of the viscidity alone remaining, the proportion would become much less than | cates ae ea — oe ° Pe ERT IEE a Ne itoreal nbbg bse cs wea “aoe CRS <-i5% Sg SS Sates a hice es _ 6.35; and as, on the other hand, it must exceed 3, we might admit that it would at least lie between the latter number and 4, so that it would closely approxi- Li a WITHDRAWN FROM THE ACTION OF GRAVITY. 273 mate the limit of stability. If, then, it were possible to exclude the viscidity also, the new decrease which the proportion would then experience, would very probably bring the latter to the very limit in question, or at least to a value differing but exceedingly iittle from it. Thus, on the one hand, the least value of the proportion, that corresponding to the complete absence of resistances, would not differ, or scarcely so, from the limit of stability; and on the other hand, under the influence of viscidity alone, the proportion appertaining to the mercury would be but little renfoved from this least value. Hence it is evident that the influence of the viscidity of mercury is small, which is moreover ex- plained by the well-known feebleness of this same viscidity. We can now understand in the case of other but very slightly viscid liqnids, such as water, alcohol, &c., where the viscidity is not able to form more than a minimum resistance, that this viscidity, notwithstanding the differences in the intensities of the configuring forces, will also exert only a feeble influence upon the proportion in question. Hence it results that, in the absence of all external resistance, the values of this proportion respectively corresponding to the various very slightly viscid liquids cannot be very far removed from the limit of sta- bility; and as the smallest whole number above this is 4, we may in regard to these liquids adopt this number as representing the mean approximative proba- ble value of the proportion in question. Starting from this value, calculation gives us the number 1.82 as the propor- tion of the diameter of the isolated spheres which result from the transformation to the diameter of the cylinder, and the number 2.18 for the proportion between the distance of two adjacent spheres and this diameter. 61. There is another consequence arising from our discussion. For the sake of simplicity let the diameter of the cylinder be taken as unity. ‘The propor- tion of the normal length of the division to the diameter will then express this normal length itself, and the proportion constituting the limit of stability will express the length corresponding to this limit. This admitted, let us resume the conclusion at which we arrived at the commencement of the preceding sec- tion, which conclusion we shall consequently express here by stating that in the case of all liquids the nortial length of the divisions always exceeds the limit of stability; we must recollect, in the second place, that the sum of the lengths of one constriction and one dilatation is equal to that of a division, (§ 57;) and, thirdly, at the first moment of the transformation the length of one constriction is equal to that of a dilatation, (§ 46.) Now, it follows from all these propositions, that when the transformation of a cylinder begins to take place, the length of a single portion, whether constricted or dilated, is necessa- rily greater than half the limit of stability ; consequently the sum of the lengths of three contiguous portions, for instance two dilatations and the intermediate constriction, is once and a half greater than this same limit. Hence, lastly, if the distance of the solid bases is comprised between once and once and a half the limit of stability, it is impossible for the limit of stability to give rise to three portions, and it will consequently only be able to produce a single dilatation in juxtaposition with a single constriction. This, in fact, e~ we have seen, always. , took place in regard to the cylinder, in § 46, which was evidently in the above condition, and the want of symmetry in its transformation now becomes explicable. 62. As stated at the conclusion of § 48, we have yet to describe a remarkable fact which always accompanies the end of the phenomenon of the transformation of a liquid cylinder into isolated masses. In the transformation of large cylinders of oil, whether imperfect or exact, + (§ 44 to 46,) when the constricted part is considerably narrowed, and the sepa- ration seems on the point of occurring, the two masses are scer to flow back rapidly towards the rings or the disks; but they leave between them a cylindri- 18 s 274 THE FIGURES OF “EQUILIBRIUM OF A LIQUID MASS cal line which still establishes, for a very short time, the continuity of the one~ | with the other, (Fig. 28;) this line then resolves itself into partial masses. It | Fig. 28. generally divides into three parts, the two extreme ones of which become lost | in the two large masses, the intermediate one forming a spherule, some milli- — meters in diameter, which remains isolated in the middle of the interval which separates the large masses; moreover, in each of the intervals between this spherule and the two large masses, another very much smaller spherule is seen, which indicates that the separation of the parts of the above line is also effected by attenuated lines. Fig. 29 (Pl. VIII) represents this ultimate state of the liquid system. ‘The same effects are produced when the resolution of the thin and elongated cylinder of oil of § 47 into spheres occurs, only there is in one or the other of the intervals between the spheres frequently a larger number of spherules, and, besides, the formation of the principal line is less easily observed, in consequence of the more rapid progress of the phenomena. Lastly, in the case of our cylinders of mercury, the resolution into spheres takes place also in too short a time to allow of our perceiving the formation of the lines; but we always find, in several of the intervals between the spheres, one or two very minute spherules, whence we may conclude that the separation is effected in the same manner.