ee es ee pene to tee rte pot AAA * sc pmatadtaomapeetl Syn tn Mm yh 4 >| ST Ua PROCEEDINGS OF THE American Philosophical Society HEED Al) REE Ader Ee FOR PROMOTING USEFUL KNOWLEDGE VOEUME XLVM IS, NULLO DISCRIMINE MDCCXLIII PHILADELPHIA THE AMERICAN PHILOSOPHICAL SOCIETY 1909 PRESS OF THE NEW ERA PRINTING COMPANY LANCASTER, PA. : PRO CLEDINGS . AMERICAN . PHILOSOPHICAL SOGTETY HELD AT PHILADELPHIA FOR PROMOTING USEFUL KNOWLEDGE. 7 ty Vor XLVI: JANUARY-—APRIL, 1909. No. 191. — ae ES eS a , CONTENTS. Geicienial Stones Used by ilies Australian Abareings By R. HH. PUD Ween na trea Hae ai te ut cura a IGN's ped ah ae a Peg The Exploration of the Upper Air by Means of Kites and Balloons , rey Cea dee: BOAT RY og lileao dase dy chau berate see C ie pean ean “ Why America Should Re-explore Wilkes Land! By Epwin Swirt '' ; pM EI cree NEE Gt La tao Be haw Ay ou aut ies ootisie Ghee scotante Ie iaaT eae 34 The Nation and the Waterways. By Lewis M. faa See 51 On.,a New Variety of Chrysocolla from Chile. By Harry F.); SPELT ES CEES ce 9s Gen st nner au Meee Mees gall Re NSWMML Af te abn 65 The Purification of Water Supplies by the Use of Hypochlorites. ” _By Wituiam Pirr Masov...... rad shaves ayeiatele/ Seataigeila © orate os ea eae a 67 The Detonation of Gun Cotton. ‘By CHARLES E. MUNROE......... 69 The Comparative Leaf Structure of the Strand Plants of New Jersey. Soya POLO thre A RGOMBERGE Ri o6 0 Ae ne) Uathaa do hacdas s hemp eur eemmee 42 The Destruction of the Fresh-water Fauna in Western Pennsy Ivania. By A. E. ORTMANN........ SZ esas fiat Seer tp MR IRR GCA GAA ns OS go On Certain Generalizations of the Problem of Three Bodies. By TD GAME OO, SNOMED wc cole ble er lad sated Saree ae Laer ree III The Past History of the Earth as Inferred from the Mode of Forma- Honor the Solar. Systems by \ Pf. WF SER eee. lewd os ee 119 Commemorative Addresses and Obituary Notices of Members Deceased. Personal Reminiscences of Charles Darwin and of the Recep- tion of the ‘‘ Origin of Species.’’ By James BRYCE...,.... 2. eam _\; Lhe Influence of Darwin on the Natural Sciences.. -By GEO_GE LEW REQ TE TE STEIN Bo: Ibe NN aM Rg MOL EU RORIPineUe DDAS eM “xU The Influence of Darwin on the Mental and Moral Sciences. Poe BORE SPAR T PULLERTON s,. . 02.) os. 2s isa ecesloostamteee enue d) Meee _ The World’s Debt to Darwin. By Epwin G. ConkLin ......cxxvidt Richard Alexander Fullerton Sas, us Dates Dey ee loite LOE TD elon OS aA GN Lo Nd Ui D8 abil arian ia ON ui AM mei Lett Minutes of Meetings from January 1 to May 21, 1909...............5- i f PHILADELPHIA THE’ AMERICAN PHILOSOPHICAL SOCIETY ‘704 SouTH FIFTH STREET 1909 American Philosophical Society General Meeting—April 21-23; 1910 The General Meeting of i910 will bé Held on April 21st to 23rd; beginning at 2 p. mi: ot Thursday, April 21st. Members desiring to preseht papers, eithet for themSelves or others; are requested to send to the Secretaries; at as early a date as practicable, and not later than March 19; 19to, the titles of these papers; so that they may be announced on the programme which will be issued immediately thereafter, and which will give in detail the arrangements for the meeting: Papers in any department of scierice come within the scope of the Society, which, as its name indicates, embraces the whole field of useftil knowledge: The Publication Committee; under the iules of thé Society, will arrange for the immediate publication of the papers presented: Se I. MINIS HAYS ARTHUR W. GOODSPEED JAMES W. HOLLAND AMOS P: BROWN Secretaries: Meinbers who have not as yet sent their photographs to the Society will tonfer a favor by so doing; cabinet size preferred: it is tequested that all correspondence be addressed To tHE SECRETARIES OF THE AMERICAN PHILOSOPHICAL SOCIETY to4 SovTH FirrH STREET PHILADELPHIA; U: S. a: PROCEEDINGS OF THE PVBERICAN PHILOSOPHICAL) SOCIETY HELD AT PHILADELPHIA FOR PROMOTING USEFUL KNOWLEDGE VoL. XLVIII JANUARY-APRIL, 1909 No. 191; BEREMONIAL STONES USED BY THE) AUSTRALIAN ABORIGINES. By R. H. MATHEWS. (Read January I, 1909.) The following is a short description of some remarkable stones used by the aborigines in certain areas scattered over the north- western portion of New South Wales, which may be approximated roughly as lying north of 34 degrees south latitude and west of 148 degrees east longitude. The objects referred to have been observed by squatters and other residents of the bush in different places for many years past, but like most other matters connected with the aborigines, very little attention has been paid to them. They are occasionally found lying on the surface of the ground, or only partially exposed, on the flanks of sand-ridges, which may have been either old camps of the natives or places of their ceremonial gatherings. They have also been discovered below the surface, having probably been overlaid by drifting sand or soil, or were per- haps purposely hidden when not in use. The scattered remnants of the tribes in the region indicated are all more or less civilized at the present time and have ceased to use these stones in their ceremonies, owing to the occupation of the district by Europeans for upwards of half a century. For this reason it is especially important that all available information should ‘ 2 MATHEWS—CEREMONIAL STONES [January 1, be recorded and published as widely as possible, in order to bring these relics under the notice of every person who may have oppor- tunities of obtaining further particulars regarding this interesting subject. The stones in question vary in length from about six inches up to as much as two feet, but the more common lengths range from eight to fifteen inches. They are widest at the base, gradually de- creasing in dimension towards the other end and terminating in a blunt point. They consist of different material, including sandstone, quartzite, clayslate, kaolin and such other kinds of stone as might be available. For the present I shall describe only four of the specimens in my possession. One is a fine-grained piece of clayslate, which when found by the maker was probably very close to the requisite form and needed only a little trimming or grinding to bring it to its present shape. It is just a trifle under one foot in length by a maximum width at the base of two and four-fifth inches, by a thickness of one and a quarter inches. The weight is two pounds six ounces. It was found in the bush by Mr. E. J. Suttor, owner of Tankarooka Station, on the Darling River, near Tilpa, New South Wales. I have prepared two diagrams exhibiting the two wide faces and the edge of the implement, together with a view of the extremity of the base and have numbered the figures from 1 to 12. One face of the stone is practically flat throughout its length, being rounded off towards the edges on either side. The opposite face is slightly convex. Fig. 1 delineates the flat face of the stone, which contains a large number of marks cut or scratched into the surface with some sharp instrument, such as a mussel shell, a sharp flake of hard stone, or a marsupial’s tooth. Some of them are merely well-defined scratches, whilst others are cut into the stone about one-sixteenth of an inch. The marking extends from the base to the apex. Fig. 2 shows one of the edges of the implement, the marks upon which are not reproduced, because they are continuations of those given on the two faces. I have, however, shown the position of three 1909.] USED BY AUSTRALIAN ABORIGINES. 3 principal incisions, which will be again referred to in dealing with Fig. 4. Fig. 3 is the convex face of the stone, which contains about eighty marks similar in character to those of Fig. 1. Fig. 4 has been introduced to exhibit the position of an irregular spiral incision which extends quite around the implement in a little over three folds. The firm black line on the diagram represents the cuts facing the observer; the dotted lines indicate their position on Scale of Inches a Cr die 2.3 ae RG) 2), B Ce RH M, del. Fics. 1-5. Views of a Ceremonial Stone used by the Australian Aborigines. the other side, if the stone were transparent. The position of the spiral on one of the edges of the stone is shown in Fig. 2. The com- mencement and end of the spiral appears on Fig. 1. It begins at three and seven-eighths of an inch from the apex and terminates at five and one-eighth inches. 4 MATHEWS—CEREMONIAL STONES [January 1, A spiral of this kind has not been observed by me before and consequently adds to the value of the present specimen. In a few other cases, however, I have seen a single, continuous incised line girdling the upper half or pointed end of the stone. In most of the specimens in my possession, as well as in those which have come under my notice elsewhere, a girdling incision of any sort is absent. It is on this account that I have drawn attention to the peculiar marking of the stone now described. Fig. 5 is a view of the basal end of the stone. A characteristic of all the stones of this class which I have seen consists in their having a saucer- or dish-shaped depression chipped or ground into the larger end. In our example there are three such depressions ground into the end of it. (See Fig. 5.) The two smaller ones are very shallow, although easily discernible, but the larger has a depth of nearly one-tenth of an inch in the center. The present is the only instance in which I have observed three of these depressions—one only being the general rule. Another point to which attention may be invited is the very much elongated oval form of a section through the shaft. This is prominently seen in Fig. 5, where the diameter is more than twice as great in one direction as in the other. Most of the stones of this kind are nearly circular in section, whilst an elongated oval section is rarely met with. Again, very few of these stones are so profusely inscribed as the present example. Fig. 6 is a long, thin, cylindrical spindle of a very hard clayslate, eighteen and a quarter inches long. At four inches from the base the greatest diameter is two inches, and at ten inches from the base (Fig. 7) the smallest diameter is one and eleven-twentieth inches. Fig. 7 represents the implement turned a quarter round. A large amount of chipping and grinding has been done by the native artificer to bring this specimen into its present shape, especially at the pointed end and near the base. About the middle of the shaft the original surface of the stone is seen in a few patches some inches in length. Commencing a little over an inch and a half from the base there are numerous incised marks, both horizontal and slightly oblique, all the way to the apex. About half an inch from the extreme point, 1909.] USED BY AUSTRALIAN ABORIGINES. 5 one of these incisions reaches all around the stone. At the middle of the shaft another line encircles it, but the two ends of the line, instead of meeting, overlap each other some two inches, and are from one-quarter to one-half inch apart. This encircling line is very faintly marked. There are about one hundred and forty well- © na Wleletel\ HIT Fics. 6-12. Three Ceremonial Stones used by the Australian Aborigines. defined incisions on the entire surface of this stone, one hundred and twenty of which are accurately reproduced in Figs. 6 and 7. 6 MATHEWS—CEREMONIAL STONES [January 1, In addition to this number there are many other marks which, although distinguishable, are mere scratches and have evidently never been anything more. They are of the same character as the well- defined cuts, but much shorter. Fig. 8 gives a view of the base of the stone, in which there is a saucer-like depression, the average diameter of which is nearly an inch and a quarter. This concavity has been made by picking the surface with some sharp instrument, such as a pointed flake of hard stone, the punctures being still plainly discernible. After the picking out was done the surface was rubbed or ground fairly smooth. The depth of the hollow formed in this way is a little more than one- twentieth of an inch. The specimen was found on Buckanhee Run, Darling River, and its weight is three pounds twelve ounces. Fig. 9 is a soft sandstone, sixteen and one-half inches long, with a practically circular shaft, the greatest diameter of which is two and sixteen-twentieth inches, from which it evenly diminishes to a well-defined point. At four and one-quarter inches from the point there are two slightly curved parallel lines cut well into the stone. On the opposite side of the specimen are two similar incisions, which are not of course visible in my drawing. These comprise all the marks on this stone. From the thickest part of the shaft to the base the diameter slightly decreases, until it averages a little over an inch and three quarters (Fig. 10). The diameter of the depression in the base averages nearly two inches and its depth is one-eighth of an inch. The stone was found on Kallara Station, Darling River, and weighs three pounds fourteen ounces. Fig. 11 is another specimen of decomposed sandstone, sixteen and five-eighth inches in length. At the thickest part the diameter measures two and eighteen-twentieth inches, and a section through any part of the shaft would give an almost circular outline. On the face selected for illustration there are twenty-one incised lines, comprising triplets, pairs and single marks. Fig. 12 represents the base, whose diameter varies from one and three-quarter inches to two and a quarter inches. The usual saucer- shaped concavity has a mean diameter of nearly an inch and a half 1909. ] ' USED BY AUSTRALIAN ABORIGINES. 7 and its depth is one-twentieth of an inch. This specimen was dis- covered on a sand ridge on Maira Plain Station, about fifty miles southeast of Wilcannia, and weighs four pounds and a half. A few remarks will now be made respecting the uses of these stones, information on this point being now difficult to obtain for the reasons stated in the beginning of this brochure. “ Harry Perry,” an old aboriginal of the Darling River, who died at Bourke about a year and a half ago, informed me that although he had never seen the stones in actual use himself, his father and other old men of the tribe had told him that they were employed in ceremonial observances connected with assembling of the tribe at the time the nardoo seed was ripe. The people would be invited to meet at a place adjacent to some low-lying ground which had been moistened by showers during the early spring months, or over which water had flowed in flood time, and which was consequently expected to produce large quantities of the nardoo plant. When the natives from the hin- terland, in whose country there was little or no nardoo, came to the gathering at the appointed time they brought with them articles as presents or for barter with the people who had allowed them the privilege of feasting on the nardoo seed. My native informant be- lieved that the stones in question were used in incantations for pro- ducing an abundant supply of nardoo and other seed bearing plants, as well as for an increase in game and fish. He also said that the messengers who were sent to gather the different portions of the tribe for these festivals, generally carried one of the incised stones to show the purpose of his mission. As soon as other duties will permit I shall take pleasure in sub- mitting to this Society a further article for publication, describing the various forms and materials of the interesting aboriginal relics briefly touched upon in the foregoing pages. PARRAMATTA, New SoutH WaAtEs, October 31, 1908. ibe XSPLORATION OF THE UPPER ARV BY aMEANS OP KTTES AND BALLOONS: By WILLIAM R. BLAIR. (Read March 5, 1909.) HISTORICAL. The kite, so far as we know, was first made and flown by the Chinese general, Han Sin, in the year 206 B. C. It was for a time used in war, being employed by the inhabitants of a besieged town to communicate with the outside, but later seemed to degenerate into a mere toy. Games in which kite strings are crossed and cut by the friction of one on the other are popular in China at the present time and great skill is shown in handling the small kites used for this purpose. Professor William Wilson at Glasgow University and Benjamin Franklin at Philadelphia in the years 1749 and 1752 respectively were the first to use the kite in the study of upper air conditions. Wilson obtained temperatures at “great elevations” by means of self-registering thermometers, while Franklin used his kite as a collector of electricity. Especial interest in upper air temperatures grew out of the con- sideration of the formula for refraction of light by the atmosphere, and kites carrying thermometers were again used in the years 1822 to 1827; this time by the Reverend George Fisher and Captain Sir William Edward Parry. At the same time upper and lower surface stations and captive balloons were first used for the purpose of obtaining temperatures aloft, the former by Sir Thomas Brisbane and the latter by the Earl of Minto. Readings were obtained at elevations of 400 feet with the kites and 1,340 feet with the captive balloons. An editorial in the Edinburgh Journal for January, 1827, con- tains the following paragraph: 1909.] BY MEANS OF KITES AND BALLOONS. 9 To those meteorologists who have sufficient leisure and the means of performing such experiments, we would recommend the use of kites and balloons for ascertaining the temperature and state of the upper atmosphere. The Earl of Minto has obtained several very interesting results by the use of balloons. Ten years later, Espey, in our own country, used kites to prove his theory concerning cloud altitudes. He held that the base of a forming summer cloud should be as many times 100 yards high as the temperature of the air at the earth’s surface is above. the dew point in degrees Fahrenheit, 7. e., that these clouds form in aScend- ing currents and that the air cools one degree Fahrenheit for every 100 yards it ascends. He was able to put his kite in the base of a cloud 1,200 yards above the earth’s surface and not only proved his theory within the error of observation, but found that the motion of the kite in the base of the cloud showed ascending air currents. He also obtained some striking electric effects, wire being used instead of string to fly the kite. The report of the Franklin Kite Club, about 1838, on the dis- covery of ascending air currents gave further proof of Espey’s theory and stated that this theory had the recommendation of the American Philosophical Society. A contemporary of Espey, James Swain, flew kites for the pur- pose of determining daily the height of that layer of “ electrified air whose positive electricity was concentrated enough to expand the leaves of an electrometer.” Swain used No. 30 steel wire, which he wound on a reel four feet in circumference and having a glass axle like the one used by the Franklin Club of Philadelphia. Steel wire is now universally used in kite flying. In 1847 Admiral Back flew kites from the deck of his ship, The Terror, and obtained free air temperatures over the ocean. Up to this time the kites used have been small and rather unstable in their flight. Little more was done with them until Archibald, an Englishman, began to look into the mechanics of kite flight in 1883. In the meantime mountain stations and captive balloons were further developed in an effort to get temperature readings at greater altitudes than had thus far been possible. An observatory was established at Mt. Washington in 1870 and one at Pike’s Peak in 10 BLAIR—EXPLORATION OF THE UPPER AIR [March 5, 1873. The results obtained by these observatories showed, as was pointed out by Professor Abbe and others, that the readings were not sufficiently isolated from terrestrial influences, and attention was again turned to kites. Archibald showed the value of vertical planes for steering pur- poses, constructed kites of greater lifting power and in 1887 used them to carry up a camera. Captain Baden Powell in England, interested in the possible use of kites in war, made them large enough to lifta man. Eddy, at Bayonne, N. J., in 1890, constructed a diamond kite in which the ends of the cross stick were bent back, thus introducing a vertical component in the planes which added to their stability in flight. In 1893, Hargrave, an Australian, invented the box or cellular kite. This kite, although of more complicated construction than forms heretofore used, very soon displaced them for every purpose and seems to contain the fundamental principle upon which all stable aeroplanes are constructed. Eddy’s work was taken up by Mr. Rotch and his assistants at Blue Hill near Boston, and Hargrave’s by the U.S. Weather Bureau under the immediate direction of Messrs. Marvin and Potter. Marvin's study of the mechanics and equilibrium of kites led him to make some modifications in the original box pattern. The Marvin-Hargrave kite, at present quite widely used, is not only more efficient, but is stronger and, for meteorological uses, more con- venient in details of construction than the Hargrave. About this time Marvin designed a meteorograph and convenient hand reels for the wire which were used in a series of upper air observations made at seventeen different stations during the summer of 1898. In this series daily flights were attempted but only 44 per cent. of these attempts were successful, the failures being due to lack of wind or other adverse conditions. Of the 1,217 ascensions made, about 180 were a mile in height, while two were slightly over 8,000 feet. The observations made have been reduced and are published in Bulletin F of the U. S. Weather Bureau. Nearly all first rate weather services now have one or more upper air observatories. Our own upper air work has been concentrated at Mt. Weather, Va., under the immediate direction of the writer, where, since the first of July, 1907, daily except Sunday, ascensions 1909.] BY MEANS OF KITES AND BALLOONS. 