* * We cannot avoid recognizing an analogy between the phenomenon of the formation ot liquid lines and that of the formation of laminze. In fact, in the experiment in § 23, for instance, the plane layer begins to be formed when the two opposite concave surfaces*are almost in contact with each other at their summits; and in the resolution of a cylinder into spheres, the formation of the lines commences when all the meridional sections of the figures almost touch each other by the summits of their concave portions. When treating of the layers, we have considered their formation as indicating a kind of tendency towards a particular state of equilibrium, which results from the circumstance that in the case of the thin part of the liquid system the ordinary law of pressure is moditied. For the analogy between the two orders of phenomena to be complete, it would, therefore, be necessary that excessively delicate liquid lines should connect thick masses, and should thus form with these masses a system in equ librio, notwithstanding the incompatibility of this equilibrium with the ordinary jaw of pressures. Now, wé shall show that this equilibrium is in reality possible, at least theoretically. Let us always take as example the resolution af our unstable cylinder into partial masses. When the cylindrical lines form, their diameter is even then verysmall in comparison with the dimensions of the thick masses; consequently their curvature in the direction perpendicular to the «xis is very great in comparison with the curvature of these masses. The pressure correspouuing to the lines is then originally much greater than those corresponding to the thick masses, whence it follows that the liquid must be driven from the interior of the lines towards these same masses, and that the lines, like the layers, ought to continue diminishing. Moreover, their curvatures, and conse- quently their pressure augmenting in proportion as they become more attenuated, their -tendency ‘to diminish in thickness will go on increasing, and consequently if we disregard the instability of the cylindrical form, we see that they must become of an excessive tenuity. But I say that the augmentation of the pressure will have a limit, beyond which this pressure will progressively diminish, so that it may become equal to that which corresponds to the thick parts of the liquid system. In fact, without having recourse to theoretical developments, it is readily seen that if the diameter of the line becomes less than that of the sphere of the sensible activity of the mole- cular attraction, the law of the pressure must become modified, and, the diameter continuing to decrease, the pressure must finish by also progressively diminishing, notwithstanding the increase of the curvatures, in consequence of the diminution in the number of attracting molecules. Hence the pressure may diminish indefinitely; for it ig clear that it would entirely vanish if the diameter of the line became reduced .to the thickness of a single mole- cule. Those geometricians who study the theory of capillary action know that the formule WITHDRAWN FROM THE ACTION OF GRAVITY. 275 _As we are now acquainted with the entire course which the transformation ? of a liquid cylinder into isolated spheres must take, we can represent it graphi- eally. Fig. 30 represents the successive forms through which the liquid figure passes, commencing with the cylinder up to the system of isolated spheres and of this theory cease to be applicable in the case of very great curvatures, or those the radii of which are comparable to that of molecular attraction. Now, it follows from what has been stated, that we may always suppose the thinness of the line to be such that the cor- responding pressure may be equal to that existing in thick masses which have attained a state of equilibrium. In this case, admitting that the lines are mathematically regular, se that the pressure there may be everywhere rigorously the same, consequently that they have no tendency to resolve themselves into small partial masses, equilibrium will necessarily exist in the system. In this case the form of the thick masses will not be mathematically spherical; for their surface must become slightly raised at the junctures with the lines by presenting concave curvatures in the meridional direction. This form will be the,samé as that of an isolated mass, traversed diametrically by an excessively minute solid line, (§ 10.) This system, like those into the composition of which layers enter, is composed of surfaces of a different nature; but this heterogeneity of form becomes possible here, as in the casé of the layers, in consequence of the change which the law of pressures undergoes in passing from one to another kind of surface. , We can, moreover, understand that the equilibrium in question, although possible theo- retically, as we have shown, can never be realized, in consequence of the cylindrical form of the lines. The same does not apply to the case of the plane layers; for, as we shall show in the following series, the plane surfaces are always surfaces of stable equilibrium, whatever may be their extent. 276 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS of spherules. This figure refers to the case of a very slightly viscid liquid, such as water, alcohol, &c., and where the convex surface of the cylinder is erfectly free; consequently, in accordance with the probable conclusion with which § 60 terminates, the proportion of the length of the divisions to the diameter has been taken as equal to 4. \ The phenomevon of the formation of lines and their resolution into spherules | is not confined to the case of the rupture of the equilibrium of liquid cylinders; it is always manifested when one of our liquid masses, whatever may be its figure, is divided into partial masses. This is the manner in whieh, for instance, in § 29 of the preceding memoir the minute masses which were then compared to satellites are formed.* The phenomenon under consideration is also produced when liquids are submitted to the free action of gravity, although it is then less easily shown: or instance, if the rounded end of a glass rod be dipped in ether, and then Withdrawn carefully in a perpendicular direction, at the instant at which the small quantity of liquid remaining adherent to the rod separates from the mass, an extremely minute spherule is seen to roll upon the surface of the latter. Lastly, the phenomenon in question is of the same nature as that which occurs when very viscid bodies are drawn into threads, as glass: softened by heat, except that in this case the great viscidity of the substance, and moreover the action of cold, which solidifies the thread formed, maintains the cylindrical form of the latter @nd allows of its acquiring an indefinite length. 63. To complete the study of the transformation of liquid cylinders into isolated spheres, it still remains for us to discover the law according to which the duration of the phenomenon varies with the diameter of the cylinder, and to endeavor to obtain at least some indications relative to the absolute value of this duration in the case of a cylinder of a given diameter, composed of a given liguid, and placed in given circumstances. We can understand, @ priori, that when the liquid and the external cireum- stances are the same, and supposing the length of the cylinder to be always such that the divisions assume exactly their normal length, (§ 53,) the duration of the phenomenon must increase with the diameter; for the greater this is, the greater the mass of cach of the divisions, and, on the other hand, the less the curvatures upon which the intensities of the configuring forces depend. It is true that the surface of each of the divisions increases also with the diameter of the cylinder; consequently it is the same with the number of the elementary configuring forces; but this augmentation takes place in a less proportion than tha‘ of the mass. This we shall proceed to show more distinctly. Under the above conditions two cylinders, the diameters of which are different, will be- come divided in the same manner; 7. e., the proportion of the length of a division to the diameter will be the same in both parts, (§ 55.) Now, it may be considered as evident that the similitude in figure will be maintained in all the phases of the transformation; this is, moreover, confirmed by experiment, as we shall soon see. ‘Hence it follows at each homologous instant of the transformations of the two cylinders the respective surfaces of the divisions will always be to each other as the squares of the diameters of these cylinders, whilst the masses, which evidently remain invariable throughout the entire duration of the phenomena, will always be to each other as the cubes of these diameters. Thus, at each homologous instant of the respective transformations, the extent of the.super-, ficial layer of a division, consequently the number of the configuring forces which emanate from each of the elements of this layer, change from one figure to the other only in the proportion of the squares of the primitive diameters of * It is clear that this mode of formation is entirely foreign to La Place’s cosmogonie hypo- thesis ; therefore we have had no idea of deducing from this little experiment, which only relers to the effects of molecular attraction, and uot to those of gravitation, any argument in. favor of the hypothesis in question—an hypothesis which, in other respects, we do not adopt. WITHDRAWN FROM THE ACTION OF GRAVITY. 277 these figures; whilst the mass of a division, all the parts of which mass receive, under the action of the forces in question, the movements constituting the transformation, changes in the proportion of the cubes of these diameters. As regards the intensities of the configuring forces, we must remember, first, that the measure of that which corresponds to one element of the superficial layer has (§ 59) for its expression 3 G -- u) This granted, if, at an homologous instant in the transformations of the two figures, we take upon one of the divi- sions of each of the latter any point similarly placed, it is clear from the simili- tude of these figures that the principal radii of curvature corresponding to the point taken upon the second will be to those corresponding to the point taken upon the first in the proportion of the diameters of the original cylinders, so that if this proportion be x, and the radii relating te the point of the first figure be R and R’, those belonging to the point of the second will be xR and 2B’; whence it follows that the measure of the two configuring forces corresponding ‘ : fet (el gt 1 A 1 1 to these points will be respéctively 3 Rt ry and a is 4 Ry = uv 1- A 1 1 : : Ss Gt a) Thus, in passing from the first to the second figure, the intensities of the elementary configuring forces in all the phases of the trans- formation will be to each other in the inverse proportion of. the diameters of the cylinders. I have convinced myself, by means of cylinders of mercury 1.05 millimeters and 2.1 millimeters in diameter, (§ 54 and 55,) that the duration of the phe- nomenon increases, in fact, with the diameter: although the transformation of these cylinders is effected very rapidly, yet we have no difficulty in recognizing that the: duration relating to the greater diameter is greater than that which refers to the least. 64. As regards the law which governs this increase in the duration, it would undoubtedly be almost impossible to arrive at its experimental determination in a direct manner, 2. e., by measuring the times which the accomplishment of the phenomenon would require in the case of two cylinders of sufficient length to allow of their being respectively converted into several complete isolated spherules, and of their satisfying the conditions indicated at the commencement - of the preceding section. In fact I can hardly see any method of realizing such eylinders without giving them very minute diameters, like those of our cylinders of mereury, and then their duration is too short to allow of our obtaining the proportion with sufficient exactness. But we may be able to arrive at the same result, but with certain restrictions, which we shall mention presently, by means of two short cylinders of oil formed between two disks, (§ 46;) there is nothing to prevent these cylinders from being obtained of such diameters as to render the exact measure of the durations easy. In the transformation of a cylinder of this kind, only a single constric- tion and a single dilatation are produced; but as in the transformation of cyl- inders which are sufficiently long to furnish several complete isolated spheres, the phases through which the constrictions and the dilatations pass are the same for all, we need only consider one constriction and one dilatation. We can understand that the relative dimensions of the two solid systems ought to be such, that the relation between the distance of the disks and their diameters is the same in both parts, in order that similitude may exist between the two liquid figurés at their origin and at each homologous instant of their transformations. Before giving an account of the employment of these figures of oil for the determination of the law of the durations, we shall take this opportunity of making several impoftant remarks. We shall only require to make use of the law in question in that case, which in other respects is the most simple, where 278 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS the cylinders are formed im vacuo or in air, and are free from all external resist- ance, or, in other words, free upon the whole of their convex surface. Now our short cylinders of oil are formed in the alcoholic liquid, and it might be asked whether this circumstance does not exert some influence upon the proportion of the durations corresponding to a given proportion between the diameters of these cylinders. At first, a greater or less portion of the alcoholic liquid must be displaced by the modifications of the figures, so that the total mass to be moved in a transformation is composed of the mass of oil and this portion of the alco- holie liquid; but it is clear that in virtue of the similitude of the two figures of oil and that of their movements, the quantities of surrounding liquid respectively displaced will be to each other exactly, or at least apparently, as the two masses of oil; so that the relation of the two entire masses will not be altered by this circumstance. Hence it is very probable that this circumstance will no longer exert any influence upon the proportion of the durations, except that the abso- lute values of these durations will be greater. On the other hand, the mutual attraction of the two liquids in contact diminishes the intensities of the pressures, (§ 8,) and consequently the configuring forces; but it is easy to see that this