11 have been made with either kites or captive balloons, the latter being used only when the wind is insufficient to support the kites, or about one day in twenty. The apparatus in use at Mt. Weather is still undergoing improvement. The mean height at which daily (except Sunday) temperature and other observations are obtained is ap- proximately 3,000 meters, or about 2 miles, above sea level. The highest altitude so far attained by means of kites is 7,044 meters, about 42 miles. This flight was made at Mt. Weather on October 3, 1907. Flights closely approximating this in height were made at the same observatory on April 14 and September 30, 1908, while the fourth highest record, 6,430 meters, was made by the German Observatory at Lindenburg in November, 1905. In the same year that Hargrave invented his kite, Charles Renard suggested the use by meteorolgists of small free balloons made of paper or other suitable material and having sufficient lifting power to carry up self-recording instruments. A balloon of this sort par- tially inflated with hydrogen at the earth’s surface rises until the gas expands sufficiently to burst it, and the instrument is let down safely from this point by means of a small parachute. Teisserenc de Bort, at his observatory at Trappes, Paris, and from the decks of ocean steamers, has obtained upper air records of great importance to meteorology with these paper balloons as well as with kites. More recently Assmann introduced india-rubber balloons about six feet in diameter. These are now the more gener- ally used. Preparatory to an ascension, this balloon is filled until the rubber begins to stretch, 7. e., from 3.5 to 4 cubic meters, depending on the weight it is to carry. The instrument is suspended from a small parachute thrown over the balloon, space being provided for the expansion of the latter to two or three times its diameter or to about twenty times the volume it had at the earth’s surface. Sometimes two balloons are used, one of which bursts—the other lets the instru- ment down slowly. Records of temperature and humidity have been obtained at altitudes of 25,000 meters, over 15 miles above sea level with sounding balloons. At present about twenty-five observatories—two in this conti- nent, one in India, the others in Europe—are codperating with the 12 BLAIR—EXPLORATION OF THE UPPER AIR [March 5, International Commission for Scientific Aéronautics, using either kites or sounding balloons, or both. Captive and manned free bal- loons are occasionally used. Of these observatories, the universities of Manchester and Kasan each maintain one. APPARATUS AND METHODS. The site chosen for an upper air observatory is to some extent determined by the kind of work to be done. A kite field should be clear of trees and other obstructions that might either entangle the wire or hinder the movements of the men who manipulate the kites. It should be situated on an eminence just high enough to prevent its being sheltered by any other in the immediate vicinity, but not high enough to introduce the complications of mountain and valley effects, unless indeed such local effects and not the general condi- tions obtaining in storms as they pass, be the object of the study. It is well if the country for thirty miles around in the vicinity of the field be free from large bodies of water and inhabited, for kites break away at times and these conditions facilitate their return. Close proximity to a city, on the other hand, is likely to bring kite flyers into unpleasant relationships with the local telephone and other electric companies who transmit power on overhead wires. For captive balloons the conditions should be the same as for kites. Sounding balloons may be started from any place at which the true surface conditions can be recorded for comparison with the upper air data, except that the land area immediately to the east should be free from large lakes and fairly well settled. The balloons set free in this country by Professor Rotch have invar- iably traveled in an easterly direction and landed within a radius of 300 miles from their starting point. Each balloon carries with it instructions to its finder for packing and shipping and informs him that he will be rewarded for his trouble. This plan has brought back about 95 per cent. of all sounding balloons liberated in St. Louis, the only place in our country so far chosen for this work. The ideal upper air observatory is one at which all three of these methods may be used, kites and captive balloons being less expensive and more efficient for levels up to 3,000 or 4,000 meters, 2 or 3 miles, and sounding balloons for higher levels. 1909.] BY MEANS OF KITES AND BALLOONS. 13 The self-recording instruments used in kite and sounding balloon work are numerous in variety. Many observatories have instru- ments made from special designs. All are built on essentially the same plan. A clockwork rotates a cylinder which is covered with either a sheet of paper ruled to scale or a sheet of smoked paper or aluminium. Upon this sheet the pens or points, as the case may be, connected with their respective elements, trace the conditions. Paper scales are the more convenient and are used when the tem- peratures to be recorded are not so low as to freeze the ink. The instruments are made as light as possible, aluminium being the metal used in the construction wherever it can be adapted. From 750 to 1,500 grams is the usual weight of an instrument, those for use in kites being more substantially built than those for use in balloons. The anemometer usually consists of a small aluminium pin wheel mechanically geared to the pen—some are electrically connected. The hair hygrometer is the only form yet available for self-recording purposes that is light enough. The temperature is measured with either a bimetallic element or a partially coiled tube containing toluene. The barometer is of the aneroid type. The order of accu- racy of these instruments is not high. Difficulty is experienced in keeping the anemometer properly oriented while the kite is flying. The hair hygrometer, if kept in good condition, probably records within less than 5 per cent. of the correct value. Records of pres- sure are, in nearly all cases, correct to within 2 mm., in many to within I mm. The temperature may be relied upon to one degree Centigrade in the records obtained from most kite flights, to less in many. When used in sounding balloons at very great altitudes the absolute error in any element is of course greater than those men- tioned. In this case no anemometer is used, the wind velocity being determined from observations on the drifting balloon with one or more theodolites. The differences in the various instruments consist chiefly in the way of exposing the elements so as to best obtain true records of the conditions in the vicinity of the instrument. It is essential that the temperature element especially be properly ventilated and insu- lated. The method of ventilation is of course different in sounding balloon and kite instruments. The former, being carried by the [March 5, OF THE UPPER AIR BLAIR—EX PLORATION 14 ‘ydeiso1oajaw prVYyIy ‘I ‘OL SRREPCERRSUaL 1909.] BY MEANS OF KITES AND BALLOONS. 15 wind, is in a calm except for its own upward motion through the air. It is therefore exposed in a vertical tube at the top of which is a funnel to insure the passage of a sufficient air current through the tube and about the element. The latter are held by the kites in the horizontal current in which the kite flies. The velocity of this cur- rent is always sufficient to keep the temperature element well venti- lated so that care need be taken only to see that the element is in this current and screened from either the direct or reflected rays of the sun. The meteorographs in use need comparison with standard instru- ments, at first to determine their scale values, frequently thereafter to guard against error due to slightly defective elements. Before and after an ascent the instrument is placed in a standard shelter with standardized instruments and allowed to record. Frequent readings of the latter are taken not only at these times but during the entire ascension. A base line for computation of altitudes is thus furnished, also a record of surface conditions for comparison with those of the upper air. To facilitate this computation and comparison, as well as to avoid errors due to the sluggishness of the elements, stops in the ascent and descent are made at frequent inter- vals. These stops need be for but a few minutes. Their times are recorded at the lower station and they are easily distinguishable on the traces. Of course it is impossible to make such stops with sounding balloons, and consequently instruments sent up by means of them should be, to some extent, at least, tested for sluggishness in addition to the tests made for scale values. The cellular kite invented by Hargrave or some of its numerous modifications is the one most generally used for meteorological pur- poses. The Marvin-Hargrave kite, in which three planes are put in the front cell and the entire framework strengthened by fine steel wire braces, is the one in use at Mt. Weather. With slight modifi- cations in the size and shape of the planes and in the proportion and distribution of lifting and steering surfaces, this kite has been made to serve in all winds from 3.5 to 22.5 meters per second. The dimen- sions of a medium-sized kite, one well adapted to carrying an instru- ment in winds of from 5 to 10 meters per second, are as follows: PROC, AMER. PHIL. SOC., XLVIII. I9I1 B, PRINTED JUNE 30, I909. ‘ydeisO10djoW UIAIRI, “2 “DI [March 5, ues atahg ay it) 3 = i aoe = < m4 ea Ay py =) fx) a by O Z ) e < a O 4 Ay BG | pA < 4 eal 1s BY MEANS OF KITES AND BALLOONS. 1909.] *LO61 ‘€ 19q019Q JO WYSIY wWoIZ prody “f ‘OWT Ea Gra {yy vi A a8 iin ia SA ee See iS P| nine i i Hl Tf les ont nl HH = ee Be = Bama = aS rss] a Bae GV. ye PRS \ | Tet le nh. Sill HTT UT TTT EE manna TT TTT UI REE REE it 1 i | il \ Y } i ll | \ it Mt Ae LN wi qi) | HS aa a i | | . | D | es = S i a a CE Gata See SE Gee SS SEM ee Ge We ee ee 1) Sa a | a en GC en it S iN it I f i | a | yal Hl l [ it MH ‘Al HL Uillddeer: it ill iit HH". ) ‘aD it ith ill Ti ii idl ill the tots a= = a i i il rua Wid ahabhialin ns ih ll, Net ll B74 I| | ll TTT lik HI lll \3 § § pane tv bit nt Pi is ‘ eS . a. aed by fa | LY eae? 2S 7 18 BLAIR—EXPLORATION OF THE UPPER AIR [March s, 1 ICES Ved aici Neen Ao aea ie Uns AC Fev Ea. aca Ui cm 204 cm, NAVA hn op ama OR ARORA ese iA tn me Cet ee A 197 cm. IS) rp Ula epcet vcd lets aes aN URC etm aaa 81 cm. Wiadthe ofsiplames es: soci Asien emu ee ee cen 64 cm. Planes TSPacey Larval tetsecseacin He ene ENCES rae eT 76 cm. AAG Fea GIRL Atom ec Re ra Gator To ay eu ey eu a ett 3.2 to 3.8 kg. ’ There are five lifting planes, so called, and four steering. The area of the lifting planes is 6.3 square meters, while that of the steering planes is one third as much. Kites varying from these di- mensions and necessarily therefore from these proportions are built for winds higher and lower than those to which the above-described kite is adapted. TO CLOUT § ie Sop liam UT Noo) 5 eo! 7 TT C3 [am + tsdasroununsey) " * ee rT) ." het oeal AR mi | ice Po PROCEEDINGS Am. PHILos. Soc. VOL. XLVIII. No. 191 PLATE V = ay aN Lt) 1909. ] STRAND” PEANTS OF NEW JERSEY. 89 species of Bermudan plants with relation to the environmental fac- tors of the sand dunes upon which the plants grew. In this paper a short bibliography of the principal papers is given. EXPLANATION OF THE PLATES. In Plate II, Fig. 1, is shown the frontal sea dune at Sea Side Park covered with the marram grass Ammophila arenaria and a large clump of Cakile edentula, while in Fig. 2 is represented the crest of the frontal dune covered with marram grass, back of which occur the waxberry Myrica carolinensis and the clumps of Hud- sonia tomentosa. The photograph reproduced in Plate III, Fig. 3, represents the thicket formation at South Sea Side Park composed of Jlex opaca, Sassafras officinale, Rhus radicans and Solidago sempervirens. In Fig. 4, Plate III, is represented a slough with floating rafts of Eleo- charis pygmea. The twenty enlarged figures with details of stomata, shown in Plate IV, represent the structure of the leaves of the sand strand plants of New Jersey, while the twelve figures and stomata enlargements represent the leaf structure of typic salt marsh species (Gelate 3V)). THE DESTRUCTION OF THE FRESH-WATER FAUNA IN WESTERN PENNSYLVANIA. (PiaTeE VI.) By DR. A. E. ORTMANN. (Read April 23, 1909.) It is generally known that the advance of civilization in a coun- try is connected with a retreat and the disappearance of the indige- nous fauna. This has been observed most distinctly in those parts of the world which have been settled by the white man in more recent times, and in many cases we have positive records with ref- erence to the killing and crowding out of the original inhabitants of the country, belonging to the animal kingdom; yet these records chiefly concern the more highly developed forms of life (mammals or vertebrates in general), which preéminently attract attention. But there are many other forms of animal life, chiefly among the invertebrates, which suffer the same fate. Such cases generally are not noticed, but students particularly interested in such groups often have reason to deplore the disappearance of interesting creatures, which used to be abundant. The present writer, in connection with his duties as curator of invertebrate zodlogy at the Carnegie Museum, has made it one of his chief objects to study and to preserve records of the fresh-water fauna of the northeastern section of the United States, and first of all, of the country lying in the immediate vicinity of Pittsburgh. This region belongs to the drainage of the upper Ohio and of Lake Erie, and it is well known that originally a very rich fauna was present here, a fauna which forms part of the great fauna of the interior basin, eminently rich in all forms of fresh-water life. It is also a well-known fact that on account of the progress of civiliza- tion in western Pennsylvania, on account of its industrial and com- mercial development, and all the various features of “improve- 90 1909.] FRESH-WATER FAUNA IN PENNSYLVANIA. 91 ments” connected with it, the fresh-water fauna has deteriorated, has become poor, and in many cases extinct. Yet it is not realized how far this process has advanced, and to what extent the fresh water of this region has become unfit for the indigenous life. The present paper has the object to record the present state of things in this respect, and to point out which rivers and creeks are in such a state that they do not offer any more the required conditions for animal life, and which are yet in a good or fair condition. It may be remarked that all facts collected here have been ascertained by the writer in person, in the course of his studies during the last five years. All streams recorded on the map accompanying this paper (Plate VI) have been visited by the writer, and collections of their invertebrate fauna and observations on their vertebrate fauna have been made, wherever such was still present: but in many cases his efforts were in vain, and life had entirely disappeared in many streams. The blue color on our map tells a pitiful story, pitiful not only from the standpoint of the scientific man, but also with refer- ence to the question of utility. For we must not forget that the original fauna of the fresh water forms part of the sources” of the country. In many cases the direct economic value, ce natural re- chiefly of the fresh-water invertebrates, is not very apparent; but considering the fact that all forms of life in an ecological com- munity are mutually dependent upon each other, we realize that the more important forms (mussels, fishes and aquatic mammals) can- not be preserved, unless the creatures which furnish the necessary conditions for their subsistence are also preserved. Thus the de- struction of our fresh-water fauna forms a chapter of the book on the destruction of our natural resources, a record which is not at all to the credit of the nation. I. THe FrReESH-WATER FAUNA. The part of the fresh-water fauna which has chiefly been studied by the writer is, as has been stated, the invertebrates. However, during his investigations, he kept his eyes open for vertebrate life, and among the latter it is chiefly the fishes to which he paid atten- tion. He did not make systematic collections of the fishes, and thus 92 ORTMANN—THE DESTRUCTION OF [April 23, he cannot give positive information as to the presence or absence of particular species of them. But the question of their existence in general in the different streams is easily settled, in fact this is the most conspicuous criterion by which people generally judge the con- dition of a stream—whether there is “ good fishing” or not. However, the presence of fishes in a stream does not always indicate that the latter is in good shape. The condition of the streams, as we shall see below, often changes during the season; it is bad in dry weather, but improves when there has been copious precipitation. The fishes are most apt to take advantage of such temporary improvement on account of their great power of locomo- tion (vagility) ; in fact, many fishes migrate more or less regularly up or down stream, and thus may be present at certain seasons in parts of our water-courses, which are barren in other seasons. Other vertebrates are of minor importance. Among the mam- mals we should mention the muskrat (Fiber zibethicus). This animal is fairly abundant everywhere, but, as might be expected, tends to disappear, where its food disappears. The latter consists only in part of invertebrates (mussels for instance), while in another part it is vegetable (roots of aquatic plants, and also various parts of land plants). Thus it is understood that the pollution of a stream does not render the existence of muskrats impossible. And further, the bad condition of the water does not harm the animal directly, since it is an air-breathing form. The fact that the musk- rat is decidedly less frequent in polluted streams is probably due to the fact that the pollution is greatest in the vicinity of larger settle- ments, where there is greater danger for them by being hunted by man. Of the reptiles, water-snakes (Natrix sipedon and leberis) and turtles should be considered. As regards the former, it is a general rule that they disappear from polluted streams, and very likely not on account of the direct influence of the water upon their body, but on account of the destruction of their food—fish and crawfish. The turtles live in part upon animal, in part upon vegetable food; they are found, at present, in numbers only in streams which are in good condition, and have disappeared, more or less, in those with 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 93 polluted waters; this, however, at least in certain species, is appar- ently due also to direct extermination by man. The soft shell turtle (Aspidonectes spinifer) is a good example; it used to be present almost everywhere, but it has been exterminated practically in the Ohio, the lower Allegheny, the Monongahela and Youghio- gheny. It is still present, for instance, in the clear waters of the upper Youghiogheny, the upper Allegheny, in Lake Erie, ete. Among the amphibians, frogs and toads do not prefer the streams ; they rather are pond and lake forms, and, besides, inhabit the water only at certain seasons. They do not seem to be very susceptible to the quality of the water, since they are air-breathing animals, and, consequently, are still abundant, although certain spe- cies show a tendency to become rare. Thus the bullfrog is met with in numbers only in the northwest of the state, where clear streams, ponds and lakes prevail. Yet in this case, extermination by man has surely played a part. Of the Urodela, the smaller salamanders and newts do not in- habit in large numbers the rivers and creeks, but prefer rather the mountain streams, the ponds and lakes, where generally the condi- tions are yet good. ‘Thus there does not seem to be an appreciable reduction of their number. The two large salamanders, the hell- bender (Cryptobranchus allegheniensis) and mud puppy (Necturus maculosus) surely are influenced by the pollution, yet not directly, but by the destruction of their food. They seem to be the last mem- bers of the fresh-water fauna which disappear, and are occasionally found where there is no other permanent life. (Hellbenders were frequent in the Conemaugh River at New Florence, Westmoreland Co. Nothing but a few fish and crawfish were at this locality, which apparently came from a clear tributary.) The most important forms of invertebrates, which I have studied more closely, are the crustaceans and the mollusks. Occasionally I have collected fresh-water sponges, worms, bryozoans, but of all these we may say that they disappear very soon after the stream has become polluted. They are found only in such waters which contain an abundance of other life. The crustaceans of the genus Cambarus (crawfishes) are rather susceptible, and we may say that generally the pollution of a stream 94 ORTMANN—THE DESTRUCTION OF [April 23, destroys them. They seem to be slightly more resistant than the Unionide (see below), but their presence in a polluted stream is in many cases clearly due to a restocking of the stream, by immigra- tion from a clear tributary. The crawfishes are rather vagile, and possess the power to migrate, although less so than the fishes. There surely is the possibility for them to take advantage of a temporary improvement of the condition of a stream. The most important group, with reference to the matter in ques- tion, are the bivalve mollusks of the family Unionide, the fresh- water mussels or river-clams. They are the most reliable indicators of the pollution of a stream. Being rather sedentary, living on the bottom of the rivers, breathing water, they are easily influenced by the deterioration of the water. Of all the more important groups of our fresh-water fauna, they die first, and after they have been exterminated, it is exceedingly difficult to restock the stream on account of the complex life history of the young mussels. It is known that the young Unionidz are transported and dispersed by fishes, but in a polluted stream the fishes have also disappeared, and even in a case of a temporary recovery of a stream, in times of a high stage of the water, if there should be a restocking with young mussel-fry, the latter will surely be killed during the next low stage, when the pollution again is concentrated. In this respect the Union- ide surely are worse off than the fishes and crawfishes. Of other mollusks, the gasteropods belonging to the family Pleu- roceride (Pleurocera, Goniobasis, Anculosa) should be mentioned. They are generally absent in polluted rivers, but have been found surviving, together with crawfishes, in parts where Unionide were entirely, and the fishes for the greater part gone (Allegheny River in southern Venango County). Other mollusks, which are air breathing (genera Lymnea, Planorbis, Physa) are more resistant, and this is especially true of Physa, which represents in certain instances the only remaining life in certain rivers. But there also seems to be a limit to its power of endurance, and in very badly pol- luted streams also Physa is absent. Thus we can establish, in a rough way, a certain succession for the disappearance of our fauna. The first sign of pollution of a dangerous character in a stream 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 95 is given by the disappearance of the Unionidz, and, generally, this fauna is irreparably lost. Close upon this follows the disappear- ance of the fishes, yet in times of recovery of the rivers (at high- water stages), fishes reappear, coming from tributaries, etc., which have acted as preserves, and this may go on indefinitely as long as the river is recovering again at times, since the fishes possess a high power of locomotion (as we shall see below, the construction of dams in a river puts an end also to this). Crawfishes stand it a ‘little longer than fishes, but they also disappear finally, and the tem- porary restocking of a stream takes place only in a limited degree.* With the crawfishes, or soon after them, the Gasteropods of the family Pleurocerid@ are driven out. When the process has reached this stage, the higher forms of life, which subsist on these various forms are compelled to abandon the stream: tailed Batrachians, Snakes, and part of the Turtles. Finally, only Lymnea, Planorbis and Physa, and the muskrat survive. Of these, Physa disappears last, while the muskrat may stay indefinitely, being not entirely dependent upon animal or aquatic food. II. Tue CAUSES OF THE DESTRUCTION OF THE FAUNA. A. Direct Extermination by Man. A number of fresh-water animals are directly killed by man, and thus disappear in streams, the character of which has not been changed unfavorably for life. This is true in the first line for the fishes. Fishes, forming part of human food, are sought for every- where, and in consequence of the increase of the population neces- sarily must be decimated in number. Yet a complete destruction of the fish life hardly has ever been brought about by man alone, chiefly so, if the fishing is carried on under the restrictions put upon it by law. The fact is that there are many places where “ fishing is good,” and where fishermen freely avail themselves of this chance, but where fishes are still abundant (upper Allegheny River, for ‘It happens sometimes that restocking of the lost territory is done by a different species. Thus in the Mahoning Creek at Punxsutawney, Jefferson Co., and in Slipperyrock Creek at Branchton, Butler Co., the original species, which was destroyed, was Cambarus obscurus, and subsequently, C. bartoni entered the creek. PROC. AMER, PHIL. SOC, XLVIII. I9I G, PRINTED JULY 6, 1909. 