diminution does not alter the relation of these intensities in the two figures. For let us imagine that at an homologous instant of the two transformations the alcoholic liquid becomes suddenly replaced by the oil, and let us conceive in the latter the surfaces of the two figures as they were at that instant. ‘The configuring forces will then be completely destroyed by the attraction of the oil outside these surfaces, or, in other words, the external attraction will be at each point equal and opposite to the internal configuring force. If we now replace the alcoholic liquid, the intensities of the external attractions will change, but they will evidently retain the same relations to each other; whence it follows that those corresponding to two homologous points taken upon both the figures will still be to each other as the configuring forces commencing at these points; so that in fact the respective resultants of the external and internal actions at these two same points will be to each other in the same proportion as the two internal forces alone. 'Thus the attractions exerted upon the oil by the sur- rounding alcoholic liquid will certainly diminish the absolute intensities of the configuring forces, but they will not change the relations of these intensities, . consequently they may be considered as not exerting any influence upon the durations. But it is clear that this cause will nevertheless greatly increase the absolute values of the latter. Jor the two reasons which we have explained, the presence of the alcoholic liquid will then increase the absolute values of the two durations to a considerable extent ; but we may admit that it will not alter the relation of these values, so that this proportion will be the same whether the phenomenon take place em vacuo or inair. We shall, therefore, consider the law which we deduce from our experiments upon short cylinders of oil as inde- pendent of the presence of the surrounding alcoholic liquid, and this will be found to be supported by the nature of the law itself. But the exact formation of our short cylinders of oil requires (§ 46) that in these cylinders the proportion between the length and the diameter, or what comes to the same thing, between the sum of the lengths of the constriction and the dilatation and the diameter, exceeds but little the limit-of stability. Now, in the transformation of cylinders sufficiently long to furnish several spheres, which would be formed ¢z vacuo or in the air, and free upon their entire convex surface, and the divisions of which have their normal length, the proportion of the sums of the lengths of one constriction and one dilatation to the diameter, which proportion is the same as that of the length of one division to the diam- eter, would vary with the nature of the liquid, (§ 59,) and we are ignorant whether the law of the durations is independent of the value of this proportion. The law which we shall obtain in regard to short cylinders of oil can only there- WITHDRAWN FROM THE ACTION OF GRAVITY. ~* 279 | fore be legitimately applied to cylinders of sufficient length to furnish several sphéres supposed to be in the above conditions, in the case where these latter cylinders are formed of such a liquid that they would give for the proportion in question a value but little greater than that of the limit of stability. Now this is the case of mercury, (§ 60,) and it is also very probable that of all other very slightly viscid liquids, (§ 60.) ‘Thus the law given by the short eylinders of oil will be exactly or apparently that which would apply to eylin- ders of mercury of sufficient length to furnish several spheres, supposing the latter to be produced iz vacuo or in air, free at the whole of their convex surface, and of such length that the divisions in each of them would assume their normal length. Moreover, the same law would be undoubtedly applicable to cylinders formed of any other very slightly viscid liquid, and supposed to be in the same conditions as the preceding. The law may possibly be completely general, 7. e., it may apply to cylinders formed, always under the same circumstances, of any liquid whatever; but our experiments do not furnish us with the elements necessary to decide this ques- tion. Lastly, the transformation of our short cylinders presents a peculiarity which entails another restriction. The two final masses into whieh a cylinder of this kind resolves itself being unequal, the smallest acquires its form of equilibrium considerably before the other, so that the duration of the phenom- enon is not the same. Hence we can only determine its duration up to the moment of the rupture of the line; consequently the proportion which we thus obtain for both cylinders will only be that of the durations of two homologous portions of the entire transformations. Moreover, the proportion of these partial durations is exactly that of which we shall have hereafter to make use. 65. I made the experiments in question by employing two systems of disks, the respective dimensions of which were to each other as one to two; in the former, the diameter of the disks was 15 millimeters, and they were 54 milli- meters apart; and in the second their diameter was 30 millimeters, and their distance apart 108 millimeters. The cylinders formed respectively in these two systems were therefore alike, and, as I have previously stated, (§ 63,) these two figures exactly maintained their similarity, as far as the eye was capable of judging, in all the phases of their transformations. It sometimes happened that the cylinder, when apparently well formed, was not at all persistent and imme- diately began to alter; this circumstance being attributable to some slight remaining irregularity in the figure, I immediately re-established the cylindrical form,* and the time was only taken into,account when the figure appeared to maintain this form for a few moments. Another anomaly then sometimes pre- _ sented itself, which consisted in the simultaneous formation of two constrictions with an intermediate dilatation; this modification ceased when it had attained a very slightly marked degree, and the figure appeared to remain in the same state for a considerable period ;+ then one of the constrictions became gradually more marked, whilst the other disappeared, and the transformation afterwards went of in the usual manner. As this peculiarity constituted an exception to the regular course of the phenomenon, I ceased to reckon as soon as it showed itself, and I again re-established the cylindrical form. The estimation of the time was only definitively continued in those cases in which, after some per- sistence in the cylindrical form, a single constriction only was produced. I repeated the experiment upon each of the two cylinders twenty times, in order to obtain a mean result. As soon as one transformation was completed, * See the second note to paragraph 46. ; t We shall see, in the following series, to what this singular modification in the figure is owing. 