96 ORTMANN—THE DESTRUCTION OF [April 23, instance). This is not so in certain remote streams, but not on account of the legitimate pursuit of the sport, but in consequence of the illegal destruction of the fishes. The worst is the dynamiting of the streams which, of course, can be carried out safely only in such places where the fish warden is likely not watching. I can name at least one stream, in which this has had serious conse- quences: Raccoon Creek in Beaver County, and here it is done, as I have been informed, by parties that come over the state line from West Virginia and Ohio, and that have no right whatever to fish in our waters. The fish warden cannot be on the spot all the time, and the farmers of the region are powerless to stop the abuse, and thus Raccoon Creek, which is physically in good condition, and which used to teem with fish life, has been spoiled. For the dyna- miting kills all fishes, old and young indiscriminately, and must be regarded as the most contemptuous way of wanton destruction. I do not doubt that it is resorted to in other parts (I heard of one case in Deer Creek, Allegheny County, not far from Pittsburgh), yet, of course, since it is executed by the guilty parties only under rigorous precautions, in order that they may not be caught by the authorities, such cases generally escape detection. There is only one other group of fresh-water animals which is of direct value to man (if we disregard the muskrat, which is hunted for its pelt, and some turtles, which are eaten). These are the fresh-water mussels (Unionide). For food they are not much sought, but the occasional occurrence of pearls in them makes them valuable. In Pennsylvania pearl fishing is not much practiced, yet I know that certain individuals hunt for pearls in mussels along the Allegheny River in Armstrong County, and once I came across a party of three, hunting pearls in the Ohio in Beaver County. These people were from somewhere down the Ohio in the state of Ohio or West Virginia, and it was indeed a sight to look upon the wholesale destruction carried on by them. In general we may say that by the direct action of man our fresh-water fauna, chiefly that of the fishes, has suffered a good deal, but the complete extermination has not been brought about by it in any stream. Fishing might go on in the usual way, under the established legal restrictions, and our fish fauna will survive indefi- 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 97 nitely. If we further consider the fact that the state is trying to restock our streams artificially, this might entirely counterbalance the losses caused by the fisherman, and thus we may say that fishing alone would never destroy our fish fauna. B. Pollution of Streams. The worst damage to our fauna is done by the pollution of the streams, that is to say, by the discharge into them of substances which are directly injurious to life. This is connected directly with our commercial and industrial progress, and the damage done by it is irreparable, unless there is some radical change in the way of the disposal of the industrial refuse, which at present is generally allowed to run directly into the nearest stream. The most widely distributed pollution of a stream is by sewage from the larger towns and cities. This in itself is rather innocent. I am not discussing the deterioration of the waters from a sanitary standpoint ; but with regard to animal life in our rivers, sewage does not seem to be harmful; on the contrary, certain forms (fishes, craw- fishes, mussels) seem to thrive on it. Only in a few cases I have seen sewage so concentrated (certain small runs in the city of Pitts- burgh), that animal life is killed. Much more dangerous sources of pollution are given by our coal mines. Under this head I unite all sources of pollution, which are connected with the mining of coal, with the coking process, and with the steel industry. This kind of pollution is very widely distributed in the western part of the state. It is a process which charges the water of our streams with certain acids, which, when they reach a certain degree of concentration, directly kill the life.* A stream polluted by “mine water” is easily recognized (when clear) by the peculiar bluish-green color of the water, and by a peculiar rusty-red deposit upon its bottom. Another source of pollution is furnished by the oil wells and the oil industries. The simple working of an oil well already yields injurious matter: during the drilling of the well invariably salt water is pumped up, and the oil itself is capable of destroying life, if present in excess, and forming, at low stages, a deposit upon the *See Stabler H., Water Supply and Irrigation Paper no. 186, 1906, p. 5. 98 ORTMANN—THE DESTRUCTION OF [April 23, bottom of a creek. But the worst are the oil refineries, which dis- charge into the water chemicals which are utterly destructive to life. These are the two most important sources of the pollution of our streams: coal and oil. In addition, there are others, which are more or less local, yet may become quite important in certain sections. These are various industrial establishments, such as glass factories, china factories, different kinds of chemical factories, wood-pulp mills,? saw mills, tanneries, etc. There are certain sections of the state, for instance the region of the headwaters of the Allegheny and of Clarion River, where establishments of this kind are the chief source of contamination. It is not my intention here to treat of the chemical side of the process, because it is rather complex, and needs careful investiga- tion by experts. This investigation is rendered more difficult, since in most of our streams it is not one cause, which contributes to the pollution, but several, often all of them, which contribute their share in a particular stream. Finally, a last cause of destruction of life should be mentioned, which, however, is not connected with a deterioration of the quality of the water. This is the damming up of certain rivers. This has been done most extensively in the Monongahela River, and in a part of the Ohio below Pittsburgh. The dams and locks have been built for the advantage of the shipping interests, producing a more uniform level of the water, permitting navigation all the year round. By this process the rivers, which originally possessed a lively cur- rent, with riffles, islands, etc., have been transformed into a series of pools of quiet, stagnant water, and this change has driven out certain forms of life. It is most destructive to mussels, most of which require a lively current. Dams also prevent free migration, for instance of fishes, and thus they must be an obstacle to the nat- ural restocking of the rivers in periods of high water. ® See Phelps, E. B., Water Supply and Irrigation Paper no. 226. 1909. 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 99 III. SKETCH OF THE PRESENT CONDITION OF OuR RIVERS. (See map, plate VI.) 1. The Ohio River Below Pittsburgh. At Pittsburgh, the two main rivers, Allegheny and Monongahela, unite to form the Ohio. As we shall see below, both the Allegheny and Monongahela are as badly polluted as they possibly could be, and, consequently, it is not astonishing that the Ohio immediately below Pittsburgh is also in a deplorable condition. In addition, it is “ec dammed up, this “improvement” extending down to dam No. 6 at Vanport (below Beaver) in Beaver County. Generally, there is not much life in this part of the Ohio. Fishes are found occasion- ally, during high water, due to some migration, probably from farther down the river, but even this has been rendered difficult or even impossible in consequence of the perfection of the dams (dam No. 6 was finished and put in operation toward the end of 1907). There are crawfishes in this part of the river, but they are disap- pearing fast. Unionidze have disappeared long ago. There was a colony of them in the left branch of the Ohio at Neville Island, Allegheny County, up to 1904; during that year, however, they died out, and in 1905 the last living one was found there. Farther down, below dam No. 6, conditions improve. This is a very interesting and important fact. Although the Ohio collects most of the polluted water of the western section of the state, and although it is in a very bad condition below Pittsburgh, it loses its bad qualities, at least in part, about thirty miles farther down. Since there are only two important tributaries along this part of its course, Chartiers Creek and Beaver River, both of them also badly polluted, this improvement of the water cannot be due to dilution alone, but it is evident that some of the injurious substances in the water must be removed from it, and very probably by precipitation upon the bottom of the river. We shall observe indications of this process elsewhere, and shall discuss its significance below. Here it is sufficient to point out, that at present (1908) the condition of the Ohio below dam No. 6 is good or fair, life being not only possible, but abundant in it, all the way down to the state line at Smith’s 100 ORTMANN—THE DESTRUCTION OF [April 23, Ferry. This is shown first of all by the abundance of Unionide in this part of the Ohio; in fact, here are found the most favorable localities for them known to me in western Pennsylvania. It seems that in 1907 these conditions extended a certain distance farther up; at any rate, in that year I found evidence of the presence of Union- idz in the Ohio at Beaver (the stage of the water was not low enough for proper investigation). But since the completion of dam No. 6 this is all over now, and if there should be life in the pool above dam No. 6 it will have disappeared by this time, at least most of it. Moreover, there are indications that the fauna in the Ohio below Vanport is already suffering. There are at least two tremendous banks, consisting chiefly of dead shells (with many living ones among them) in the river, one at Industry, the other at Shipping- port. Since dead shells are dissolved rather rapidly, these masses indicate a recent dying of mussels on a large scale. And further, it is very remarkable that among the living shells collected by myself there are hardly any young individuals. It seems to me that, while the old and tough ones (some of them probably_ten years old and older) are able to stand the poor condition of the water, the latter is too much for young and delicate ones, so that there is no new generation growing up. This, of course, would be the first step toward the final destruction of the mussels in this part of the river, and the destruction of the other forms of life then will also be accomplished in due time. 2. The Smaller Tributaries of the Ohio. There is a group of streams in Greene and Washington Counties, running westward through the panhandle of West Virginia into the Ohio. These are (from south to north): Pennsylvania Fork of Fish Creek, Wheeling Creek, Buffalo Creek, Cross Creek, Harmons Creek. They are all clear creeks, only Harmons Creek and Cross Creek are slightly polluted by mine water, but not much damage has been done yet. They are all rich in aquatic life. I have not visited Wheeling Creek in Pennsylvania, but I know it in West Virginia, above Elm Grove, near Wheeling, where it is in good condition. Raccoon Creek, which empties from the south into the Ohio 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 101 below Vanport, is in very good condition for most of its length, only way up at its sources, in Washington County, it is slightly polluted by mine water. This creek used to be rich in all forms of life, and is yet so here and there, but, as has been said, its fish fauna has greatly suffered in consequence of illegal fishing. At the point where the Ohio leaves the state a very beautiful tributary flows into it from the north—Little Beaver Creek. This was, and partly is, a model stream with regard to all forms of fresh- water life. Yet in 1908 there were, in its upper parts, near New Galilee, in Beaver County, signs of pollution, in this case in conse- quence of new oil wells being drilled in the vicinity. Salt water and oil was discharged into the creek, and the fauna (chiefly the mussels) indicated distinctly the deteriorating effect by their dis- eased condition and by the frequency of shells which had died recently. This may be only a temporary effect, and if there is no additional pollution, conditions may remain favorable. Immediately below Pittsburgh, Chartiers Creek, coming from the south, empties into the Ohio. It is hopelessly polluted by the coal mines and oil refineries in Allegheny and Washington Counties. There is no life whatever in this creek: the last traces are known to have existed in it as late as 1900, when a few Unionide were col- lected in it for the Carnegie Museum. The condition of Chartiers Creek is now beyond repair. 3. The Beaver River Drainage. Beaver River flows into the Ohio from the north at Beaver, Beaver County. It is utterly polluted in its whole length, up to the point where it is formed by the confluence of Mahoning and Shenango rivers. The source of the pollution is situated on the Shenango River, along its last two miles, in and below Newcas- tle, Lawrence County. The steel mills and various other establish- ments furnish a tremendous amount of injurious refuse draining into the river, and rendering it entirely unfit for life. This state of affairs has been brought about during the last ten years, for in 1898 the fauna of the river was very rich at Wampum, Lawrence County, as is shown by collections preserved in the Carnegie Museum. 102 ORTMANN—THE DESTRUCTION OF [April 23, Connoquennessing Creek, flowing into the Beaver from the east, is another badly polluted stream. In this case there are various causes of pollution, but the chief one is the refuse from the glass works at Butler, Butler County. In the lower parts of Connoquen- nessing Creek traces of life are yet present, but in a few years every- thing will be gone. Above Butler, the creek is in a fair condition. Of its tributaries, Glade Run is polluted by oil well products. Brush Creek is good, and also Slipperyrock Creek in its lower course. The latter is an example of the natural clearing of the water, for in its upper parts, in northern Butler County, it is in a very bad con- dition, polluted by mine water. In this case dilution of the pollution apparently plays an important part, for at least two of its tributaries, Wolf and Muddy Creeks, are in good condition. In Wolf Creek the effect of plain sewage is distinctly seen by the fact that the fish- and mussel-fauna are favored by it—the Unionide attain an unusual size just below the point where the sewage from Grove City, Mercer County, goes into the creek. Of the two rivers which form the Beaver, Mahoning River is, as has been shown by Leighton,* badly polluted in the state of Ohio at Alliance, Warren, Niles and Youngstown. Yet in Pennsylvania, in its lower parts, it is rich in life. We again have to deal here with the natural clearing process of the water. At Hillsville, where the Mahoning enters our state, it is in poor condition, yet there is some life. Then comes a dam at Edinburg, and below this dam condi- tions are much better. In fact, the fauna is rich, and continues so till the river joins the Shenango. In this case, there are no impor- tant tributaries along this stretch, and the clearing of the water cannot very well be attributed to dilution. The Shenango River above Newcastle is in good condition all the way up to its sources, and so are its tributaries, Neshannock Creek, Pymatuning Creek and Little Shenango River. Only at and below Sharon and Sharpsville, in Mercer County, some pollution goes into the Shenango from the steel mills, but it has not had much effect yet. However, the damage is bound to increase, and I am afraid in a few years the effect will be noticeable. At the present *See Leighton, M. O., U. S. Geol. Surv. Water Supply and Irrigation Paper no. 79; 1003, p. 133. 1909.] FRESH-WATER FAUNA IN PENNSYLVANIA. 103 time these creeks are in splendid condition at many points, and this is preéminently the case, as regards the fish fauna, in Neshannock Creek. 4. The Monongahela Drainage. We may say that of the Monongahela drainage by far the great- est part is utterly polluted, chiefly by mine water.2 The Monon- gahela and its chief tributary, the Youghiogheny, drain the most important coal regions of the state, and there are, in this whole region, only a few streams left which have clear water. They are the following: Ten Mile Creek and Dunkard Creek in Washington and Greene Counties, yet the South Branch of Ten Mile Creek became polluted in the spring of 1908 by the bursting of an oil pipe- line near Waynesburg, Greene County. Dunkard Creek is yet splendid in every respect. Cheat River is clear, but there are only two or three miles of it in the state, and on its right banks, at Cheat Haven, a small run empties into it, which brings a great amount of mine water from the coke-ovens at Atchinson, killing everything along its right banks.® The Youghiogheny is in a fair condition above Connelsville, Fayette County, and Indian Creek, one of its tributaries, is very good (trout stream). However, the Youghiogheny has improved from Confluence down. For at this place it receives a badly pol- luted tributary, Casselman River, which brings mine water from the mines in southern Somerset County. The Youghiogheny above Con- fluence, south into Maryland, is very clear and pure. For the rest, all the more important creeks tributary to the Monongahela system, in Washington, Fayette and Westmoreland Counties, are polluted by mine water. This is especially true in the cases of George and Redstone Creeks, draining the Uniontown dis- trict, Jacobs Creek, coming from the Mount Pleasant and Scottdale mines, and, worst of all, Turtle Creek, with its tributary, Brush Creek, which drain the coal fields of Westmoreland County. * Leighton, ibid., p. 126 ff. This condition obtained already in 1808, see Rhoads, S. N., in Nautilus, 12, 1899, p. 133. °*The condition of the Cheat below Parsons, Tucker Co., W. Va., is dreadful, it being polluted by the refuse from a wood pulp mill. But it improves farther down. 104 ORTMANN—THE DESTRUCTION OF [April 23, 5. The Allegheny Drainage. (a) The lower Allegheny, from Oil City and Franklin (Venango County) downward, is first badly polluted, then it improves, and is again polluted to a very considerable degree. The chief source of pollution are the oil refineries at Oil Cityand Franklin. The injurious substances discharged into the river at these two places are simply amazing, and render the river entirely unfit for life; for thirty miles and more below there is not a mussel, not a crawfish, nor a fish able to live in this water. Then a gradual improvement begins in south- ern Venango County (pond snails, Physa and Goniobasis are pres- ent, also crawfishes begin to appear), and in northern Armstrong County conditions become almost normal. In spite of some addi- tional pollution going into the river at Kittanning and Ford City (china factories), the good condition continues down to the point where the Kiskiminetas River discharges its mine water into the Allegheny from the left side. This destroys life on the left banks of the Allegheny, but conditions continue favorable on the right banks into Allegheny County, till we reach Natrona and Tarentum. Here additional pollution comes in in the shape of salt water (salt works at Natrona) and the refuse of various mills, and this goes on all along the river down to where it unites with the Monongahela at Pittsburgh. Here the Allegheny is utterly polluted, and we have here possibly the greatest variety of pollution of any of the streams in the state.’ (b) The Smaller Tributaries of the Lower Allegheny River.— Of the following smaller tributaries of the lower Allegheny, the condition is known to the writer. On the right side, Pine Creek, in Allegheny County, is polluted more or less, chiefly by oil wells, but its headwaters are in a fair condition. Deer Creek and Bull Creek are rather good. Buffalo Creek, running along the boundary line of Butler and Armstrong Counties, is in very good condition, and contains an abundance of life. On the left side is Puketta Creek, forming the boundary of Allegheny and Westmoreland Counties, which also is in rather good condition. (c) The Kiskiminetas Drainage.—As has been stated above, the *See Leighton, M. O., I. c., p. 122. 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 105 Kiskiminetas River, at its point of union with the Allegheny, is in a fearful condition, the pollution consisting chiefly of mine water from the extensive coal regions of Westmoreland, Indiana, Cambria and Somerset Counties. In fact, we may say, that in almost all of the drainage basin of the Kiskiminetas fresh-water life is extinct.® For the main stream, the Kiskiminetas-Conemaugh, this is true for its whole length, from above Johnstown in Cambria County down- ward. The Loyalhanna River from Latrobe downward is even worse than the Conemaugh. Black Lick Creek and its tributaries, Two Lick and Yellow Creeks, in Indiana County, are also polluted, and so is Stony Creek in Somerset County. There are, in the whole Kiskiminetas drainage, only very few streams possessing clear water and a tolerably well preserved fauna. In Westmoreland County we have a small stream, Beaver Run, which is good, and the Loyalhanna River above Latrobe contains a rich fauna. In Indiana County Blacklegs Run and the upper parts of Two Lick and Yellow Creeks are in good condition; in the lower part of Yellow Creek the fauna was destroyed during 1908. A mine had been opened in 1907 above Homer City, and the mine water discharged into the creek did its deadly work in the summer of 1908, when the stage of the water for the first time after the opening of the mine became so low that the concentration of the pollution was great enough to kill the fauna. On July 23, 1908, the writer personally witnessed the actual destruction of the fauna, and the number of dead and dying fishes seen in Yellow Creek at Homer City was perfectly appalling. Clear tributaries of the Conemaugh are found in the valley between Chestnut Ridge and Laurel Hill: Tub Mill Run, for in- stance, near New Florence, is very good (trout stream). As has been said, Stony Creek, in Somerset County, is polluted. Of its tributaries, at least one is in good condition: Quemahoning Creek; others have not been investigated, but probably there are more clear streams, chiefly among the headwaters coming down from Laurel Hill and Allegheny Front. (d) The Great Eastern Tributaries of the Allegheny.