280 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS I reunited the two masses to which it had given rise, and again formed the eylinder,* in order to proceed to a new measure of the’time. wh The number of seconds are given below; each expresses the time which elapsed from the moment of the transformation of the cylinder to that of the rupture of the line. ‘These periods were determined by means of a watch, which beat the 1ths of a second. Cylinder Cylinder 15 millims. in diameter, f 30 millims. in diameter. u WI " Ws 25.0 36.4 59.6 51.6 26.6 32.0 73.0 68.0 28.0 30.4 57.0 73.6 . 30.0 24.6 61.0 61.8 24.8 32.6 67.8 53.0 35.2 33.8 60.0 58.0 27.0 33.8 : Goon 63.8 30.0 20.2 54.2 60.0 30.4 28.6 61.0 52.6 29.8 32.6 52.6 oo0.2 eee ————— Mean 29’.59. Mean 60”.38. It is evident that the numbers relating to the same diameter do not diffe” sufficiently from each other to prevent our regarding the proportion of the two means as closely approximating tothe true proportion of the durations. Now the proportion of these two means is 2.04, z. e., almost exactly equal to that of the two diameters. Moreover, it is evident that in the case of each of the latter the greatest of the numbers obtained must correspond to that case where the cylinder is formed in the most perfect manner; consequently it is probable that the pro- portion of these two greatest numbers also closely approximates to the true proportion of the durations. Now, these two numbers are, on the one hand 36.4, and on the other 73.6, and their proportion is 2.02, which number differs still less from 2, or from the proportion of the diameters. We may, therefore, admit that the durations relating to these two cylinders ' are to each other as their diameters; whence we deduce this law, that the par- tial duration of the transformation of a cylinder of the same kind is in proportion to its diameter. I have said (§ 64) that the law thus obtained would of itself furnish a new motive for believing that it would not change if our short cylinders of oil were produced zz vacuo or in air. In fact the proportionality to the diameter is the simplest possible law; and, on the other hand, the circumstances under which the phenomenon is produced are less simple in the case of the presence of the alcoholic liquid than they would be in that of its absence; consequently, if the . law changed from the first to the second, it would follow that a simplification in the circumstances would, on the contrary, induce a complication of the law, which is not very probable. : * This was effected by conducting the large mass towards the small one, by means of the ring of which I spoke in the first note to paragraph 46. But care must be taken to prevent the ring, on separating from the liquid figure, from carrying away with it any perceptible quantity of oil; for this purpose, instead of making the entire ring adhere to the great mass, 1 left a small portion of the latter free, and, as its action was then insufficient to make the large mass reach the other, I aided it by gently pushing the oil with the extremity of the point of the syringe. On withdrawing the ring after the reunion of the two masses, only a very smal] spherule of oil separated from it in the alcoholic liquid, which in the next experi- ment I again united to the rest of the oil by means of the ring itself, as also the largest of the spherules arising from the transformation of the line. WITHDRAWN FROM THE ACTION OF GRAVITY. 281 We may, therefore, I think, legitimately generalize the above law in accord- ance with the whole of the remarks made in the preceding section, and deduce the following conclusions: 1. If we conceive a cylinder of mercury formed iz vacuo or in air, of sufficient length to furnish several spheres, its convex surface: being entirely free, and its length such that the divisions assume exactly their normal length, the time which will elapse from the origin of the transformation to the instant of the rupture of the lines will be exactly or apparently proportional to the diameter of this cylinder. 2. The same very probably applies to a cylinder formed of any other very slightly viscid liquid, as water, alcohol, &c., and supposed to exist under the same circumstances. 3. It is possible that this law is completely general, 2. e., applicable to a cyl- inder formed, always under the same circumstances, of any kind of liquid what- ever; but our experiments leave us in doubt on this point. 66. Let us now enter upon the consideration of the absolute value of the time in question for a given diameter, the cylinder always being supposed to be pro- duced iz vacuo or in air, of sufficient length to furnish several spheres, its entire convex surface free, and its length such that its divisions assume their normal length. It is clear that this absolute value must vary according to the nature of the liquid; for it evidently depends upon the density of the latter, upon the intensity of its configuring forces, and, lastly, upon its viscidity. The experi- ments which we have detailed give with regard to oil a very remote superior limit; this results, first, from the two causes which we have mentioned in § 64, and which are due to the presence of the alcoholic liquid; but with these two causes is connected a third, which we must make known. If we imagine a cyl- inder of oil formed under the above conditions, the sum of the lengths of a constriction and a dilatation will necessarily be much greater in regard to this cylinder than in regard to one of our short cylinders of oil of the same diameter; for in the former this sum is equivalent to the length of a division; and in con- sequence of the great viscidity of the oil, this latter quantity must greatly exceed the length corresponding to the limit of stability. Now, it may be laid down as a principle, that, all other things being equal, an increase in the sum of the lengths of a constriction and a dilatation.tends to render the transformation more rapid, and consequently to abbreviate the total and partial durations of the phenomenon. In fact, for a given diameter, the more the sum in question differs from the length corresponding to the limit of stability, the more the forces ‘which produce the transformation must act with energy ; moreover, as the trans- formation ceases to take place immediately above the limit of stability, the duration «f the phenomenon may then be considered as infinite, whence it fol- lows that when this limit is exceeded, the duration passes from an infinite to a finite value, consequently it must decrease rapidly as it deviates ‘from this limit ; lastly, this is also confirmed by the results of observation, as we shall sLow hereafter. ‘Thus, even if it wefe possible to form 7 vacuo or in air one of our very short cylinders of oil, consequently to eliminate the two causes of retarda- tion due to the presence of the alcoholic liquid, the duration relative to the eylinder would still exceed that which would relate to a cylinder of oil