—There are * This is very deplorable in view of the fact that for several fresh species, described by Professor. Cope, the Kiskiminetas is the type-locality. No topotypes can be secured any more. 106 ORTMANN—THE DESTRUCTION OF [April 23, a number of important tributaries, running about parallel to each other from the east to the west into the Allegheny. These are (from south to north): Crooked Creek, Mahoning Creek,®? Red Bank-Sandy Lick Creek and Clarion River. Crooked Creek is good, indeed, one of the best creeks in the state, yet in the region of its headwaters pollution begins. Near Creekside, Indiana County, new mines have been opened during the last years, and a small tributary discharges here a considerable amount of mine water into Crooked Creek, killing the fauna for several miles. Of course this is bound to become worse in the future. Mahoning Creek is utterly polluted, the pollution beginning in the region of Punxsutawney in Jefferson County, and consisting chiefly of mine water. Yet a tribu- tary, Little Mahoning Creek in northern Indiana County, has clear water, and correspondingly a rich fauna. Red Bank-Sandy Lick Creek also is polluted, chiefly by mine water, which reaches it from the numerous mines existing in its drainage basin. Clarion River possibly is one of the worst streams in the state. In the region of its headwaters, in Elk County, it is not mine water, but the refuse of various establishments, such as wood-pulp mills, tanneries, chem- ical factories (Elk Creek), which renders the water unfit for life, and finally Toby Creek, emptying into it in the southwestern portion, of Elk County, adds its share in the form of mine water. The water of Clarion River, in this region, is black like ink, and retains its peculiar color all the way down to where it empties into the Allegheny (at Foxburg) ; here the deep blackish brown color of the Clarion River water contrasts sharply with the bluish green water of the Allegheny River. (e) French Creek Drainage.—In contrast to most of the streams mentioned so far, French Creek and its tributaries are generally clear and possess a wonderfully rich fauna. In fact, this region is one of the best collecting grounds for all forms of fresh-water life. French Creek is fed by several streams draining some of our glacial lakes—Conneaut Lake in Crawford County, and Conneauttee Lake and Lake Lebeuf in Erie County. Also these have clear water and a rich fauna. (f) The Upper Allegheny.—Above Oil City, Venango County, ® Not to be confounded with Mahoning River in Lawrence County. 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 107 the Allegheny itself is clear, and also forms a fine collecting ground for the zoologist. This is especially true for the fish fauna and the fauna of fresh-water mollusks. This good condition continues up to the New York state line in Warren County. Of the tributaries, Oil Creek is badly polluted at Oil City, where it falls into the Alle- gheny, but it is pure at its headwaters. The intermediate parts have not been studied by the writer, so that he cannot name the exact spot where the pollution begins. It is due chiefly to oil refineries. Tionesta Creek, in Forest County, is polluted by chemical refuse, at least where it enters the Allegheny; the upper parts have not been investigated. Brokenstraw Creek, in Warren County, is ina fair con- dition, but it belongs to the class of streams which improve during their course: its headwaters are polluted by refuse from tanneries at Cory in Erie County. Connewango Creek, in Warren County, which brings the outflow of Chautauqua Lake in New York, is good. The headwaters of the Allegheny in McKean and Potter Counties are generally good, but there are some tributaries which are polluted, for instance, Potato Creek, in McKean County (polluted by chemical factories). Where Potato Creek falls into the Allegheny it is in a very bad condition, but its size is not sufficient to influence the Allegheny noticeably. 6. The Lake Erie Drainage. Of course Lake Erie itself is clear, and contains a rich fauna.?° In our state there are rather insignificant streams draining into the lake, and they all have pure water, and, as far as they have been examined, a well-preserved fauna. The largest is Conneaut Creek, in Crawford and Erie Counties, which has been investigated at sev- eral places by the writer, and found to be in good condition. The only other streams known to the writer are Elk and Walnut Creeks, in Erie County, which are also good. 7. The Potomac and Susquehanna Drainages. Only the headwaters of these streams or their tributaries are situated in western Pennsylvania, and the investigations of the writer are not very extensive in this region. * Our knowledge of the Lake Erie fauna is deplorably poor, chiefly so with reference to the Pennsylvania shores. 108 ORTMANN—THE DESTRUCTION OF [April 23, Wills Creek, in southern Bedford County, flowing to the Potomac is clear, but it becomes polluted by mine water farther down, at Mt. Savage Junction in Maryland." Several of the headwaters of the Jumata River, in Blair County, chiefly in the region of Altoona and Tyrone, are polluted by industrial establishments.1? The headwaters of the West Branch of the Susquehanna and Clearfield Creek, in Cambria and Clearfield Counties, are generally polluted by mine water,* but there are some clear tributaries. A rather good one is Cush-Cushion Creek, in Indiana County. The latter fact is very important, for it is the point of the Susquehanna system which is most advanced in a westerly direction, and marks the most western extension of the Atlantic fresh-water fauna in our state, and it may be said here that Cush-Cushion Creek indeed contains a pure At- lantic fauna, which is in sharp contrast to the western fauna present in some of the tributaries of the Allegheny in the same (Indiana) county, Little Mahoning, Crooked, Two Lick and Yellow Creeks. CONCLUSIONS. The sketch given above of the present condition of our streams and their fauna is sufficient to give an idea of the tremendous damage done in recent times to our fresh-water fauna. Considering the fact that most of this destruction has been accomplished during the last twenty years; that it is going on continually, and that every year new stretches of the rivers, new creeks are added to the list of the polluted waters, conditions are indeed alarming. I think a glance upon the map accompanying ,this paper will tell more than any words possibly could. It is not for the writer to suggest remedies, yet two conclusions are forced upon him. The first is, that with regard to the improve- ment of the fish-fauna, which is attempted by the State Fish Commis- See Parker, H. N., Water Supply and Irrigation Paper no. 192, 1907, 210: : The quality of the water was poor already in 1904, see Leighton, M. O., in Water Supply and Irrigation Paper no. 108, 1904, p. 65. * Leighton (ibid., pp. 56 and 57) gives in 1904 a rather favorable report on the quality of the headwaters of the West Branch of the Susquehanna (chiefly with regard to drinking purposes). Apparently this has changed to the worse during the last four years. 1909. ] FRESH-WATER FAUNA IN PENNSYLVANIA. 109 sion by way of restocking our rivers with game and food fishes, this is a useless undertaking in all those streams which are polluted. Any fishes set free in such waters will not live, or will not stay there, if they can. The other suggestion is furnished by the fact, repeatedly mentioned above, that a river, badly polluted at a certain point, improves in its further course, provided no additional pollu- tion in great quantities is reaching it. This is seen first of all in the Ohio itself in Beaver County, and further in the Allegheny in Armstrong County. Additional examples are Slipperyrock Creek, Mahoning River (Lawrence County), Raccoon Creek, Brokenstraw Creek, Cheat River. This improvement of the waters, of course, is partly due to the dilution of the injurious substances by the addition of clear water from tributaries. But it seems as if this is not the only source of the improvement. In the case of the Allegheny in Armstrong County, the main tributaries (Clarion, Red Bank, Ma- honing) themselves are polluted, and the other tributaries are very insignificant in comparison with the size of the Allegheny. This is also seen in the Mahoning River in Lawrence County, which hardly has any tributaries along its course, where the improvement takes place. I think the precipitation of the injurious substances to the bottom plays an important part here. We always have, in polluted streams, some sort of precipitate upon the bottom, most noticeable in streams charged with mine water, where it consists of sulphate of iron,!® and, consequently, the injurious element must be elimi- nated, at least to some degree, from the water. This observation suggests a natural remedy—if we could prevent the water charged with polluting substances from reaching our streams directly, that is to say, if we could arrange it that this water is kept in basins or reservoirs for some time, till it has gone through this natural clearing process, and if we allowed only the overflow of these clearing basins to reach our rivers, that is to say, the most superficial strata, which contain the smallest amount of polluting substances,*® I think this ™See Stabler, Water Supply and Irrigation Paper no. 186, 1906, p. 28. * See Leighton, I. c., p. 24. 7 Of course, the oil from the oil wells floats on the surface, but this floating oil does not do much damage. It is well known that before the discovery of oil in these parts, the Allegheny was famous for the oil floating upon its surface. 110 DESTRUCTION OF FRESH-WATER FAUNA. [April 23, would improve conditions considerably. The presence of dams in our rivers or creeks furnishes, to a certain degree, the conditions required for such clearing basins, and we have observed instances (Mahoning River at Edinburg, Lawrence County), where such a dam actually improves the river to a considerable degree. This is also the case, although not so strikingly, with dam No. 6 in the Ohio River. But the trouble is these dams improve the water after much damage has been done already, and are injurious in other respects (see above). This much, however, should be clear—unless we improve the quality of the water of our rivers, it is impossible to bring back the original condition of their fauna, and attempts to restore our nat- ural resources with regard to the fish fauna, by restocking our pol- luted streams with fish, will be labor and money thrown away. CARNEGIE MusEUM, PITTSBURGH, Pa. PROCEEDINGS AM. PHILOS. Soc. VoL. XLVIII. No. 191 PLaTe VI WESTERN PENNSYLVANIA a= watersin good condition ~—~—~—_ waters unfit for life Scales }—*—+—_5—_ 5 4s Miles Ose: Leet —. eee showing: CLEARFIELD CD Sd 2 ick eve Blactelis “s cA ye %| L WESTMORELAND / BEDFORD | GREENE Fish ha Nae 6 Rai, ON CERTAIN GENERALIZATIONS OF THE PROBLEM OPFTHREB? SODIES. By EDGAR ODELL LOVETT, Tue Rice Institute, Houston, TEXAS. (Read April 23, 1909.) The object of the following note is fourfold: first, to determine all the problems of three bodies in which the bodies describe conic sections, under central conservative forces, whatever be the initial conditions of the motion; second, to specialize the preceding solu- tions, so as to single out those in which the force-function contains only the masses of the bodies and their mutual distances; third, to generalize the latter group to the case in which the orbits are the most arbitrary possible; fourth to generalize the last to the case in which the functions defining the orbits appear in the poten- tial function. 1. If three given particles (7,,0,;7%,), (12923 M2), (1, 933 Ms) describe, under central censervative forces, three given coplanar curves whose equations in polar codrdinates referred to the center of gravity of the system are (1) fitte 6, )=0, fale, 6,)—=0, Tel tes 6; )==0, the forces are derived from a potential function which may be written in the form* om rete *Onemploying the usual substitutions the form given follows immediately from Oppenheim’s solution in rectangular coordinates. See his memoir in the third volume of the Publications of the von Kuffner Observatory. tet PROC, AMER. PHIL. SOC., XLVIII. 191 H, PRINTED JULY 6, 1909. 112 LOVETT—PROBLEM OF THREE BODIES. [April 23, where c is the constant in the integral of areas, that is, 3 0, (3) == DUE E. 4=1 In case the orbits are described independently of the initial condi- tions, Oppenheim has remarked that it must be possible to throw the function P into the form (4) P=P,+h, where h is a constant independent of the parameters which enter P,; if such a decomposition of P is impossible, the motion takes place only for special values of the initial constants. When the orbits are conic sections the equations (1) become (5) fi(ri, 0: )=77i (Ai cos? 6; + 2H; sin 0; cos 6; +B; sin? 6;)+ 2ri (Gs cos 6; + F,; sin 6; )— C; =O, (i Is 2 3.) If the corresponding functions Che Wilop ener. By) Gn web, are constructed, and substituted in the form (2) the latter becomes 3 > m,{(H? = A Br? + 2 [(Z,F, va B,G;) oo 0; i=1 +(4,C,—4,F) sin 04-774 G?+(4,+ 8) Ci} ‘ 3 2 ’ > .[(G, cos 0, + F;sin 6,)r,— C] Gail (6) Om this is the most general form of potential function giving rise to conic section trajectories in the problem of three bodies under central conservative forces. 2. From the relations (7) mimypig? =i (mm + m;)r? + mm + m;) ri? — men, ijk == 122, 231, aoe where pi; is the distance between the bodies (7i, 6:3; mi) and (rj, 0;; m;), it follows that if Q is to be a function of the masses and mutual distances alone we must have (8) Po —=1G, == 0; (== 2a 1909.] LOVETT—PROBLEM OF THREE BODIES. 113 If in addition we have H? — AB, = H? — A,B, = Hj — A,B, = some constant, (9) ee abs De ne ls the function Q may be written | mA, + BC, (10) Q= bmg} +e > s y= O+h. mC} Finally, no noting that the equations (7) lead to the relation 3 3 2 2 2 2 (11) 3 m,) ye MS; = M,N pio + MINP,, + MMP, , t=1 i—) we have Q, in the well-known form (12) Q= 2 2 2 (172,11 ,Pio + ,)1Po,° + 2,1,P,, ), Mt. 4 i=1 which is thus made to appear as the unique case of conic section orbits for all initial conditions under forces varying as the masses and a function of the mutual distances. It may be observed here parenthetically that if a similar study be made for the cubic a first condition will be found to demand that the orbits be defined by equations of the form (13) avi? + 3014.7; — 3a:419.? — Diy —C,=0, (1=1, 2,3); the remaining analysis of the problem offers no difficulty. 3. Writing af, af (14) ae aL the function (2) becomes 9 EE mete) /|Eecal" 114 LOVETT—PROBLEM OF THREE BODIES. [April 23, considering the case in which Dm, ( U2 + =) > m(7r;) (16) Se we find immediately that $; (17) iar a and on subjecting these values of u; and v; to the condition of in- tegrability we have the following relations (18) ri? — i? = Some constant, say Ay7, (1=—1, 2,3), connecting the functions ¢; and y;. The construction of the func- tions defined by the equations (17) and (18) is effected directly by a simple integration which yields the result that under forces derived from the potential function ty ete (ee a three arbitrary masses m; describe the respective orbits A 7. : (20) [eee = +20. + pf, C=)i eta) where the function y; is absolutely arbitrary, and the quantities Aj, pi are any two constants. In virtue of the relations (7) the function R contains only the masses and mutual distances of the bodies, further, on writing the function y;? in the form (21) wi? = air? + oi(7s), where w; is an arbitrary function and a; any constant, it is evident that R can be written in the form (4); whence it follows that the three bodies under forces derived from (19) describe orbits of the form (20) whatever be the initial conditions of the motion of the system. 1909.] LOVETT—PROBLEM OF THREE BODIES. 115 4. In order to generalize certain of the preceding results further, let us write the equations of the orbits thus (22) oi =filr%, Vi )— Ci =0, (11, 2, 3) and the potential function as follows: t=1 2 3 3 2 (3) P=S mor + 0d/ | Dmtea. + x00], the axes being rectangular about the center of gravity of the system as origin. Let us consider now the case in which we have (2 ) fe 35 qi> = pi (+4, Vis Fi 5 Tas (24 Vipi + Vidi = Wil Li, Vin 245 74) 5 from these it at once follows that i — Ie ea ez) a —— Vii EVi Vri72di — Wi?, (25) 17d ai He ViV 17h — We. The condition of integrability applied to (25) gives r?{2o(1 ae) hates +I:Pi, +739, + VP, } = 2h i(rivi,. TIM ae.) = 2(r Wi, Iii, VP —Vi =O, v= Ein? 3) an equation whose integration determines ¢; when yj; is given, and conversely. (@——1,72)3)) (26) (a) In case the functions ¢; and y; contain only r; the equation (26) becomes : @ ia EN a (27) PE Ai ame ari that is to say, it takes the form (18). Accordingly the equations (25) assume the simpler forms (28) 17pi His HAM, 17 Ci— Vai FAM, whence, by integration, the orbits (20) reappear. (b) Let ¢; be a function only of 7; and y; a function of nj(2:, 116 LOVETT—PROBLEM OF THREE BODIES. [April 23, where ; is an arbitrary constant ; then the condition (26) becomes a (29) 7; 2u TP; — a Vi bi) | =a (2 = I, 2, 3), from which we conclude that (30) b= aT, a; being any constant. The expressions (25) in this case assume the form rp as 24, 2n;—1) 22 ( ) rip, = NXE, IV ar ae ie 31 2 2 Pon) ly Ale TG NW) See Ay Gar n: The determination of the form of 2; from the equations (31) can be affected perhaps most simply in the following manner: That yi is a function only of 1,2; amounts to saying that (32) a= 207%); substituting the partial derivatives of this function in one or the other of the expressions (31) we obtain the following equation: 2 (33) ae Vase my eae = n, “ f, Heal ( er 2) a whence we have the ordinary differential equation G34) f= =p (ub fb VON + 1a}, Bas. The integration of the latter equation may be facilitated by the substitution (35) 2u; = mi log(é? + 1), under which (34) takes the form df, (36) a S25 —— V ate — 2 2f2, n,Ne" — 1 Putting now (37) jilae —= sin, 1909.] LOVETT—PROBLEM OF THREE BODIES. 117 the equation (36) becomes au. I (38) Gin fae Ver —1 whence 20; (39) u; =n, tan— {er Sel e.s that is (40) f= (EF + 1)? sin (w, tan £, + 8); or finally the equations of the orbits become (41) ri sin (20; + B,) = 1; the corresponding form of the force-function may be written down without difficulty. If we note that for three equal masses the relations (7) squared give (42) pit=4(rit tri*)+ rt, ik = 123, 231, 312, we see that the solution (41) for 1= 3 is also a solution of the problem of three equal masses under forces varying as the masses and the cube of the distance. (c) Let ¢; contain both 2; and r;, while yi is a function only of nisi; the condition (26) becomes (43) 2(1 — 2,)>;, + NE Di, a ri, = oy (2 = 1,72, 3). whence it appears that ¢; must have one of the forms 2(my—1) ri 2(n;—1) a : i m4 A (44) z, ™ ©, ( : ), ip Wy ( : ) i a in case m; is unity an arbitrary additive constant may be appended to each of these forms. Since ®; and ; are arbitrary functions we have here an infinitude of problems. Considering the second of the forms (32) a little further, the equations (25) become in this case 2 os . 2n; ey ns Wh Ve Pp hho = J), Nr A (25) Mees, a (45) Pee = | Qn; & acai V9; = NIE, FEN" v,( 2) aes t 7 V 118 LOVETT—PROBLEM OF THREE BODIES. [April 23, and if in particular the symbol © indicates the square we have Ti" Ds =e Meas =o vViVI— ni”), (46) a Aaa 1i7qQi = 21 (Mis SH TiV I — 1:7) 5 from which we conclude that the orbits are represented by the equa- tions (47) y Sigs Oil I—n2+ Bi = ¥,, (F— A aaa (d) The case in which each of the functions ¢; and y; contains both variables 7; and 2; leads to a multitude of problems in which these functions are subject to the single conditions (QS) heGAl — rich 7G. WPe 2 VW nO! (e) lf = ys nj y: sap ft ape ( ot zs o(2)}, (49) ?; i i Le a a v= (1-4, — 1) 3, where a; an arbitrary constant, w; an arbitrary function, the inte- gration follows a course parallel to that pursued under (0) above, and leads to complicated transcendental equations for the determina- tion of the corresponding orbits. VIENNA, February 25, 1900. Pie we AS HiStORY) OF THE SEARTE As INFERRED FROM THE MODE OF FORMATION OF THE SOLAR SYSTEM. BY: hee See (Read April 23, 1909.) In No. 4308 of the Astronomische Nachrichten (February, 1909) it is proved that the mode of formation of the solar system has been very different from that heretofore imagined by astronomers. It will, therefore, be of decided interest to physicists and geologists, as well as to astronomers and mathematicians, to consider the bearing of this new work upon the past history of the earth. If we could certainly recognize the general process by which the solar system was formed, it would of course follow that the earth, as one of the inner planets of that system, originated in the same way, and much new light might be thrown upon the problems of the physics of the globe. The investigation outlined in the Astronomische Nachrichten, No. 4308, was undertaken for astronomical purposes only, and was therefore in no way biased by other considerations. And since the new method is accurate and conclusive, so as to demonstrate with all rigor the actual processes involved in the formation of our sys- tem, it becomes peculiarly valuable in throwing light upon the past history of the earth. In fact this new theory gives the only accurate and reliable data that we have on the subject, and it is difficult to see where other data of equal trustworthiness could be obtained. We shall therefore first summarize the process by which the solar system was formed, as shown by the researches in astronomy, and then apply this general theory to the past history of our particular planet. Though Laplace was the greatest master of celestial mechanics since Newton, and formulated the nebular hypothesis as the culmi- nation of his researches on the dynamics of our system, yet it was. mg 120 SEE—THE PAST HISTORY OF THE EARTH. [April 23, TABLE SHOWING THE APPLICATION OF BABINET’S CRITERION TO THE PLANETS AND SATELLITES WHEN THE SUN AND PLANETS ARE EXPANDED TO FILL THE ORBITS OF THE Bopiges Revotvinc Asout THEM. Solar System. Ro Po R, Planet. The Sun’s Observed Observed Period of ate ie Rouen Time of Rotation. Planet. Criterion, Mercury 25.3 days = 0.069267 yrs. 0.24085 yrs. 479 yrs. Venus 0.61237 ‘ 1673 <° The earth 1.00000 ‘‘ BLg2ii6° Mars 1.88085 <é 7424 ‘¢ Ceres 4.60345 ‘‘ 24487 ‘ Jupiter 11.86 “ 86560 ‘§ Saturn 29.46 Ke 290962 ‘< Uranus 84.02 Os 1176765 <‘ Neptune 164.78 “e 2888533 << Sub-systems. Ro Po : Rasta Planet. Satellite. ; Adopted Revron of Obscved Fesioe of felon Calculated by) : : D Babinet’s Criterion. The earth | The moon I day 27.32166 days 3632.45 days Mars Phobos 24",62297 7.6542 hours 190.62 hours Deimos 30:2052))65 TEQ3" 52 yee Jupiter V g".928 EI.9503)) 66 64.456 hours I 1.7698605 days 14.60 days II 3.5540942 « 35-900“ Ill 7.1663872 ‘ 93.933 ‘ IV 16.7535524 ‘S 290: 030 co VI 250.618 “< | 10768.8 ac VII |265.0 $c) TTOO2"4| GG Vill 930.73 «* | 61997.1 ae Saturn Inner edge of ring 10".641 0.236 ‘f 0.6228 days Outer edge of ring 0.6456 Ss 25250 Mimas 0.94242 es A 2002) ee Enceladus 1.37022 ce TROOL5 ieee Tethys 1.887796 ‘<< TOLS22) SE Dione 257320913) 6s fay fig) tae ye Rhea 4x5 5OO tice Ba-620— <8 Titan 15.945417 ‘°° TSOL05) es Hyperion 21027739016 273.06 a Japetus 793329375. <5 1580.1 JG Phoebe 546.5 20712 oe Uranus Ariel 105, 1112 2520303) <* sepypyd © GC (Cf. A. N., 3992) Umbriel 4.144181 << 65-435 ae Titania 8.705897 ‘< 176.05 Gc Oberon 13.463269 ‘ 314.83 OC Neptune | Satellite 125.84817 5.87690 ce 141.8 u (Cf. A. N., 3992) 1909. ] SEE—THE PAST HISTORY OF THE EARTH. 1 reserved for Babinet of Paris to point out? a rigorous mechanical law which enables the mathematician to test the nebular hypothesis. Nevertheless, Laplace himself constantly uses the same principle, in the law of the conservation of areas, though he does not apply it to the development of our system. The principle involved is that of the constancy of the moment of momentum of axial rotation. Ac- cording to this law, we have C= miro = od mr =o mr", (1) where + is the radius of the rotating globe, w the angular velocity of rotation, and C a constant; while 7’ and o’ are the corresponding quantities at some other epoch. Thus at any two epochs, however much the freely rotating globe may have changed by contraction or expansion, we always have On —onee (2) By taking accurate values of the radii and rotation-periods of the sun and planets as now observed, we may calculate the corre- sponding rotation-periods when the globes are imagined expanded to fill the orbits of the planets and satellites. The accompanying table gives the most important data for the solar system.” It will be found from this table that the sun would have rotated with extreme slowness if it had been expanded to the orbits of the several planets, and the planets also would have rotated very slowly if they had been expanded to fill the orbits of their satellites. The difference between the observed periods of revolution and the calculated periods of rotation is so great that we readily see that the planets could never have been detached from the sun, and the satel- lites could never have been detached from the planets, by accelera- tion of rotation as imagined by Laplace. It is evident, therefore, that all of these bodies have been captured or added from without, and have had their orbits reduced in size and rounded up under the secular action of the nebular resisting medium formerly pervading the planetary system. Ever since the time of Laplace it has been believed that our *Comptes Rendus, Tome 52, p. 481, March 18, 186r. * Cf. Astron. Nachr., no. 4308. 122 SEE—THE PAST HISTORY OF THE EARTH. [April 23, system was formed from a nebula, and to-day we know that this nebula was of the spiral type, due to the automatic coiling up under mutual gravitation of two or more streams of cosmical dust. Wher- ever stich streams meet, or pass near one another, there is developed a cosmical vortex, with rotation about a center, and a definite mo- ment of momentum about an axis. This is due to the fact that the impact is never central, but always unsymmetrical, and thus gives rise to a rotation. The two or more streams which meet continue to wind up, under the effects of mutual gravitation, and thus we have the different observed types of spiral nebulz. The nebula continues to rotate and the coils are drawn closer and closer together, and the whole mass slowly ‘settles towards its center. The planets, which are formed by the agglomeration of cosmical dust in the convolutions of the nebula, revolve constantly in the surrounding nebular medium. As the planetary bodies grow by the gathering in of the cosmical dust in which they revolve their orbits are reduced in size and rounded up under the secular action of the resisting medium. It is shown by this line of inquiry, and especially by the round- ness of Neptune’s orbit, that our system extends much beyond Nep- tune; and that the orbits now observed to have a round form were originally much larger and also much more eccentric than they are now seen to be. It is impossible to determine definitely how much the orbits have been reduced in size, but owing to the almost total obliteration of the eccentricity, it seems certain that they were origi- nally two or three times larger than they are now. Moreover, it is proved that in a resisting medium of given den- sity the secular effect is proportionally greater on a small planet than on a large one. This is owing to the fact that the mass, and therefore the moment of momentum, is proportional to the cube of the planet’s radius, but the surface, and therefore the resistance of the medium, proportional to the square of the radius; so that the changes in the orbit of a small body are greater than in that of a large body in the inverse ratio of the radius, for masses of the same mean density. Accordingly it follows that small planets, such as the asteroids or inner planets were at a former epoch, when revolving in a 1909. ] SEE—THE PAST HISTORY OF THE EARTH. 123 -_ nebula, have a tendency to settle towards the center more rapidly than large planets. In our system the asteroids have been gathered into their present position partly by the effects of resistance, and partly by the disturbing action of Jupiter, which throws them into the stable region within his orbit. When the paths of the asteroids cross his orbit, the motion is shown to be unstable, and therefore such overlapping orbits are temporary and not permanent. It follows, therefore, that the orbit of the earth was originally much larger and much more eccentric than at present. The earth may have begun to form almost as far away as Jupiter’s orbit, or even beyond it. In time the primordial earth was thrown within that orbit, where the asteroids now revolve. Thus the earth re- volved in safety and continued to grow by gathering up more and more cosmical dust. The history of Mars was similar. The major axis of the orbit was decreased by the effects of resistance, and at the same time the eccentricity steadily diminished, till we have the planets as they are to-day. This is as certain as anything can be, and it throws an interesting light on the past history of our earth. While the information thus given us is meager, it is, so far as I know, our only means of fathoming the mystery which has always surrounded the origin of our planet. We may therefore say that in the beginning the earth was a small body like one of the asteroids; it then revolved in a much larger and more eccentric orbit than at present, and was augmented gradually by the sweeping up of cosmical dust in its ceaseless motion around the sun. In general, this process of building up the earth was excessively slow, though at times the motion through streams may have given larger additions of matter; but the full process may have occupied a billion years. Of course, geological history began only after the earth had attained about its present dimensions. And the study of the crust of the globe shows that no large additions to the matter of our planet have been made since geological history began. The sedimentary rocks are not filled with any considerable amount of meteoric matter precipitated from the heavenly spaces. From these considerations it follows that the earth was built up very gradually by accretion; and that this growth took place because our globe was revolving in a resisting medium made up of 124 SEE—THE PAST HISTORY OF THE EARTH. [April 23, fine cosmical dust. In the later periods of the earth’s history, the medium has been so rare that but little matter has been added to our globe; so that not only is the whole history very long, but the latter part longer than the earlier part, as measured by the accretion then going on. In other words, the accretion now taking place is so slow as to give us by calculation, based on the observed rate, an exorbitant age of the earth; while that once going on was so large as to give too short a duration for the genesis of our planet. All estimates on the age of the earth must therefore be subject to a wide margin of uncertainty. But we may feel entirely confident that we have at length recognized the true process by which the earth was formed. There is, however, a modifying cause which should be taken into account, in our final judgment of the process involved. It cannot be assumed that the sun was of its present mass at the start; on the contrary, we must suppose this mass to have steadily in- creased. The result of the augmentation of the sun’s mass would be a decrease in the length of the year. Thus while the resisting medium reduced the major axis and eccentricity of the planetary orbits, the growth of the sun’s mass also shortened the periodic times, without, however, decreasing the mean distance of these masses to any appreciable extent.® In the actual history of our system, these two causes have there- fore conspired together and the results now observed must be ascribed to both causes combined. If we wish to inquire at what rate a change of a given percentage in the sun’s mass would affect the length of the year, we may proceed as follows. By a well known law for circular motion we have M+m=*. (3) If we differentiate this expression, considering M and ¢ alone to be variable, we shall get dM (t?) + (M+ m)atdt—o, or dM 2dt Mtm "ann WHES (4) *Cf. Laplace, “ Mécanique Celeste,’ Liv. X., Chap. VII., § 21. 1909.] SEE—THE PAST HISTORY OF THE EARTH. 125 This simple expression shows that a change of a given percentage in M produces a contrary change half as large int. In other words, if the sun’s mass be increased by one per cent., the length of the year will thereby be decreased by two per cent. Thus in the lapse of ages the augmentation of the sun’s mass may have shortened the periods of the planets very materially; and this would slightly decrease their mean distances, as in the case of the resisting medium. Nevertheless, a gradual change in the sun’s mass would not affect the eccentricity as it does the major axis. Accordingly the small size and round form of the planetary orbits must be explained mainly by the secular effects of the resist- ing medium formerly pervading our system. And as the earth has been formed by accretion, and not at all by detachment from the sun, as supposed by Laplace, it follows that the matter of the globe is essentially of the same character throughout. For we have else- where shown that friction and resistance to motion in the body of our globe would prevent the heavier elements from separating from the lighter ones. So that the old theories which ascribe an iron nucleus to the earth must be given up as unjustifiable and mis- leading. And the increase of density, rigidity, and temperature towards the center is due principally to the pressure of the super- incumbent matter upon the layers confined within. It is this pres- sure which gives the globe its great effective rigidity. If the pres- sure were relieved, the imprisoned matter, which now behaves as solid, would expand as vapor, owing to the high temperature still existing within the globe. U. S. Nava OBSERVATORY, Mare IsLaAnp, CALIFORNIA, April 5, 1900. 126 SEE—THE PAST HISTORY OF THE EARTH. [April 23, ADDENDUM ON THE VIEWS OF EULER, 17409. EULER’S REMARKS ON THE SECULAR EFFECTS OF THE RESISTING MEDIUM UPON THE ORBITAL MOTION OF THE EARTH, AND ON THE ORIGIN OF THE PLANETS AT A GREAT DISTANCE FROM THE SUN. In view of the results briefly indicated in Astronomische Nach- ricten, No. 4308, and of the paramount part played by the resisting medium in shaping the orbits of the planets and satellites, as well as the orbits of the attendant bodies in other cosmical systems observed in the immensity of space, some remarks of the celebrated Leonard Euler are of much interest to contemporary astronomers and mathematicians. These remarks are included in the Philosoph- ical Transactions of the Royal Society for 1749, pp. 141-142, under the title: “ Part of a Letter from Leonard Euler, Professor of Mathematics at Berlin and F.R.S., to the Rev. Mr. Caspar Wetstein, Chaplain to the Prince of Wales, dated, Berlin, June 28, 1749; read November 2, 1749.” And this is followed by a similar extract from a second letter to Wetstein, dated, Berlin, December 20, 1749, read March I, 1750. | The views of Euler here set forth are very remarkable not only for the insight they show into the mechanism of the heavenly motions, but also into the true mode of origin of our solar system. It must be remembered that, in reaching these views on cosmogony, Euler preceded both Kant (1755) and Laplace (1796), and that he was the first mathematician since Newton to consider the secular effects of a resisting medium. His views on the origin of the planets are therefore free from every possible prejudice, and the direct outcome of the continued action of forces which he believed to be operative in the heavenly spaces. Newton seems to have held that the spaces where the planets move are essentially as devoid of matter as a vacuum. This is expressly stated in first paragraph of the General Scholium to the “Principia.” Yet he may have believed that some waste matter is diffused in the celestial spaces, for in the paragraph just before the General Scholium, he says: 1909. ] SEE—THE PAST HISTORY OF THE EARTH. 127 The vapors which arise from the sun, the fixed stars, and the tails of the comets may meet at last with, and fall into, the atmosphere of the planets by their gravity. Cheseaux was the first to express the view that the heavenly spaces are not perfectly transparent, but that light suffers a certain amount of absorption or extinction in passing over great distances. (Cf. L. de Cheseaux, “ Traité de la Cométe qui a paru en 1743 et 1744,” 8°, Lusanne & Geneva, 1744, p. 223.) This account of Cheseaux was written five years before the promulgation of Euler’s views, and it is uncertain to what extent, if at all, Newton and Cheseaux had influenced Euler in reaching the conclusion that the planets suffer resistance in their motion about the sun. The extracts from Euler’s letters are as follows: 1. First Letter: XXII. Monsieur le Monnier writes to me that there is, at Leyden, an Arabick manuscript of Ibn Jounis (if I am not mistaken in the name, for it is not distinctly written in the letter), which contains a history of Astro- nomical observations. M. le Monnier says, that he insisted strongly on publishing a good translation of that book. And as such a work would contribute much to the improvement of Astronomy, I should be glad to see it published. I am very impatient to see such a work which contains obser- vations, that are not so old as those recorded by Ptolemy. For having carefully examined the modern observations of the sun with those of some centuries past, although I have not gone further back than the 15th cen- tury, in which I have found Walther’s observations made at Nuremberg; yet I have observed that the motion of the Sun (or of the Earth) is sensibly accelerated since that time; so that the years are shorter at present than formerly; the reason of which is very natural, for if the earth, in its motion, suffers some little resistance (which cannot be doubted, since the space through which the planets move, is necessarily full of some subtile matter, were it no other than that of light), the effect of this resistance will grad- ually bring the planets nearer and nearer the sun; and as their orbits thereby become less, their periodical times will also be diminished. Thus in time the earth ought to come within the region of Venus, and in fine into that of Mercury, where it would necessarily be burnt. Hence it is manifest that the system of the planets cannot last forever in its (present) state. It also incontestibly follows that this system must have had a beginning; for whoever denies it must grant me, that there was a time, when the earth was at the distance of Saturn and even farther, and consequently that no living creature could subsist there. Nay there must have been a time when the planets were nearer to some fixt stars than to the Sun; and in this case they could never come into the solar system. This then is a proof, purely physical, that the world in its present state, must have had a beginning, and PROC, AMER. PHIL. SOC. XLVIII. 191 I, PRINTED JULY 8, 1909. 128 SEE—THE PAST HISTORY OF THE EARTH. [April 23, must have an end. In order to improve this notion, and to find with exacti- tude how much the years become shorter in each Century; I am in hopes that a great number of older observations will afford me the necessary succours. 2. Second Letter: XXIII. I am still thoroughly convinced of the truth of what I advanced that the orbs of the planets continue to be contracted, and consequently their periodic times grow less. ... The late Dr. Halley has also remarked that the revolutions of the moon are quicker at present than they were in the time of the ancient Chaldeans, who have left us some observations of Eclipses. Euler then discusses the difficulty of finding the number of days since the time of Ptolemy, and thinks the uncertainty may be a day or two, also raises the question whether the length of the day is constant. At present we measure the length of the day by the number of oscilla- tions which a pendulum of given length makes in this space of time; but the ancients were not acquainted with these experiments, whereby we might have been informed, whether a pendulum of the same length made as many vibrations in a day as now. But even though the Ancients had actually made such experiments, we could draw no inferences from them, without sup- posing, that gravity on which the time of an oscillation depends, has always been of the same force; but who will ever be in a condition to prove this invariability in gravity? He finally concludes that both the lengths of the year and day are diminishing, “so that the same number will answer nearly to a year.” The views of Euler here set forth that the earth and other planets were at one time farther from the sun than at present are so remark- able that it is scarcely necessary to do more than bring them to the attention of astronomers. U. S. Navat OBSERVATORY, Mare Istanp, CALIFORNIA, April 24, 1900. Bee... FounpEp IN 1786 By JOHN HYACINTH DE MAGELLAN, oF LoNDON =~ : | 1gio se * THE AMERICAN PHILOSOPHICAL SOCIETY HELD AT PHILADELPHIA, FOR PROMOTING USEFUL KNOWLEDGE ANNOUNCES THAT IN | DECEMBER; IgIo IT WILL AWARD ITS MAGELLANI€ GOLD MEDAL TO THE AUTHOR OF THE BEST DISCOVERY, OR MOST USEFUL INVENTION, RE- LATING TO NAVIGATION, ASTRONOMY, OR NATURAL PHILOSOPHY (MERE NATURAL HISTORY ONLY EXCEPTED) UNDER THE FOLLOWING CONDITIONS : 1.. The candidate shall; on or before Nov ember 1, 1910, deliver free of postage or other charges, his discovery; invention or improvement, addressed to the President of the American Philosophical Society, No. 104 South Fifth Street; Philadelphia, U.S. A., arid shall distinguish his performance by some motto; device, or other signature. 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Subscription—Five Dollars per Volume wy) 1 ui Separate parts are not sold ee Address THE Tee OF THE : pans is) AMERICAN PHILOSOPHICAL SOCIETY No. 104 SouTH FirtH STREET “ve ei Li PHILADELPHIA, U.S. A. PROCEEDINGS - AMERICAN PHILOSOPHICAL SOCIETY - - HELD AT PHILADELPHIA Cet toate nar ae > OF THE FOR PROMOTING USEFUL KNOWLEDGE VoL. XLVIII. May-—Aucusr, 1909. ety 24) OF fhe CONTENTS. 1208 Pe. “Hera a ey ee _ The Evolution of the City of Rome from its Origin to the Gallic Catastrophe. By JESSE BENEDICT CARTER .............0.0.0e00000: 129 The Linear Resistance Between Parallel Conducting Cylinders ina Medium of Uniform Conductivity. By A. E. KENNELLEY...... 142 On an Adjustment for the Plane Grating Similiar to Rowland’s _ Method for the Concave Grating. By Cari Barus.............. 166 The Electron Method of Standardizing the Coronas of Cloudy Con- | densation., aby CART DARUS .... .ipsctav-cacencgesass counnmes cueeeee ae er, _ The Electrometric Measurement of the Voltaic Potential Difference, Between the Two Conductors of a Condenser, Containing a Eiphiy tonized Mediuny. «By Cart Barus. .):.0..08ib ick tenet 189 _ The Absorption Spectra of Various Potassium, Uranyl, Uranous and Neodymium Salts in Solution and the Effect of Temperature on the Absorption Spectra of Certain Colored Salts in Solution. iy Piarey C. Jonrs and WW: STRONG (ucscid Akasa 194 _ Earthquakes: Their Causes and Effects. By Epmunp O1ls Hovey 235 The Evolution and the Outlook of Seismic Geology. By WiLL1am STS EST SITS eg 8 06) 9 Sa Sse py Sete ee arte st ON 259 ‘Seismological Notes. By Harry FIELDING REID.....................-.. 303 Some Burial Customs of the Australian Aborigines. By R. H. SUMEEESIOWS ccs ccc bee o's PRON cess ocxatem ran iia care mene aap ane meee 313 PHILADELPHIA o THE AMERICAN PHILOSOPHICAL SOCIETY ‘ 104 SouTH FirTH STREET 1909 es -American Philosop x General Mccting Sie 21- 23). 1910 The General Meeting of 1910 will be held on ‘Ayal aast to 23rd, beginning at 2 p. m. on Thursday, April 21st. Members desiring to present papers, either for themselves or others, are requested to send to the Secretaries, at as early a date as practicable, and not later than March 19, 1910, the titles of these papers, so that they may be announced on the programme which will be issued immediately thereafter, and which will give in detail the ar1angements for the meeting. Papers in any department of science come within the scope of the Society, which, as its name indicates, embraces the _ whole field of useful knowledge. The Publication Committee, under the rules of the’ Society, will arrange for the immediate publication of the papers presented. I. MINIS HAYS ARTHUR W. GOODSPEED ee JAMES W. HOLLAND a : AMOS P. BROWN Secretaries. = Members who have not as yet sent their photographs to the Society will confer a favor by so doing; cabinet size preferred. It is requested that all correspondence be addressed os To THE SECRETARIES OF THE | AMERICAN PHILOSOPHICAL SOCIETY 104 SouTH FIFTH STREET PHILADELPHIA, U.S. A. PROCEEDINGS OF THE myer ICAN PHILOSOPHIGAL SOCIETY HELD AT PHILADELPHIA FOR PROMOTING USEFUL KNOWLEDGE Wot. XLVITI APprRIL—AuGusT, 1909 No. 192. THE EVOLUTION OF THE CITY OF ROME FROM ITS GCRIGIN LOWE GALLIC. CATASTROPEM: By JESSE BENEDICT CARTER. (Read April 22, 1909.) In a normally constituted man time and space are in permanent codrdination. In the world of historical science such a permanent coordination is sought after, but not yet everywhere obtained. The student of history and the student of topography are too apt to work in ignorance of each other. The history of Rome has usually been written with small regard for that material and physical thing, the city of Rome; while the writer on topography is far too apt to see the buildings and the piazzas of ancient Rome as an empty stage, a place for action, but for an action in which he is not pro- fessionally interested. Yet the transition through which so many of the natural sci- ences have recently gone, the change from being merely descriptive to being biogenetic, ought to serve as a lesson to the topographer. It is not possible to study even the site of ancient Rome without taking into account the vicissitudes of history in which this site has been involved. I would accordingly ask your attention today to an attempt to sketch in its outlines the development of the city of Rome from its earliest beginnings through the Gallic catastrophe. Such a bio- PROC, AMER. PHIL, SOC., XLVIII. 192 J, PRINTED SEPTEMBER 2, I909. 130 CARTER—EVOLUTION OF THE CITY OF ROME. _ [April 22, graphical sketch (for under this treatment the city itself becomes endowed with life and the product is veritably a biography) covers a distinct field in that long series of periods which follow one another in the story of the Eternal City. . Yet this period of the origins has been strangely neglected by modern scholars, at least in so far as attempts at the coordination of material are concerned. ‘The student of ethnography has formed his own opinions regarding the early settlement of this part of Italy, the student of language has drawn his own deductions; the student of religion has discovered certain perfectly definite things regarding the civilization of these primitive peoples; and the stu- dent of topography has made his own discoveries, but has also held his own counsel. Yet the language of communication between these special students has been in the main the old traditional one of Rome’s founding. The greatest difficulty which confronts the student of the origins of Rome is not the absence of statements regarding it, but rather the superabundant presence of such statements. If what was after- wards the great city of Rome had been entirely unknown in its birth, we would have placed it in the category of many other famous individuals, and thought nothing of it. But the presence of such a plenitude of sources has at least two bad results; first it leads to endless and hopeless attempts to reconcile conflicting statements’ ; and second even after our reason has convinced us that these statements are without authority and represent merely the late prod- ucts of artificial legend making, we have great difficulty in casting them to one side, and we unconsciously and instinctively recur to them, so much are they a portion of our intellectual heritage. We may prove that Romulus was not known in Rome until after the Gallic catastrophe? and that we have no reason to suppose the Palatine settlement to be any older that the Capitoline or the *Compare the attempts periodically made to reconstruct the early history of Rome on the basis of the legendary accounts. *See Carter: “The Death of Romulus,’ American Journal of Archeol- ogy, 19090, pp. I9-29; and (more fully) my forthcoming article, s. v. “Romulus,” in Roscher’s “Lexikon der griechischen und romischen Mythologie.” 