of the same diameter formed under the conditions we have supposed. | I have said that the principle above established is confirmed by experiment, i. e., for the same diameter, the same liquid, and the same external actions, if any exist; when, from any cause, the sum of the Jengths of a constriction and a dilatation augments, the total and partial durations of the transformation become less. We shall proceed to make this evident. In the experiments of the pre- ceding section, the partial duration relating to the cylinder, the diameter of which was 15 millimeters, was, for instance, about 30 scconds, the mean, as shown by the table. Consequently, if we Were to form in the alcoholic liquid a similar 282 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS cylinder of oil, the diameter of which is 4 millimeters, the partial duration of this, in virtue of the law which we have found, would be nearly equal to anil a — 8”. Now, in the nearly cylindrical figure of oil of § 47, which 15 figure is also formed in the alcoholic liquid, the mean diameter was (§ 56) about 4 millimeters. In this and the preceding figure, the diameter, the liquid, and the external actions then are the same; but in the former, the sum of the lengths of the constriction and the dilatation would only be equal to 4 millimeters, + 3.6 = 14.4 millimeters, whilst in the second, this sum, which is equivalent to the length of a division, was (§ 56) approximatively 66.7 millimeters. Now, on observing this latter figure, we recognize easily that the duration of* its trans- formation is much less than 8’. In truth, from the nature of the experiment, it is impossible with regard to this same figure to fix upon the commencement of the formation of a given constriction or dilatation, so that the complete dura- — tion should considerably exceed that which would be deduced by the simple inspection of the phenomenon; but the latter does not amount to one second, and there cannot be any doubt that it would be going too far to extend the complete duration, and @ fortiori, the portion which terminates at the rupture of the lines, to two seconds. ‘Thus in the case we have just considered, the sum of the length of a constriction and a dilatation becoming about four and a half times greater, the partial duration becomes at least four times less. - 67. But if, in reckoning the absolute duration in the case of one of our short eylinders of oil, we only obtain with regard to this liquid one upper limit, and this much too high, the cylinder of mercury in § 55 (which cylinder is formed in the air, and the length of which in proportion to the diameter is sufficient for the divisions to have,assumed exactly, or very nearly, their normal length) will furnish us, on the contrary, in regard to this latter liquid, with a limit which is probably more approximative and which will be very useful to ws. First, in the case of this cylinder, the diameter of which, as we have said, was 2.1 millimeters, the transformation does not take place in a sufficiently short time for us to estimate with any exactitude the total duration of the phenomenon; I say the total duration, because in so rapid a transformation it would be very dificult to determine the instant at which the rupture of the lines occurs. To approximate as closely as possible to the value of this total duration, I have had recourse to the following process. By successive trials, i regulated the beats of a metronome in such a manner, that on rapidly raising, at the exact instant at which a beat occurs; the system of glass strips belonging to the apparatus serving to form the cylinder, (§ 50 and 51,) the succeeding beat appeared to me to coincide with the termination of the transformation ; then having satisfied myself several times that this coincidence appeared very exact, I determined the duration of the interval between two "beats, by counting the oscillations made by the instrument during two minutes, and dividing this time by the number of oscillations. I thus found the yalue 0'’.39 for the interval in question. The total daration of the transformation of our cylinder of mereury may therefore: be valued approximatively at 0.39, or more simply, at.0/’.4. ; But the entire convex surface of this cylinder is not free, and its contact with the plate of glass must exert an influence upon its duration, both directly as well as by the increase which it produces in the length of the divisions. Let us examine the influence in question under this double point of view. The direct action of the contact with the plate is undoubtedly very slight ; for as soon as the transformation commences, the liquid must detach itself from the glass at all the intervals between the dilated parts, so as only to touch the solid plane by a series of very minute surfaces belonging to these dilated parts; consequently, if the direct action of the contact of the plate were alone eliminated, 2. é» if we could manage so that the entire donvex surface of the cylinder should q e . WITHDRAWN FROM THE ACTION OF GRAVITY. 283 & be free, but that the divisions formed in it should acquire the same length as before, the total duration would scarcely be at all diminished. There still remains the effect of the elongation of the divisions. The length of the divisions of our cylinder is equal to 6.35 times the diameter, (§ 56,) whilst, according to the hypothesis of the complete freedom of the convex sur- face, this length would very probably be less than four times the diameter, -(§ 60.) Now, in virtue of the principle established in the preceding section, this increase in the length of the divisions necessarily entails a diminution in the duration, which diminution is more considerable in proportion as it occurs in the vicinity of the limit of stability ; consequently, if it could be managed so that the elongation in question should not exist, the total duration would be very considerably increased. Thus the suppression of the direct action of the con- tact of the plate would only produce a very slight diminution of the total duration ; -and the annihilation of the elongation of the divisions would produce, on the other hand, a very considerable increase in this same duration. ° If, then, these two influences were simultaneously eliminated, or, in other words, if the entire ee - convex surface of our,cylinder were free, the total duration of our transformation would be very considerably greater than the direct result of observation. Now, the quantity which we have to consider is the partial, and not the total duration; but, under the same circumstances, the first must be but little less than the second; for when the lines are about to break, the masses between which they extend even then approximate to the spherical form; consequently, in accordance with the conclusion obtained above, we must admit that the partial duration under our present consideration, 7. e., that referring to the case of the complete freedom of the convex surface of the cylinder, would still exceed considerably the total duration observed, 7. e., 0!'