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. 131 Quirinal,? but out of the ruins of our tradition Romulus, Remus and the wolf arise. Thus it is that we are still presenting the subject according to the scheme and phraseology of Varro, though there is scarcely any other part of Varro’s learning which we ac- cept unhesitatingly. In the first place our study of Roman religion and its coordina- tion with the study of the primitive religions of today have shown us that, down to the dawn of history, the inhabitants of the region of Rome were a semi-barbarous people. Their religion was still involved in animism. They felt themselves surrounded by a count- less host of potentialities, whose names they knew, but of whose nature they were otherwise ignorant, except in so far as that nature externalized itself in definite acts. Their religious organi- zation shows that this primitive people was divided, as its most original division, into curiz or brotherhoods, and that every mem- ber of the community must of necessity belong to one of these curie.® Their religion shows us further that their interests were agricultural.® Further we know that they lived in little communities on the hilltops surrounded by a circular wall or stockade. Such a primi- tive settlement was certainly not a city—an urbs. At best it might be dignified by being called a town, an oppidum.” The geological character of the campagna, the presence of vast *See below, and also “Roma Quadrata and Septimontium,”’ American Journal of Archeology, 1908, p. 181. *See Wissowa: “Religion und Kultus der Roemer,’ p. 20, “ Sammtliche Gottheiten sind sozusagen rein praktisch gedacht als wirksam in_ all denjenigen Dingen, mit denen der Roemer im Gange des gewohnlichen Lebens zu thun hat”; and Carter, ‘“ Religion of Numa,” p. 5 ff. °If we accept the theory that matriarchy existed in Rome before the institution of the patriarchal system, we are virtually driven to consider the Curie as preceding the family. For an excellent discussion of the Curie, cp. Eduard Meyer, ‘ Geschichte des Altertums,” Vol. II., p. 511 ff. °Cp. the table of gods for this early period, as reconstructed by Mommsen, “ Corpus Inscriptionum Latinarum,” Vol. I., Part 1, ed 2, p. 288, or by Wissowa, “ Religion und Kultus, ” p. 18 and cp. p. 20: “es spiegeln sich in ihr (der alten Gotterordnung) die Interessen einer in Ackerbau und Viehzucht . . . lebenden Gemeinde.” “Cp. the investigations of E. Kornemann, “ Polis und Urbs,” in “ Klio Beitrage zur alten Geschichte,” 1905, p. 72 ff. 1382 CARTER—EVOLUTION OF THE CITY OF ROME. [April 22, quantities of running water, and the consequent erosion, produced a large number of tongue-shaped or circular elevations, admirably suited to such settlements. These clusters of houses surrounded by a ring-wall were merely habitations. The people tilled the fields in the valleys below. It is impossible for us to distinguish clearly between these hill-top towns in their early history. They were probably very similar in population and consequently in customs. Judging however by the presence or absence in historic times of old cult centers it would seem that there was no settlement upon the Aventine,® possibly because it was too close to the river. Nor does there seem to be any particular justification for supposing that the Palatine was in any sense the leader in this group of hill towns, by virtue either of its superior age or of its greater influence. The Palatine is singularly free from old cult associations.1° Such associations as seem old are connected with the later legends, for example that of Romulus and Remus, which did not arise until the fourth century, and even in these cases the Capitoline offers a dis- tinct rivalry to the Palatine.** It is easy to understand how at a later day the Palatine might have been elevated into this position of superiority.'* * Cp. the presentation of Richter: “ Topographie der Stadt Rom,” p. 25, 26. ° At least in later times it is known as pagus Aventinensis, CIL., XIV., 2105 (inscription from Lanuvium) ; and the fact that it was later opened to the plebeians for settlement would indicate the absence of any older settlement. The town of Aventum is an unfortunate suggestion of Jordan (‘ Topographie,” I., 1, 182) and never had existence. Cp. Huelsen in Pauly- Wissowa’s “Encyclopedie der classischen Altertumswissenschaft,” s. v Aventinus, Sp. 2283, 23 ff. ” Cacus and the very doubtful Caca, in whom Wissowa (“R. und K.,” p. 24, note 1) is inclined to see a pair of ancient gods, belong really on the Aventine rather than on the Palatine. Huelsen’s statement (Jordan- Huelsen, I. 3, p. 45), “von den Kulten auf dem Palatin cheinen einige in sehr alte Zeit hinauf zu gehen, wie der der Febris, der Fortuna, der Dea Viriplaca, der Luna Noctiluca,’ must be taken merely relatively, as none of the deities mentioned (with the exception of the uncertain Dea Viriplaca) precede the later kingdom. 4 Cp. the rival casa Romuli on the Capitoline; and the Salii Palatini versus the Salii Collini. * Owing to its popularity as a residence during the closing years of the Republic, and the preference of Augustus and his successors. 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. 133 This little group of towns is not as yet however the city of Rome: it is possible that in the course of time it might have become the city of Rome, either by the superior power of one oppidum which would shortly have added the others to its territory, in some- what the way in which the traditional account considers that Rome was actually founded,—the Varronian scheme, which proceeds from the presupposition of the primacy of the Palatine,—or by some sort of reciprocity, resulting in union, of which we see the first traces in the annual joint sacrifices of the Septimontium.** But either one of these ways would have required a very long period of time, and in either case the intellectual development of the people would have been continuous so that the traces of barbarism even in the conservative field of religion would have been much fewer in num- ber. Every indication points to a rapid change and one which affected the towns equally. Such a change could come only from outside, and from a people superior to Rome in culture. When we ask what this people was, the answer comes more clearly every year,—the Etruscans. It seems fairly certain that the Etruscans as we know. them in the history of Italy were a composite people made up of a native Italic stock combined with an invading stock, whose original home was in Asia Minor.* Further it seems probable that the invading stock came by sea across the Mediterranean and landed on the west- ern coast of Italy, and that their advent did not precede the begin- ning of the eighth century.** Allowing them about two centuries “On the Septimontium, compare Varro, L. L. 6, 24: dies Septimontium nominatus ab his septem montibus, in quis sita urbs est, feria non populi sed montanorum modo, ut paganalia qui sunt alicuius pagi; and the interest- ing treatment by Wissowa in the Satura Viadrina-Gesammelte Abhandlungen, p. 230 ff. Cp. also Platner: “ Classical Philology,” I., 1906, p. 60. “The hypothesis of the East, more especially of Asia Minor, as the original home of the Etruscans is at present pretty generally adopted. Their acquaintance with the Babylonian haruspicina and with Greek mythology, the general plan of their houses and the shape of their helmets all indicate an eastern origin. For details see the admirable résumé of the present condition of the Etruscan problem by Korte in Pauly-Wissowa s. v. Etrusker. ® Whether the Etruscans came by land or by sea is still a subject of dis- cussion, though the hypothesis of the sea route seems to be gaining strength at the expense of the other. There seem to be traces of their movement on 134 CARTER—EVOLUTION OF THE CITY OF ROME. [April 22, to accomplish their amalgamation and conquer the region afterwards known as Etruria, they would come into contact with the Roman stock in the plain of Latium about the beginning of the sixth century.*® The Etruscans, therefore, a sea-faring and so a city-loving folk, conquered these hill towns and enclosed them all together with the intervening valleys with one wall. But before building this wall, they drew the plough about the space to be enclosed and thus created the pomerium ritu Etrusco.7 We do not know very much about their wall but we do know about the pomerium, and as the wall was surely inside of it,1* we have a general idea of its position. the islands of the eastern Mediterranean, especially on Lemnos, where an inscription practically Etruscan in character has been found. It is uncertain exactly what we are to call these people before the “ Etruscan” people were brought into being by the amalgamation of this immigrant stock with the Italic stock. It has been suggested with a reasonable degree of probability that they were the Pelasgians. The date at which they entered Italy is a matter of some considerable uncertainty. The date as given above (circa 800) depends upon the validity of the supposition that in the long series of tombs which the cemeteries (especially near Bologna) show, the earlier tombs are not of the Etruscans but only the later ones, the tombe-a-corridoio, and the tombe-a-camera. However several scholars, who are in hearty accord with the eastern origin, and the journey by sea, are not content with so late a date as the eighth century, on the ground that it does not allow sufficient time for the development of the Etruscans in the peninsula of Italy. According to them the coming of the Etruscans should be placed two or three centuries earlier. 1% This date corresponds with the tradition of the later kingdom. Tarquinius Priscus reigned thirty-eight years, Servius Tullius forty-four years, Tarquinius Superbus twenty-five years, a total of one hundred and seven years, which added to B. C. 500, the supposed year of the founding of the Republic, gives B. C. 616, as the beginning of the so-called Later Kingdom. Such an agreement may be of absolutely no value, on the other hand it may have a certain significance if the tradition represents the faint reflection of the period of time when the new influence came. “Not only the Pomerium, but the whole idea of delimitation seems to have come to Rome from Etruria. Much of the terminology of Roman surveying bears the imprint of Etruria. Roman tradition recognized the Etruscan origin of the Pomerium: cp. Varro, L. L. V., 143: oppida condebant in Latio Etrusco ritu multi, id est iunctis bobus, tauro et vacca, interiore aratro circumagebant sulcum. On the whole question of the pomerium and its relation to the city wall, compare American Journal of Archeology, 1908, p. 177. 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. 135 Thus was created what the topographers call “the city of the four regions.”1® It would be preferable to use the old Roman term urbs et capitolium, for this city, the urbs did indeed contain four regions, but apart from the city though inclosed in the same wall was the citadel, the capitoliwm.?° Such an arrangement is in itself an added proof that the Palatine was not the ruling spirit. The Etruscans coming from without were free from prejudice and chose the Capitoline as their citadel simply because it offered su- perior advantages from the fortificatory standpoint. On the Capitoline arose the Etruscan temple of Jupiter, Juno and Minerva. It is strange that the Etruscan character of this cult has not been more readily recognized. Minerva herself is more than half an Etruscan deity, hitherto unknown to Rome,” and the triad, Jupiter-Juno-Minerva, is a favorite among the Etruscans. The temple was built in the Etruscan style by Etruscan workmen and the ornamentation and the very images of the gods came from Etrunia.24 With the coming of the Etruscans begins a tradition which has in part an historical value. This tradition presents us with the figure of Servius Tullius, unquestionably a real person, probably the *“QDie Vierregionenstadt” of the Germans. I do not know of any instances of the term in antiquity. The ancient term seems to have been urbs et capitolium. ” The capitolium had of course a protecting wall of its own. This is clear from the fact that it was capable of being held against the Gauls, even after the Gauls had captured the city proper. The other hill-top oppida which were included in the urbs certainly had walls of their own, but these walls probably ceased to be kept up after the large surrounding wall was built. In the case of the Capitolium however the original wall was pre- served and probably strengthened. *t Minerva has no festival in the old calendar, the so-called calendar of Numa. The Quinquatrus which occurs in that calendar and which is ordi- narily associated with Minerva had originally no connection with her, but belonged entirely to Mars. Minerva’s cult seems to have originated at Falerii and to have spread from there into Etruria and also into Rome. On Minerva, cp. Wissowa in Roscher’s Lexikon, s. v. Minerva, and “ Religion und Kultus,” p. 203; and Carter, “Religion of Numa,” p. 44 ff. “The image of Jupiter came from Etruria; compare Pliny (N. H., XXXV., 157) and Ovid (F., I., 201 ff.); also the quadriga on the roof (Pliny, J. c.). The workmen employed on the temple gave the name to the Vicus Tuscus, where they lived. 136 CARTER—EVOLUTION OF THE CITY OF ROME. [April 22, first historical character in the annals of Rome. But though the character of Servius is a real one, legend has added many of the “events” attributed to him. One of these events concerns our own theme—it is the building of the wall of Rome. The tourist knows this wallas the inner of the two walls, of which traces still remain in Rome, that wall of which there are remnants beside the railway station and on the Via Nazionale.** Up to the present the state- ment that Servius built a wall has been accepted as an historical fact, and though it was recognized that the so-called Servian wall as we know it dates from the end of the fourth century before Christ, scholars have almost always assumed that there was another wall on the same spot and that this previous wall dated from the Servian age.** But, as I hope to be able to show in a moment, this is an altogether gratuitous assumption, and serves simply to hinder the understanding of history. In the first place there is absolutely no proof that Servius Tullius built a wall, other than the name “ Servian wall” which attaches to a structure obviously of the fourth century. The tradition would in any case be worthless, but we have not even a consistent tradition. A study of the growth of the city as at- tributed to the various kings brings no profit, but exhibits merely a mass of contradictions and inconsistencies.** So far as the name * Sections of this wall are constantly being discovered. At the date of writing (April, 1909) a very fine piece has been unearthed near the Spithoever property. “The only exception to this statement known to me is Eduard Meyer (Hermes, XXX., 1895, p. 13): “dass die Servianische Mauer nicht alter ist als das vierte Jahrhundert, ist seit O. Richter’s Nachweis unumstosslich. Sie umschliesst die Grossstadt der Samniterkriege.” That this statement has not been more appreciated is doubtless owing to the fact that it is capable of being understood to apply merely to the date of the actually existing Servian wall, leaving always the possibility that it implies another wall on the same site preceding the “Servian” wall. **In Dionysius of Halicarnassus (4, 13) and in Strabo (p. 234M) Servius Tullius is aid to have added the Esquiline and the Viminal; but Livy (1, 44, cp. the author of de vir. ill. 7) says that he added the Quirinal and the Viminal and increased the Esquiline; whereas the Quirinal is else- where (Dionys. 2, 50, Strabo, p. 234M) supposed to have been included in the city of Romulus and Titus Tatius. On the other hand the so-called Servian wall included the Aventine, hence Servius is supposed to have added this hill to the city, whereas a very strong ancient tradition attributed the 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. itself is concerned, in the minds of the conten. oraries and succes- sors of Cato a wall at that time nearly two hundred years old would be easily associated with the kingdom and might readily be named after the most famous of the kings, Servius Tullius. There are in other words no traces of a real Servian wall either preserved in monumental form for the topographer or found in the historical records. The occasional references found in Livy to the gates of what we know as the “ Servian Wall,” in connection with events which happened at or before the Gallic catastrophe, are most rightly explained as anachronisms, and they offer no difficulty to one who is accustomed to the vagaries of the Roman historians.*° On the contrary, it is on the face of it extremely unlikely that an enlargement of the city limits would have been necessary so soon after the building of the large encircling wall which we at- tribute to the Etruscans. Yet, as a matter of fact, the so-called “Servian Wall” includes a much larger space than the wall of the “ Four-Region City.’’?* It includes on the northeast the high table- land where the Quirinal and the Viminal unite, but still more im- portant it includes the Aventine. It is the inclusion of the Aven- tine which creates the chief difficulties in understanding the history of Rome until after the Gallic catastrophe. Let us try the experi- ment of considering the Aventine as a suburb and of reading our history under such a condition.** The city which the Etruscans founded and in which Servius Tullius lived, and according to our present assumption the only city of Rome until after the Gallic addition to Ancus Martius (Cicero de rep. 2, 18; Dionys. Hal. 3, 43; Strabo, p. 234M; Liv. 1, 33; de vir. ill. 5). The difference of opinion regarding the Caelian is still more marked. On the whole question compare Jordan, “ Topographie,” II., p. 206, 207. ** FE. g., Livy (5, 41) speaks of the Gauls as entering by the Porta Collina, referring doubtless to the gate in the “ Servian” wall, as it existed in his day. * At this point the reader may be inclined to challenge these statements and to ask what we know of the course of the wall of the Four Region City. Of the wall itself we know nothing, but we do know that it lay inside the pomerium, and we know approximately the course of the pomerium, and to what extent it in its turn lay inside the Servian wall. *It may require a certain amount of practice to conduct this experiment successfully, just as it takes practice to eliminate the arch of Severus in reconstructing the Forum of the Republic and early empire. 138 CARTER—EVOLUTION OF THE CITY OF ROME. [April 22, * ‘ catastrophe, was that particular form of the city which the topog- raphers call “the city of four regions” and which was more fa- miliarly known in history as urbs et capitolium. In the first place we note the permanency of the phrase urbs et capitolium”® and we ask whether it is likely that the phrase would have obtained such immortality if the form of the city to which it was applicable had so soon given way to the other form, the so- called Servian city. The permanence of the name seems to argue for the long existence of that particular city from which the name was derived. In the second place the annals of religion offer us in this early period at least this knowledge, namely, the establish- ment of temples to various deities more or less strangers to Rome, in the region outside of the pomerium.*® One of the most important of these deities was Diana. She came into the religious life of the state merely because of her connection with the Latin league, and her temple was not a temple of Rome alone but of the whole league.*t.| This temple was situated on the Aventine,®* and while of course it was outside the pomerium it has always been difficult to understand why Rome made bold to put a league temple inside her city wall, when all the expanse of the Campus Martius was at her disposal. But if as we are now supposing the Aventine also was a suburb, the difficulty disappears. Conversely when the temple of Apollo*? was built, while it must of necessity have been outside the pomerium, it is difficult to see why it should have been placed in the exposed Campius Martius, when there was the possibility of placing it on the Aventine itself outside the pomerium but sup- ® Urbs et capitolium occurs; Czsar de bell. civ. 1, 6, 7; Liv. 3, 18, 0; cp. Liv. 38, 51, 135 Fler. Epit, 2; 6,45; Jord: Rom: 202: * A useful list of these temples and their dates is given in Wissowa’s “Religion und Kultus,” p. 516 ff. It is based largely on E. Aust, de zdibus sacris populi Romani unde a primis liber reipublice temporibus usque ad Augusti imperatoris etatem Rome conditis. Marburg, 1880. “Cp. Carter, “Religion of Numa,” p. 53 ff.; Wissowa, “Religion und Kultus,” p. 198 ff. and in P. W. sub verbo. Diana came into the worship of the league as the goddess of Aricia. “For the question of the exact location of this temple, cp. Jordan- Huelsen, “ Topographie,” I. 3, p. 158 ff. It is found on fragment 3 of the Forma Urbis Rome. °8On the temple of Apollo, cp. Jordan-Huelsen, “ Topographie,” p. 535 ff. 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. 139 posedly protected by the city wall. For the worship of Apollo was purely an affair of the Roman state, and hence could well be inside the wall provided it was outside the pomerium. But again under our present supposition we realize that the Aventine also was a suburb and hence, so far as protection was concerned, it would be a matter of indifference whether the temple was on the Aventine or in the Campus Martius. Turning from the field of religion to that of constitutional de- velopment, it has always been difficult to understand why there should have been only four city tribes, named after the four regions, in case the city so soon extended its borders and took in the Aven- tine. But if the Aventine was added two centuries later it will readily be seen that the force of habit two centuries old caused the number of city tribes to be limited to four even when the city had exceeded the local limits of the four old regions. But when we turn to the question of the increase in Rome’s population and the disposal of it we have our best argument for treating the Aventine as a suburb. The population was increasing rapidly—we see signs of it in the growing number of foreigners both tradespeople and handicraftsmen. By degrees there arose a problem very similar to that of modern Rome, a dearth of houses for the working classes. It was then (456) that a law was passed pro- viding for the plebeians on the Aventine.** Had the Aventine been an internal part of the city it is difficult to see why it would not have been occupied long before. But as an extreme measure the expedient of giving the plebeians land in the suburbs might easily have been adopted. Thus it was that the city began to outgrow its walls, both in the Aventine region and in the Campus Martius. The proof of this outgrowing is given us in the story of the Gallic catastrophe in B. C. 390. For it is only thus that we can understand why the city was no longer capable of defending itself, and why the Gauls cap- tured it without difficulty, the capitolium alone offering a successful resistance. The tradition of the Gallic catastrophe seems to do * On this law, the lex Icilia, cp. Dionys. 