.4. In starting from this value 0’’.4 as constituting the lower limit corresponding to a diameter of 2.1 millimeters, the law of the proportionality of the partial duration to the diameter will immediately give the lower limit corresponding to any other diameter; we shall find, e. g., that for 6 millimeters this limit would be 0”.4 + 10 2.4 If, then, we imagine a cylinder of mereury a centimeter in diameter, formed in vacuo or in air, of sufficient length to furnish several spheres, entirely free at its convex surface, and of such a length that its divisions assume their normal = 1".9, or more simply 2”. _ length, the time which will elapse from the origin of the transformation of this cylinder to the instant of the rupture of the lines will considerably exceed two seconds. 68. It will not-be superfluous to present here a resumé of the facts and laws which the experiments we have described have led us to establish with respect to unstable liquid cylinders. 1. When a liquid cylinder is formed between two solid bases, if the proportion of its length to its diameter exceeds a certain limit, the exact value of which is comprised between 3 and 3.6, the cylinder constitutes an unstable figure of equilibrium. The exact value in question is that which we denominate the limit of stability of the cylinders. 2. If the length of the cylinder is considerable in proportion to its diameter, it becomes spontaneously converted, by the rupture of equilibrium, into a series of isolated spheres, of equal diameter, equally distant, having their centres upon the right line forming the axis of the cylinder, and in the intervals of which, in the direction of this axis, spherules of different diameters are placed ; except that each of the solid bases retains a portion of a sphere adherent to its surface. 3. The course of the phenomenon is as follows: The cylinder at first eradually swells at those portions of its length which are situated at equal distances from . 284 THE FIGURES OF EQUILIBRIUM OF A LIQUID MASS each other, whilst it becomes thinner at the intermediate portions, and the length of the dilatations thus formed is equal, or nearly so, to that of the constrictions ; these modifications become gradually more marked, ensuing with accelerated rapidity, until the middle of the constrictions has become very thin; then, com- mencing at the middle, the liquid rapidly retires in both directions, still, however, leaving the masses united two and two by an apparently cylindrical line; the latter then experiences the same modifications as the cylinder, except that there are in general only two constrictions formed, which consequently include a dilatation between them; each of these little constrictions becomes in its turn converted into a thinner line, which breaks at two points and gives rise to a very minute isolated spherule, whilst the above dilatation becomes transformed into a larger spherule; lastly, after the rupture of the latter lines, the large masses assume completely the spherical form. All these phenomena occur symmetrically as regards the axis, so that, throughout their duration, the figure is always a figure of revolution. 4. We denominate divisions of a liquid cylinder, those portions of the cylinder, -each of which must furnish a sphere, whether we conceive these portions to exist in the cylinder itself, before they have begun to be apparent, or whether we take them during the transformation, 2. e., whilst each of them is becoming modified so as to arrive at the spherical form. The length of a division consequently measures the coustant distance which, during the transformation, is included between the necks of two adjacent constrictions. Moreover, by normal length of the divisions, we denominate that which the divisions would assume, if the length of the cylinder to which they belong were infinite. In the case of a cylinder which is limited by solid bases, the divisions also assume the normal length when the length of the cylinder is equal to the pro- duct of this normal length by a whole number, or rather a whole number and a half. Then, if the second factor is a whole number, the transformation becomes disposed in such a manner that during its accomplishment the figure terminates on one side with a constriction, and on the other with a dilatation; if the second factor is composed of*a whole number and a half, the figure terminates on each side in a dilatation. When the length of the cylinder fulfils neither of these conditions, the divisions assume that length which approximates the most closely possible to the normal length, and the transformation adopts that of the two above dispositions which is most suitable for the attainment of this end. 5. In the case of a cylinder of a given diameter, the normal length of the divisions varies with the nature of the liquid, and with certain external cireum- stances, such as the presence of a surrounding liquid, or the contact of the convex surface of the cylinder with a solid plane. In all the subsequent state- ments we shall take the simplest case, z. e., that of the absence of external cir¢umstances ; in other words, we shall always suppose that the cylinders are produced tm vacuo or in air, and that they are free as regards their entire convex surface. 6. 'T'wo cylinders of. different diameters, but formed in the same liquid, and the lengths of which are such that the divisions assume in each of them their normal length, become subdivided in the same manner, 7. e, the respective normal lengths of the divisions are to each other as the diameters of these cyl- inders. In other words, when the nature of the liquid does not change, the normal length of the divisions of a cylinder is proportional to the diameter of the latter. The same consequently applies to the diameter of the isolated spheres into which the normal divisions become converted, and to the length of the intervals which separate these spheres. 7. The proportion of the normal length of the divisions to the diameter of the cylinder always exceeds the limit of stability. WITHDRAWN FROM THE ACTION OF GRAVITY. 285 8. This proportion is greater as the liquid is more viscid and as the config- ng forces in it are weaker. 9. In the case of a cylinder of mercury, this proportion is mucli less than 6, and we may admit that it is less than 4. In the case of a cylinder composed of any otlier very slightly viscid liquid, such as water, alcohol, &c., it is very probable that the proportion in question is very nearly 4. Hence, in the case of the latter liquids, we have for the _ probable approximative value of the proportion of the diameter of the isolated _ spheres resulting from the transformation and the diameter of the cylinder, the number 1.82; and for that of the proportion of the distance of two adjacent _ spheres to this same diameter, the number 2.18. 