10, 31, and Liv. 3, 31, I. 140 CARTER—EVOLUTION OF THE CITY OF ROME. [April 22, violence to the truth in at least two respects; first in underesti- mating the completeness of the Gallic victory; and second with that sublime indifference to contradiction which is so apt to char- acterize tradition, by overestimating the amount of physical damage which the Gauls did to the city. Ata later time it was customary to attribute all the crookedness and lack of plan which characterized the arrangement of the city streets and buildings to the haste with which Rome was rebuilt after it had been destroyed by the Gauls.* But this presupposes that the Gauls wrought an amount of destruc- tion which would partake of an industry quite at variance to what we know of their natural indolence. But quite-aside from the question of destruction the Gallic catastrophe had brought one lesson home 'to the Romans, namely, that their city needed a defence. It is not surprising that in the years following the retreat of the Gauls a new wall was built on a new line so as to include the now populated Aventine. To include the suburb at the south of the Campus Mar- tius was impossible because of engineering difficulties. It is no wonder therefore that a passage in the sixth book of Livy (chapter 32) dealing with the year B. C. 378 speaks of the building of a wall,°° and that another passage (Book VIL, Chapter 20, under the year B. C. 353) speaks of repairs to walls and towers.*7 Rome was beginning her conquest of Italy, and it was necessary that she should herself be protected from hostile forces. This is accordingly the epoch from which dates the so-called Servian Wall. ®Cp. the striking passage in Livy (5, 55): antiquata deinde lege promisce urbs edificari ccepta. Tegula publice prebita est, saxi materiaque cedendz, unde quisque vellet, ius factum predibus acceptis eo anno edificia perfecturos. Festinatio curam exemit vicos dirigendi, dum omisso sui alienique discrimine in vacuo edificant. Ea est causa, ut veteres cloace, primo per publicum ductz, nunc privata passim subeant tecta, formaque urbis sit occupate magis quam divise similis. Cp. also the passage in Tacitus (Annal., 15, 38) where he compares the rebuilding of Rome afier the Gallic - catastrophe with the rebuilding after Nero’s fire. °° Et tantum abesse spes veteris levandi fenoris, ut tributo novum fenus contraheretur in murum a censoribus locatum saxo quadrato faciundum. *“TLegionibusque Romam reductis reliquum anni muris_ turribusque reficiendis consumptum, et edis Apollinis dedicata est. 1909.] CARTER—EVOLUTION OF THE CITY OF ROME. 141 With the capture of the city by the Gauls, Rome enters upon her period of inviolability for almost exactly eight hundred years, and the thought suggests itself irresistibly that the reputation for inviolability thus gained may have been a large factor in pre- serving her inviolate. Even in these early days the city began to be “that so holy spot, the very Rome.” Rome, April 2, 1900. THE LINEAR, RESISTANCE “BETWEEN -PARACE EE CONDUCTING CYLINDERS IN A MEDIUM OF UNIFORM ACONDUCIIV Id Y> By A. E. KENNELLY. (Read April 24 1909.) It is the purpose of this paper to present formulas and tables for the computation of the linear resistances, conductances and capacities between parallel cylindrical conductors, or between a cylindrical conductor and a parallel indefinitely extending conducting plane. As is shown in the appended bibliography, the problem is by no means new; but the mathematical mode of presentation, and the arithmetical tabulation, here offered, are believed to be new. It is hoped that these will be useful to students of electrical engi- neering. Antihyperbolic functions are the natural vehicles of ex- pression adapted to this problem. ; INFINITE CONDUCTING PLANE AND PARALLEL CYLINDER. Linear Resistance.—Let a uniform conducting cylinder of radius Zz! O Z Fic. 1. Section of a conducting cylinder DEF parallel to the indefinitely extending conducting plane Z’OZ. o« cm., shown in section at DEF in Fig. 1, be situated at an axial distance d cm. from a parallel indefinitely extending conducting 142 1909.]} BETWEEN PARALLEL CONDUCTING CYLINDERS. 143 plane Z’OZ. Let the space above the plane unoccupied by the cylinder be filled by an indefinitely extending medium of uniform resistivity p absohm-cm. Then the linear resistance between the plane and the cylinder, 7. e., the resistance of the medium between them, as comprised between a pair of infinite parallel planes per- pendicular to the cylinder and I cm. apart, will be p ce absohm-cms. or C.G.S. magnetic Y_ = — cosh ; , ; , (1) units of resistance in a linear cm. If the conducting surface EDF of the cylinder were unrolled into a flat conducting ribbon 270 cm. in breadth, and the ribbon were supported parallel to the plane Z’OZ at a uniform distance L=co cosh*(d/c) cm. above it, as indicated in Fig. 2, with ver- tical insulating side walls, Ez’ and Fez, to limit the flow of current through the medium to the parallel distribution shown; then the rectangular slab of medium EFzz’ of Fig. 2, would be the equi- valent in electric resistance to the indefinitely extending plane and cylinder system of Fig. 1. In Fig. 2 the depth, or distance across the slab, following the lines of current flow, is L=o cosh(d/c) cm., and the Fic. 2. Equivalent slab section corresponding to infinite plane and parallel cylinder of Fig. 1. surface area of each face of the slab, per linear cm. of its length, is S == 270 cm.?/cm. so that the linear resistance of the whole is z acosh"' (d/o) p mae eee == cosh-! (“) absohm-cm. (2) 270 Since the linear resistance of the plane cylinder system of Fig. 1, or of the slab in Fig. 2, does not depend upon its absolute dimen- sions, the scale of linear dimensions in the diagram may be chosen 144 KENNELLY—THE LINEAR RESISTANCE [April 24, such that o==1 unit, in which case the depth of the slab is coshd units and the breadth of the slab is 27 units. The quantity Y defined by the relation Yi —— cosh (d7 a) numeric (3) may be called the distance factor of the plane-cylinder system; because the distance between electrodes in the equivalent slab of Fig. 2 is Lz Vo cm. When the radius o of the cylinder is very small with respect to the distance d; so that d/o is a large number, we have ad los “2 numeric (4) so that for such cylinders the linear resistance a oe log,“ absohm-cm. (5) The accompanying table gives for successive values of d/o in column I., the corresponding value of Y in column II. Column III. gives the resistance factor Y/2r which, when multiplied by the resistivity p of the medium, gives the linear resistance of the plane- cylinder system considered. ? Thus, if a conducting cylinder with a radius of 2 cm. is sup- ported at an axial distance of 10 cm. from an infinite conducting plane, in a medium of resistivity p==3 X 107° absohm-cms., we have d/o=5. The table gives for this ratio the value of Y as 2.2924, and the value of the resistance factor Y/2r—0.3649; so that the linear resistance of the system will be 3 X 10° X 0.3649 == 1.0947 X 10! absohm-cms.; or 10.947 ohms in a linear cm. Linear Conductance.—The linear conductance, or conductance per linear cm. of the plane-cylinder system will be by (1) 20 20 op picosh “(7c empha uf where y is the uniform conductivity of the medium in abmhos per oO abmhos per cm. (6) 1999] BETWEEN PARALLEL CONDUCTING CYLINDERS. 145 em. The quantity 2x/Y may be called the conductance-factor of the plane-cylinder system. It appears in column V. of the table. Thus, if a conducting cylinder of radius o—0.5 cm. be sup- ported at an axial distance of d=7.5 cm. from an infinite con- ducting plane, in a medium of conductivity y==1071° abmhos per cm., the ratio d/o in column I. is 15, and the conductance factor for this ratio appears in column V. as 1.848. The linear conduct- ance of the system is thus 1.848 X 10°? abmhos per cm. The distance-factor of the system is given in column II. as 3.4001; so that the depth of the equivalent rectangular slab of medium is 1.700 cm., the breadth being 3.142 cm. Linear Electrostatic Capacity—The linear capacity cp of a plane-cylinder system in a dielectric medium of specific inductive capacity x, is numerically the same as the linear conductance of the same system in a medium of conductivity «/4m or resistivity 47/k; so that, in C.G.S. electrostatic units : K I oy = 5 ecse (eye = a7 statfarads per cm. (7) The values of the capacity factor 1/(2Y) appear in column VI. of the table for each selected value of d/o. Thus, a cylinder of radius c==-0.4 cm. is supported at an axial distance of I cm. from an infinite conducting plane in a medium of m— i. ere d/o == 2:5. and 1/(2Y )—-0.3192. The linear capacity of the system is therefore 0.3192 statfarad per cm. In order to convert the linear capacity cp statfarads per cm. into microfarads per km., expressed by cp’, we have: CG = Fs Tiss + microfarads per km. (8) C / P Similarly, to express the linear capacity in microfarads per mile * Gy K I (a = = = — SS eS SOS SOL! (219 microfarads per mile (9) That is, we must divide the capacity-factor of the table by 9 to obtain microfarads per km. or by 5.591 to obtain microfarads per mile. PROC, AMER. PHIL. SOC., XLVIII. 192 K, PRINTED SEPTEMBER 2, I909. 146 KENNELLY—THE LINEAR RESISTANCE [April 24, POTENTIAL DISTRIBUTION. On the Median Line Beneath the Cylinder.—It is well known that the flow of electric current, and the distribution of potential, between the conducting cylinder and the plane, are such as might be produced by removing the conducting cylinder and substituting a conducting polar line at A, parallel to the plane. The point 4 lies on the line OC, and at a distance a from the plane defined by the relation a=o sinh Y —\/d? — o?. cm. (10) The values of the polar ratio a/o are given in the table in column VII. for each of the selected ratios: d/o, up to ¢@/o—50, beyoud which the difference between a/o and d/o is less than 1 part in 5,000. For most practical purposes, it is, therefore, sufficient to regard the polar line as coinciding with the cylinder axis when the distance of that axis from the plane exceeds 50 radii. In the steady state of flow, the potential at any point y, on the line OA (Fig. 3) distant y, cm. from O, will be a P tanh- (7) *\ Jrabvolts™ (am) 7 a where J is the current strength per linear cm. of the system in absamperes, the potential of the plane Z’OZ being taken as numer- ically zero. Similarly, the potential at any other point y, on the median line OY, below A, distant y, em. from O, will be: T u,= TL p tanh7! (2) abvolts (12) Consequently, if the potential of the surface of the cylinder be 1,, and y, be the distance of the lowest point of the cylinder from the plane, the potential of any other point on the line OA between the cylinder and the plane, distant y, cm. from the latter, will be: tanh“! (y,/a@) >" tanh (y,/4) Potentials on the Median Line Above the Cylinder.—In the steady state of flow, the potential at any point y, on the median line OY, and distant y, cm. from O, above the polar point 4, is: abvolts (13) u 1909.] BETWEEN PARALLEL CONDUCTING CYLINDERS. 147 u, = rf coth—! (2) abvolts (14) where / and zw have the same meanings as above, and the potential of the plane Z’OZ is reckoned as zero. Similarly, the potential at any other point y, on the median line OY, distant y, cm. from O, and above the polar point J, is: 4 He rain 2 ee coth (2 ) abvolts (15) Consequently, if the potential of the surface of the cylinder be u,, and y, be the distance of the highest point of the cylinder from the plane, the potential at any other point on the median line, above the cylinder, and distant y, cm. from the plane, will be: coth™ (4,/@) 1s coth! (y,/2@) Potentials at Points Outside the Cylinder and off the Median Line—If the point in the plane Z’YZ at which the potential is required, lies off the median line OY, the potential may be expressed u abvolts (16) either : (a) In terms of rectangular coordinates g and y of the point. (b) In terms of the ratio of radii vectores to the point, from the polar point A, and from its image. (a) Potential in Terms of Rectangular Coodrdinates—Let P, Fig. 3, be the point whose potential is required, and whose rectan- gular coordinates are y and 3, measured respectively along the me- dian line OY, and the line OZ in the infinite conducting plane. Then wu, the potential of P, is: eer tanh (aise) abvolts (17) where /, p and a have the values previously assigned, and the poten- tial of the plane Z’OZ is reckoned as zero. Eliminating Jp/m with the aid of (11), we have: 2 2ay tanh 1 Gens +H =) bO)0 axtanhh =" (yt ka) i= tt abvolts (18) 148 KENNELLY—THE LINEAR RESISTANCE [April 24, u, is the potential of the conducting cylinder, upon the lowest point of which yy, and 2==0. -Whus, taking the point P im hae es: defined by the coordinates y==1 and g=2, and referring the B: Fic. 3. Coordinates of a point at which the potential is required. potential wu of P to u,, the potential of the surface of the cylinder, where y, — 2, 2==0, we have a= 3.4642 and tanh~'(6.9284/17) 13 tanh— (2) 224642) Formula (18) may also be presented in the form: 2a tanh—! palate Canta J + 2 ; : abvolts (19) tanh— (gs so y en (b) Potential in Terms of Radu Vectores.—A line parallel to the axis of the conducting cylinder, drawn through the point B, Fig. 3, on the median line OY and with the distance OB = OA, may “= = 0.3285u,. “w= tu 1909.1] BETWEEN PARALLEL CONDUCTING CYLINDERS. 149 be called the image of the polar line through OA. The point B, thus defined, may be called the image polar point. The points 4 and B, taken together, may be called the polar points of the diagram with respect to the infinite plane and cylinder. Let P be any point in the plane of the diagram (Fig. 3). Then let r’ and r be the lengths of a pair of radii vectores BP, AP, drawn from the polar points B, A, to P respectively. Let these distances r'y be called the polar distances of the point P. Then the ratio m of these polar distances will be: Wig Te numeric (20) This ratio may be called the polar ratio, for purposes of reference. The polar ratio will manifestly be a number greater than unity for all points in the diagram above the infinite conducting plane Z’OZ. It is a well known result that /p be log, m abvolts (21) If a point be selected on the surface of the cylinder, having a poten- tial u, abvolts, and for convenience the lowest point of coordinates y, and g= =o, the polar distances of this point may be denoted by r,’ and r,; while their ratio may be denoted by m,—r,'/r,. Con- sequently Ip ie log, m, abvolts (22) and eliminating J, p and 27 between (21) (22), we have “=u, —*— = 4, —— _ abvolts (23) The potential of the infinite plane is here reckoned as zero. It may be observed that ri atd—c a+d i ee numeric (2 ! ie Fa o ( 4) When the cylinder radius is very small, compared with the axial distance d, d—=a, and 150 KENNELLY—THE LINEAR RESISTANCE [April 24, ai / 2d D oO oe i numeric (25) 1 It follows from the preceding equations that the equipotential surfaces in an infinite plane-cylinder system are all cylinders having their axes situated on the median line. If u, be the potential of the conducting cylinder, and if we denote by Y, the value of the distance factor Y for this cylinder, according to formula (3), or to column II. of the table, then the distance factor Y of any cylindricai equi- potential surface whose potential is « becomes Vows numeric (26) ae, We have for any such cylinder the equations of condition: Y= cosh-"(d/c) — sinhs(a/c )—tanhs.(a/d )—— cote (a) == 2 tanh?(y/a) numeric (27) whence d, the axial distance, or y coordinate, of the cylinder whose potential is u, will be along the median line OY: a a= 7 ~ cm. (27) tanh ( y= ) uy and the radius o of this equipotential cylinder is: a sinh ( VG =) ut, The coordinate y of the lowest point of any such equipotential cylinder will be: Wt — I cm. (28) on— so that tanh! é =) u=U amas abvolts (31) 19099.} BETWEEN PARALLEL CONDUCTING CYLINDERS. 151 an expression for the potential of a point in the medium in terms of its polar ratio m, and the distance y, of the conducting cylinder from the plane. The current density 6 at any point whose polar distances are ry and r’ will be perpendicular to the equipotential cylinder passing through the point and will be equal to a Seen: ; absamperes per cm.’ (312) 3 VE The preceding formulas for potential distribution have been de- veloped with reference to a conducting medium between the infinite plane and cylinder. They are, however, applicable to the case of a dielectric medium, if the electric flux ¢ replace the electric current I, and the dielectric constant x be substituted for y or 1/p. No substitution will be needed in formulas (13), (16), (18), (19) and (23) to (31), inclusive, which apply either to an insulating or to a conducting medium. Two EQUAL AND PARALLEL CONDUCTING CYLINDERS. If, instead of an infinite conducting plane and a parallel conduct- ing cylinder, as in Figs. 1 and 3, we have two indefinitely long par- allel conducting cylinders of equal diameter, as in, Fig. 4, at an interaxial distance CC’ of D cm., then each cylinder may be regarded as forming an independent plane-cylinder system with a fictitious infinite conducting midplane Z’OZ, axially distant d—=D/2 cm. from each. This midplane will be perpendicular to the central line CC’. The double-cylinder system will have two polar lines equi- distant from the system center O, and represented in Fig. 4 by the polar points AA’. The potential of the midplane Z’OZ will be midway between the potentials of the two cylinders; so that if these have equal and opposite potentials, the potential of the midplane will be zero. All of the preceding formulas for plane-cylinder sys- tems may, therefore, be applied, in duplicate, to the double-cylinder system of Fig. 4. Linear Resistance of Double Cylinder Systems.—The linear resistance from either cylinder to the midplane is given in formula 152 KENNELLY—THE LINEAR RESISTANCE [April 24, (1). Consequently, the linear resistance of the double cylinder system of Fig. 4 is Tog = cosh (d/o) = = Y _ absohm-cms. (32) where d=D/z2. The resistance factor of the system is thus Y/n, or double that given in column III. of the table. Thus, if the two cylinders, each of radius o==2 cm. separated ' $ Fic. 4. Two equal and parallel conducting cylinders at interaxial distance of D cm. by an interaxial distance D—8 cm. in a medium of resistivity p==5 X I0' absohm-cms. we have d = 4, and d/o = 2. Y —=cosh2= 1.317, and the linear resistance is Bux Ow peg Sa ete ee 10 x ry) = 31416 ull3 07) — 02 O00. Oo absohm-cms. 1999] BETWEEN PARALLEL CONDUCTING CYLINDERS. 153 Linear Conductance of Double-Cylinder Systems.—The linear conductance of a double cylinder system will be half that of a plane- cylinder system of equal d/o; so that: 7 7 YT Ly = ecosha(aic) ea: abmhos per cm. (33) where y is the conductivity of the medium. The conductance- factor of the double-cylinder system is therefore half of that given in column V. of the table. Linear Electrostatic Capacity of Double-Cylinder Systems.—The linear capacity C,, of a double-cylinder system in a dielectric me- dium of specific capacity x is half the capacity of a plane-cylinder system of equal d/o; so that: K I “oo = 4 cosh! (d/c) a ribs statfarads per loop cm. (34) The linear capacity of each cylinder to the zero-potential plane, or the capacity of the system per cylinder-cm., is given by formula (7). The capacity factors of a double-cylinder system of given d/o are thus half of the values given in column VI. of the table; but the capacity factors of the system per “wire” cm. to zero potential midplane are those recorded in column VI. At interaxial distances large with respect to the cylinder-radii, Y = log, D/c, and we obtain the well known formula K l= Ao) statfarads per cm. (35) The linear capacity of a double-cylinder system expressed in microfarads per km. is ae | : “ Sera: microfarads per cm. (36) Similarly, i “oo £ TO pra s 5-591 5.591 Potential Distribution in Double Cylinder System.—All of the formulas (10) to (31) inclusive referring to the potential distri- bution in a plane-cylinder system apply immediately to a double- I : x iy, microfarads per mile (37) 154 KENNELLY—THE LINEAR RESISTANCE [April 24, cylinder system, after the latter has been analyzed into two asso- ciated plane-cylinder systems. Two UNEQUAL PARALLEL CONDUCTING CYLINDERS. Let two parallel conducting cylinders, with their axes at C,C,, Fig. 5, have unequal radii o, and o, cm., and be separated by an interaxial distance D cm. If the radii were equal, the midplane 2’ would be the plane of zero potential, when the potentials of the cylinders are equal and opposite. The zero-potential plane is, how- Fic. 5. Two unequal parallel conducting cylinders at interaxial distance of D cm. showing the displacement of the zero-potential plane. ever, displaced from the larger towards the smaller cylinder through a distance of 3A/2D cm.; so that: Z 1) aN ie aed) mu 8 _ jou a (38) 2 BaD where {= o,-+., is the sum and Ao, —g, is the difference of the cylinder radii. 1909.] BETWEEN PARALLEL CONDUCTING CYLINDERS. 155 After having established the position of the zero-potential plane Z'OZ, the linear resistance between the cylinders may be found by using formula (1) on each side of the plane and adding the two parts. The linear conductance will then be the reciprocal of this result. The linear capacity of each cylinder to zero-potential plane is to be found by formula (7). The linear capacity per loop cm. may be found from the linear resistance per loop cm. by the formula: Cy statfarads per cm. (39) K a 2 0Ae ew) For example, if two conducting cylinders of radii o,—=2 and o,—I cm., respectively, are separated in air by an interaxial dis- tance of 8 cm., the zero-potential plane is displaced through a dis- fauice.Of is. cmi.,/So that.d,——41ts, d,—— 34% cm: The ratio d,/c, is thus 2.094, and d,/o, is 3.815. The distance factor Y, is 1.37, and Y, is 2.014. The linear capacity of C, is 0.365 statfarads per cm. and of C, 0.248 statfarads per cm., each to zero-potential plane. The linear capacity of the pair by (39) is 0.1477 statfarad per loop cm. The potential distribution in the unequal cylinder system may be obtained as easily as when the cylinders are equal, since the polar points 4,A,, Fig. 4, lie at equal distances from the zero-potential plane Z’OZ. EXCENTRIC CYLINDERS. Let the two parallel very thin conducting cylinders be hollow, with radii o, and o,. Let one be placed excentrically within the other, as shown in Fig. 6, at an interaxial distance D. Let the line C,C, joining their centers be prolonged as indicated in the figure. The infinite zero-potential plane will perpendicularly intersect this line at an inferred distance of 3A/2D cm. from the middle point of eso) that: ZA “A=spts cm. (40) and d, ie eas cm. (41) AT nD 2 156 KENNELLY—THE LINEAR RESISTANCE [April 24, The linear resistance between the cylinders can now be determined by finding the linear resistance of each to the infinite conducting plane by formula (1) and then taking the difference between these linear resistances. Thus, let o, 4 cm., o, =2cem.,D==1 cm. Then 3=6,A=2, and.d,==6,5 cm, 6, == 5.5 cmi The resistance factor for d, by the table is 0.2657. The resistance factor for d, by the table is 0.1697. The resistance factor between d, and d, 0.0960. Fic. 6. Two parallel excentric cylinders, one enclosing the other, and the inferred common zero-potential plane. which multiplied by the resistivity of the medium gives the linear resistance between the cylinders. Through the use of formulas (40) and (41) all cases of excen- tric cylinders may be computed by reduction to the equivalent pair of plane-cylinder systems. GRAPHICAL CONSTRUCTION OF EQUIPOTENTIAL AND STREAM LINES IN A PLANE-CYLINDER SYSTEM. To draw the equipotential and stream lines of a plane-cylinder system, when the polar distance OA or distance a of the polar axis 1909.] BETWEEN PARALLEL CONDUCTING CYLINDERS. 