10. If mercury is the liquid, and the divisions have their normal length, the _ time which clapses between the origin of the transformation and the instant of the rupture of the lines, is exactly or apparently proportional to the diameter of the cylinder. F nae law very: probabiy applies also to each of the other very slightly viscid liquids. , This same law may possibly be general, 7. e., it may be applicable to all - liquids; but our,experiments leave this point uncertain. . . 11. For the same diameter, and when the divisions are always of their normal length, the absolute value of the time in question varies with the nature of the liquid. es Pia. In the case of mercury, and with a diameter of a centimeter, this absolute _ value is considerably more than two seconds. 13. When a cylinder is formed between two solid bases sufficiently approx- . imated for the proportion of the normal length of the cylinder to the diameter to be comprised between once and once and a half the limit of stability, the _ transformation gives only a single constriction and a single dilatation; we then, obtain for the final result only two portions of a sphere which are unequal in volume and curvature, respectively adherent to solid bases, besides interposed spherules. (TO BE CONTINUED IN THE NEXT REPORT.) HISTORY OF DISCOVERY RELATIVE TO MAGNETISM, COMPILED FOR THE INSTITUTION PRINCIPALLY FROM THE ‘‘AUS DER NATUR.” THERE are two great. forces of nature everywhere present and at every moment exerting their influence, namely, gravitation and magnetism. The are similar in many particulars, all pervading and perhaps equally powerful. The magnetic phenomena of the earth, however, do not manifest themselves ag freely to the senses as those of gravitation, and the naturalist is obliged to em- ploy refined, and, in some cases, complicated apparatus to study the laws of its operation. In this article we purpose to present to our readers a sketch of the earlier discoveries relative to magnetism, and in doing so we shall also briefly explain the general principles of the science. ‘here is found in different parts of the earth a mineral of a dark color, principally composed of iron and oxygen, which has long been an object of in- terest to the ignorant as well as the learned, principally on account of the attrae- tion which it exhibits for iron, and the wonderful property which it imparts to steel needles of pointing toward the poles of the earth. Its composition may be expressed chemically. by the formule Fe O + Fe, 03, being a compound of the first and second oxide of iron. It is called loadstone, and occurs most generally in primary mountains of gneiss; chlorite slate, in primitive lime- stone, and sometimes in considerable masses in serpentine, and in trap. It is found in great quantity and purity at Rosslay, in Sweden, in Corsica, on the island of Elba, in Norway, Siberia, Saxony, Bohemia, and in the Hartz moun- tains. < -~- ons comes cently oe ne aoe eee 21 Cone-1n-cone, ton) Henry; Pople, INOVa SCOMa) sc cce.e eo sere soa eee eee eines 87 Contributions to knowledge. Account of vol. xil-----2.-2-s2e cose - score eee 15 PERC CAS EATON OL, SNL RY ote apa a aia 16 (Costa Rica. | bxnlorations:in |. - acen vascein cee Son ena eam ae meson eee 54 Coues, Dr: BE. Monograph of Waridse; or gulls - eee oe ne poe pen eee ne ae 16 riba. Hagploraisans AM) 2). == c/n <= mini m= = we ee peel eae ane ee ee ee 55 Daa, Louis Kr. Letter from, with ethnological specimens ..-.-.--.--.------------ 89 Danilsen, A. F. Antiquities in Tennessee and Oregon...--.-..--...------.-------- 384 Dean, Dr. John. Researches on medulla oblongata..-.....---...---...----.--.-- 16, 19 De la Rive. On propagation of electricity in rarefied elastic fluids -...--...--...--- 169 Department of Agriculture. Meteorological operations of.....-..-..----.--------- 32 IDV shine, (Onishi y sess soto oss esas Sooshs Sash su seas seeess Goss 5ee 24 Dixections) for preserving) Lepidoptera = 2 on. sea te eee elie elaine el ee 404 Distribution of specimens and collections. ----. ees lee ete 38, 57 MPO EONS Eve Te UN AS GS er ee nl 58 Draper, Dr. H. Astronomical photography... <.-- ~~ --2- == -i--= = sercningnaeen ninemsn 16 Dyeing. Azure and purple, ancient and modern....--- .----- ------ panne een- ---= 385 Earth. Investigations relative to form and size...--.---------- 2-221 csceunne------ 306 igmad one iC Olleetions Ons opm yea aan ae area ta lee eee 55 Hiducation: Project of, history of, by F. A. Packard... a2 2. ocece aaa i soee~ = 82 BeRton,) We CWeCalis iw Ong TNT CLAS = sete tae lata relate aa ee ete ae orale 24, 25 Electricity. Dela Rive on propagation of, in rarefied elastic fluids. .....---....----. 169 Entomology. Directions for preserving Lepidoptera. -...--...-.----.--.----.---- 404 SMIthsoniaN works ON - o-28e oon = eee ee saan aera eee tee 23 BEBNOlOPICAl INSHUCHONS|..5-2- oes 2 === = see ae eee eee eee aie 25 specimensifrom) Norway. 252220 te aoein Se ee eae eee ee 83 Bunmolopy. Articles ON 22i\22cnc=soccs sclriineeias een ases aes eee eee 370 Smithsonian) lahorsinees see. + t-)teetele alee eee ee eee 29 Hechances. Account of; amdistatishics = pie. .sisinn oo se ele aes Saieiee eeeee 39, 44, 46 plOrabions.. \ On" chnean-cone" 1.2.2 2220 SE ee: ae 87 Pork... -Weatharom eatinore meee eae saree teat rea ae octane ee ee ate ee eee enter tere 203 Preservation of Lepidoptera.) Method of =: Soo. se lea sae ete teeta aa 404 Prime, Temple. On" Corpicwladie.cwce sn csne = cence ts oe ae eee eee ee ncne ne 22, 23 INDEX. 419 PAGE. meen. Report on, tor 1665. .is-s202 22h. ccnp eae sna oe gen ee seen dee wuncukents 44 Programme of organization of the Institution...-..-.-...-./.--.-----.---------6- 7 Publications of the Institution. General account of...--.-...---.----.--+--------- 14 TGS te ie Oe al ales ete a ae a ate 62 Pape dyemp. Ancient and modetaies-- =. 22-2 2c2-. concen scans eoues ooo 385 Rau, Charles. Agricultural implements of the North American stone period.......- 379 Translation of Baegert’s account of aborigines of California...-...... 302 Seevenis. Journal of proceedings Of. Wo... an fee eceicekinen adscos Weoeaeeaat ae 77 Bevents oF thadnstitution, \ Wish of, 1225552. semnceeene asso see = aoe ene cee 5 Heporof the Hxecutive:Committee for 1863.22 -2- 4-4-2 see neat 74 mepams or the Institution. Account Of 52... 2/5 ocenhewe activa ta eessedae meee 15, 27 Roles for distributing 12225245 tee sie etek eee 28 Report on proceedings of Society of Physics and Natural History of Geneva, for Hebe Gas Dy; MalCets- ss - occ o sel = coors ena aetna aloo aera eee 193 Royal Society of London. History of ..---.-.----- ee et ee 137 Rush, Richard. Part of bequest left in England by-..-----.- ele a 14 Shea, J. G. Aid rendered philological publications of. ....-..---.----------, ie alee 29 PSGelise Smithsonian WOLkS | OW: o-oo = ee seis ae esas a etatelete mele eine rte 21 Bmith; Buckingham. Pima grammar ... <<< .20.- cccqcemnnn en ccre wa-napesda aden 31 MaIuHAOMe s WalliOf = 2.23 2s nc clon one ee e Pa a a ese area ae a Stereotyping Smithsonian publications ...... -... -<<2=- ons «neers -