157 from the parallel plane is known, draw zOK, Fig. 7, to represent the plane and on the median line OY, perpendicular to zOK mark | off, to scale, the polar distance a=—OA. Then to locate any equipotential circle of radius o== OL’, mark off with center O, a distance d2==OC=AE’, With center C and the required radius a, describe the equipotential circle FEB. The distance factor Y for this circle will be expressed by Y= 2 tanh7' (2: ) numeric (42) where y, is the distance OF or the y coordinate of the lowest point 4 = oO Fic. 7. Diagram for graphic construction of equipotential and stream lines. on the circle. The potential of the circle with reference to the plane will be 158 KENNELLY—THE LINEAR RESISTANCE [April 24,. “= —YV abvolts (43): To draw a stream line which shall include with the median line OA the nth part of all the linear flux in the system, mark off on OK a distance OG —a cot 2r/n; so that the angle OGA will con- tain 27/n radians. Then with center G and radius GA, describe the circular arc AH, which is the required stream-line. It may be observed that if we draw two coordinate axes ov ow in the vw plane, the function tanh (v-+wVW—1) will correspond on the yz plane to the required loci, magnified by a. The locus. of this function, when v is given successive constant values and qw alone varies, is a series of equipotential circles, while when w is successively assigned constant values and wv alone varies, the loci of successive stream-lines are produced. If w is expressed in terms of w as 7/n and 2v—Y, we have OF =a tanh v=d—o cm. (44) OB=a coth v=dto cm. (45) CE —= a7sinhi aio. cm. (46) OC «a- coth Yad ; cm. (47) also OH=a tan a/n em. (48) OK = 4 \cot -x/n cm. (49) GA = a/sin (27/n) em. (50) OG =a cot 2r/n en. (515) Fig. 8 presents the graphical construction of the function tanh (v + wy —1) carried from the vw plane to the yz plane, over the limits v=—1I to v=-+1 and w=—7/2 to w=+7/2. The points marked on the vw plane have their corresponding points marked on the yz plane. Thus the point p defined by v—r.o, w= 7/2 on the vw plane is represented by the point p defined by y = 1.313, =o, on the yz plane, or tanh (1 + 2/2:W — 1) —1.313. Corresponding areas on the two planes are shaded alike. It fol- lows from the formulas already discussed that linear resistances, con- ductances and capacities are the same between corresponding conduct- ing surfaces in the two diagrams. Thus, the linear resistance of the double-cylinder system pqrs—tuvx is equal to the linear resistance of the rectangular slab system with pqrs as one electrode and tuvx 1909.1 BETWEEN PARALLEL CONDUCTING CYLINDERS. 159 as the other; 1. e., 2/7 absohm-cm. Moreoycr, the linear resist- ance of any curvilinear element, such as between qr on one cylinder, and uv on the other, in the yz system, is equal to the linear resist- ance between the parallel electrodes gr and uv on the rectilinear vw system (10/r absohm-cms. with unit resistivity). 4 4 y € 1 qQ ey Ss : sl YW a PSS U7 sO 8 Lez N S ° #2 ° els ig AIS 3 a2: = 1 1 ince a ie Ele ee Fic. 8. Graphical comparison of (v-+-wV—1) and of tanh (v-+-wV—1). In Fig. 8, a—OA =r; but it is easy to see that the proposi- tion of equal linear resistances, conductances and capacities between corresponding conductors in the double-cylinder and corresponding rectangular slab systems, is independent of the magnification in the diagram. 160 KENNELLY—THE LINEAR RESISTANCE [April 24, l II Ill IV V VI VII Distance Resistance Conductance Capacity J Factor Factor Factor Factor sinh Y Loree TE dia coshat ( =) V jor 1/V an|V 1/(2V) 2_,/(2) —I 1.01 0.1413 0.0225 7.0787 44.47 3.5303 0.1418 1.05 0.3149 0.0501 3.1756 19.95 1.5878 0.3202 ten 0.4435 0.0706 2.2548 14.16 1.1274 0.4582 12 0.6224 0.0991 1.6007 10.005 0.8034 0.6633 1.3 0.7504 0.1204 1.3221 8.307 0.6011 0.8307 1.4 0.8670 0.1380 1.1534 7.246 0.5767 0.97908 1.5 0.9022 0.1531 1.0303 6.531 0.5197 1.1180 1.6 1.0470 0.16066 0.9551 6.002 0.4770 1.2490 a7 1.1232 0.1788 0.8901 5.504 0.4451 1.3748 1.8 1.1929 0.18909 0.8383 5.207 0.4191 1.49607 1.9 1.2569 0.2001 0.7956 4.999 0.3978 1.6156 2.0 1.3170 0.2 0.7503 4.771 0.3797 1.7321 Aa 1.3729 0.2185 0.7284 4.570 0.3642 1.8466 2.2 1.4255 0.2290 0.7015 4.407 0.3508 1.9590 2.3 1.4750 0.2348 0.6780 4.259 0.3390 2.0712 2.4 1.5216 0.2422 0.6572 4.129 0.3286 2.1817 2.5 1.5608 0.2404 0.6383 4.010 0.3192 2.2013 2.6 1.6006 0.2562 0.6214 3.003 0.3107 2.4000 2.7 1.6502 0.2626 0.6059 3.807 0.3030 2.5080 2.8 1.6886 0.2688 0.5922 B72 0.29061 2.6153 2.9 1.7267 0.2748 0.5791 3.630 . 0.2896 2.7221 3.0 1.7627 0.2806 0.5073 3.504 0.2837 2.8284 al 1.7975 0.2801 0.5503 3.495 0.2782 2.90343 Bee 1.8309 0.2014 0.5462 3.432 0.2731 3.0307 3.3 1.8633 0.2966 0.5307 3.372 0.2684 3.1448 3.4 1.8946 0.3015 0.5278 3.317 0.26390 3.2406 3.5 1.9248 0.3003 0.5195 3.204 0.2508 3.3541 3.6 1.9542 0.3110 0.5117 3.215 0.2559 3.4583 au 1.9827 0.3156 0.5044 3.160 0.2522 3.5023 3.8 2.0104 0.3200 0.4974 3.126 0.2487 3.66061 3.9 2.0373 0.3242 0.4909 3.084 0.2454 3.7606 4.0 2.0034 0.3284 0.4846 3.045 0.2423 3.8730 4.1 2.0889 0.3325 0.4787 3.008 0.2304 3.9762 4.2 Bare 7; 0.3364 0.4731 2.073 0.2366 4.0792 4.3 2.1380 0.3402 0.4677 2.939 0.2339 4.1821 4.4 2.1616 0.3440 0.4626 2.907 0.2313 4.2849 4.5 2.1846 0.3477 0.4577 2.876 0.22890 4.3875 4.6 2.2072 0.3513 0.4531 2.847 0.2205 4.4900 4.7 2.22902 0.3548 0.4486 2.8190 0.2243 4.5924 4.8 2.2507 0.3582 0.4443 2.792 0.2221 4.6047 4.9 2.2718 0.3016 0.4402 2.766 0.2201 4.7909 5.0 2.2024 0.3049 0.4362 2.741 0.2181 4.8990 5.1 2.3126 0.3681 0.4324 2.717 0.2162 5.0010 5.2 2.3324 0.3712 0.4287 2.604 0.2144 5.1029 Sie! 425 2.672 5.2048 2.3514 0.2127 1909.] BETWEEN PARALLEL CONDUCTING CYLINDERS. -161 I II III IV VI VII Distance Resistance Conductance Capacity : Factor Factor Factor Factor sinh ¥ do cosh-* (“J Y jan 1/V an|V 1/(2V) 2 (2) 5.4 2.3709 0.3773 0.4218 2.050 0.2109 5.3066 5.5 2.3805 0.3803 | 0.4185 2.030 0.2003 5.4083 5.0 2.4078 0.3832 0.4153 2.610 0.2077 5.5100 5.7 2.4258 0.3801 0.4122 2.590 0.2001 5.0116 5.8 2.4435 0.38890 0.4093 2.571 0.2047 5.7131 5.0 2.4008 0.39017 0.4004 2.553 0.2032 5.8146 6.0 2.4779 0.3044 0.4030 2.530 0.2018 5.9161 6.5 2.5500 0.4073 0.3908 2.455 0.1954 6.4226 7.0 2.6339 0.4192 0.3707 2.380 0.18908 6.9282 Ths 2.7030 0.4303 0.3609 2.324 0.1849 7.4330 8.0 2.7087 0.4407 0.3612 2.270 0.1806 7.0373 8.5 2.8297 0.4503 0.3539 2.22 0.1770 8.4410 9.0 2.8873 0.4596 0.3463 2.170 0.1732 8.9443 9.5 2.9417 0.4682 0.3399 2.136 0.1700 9.4472 10.0 2.9932 0.4704 0.3341 2.009 0.1670 9.9499 II 3.0890 0.4916 0.3237 2.034 0.1619 10.9545 12 3.1763 0.5055 0.3148 1.978 0.1574 11.9583 13 3.2500 0.5183 0.3071 1.930 0.1530 12.9615 14 3.3309 0.5301 0.3002 1.887 0.1501 13.904 15 3.4001 0.5411 0.2041 1.848 0.1471 14.967 16 3.4648 0.5514 0.2886 1.814 0.1443 15.969 17 3.5255 0.5011 0.2837 1.782 0.1418 16.971 18 3.5827 0.5702 0.27901 1.754 0.1306 17.972 19 3.6360 0.5788 0.2750 1.728 0.1375 18.974 20 3.6882 0.5870 0.2712 1.704 0.1350 19.975 2I B97371 0.5948 0.2676 1.681 0.1338 20.976 22 3.7837 0.6022 0.2643 1.661 0.1321 21.977 23 3.8282 0.6093 0.2012 1.641 0.1300 22.978 24 3.8708 0.6161 0.2584 1.623 0.1292 23.9079 25 3.9116 0.6226 0.2557 1.606 0.1278 24.980 26 3.9509 0.6287 0.2531 1.590 0.1266 25.081 27 3.0887 0.6348 0.2507 1.575 0.1254 26.981 28 4.0250 0.6406 0.2485 1.561 0.1243 27.982 29 4.0004 0.6462 0.2463 1.548 0.1232 28.9083 30 4.0041 0.6516 0.2443 1.535 0.1221 29.983 32 4.1590 0.6619 0.2404 1.511 0.1202 31.984 34 4.2193 0.6715 0.2370 1.489 0.1185 33.085 30 4.2705 0.6806 0.2338 1.469 0.1169 35.986 38 4.3300 0.6892 0.2309 1.451 0.1155 37.987 40 4.3819 0.6972 0.2282 1.434 0.1141 390.987 42 4.4307 0.7051 0.2257 1.418 0.1129 41.088 44 4.4772 0.7126 0.2234 1.403 0.1117 43.989 46 4.5217 0.7196 0.2212 1.390 0.1106 45.9890 48 4.5642 0.7264 0.2101 277 0.10906 47.990 50 4.6051 0.732! 0.2172 1.304 0.1086 49.990 PROC. AMER, PHIL. SOC., XLVIII. Ig2 L, PRINTED SEPTEMBER 3, 1909. 162 KENNELLY—THE LINEAR RESISTANCE [April 24, I II Ill IV VI VII Distance Resistance Conductance Capacity ; es Factor Factor Factor Factor sinh } ad ne Mees PEN dio wate (<) Vien 1/V on|V ev) |F Ae) 1 52 4.0443 0.7392 0.2153 Biase 0.1077 52 54 4.6821 0.7452 0.2136 1.342 0.1068 54 50 4.7184 0.7509 0.2119 Tage? 0.1000 56 58 4.7535 0.7505 0.2104 1.322 0.1052 58 60 4.7874 0.7619 0.2088 1.312 0.1044 60 65 4.8676 0.7747 0.2054. 1.291 0.1027 65 70 4.9416 0.7864 0.2024 1.272 0.1012 70 75 5.0100 0.7075 0.1990 1.254 0.0998 75 80 5.0751 0.8077 0.1970 1.238 0.0985 80 85 5.1358 0.8173 0.1947 1.224 0.0974 85 fore) 5.1930 0.8264 0.1926 1.210 0.0963 90 05 5.2470 0.8350 0.1906 1.198 0.0053 905 100 5.2983 0.8433 0.18874 1.1859 0.09437 100 110 5.3030 0.8585 0.18540 1.1648 0.09270 110 120 5.4806 0.8723 0.18246 1.1464 0.09123 120 130 5.5607 0.8852 0.17983 1.1208 0.08992 130 140 5.6348 O. 0.17747 1.1150 0.08874 140 150 5.7038 0.9078 0.17532 1.1010 0.08760 150 160 5.7083 0.9180 0.17330 1.0892 0.08668 160 170 5.8290 0.9278 0.17156 1.0778 0.08578 170 180 5.8861 0.9360 0.16989 1.0074 0.08495 180 190 5.9402 0.0450 0.16834 1.0577 0.08417 190 200 5.9015 0.9536 0.16690 1.0486 0.08345 200 220 6.0868 0.9688 0.16429 1.0322 0.08215 220 240 6.1738 0.9827 0.16197 1.0176 0.08099 240 260 6.2538 0.9054. 0.15090 1.0047 0.07905 260 280 6.3279 1.0071 0.15803 0.9930 0.07902 280 300 6.3900 1.0180 0.15633 0.9822 0.07817 300 320 6.4615 1.0283 0.15476 0.9725 0.07738 320 340 6.5221 1.0381 0.15322 0.9634 0.07666 340 360 6.5703 1.0471 0.151990 0.9550 0.07600 360 380 6.6333 1.0557 0.15075 0.0473 0.07538 380 400 6.6846 1.0639 0.14960 0.9400 0.07480 400 420 6.7334 1.0716 0.14851 0.9332 0.07426 420 440 6.7700 1.0790 0.14749 0.9268 0.07375 440 460 6.8244 1.0862 0.14653 0.9207 0.07327 460 480 6.8660 1.0929 0.14563 0.0151 0.07282 480 500 6.9078 1.0903 0.14476 0.9096 0.07238 500 550 7.0031 1.1146 0.14270 0.8072 0.07140 550 600 7.0901 1.1284 0.14104 0.8862 0.07052 600 650 7.1701 I.I41I 0.13047 0.8764 0.06074 650 700 7.2442 1.1530 0.13804 0.8674 0.06002 700 750 7.3132 1.1640 0.13674 0.8501 0.06837 750 800 7.3778 1.1741 0.13554 0.8518 0.06777 800 850 7.4384 1.1838 0.13444 0.8449 0.06722 850 19099.] BETWEEN PARALLEL CONDUCTING CYLINDERS. 163 I Il III IV VI Vil Distance Resistance Conductance Capacity Factor Factor Factor Factor sinh ¥ dla ones (<) Vier 1/¥ onl V 1/(2V) 2=.|("— [orere) 7.4955 1.1930 0.13341 0.8383 0.06671 [eyere) 950 7.5490 1.2010 0.13246 0.8323 0.00623 950 1000 7.6009 1.2097 0.13156 0.8266 0.00578 1000 1100 7.6962 1.2249 0.12903 0.8165 0.060407 1100 1200 7.7832 1.2387 0.12848 0.8074 0.06424 1200 1300 7.8633 1.2515 0.12717 0.7990 0.06359 1300 1400 7.0374 1.2632 0.12509 0.7916 0.06300 1400 1500 8.0004 1.2742 0.12490 0.7848 0.00245 1500 1600 8.0709 1.2845 0.12390 0.7786 0.06195 1600 1700 8.1315 1.2940 0.122908 0.7728 0.00149 1700 1800 8.1887 1.3032 0.12212 0.7074 0.00100 1800 1900 8.2428 1.3118 0.12132 0.7624 0.00006 1900 2000 8.2041 1.3200 0.12056 0.7575 0.00028 2000 2100 8.3428 1.3278 0.11986 0.7532 0.05993 2100 2200 8.3804 1.3351 0.11920 0.7490 0.05900 2200 2300 8.4338 1.3423 0.11857 0.7451 0.05929 2300 2400 8.4764 1.3490 0.11798 0.7414 0.058909 2400 2500 8.5172 1.3555 0.11741 0.7378 0.05871 2500 2600 8.5504 1.3618 0.11687 0.7344 0.05844 2600 2700 8.5042 1.3678 0.11636 0.7312 0.05818 2700 2800 8.6305 1.3735 0.11587 0.7280 0.05704 2800 2900 8.6656 1.3791 0.11540 0.7251 0.05770 2900 3000 8.6005 1.3845 0.11495 0.7224 0.05748 3000 3100 8.7323 1.3808 0.11452 0.7196 0.05720 3100 3200 8.7641 1.3949 0.11410 0.7170 0.05705 3200 3300 8.7948 1.3990 0.11370 0.7144 0.05085 3300 3400 8.8247 1.4045 0.11332 0.7121 0.05060 3400 3500 8.8537 1.4090 0.11295 0.7008 0.05048 3500 3600 8.8818 1.4135 0.11259 0.7075 0.05630 3600 3700 8.9092 1.4180 0.11224 0.7053 0.05012 3700 3800 8.9359 1.4220 O.IIIQI 0.7032 0.05506 3800 3900 8.9619 1.4262 O.1II58 | 0.7012 0.05579 3900 4000 8.9872 1.4302 0.11127 0.6992 0.05504 4000 4100 9.0118 1.4342 0.11097 0.6073 0.05549 4100 4200 9.0300 1.4381 0.11007 0.6054 0.05534 4200 4300 9.0595 1.4419 0.11038 0.6936 0.055190 4300 4400 9.0825 1.4450 0.IIOIO 0.69018 0.05505 4400 4500 9.1050 1.4401 0.109083 0.6902 0.05492 4500: 4600 9.1270 1.4520 0.10957 0.6885 0.05479 4600 4700 9.1485 1.4500 0.10931 0.6869 0.05466 4700 4800 9.16905 1.4503 0.10906 0.6853 0.05453 4800 4900 Q.IQOI 1.4627 0.10881 0.6838 0.05441 4900 5000 9.2103 1.4659 0.10857 0.6822 0.05429 5000 164 KENNELLY—THE LINEAR RESISTANCE [April 24, NOTATION. a= polar distance or distance of polar axis from parallel plane in a plane-cylinder system, em. Cp = linear capacity of plane-cylinder system, statfarads/cm. Cp’ = linear capacity of plane-cylinder system, microfarads/km. Cp’ = linear capacity of plane-cylinder system, microfarads/mile Coo — linear capacity of double-cylinder system, — statfarads/cm. Coo = linear capacity of double-cylinder system, microfarads/km. Coo = linear capacity of double-cylinder system, microfarads/mile d= distance of cylinder axis from plane, cm. d,d, = distances of cylinder axes from plane in double-cylinder system with unequal cylinders, em. D = 2d or interaxial distance between two cylinders in a double cylinder system, cm. A= o,—o,=— difference in radii of two cylinders, cm. §=current density ata point inthe medium, absamperes/cm.?. p= linear conductance of plane-cylinder system, abmho/cm. Joo = linear conductance of double-cylinder system, abmho/cm. «== specific inductive capacity of medium, y= conductivity of medium, abmho/cm. J = linear current in a system, absamperes/cm. L = length of flux paths in rectangular slab, cm. m==r'/y, polar ratio, or ratio of vector lengths from poles to a point in the medium, numeric 1/n=a fractional part of the total linear flux, limited by a stream line. m= 3.14159:---. y,r’== polar distances or vector lengths from poles to a point. ’y = linear resistance of a plane-cylinder system © absohm/cm. 1) — linear resistance of a double-cylinder system, absohm/cm. ¢ = linear electric flux in a system, statmaxwells/cm. p= resistivity of medium, absohm-cm. S == linear surface area of a conducting slab, em.?/cm += o,+o,—sum of radi of two unequal cylinders, em. o= radius of a cylinder, em. = potential of a cylinder, abvolts or statvolts vw = rectangular coordinates of points in a plane, em. Y — distance factor of a system=—cosh“(d/c), numeric yz == rectangular coordinates of points in a plane, cm. VV. == y-coordinates of points on median line below acylinder, cm. V3V4== y-coordinates of points on median line above acylinder, cm. BIBLIOGRAPHY. Kirchhoff, Dr. S. 1845. Uber den Durchgang eines elektrischen Stromes durch eine Ebene insbesondere durch eine kreisformige. Poggendorf’s Annalen, 1845, Vol. 44, pp. 497-514. 1909.] BETWEEN PARALLEL CONDUCTING CYLINDERS. 165 Smaasen, Dr. W. 1846. Vom dynamischen Gleichgewicht der Electricitat in einer Ebene oder einem Korper. Poggendorf’s Annalen, 1846, Vol. 69, pp. 161-180. Vom dynamischen Gleichgewicht der Elektricitat in einem Korper und in unbegranzten Raum. Ridolfi. 1847. I] Cimento, An V., 1847, May-June. Kirchhoff. 1870. Carl’s Repertorium ftir experim. Physik, Vol. 6, 1870, p. II. Gaugain. +1862. Ann. de Chim. et de Physique, 1862, Ser. 3, Vol. 66, p. 203. Blavier. Resistance Electrique de l’Espace compris entre deux cylindres, quoted by Gaugain in 1862; also Journal de Physique, Vol. 3, p. 115, April, 1874. Smith, W. Robertson. 1869-70. Proc. Edin. Roy. Soc., 1869-70, pp. 79-99. Foster, G. C., and Lodge, O. 1875. On the Flow of Electricity in a uniform plane Conducting Surface. Phil. Mag., 1875, 4th Ser., Vol. 40, pp. 385-400 and 453-471. Heaviside, O. 1880. The Electrostatic Capacity of Suspended Wires. Jour. Soc. Tel. Engrs., 1880, Vol. 9, p. 115. Electrical Papers. London, Vol. I, pp. 42-46. Kennelly, A. E. 1892. The Problem of Eccentric Cylinders. The Electrical World, N. Y., 1892, Vol. 20, pp. 338-339. Houston, E. J., and Kennelly, A. E. 1894. The Inductance and Capacity of Suspended Wires. The Electrical World, 1894, Vol. 24, No. 1, p. 6. Lichtenstein, Leo. 1904. Uber die rechnerische Bestimmung der Capacitaét von Luftleitern und Kabeln. E. T. Z., 1904, p. 126. Benischke. 1907. Die Wissenschaftlichen Grundlagen der Elektrotechnik, Berlin, 1907, p. 44-46. ON AN; ADJUSTMENT (HOR THE PLANE (GkAdinG SIMILAR LO ROWLAND 'S (METHOD SHO THE CONCAVE GRATINGS By CARL BARUS. (Read April 24, 1909.) 1. Apparatus—The remarkable refinement which has been at- tained (notably by Mr. Ives and others) in the construction of celluloid replicas of the plane grating, makes it desirable to con- struct a simple apparatus whereby the spectrum may be shown and the measurement of wave-length made, in a way that does justice to the astonishing performance of the grating. We have, therefore, thought it not superfluous to devise the following inex- pensive contrivance, in which the wave-length is strictly propor- tional to the shift of the carriage at the eye-piece; which for the case of a good 2-meter scale divided into centimeters, admits of a measurement of wave-length to a few Angstrom units and with a millimeter scale should go much further. Observations are throughout made on both sides of the incident rays and from the mean result most of the usual errors should be eliminated by symmetry. In Fig. 1, A and B are two double slides, like a lathe bed, 155 em. long and 11 cm. apart, which happened to be available for optical purposes, in the Laboratory. They were therefore used, although single slides at right angles to each other, similar to Row- land’s, would have been preferable. The carriages C and D, 30 cm. long, kept at a fixed distance apart by the rod akb, are in practice a length of 4-inch gas pipe, swivelled at a and b, 169.4 centimeters apart, and capable of sliding right and left and to and fro, normally to each other. * The investigations in this paper were undertaken throughout in con- junction with my son, Mr. Maxwell Barus; but it seemed advisable that I should undertake the publication in these Proceeprncs myself, with the present acknowledgment. 166 1909.] SIMILAR TO ROWLAND’S METHOD. 167 The swivelling joint which functioned excellently, is made very simply of 4-inch gas pipe T’s and nipples, as shown in Fig. 2. The lower nipple N is screwed tight into the T, but all but tight into the carriage D, so that the rod ab turns in the screw N, kept oiled. Similarly the nipple N” is either screwed tight into the T (in one Fic. 1. Plan of apparatus. AA, BB, slides; C, D, carriages; R, connecting rod. method, revoluble grating), or all but tight (in another method, sta- tionary grating), so that the table ft, which carries the grating g may be fixed while the nipple N” swivels in the T. Any ordinary 168 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, laboratory clamp K and a similar one on the upright ¢ (screwed into the carriage S) secures a small rod k for this purpose. Again a hole may be drilled through the standards at K and c¢ and provided with set screws to fix a horizontal rod k or check. The rod k should be long enough to similarly fix the standard on the slide S carrying the slit and be prolonged further toward the rear to carry the flame or Geissler tube apparatus. The table tt is revoluble on a brass rod fitting within the gas pipe, which has been slotted across so that the conical nut M may hold it firmly. The axis passes through the middle of the grating, which is fastened centrally to the table t# with the usual tripod adjustment. 2. Single Focusing Lens in Front of Grating.—I shall describe three methods in succession, beginning with the first. Here a large lens L, of about 56 cm. focal distance and about 10 cm. in diameter, is placed just in front of the grating, properly screened and throw- ing an image of the slit S upon the cross-hairs of the eye-piece E, the line of sight of which is always parallel to the rod ab, the end b swivelled in the carriage C, as stated (see Fig. 2). An ordinary lens of 5 to 10 cm. focal distance, with an appropriate diaphragm, is adequate and in many ways preferable to stronger eye-pieces. The slit S, carried on its own slide and capable of being clamped to c when necessary, as stated, is additionally provided with a long rod hh lying underneath the carriage, so that the slit S may be put accurately in focus by the observer at C. F is a carriage for the mirror or the flame or other source of light whose spectrum is to be examined; or the source may be adjustable on the rear of the rod by which D and S are locked together. Finally the slide AB is provided with a scale ss and the position of the carriage C read off by aid of the vernier v. A good wooden scale graduated in centimeters happened to be available, the vernier reading to within one millimeter. For more accurate work a brass scale in millimeters with an appropriate vernier should of course be used. Eye-piece E, slit S, flame F, etc., may be raised and lowered by the split tube devise shown as at M and M’ in Fig. 2. 3. Adjustments——The first general test which places slit, grating and its spectra and the two positions of the eye-piece in one plane, 1909.] SIMILAR TO ROWLAND’S METHOD. 169 is preferably made with a narrow beam of sunlght, though lamp- light suffices in the dark. Thereafter let the slit be focused with the eye-piece on the right marking the position of the slit; next - focus the slit for the eye-piece on the left; then place the slit mid- way between these positions and now focus by slowly rotating the grating. The slit will then be found in focus for both positions Fi gua: Fic. 2. Elevation of the grating (g) and the eyepiece (£) standards. and the grating which acts as a concave lens counteracting L will be symmetrical with respect to both positions. Let the grating be thus adjusted when fixed normally to the slide B or parallel to A. Then for the first order of the spectra the wave-length jd sin 6, where d is the grating space and 6 the angle of diffraction. The angle of incidence 7 is zero. Again let the grating, adjusted for symmetry, be free to rotate with the rod ab. Then @ is zero and A=d sin 1. In both cases however if 2% be the distance apart of the car- 170 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, riage C, measured on the scale ss, for the effective length of rod ab —r between axis and axis, Nd ter (0 / 2rer, so that in either case A and + are proportional quantities. The whole spectrum is not however clearly in focus at one time, though the focusing by aid of the rod hh is not difficult. For extreme positions a pulley adjustment, operating on the ends of h Fics. 3, 4, 5. Diagrams. is a convenience, the cords running around the slide AA. In fact if the slit is in focus when the eye-piece is at the center (6=0, 1==0) at a distance a from the grating, then for the fixed grating, Fig. 4, 1909.] SIMILAR TO ROWLAND’S METHOD. uri where a’ is the distance between grating and slit for the diffraction corresponding to .r. Hence the focal distance of the grating re- garded as a concave lens is f’—ar’/x’. For the fixed grating and a given color, it frequently happens that the undeviated ray and the diffracted rays of the same color are simultaneously in focus, though this does not follow from the equation. Again for the rotating grating, Fig. 3, if a’’ is the distance be- tween slit and grating (Ge Eo =O z so that its focal distance is ” Siren cae fl! =a——, x It follows also that a’ X a” =a?. For a=8o cm. and sodium light, the adjustment showed roughly f’—=650 cm., f’— 570, the be- havior being that of weak concave lenses. The same a=8o0 cm. and sodium light showed furthermore a’ 91 and a” 70.3. Finally there is a correction needed for the lateral shift of rays, due to the fact that the grating film is enclosed between two moder- ately thick plates of glass (total thickness t= .99 cm.) of the index of refraction n. This shift thus amounts to tr ( I I ) b a ee = 5 r\Vi—# [PrP Ve—x2[P)a But since this shift is on the rear side of the lens L, its effect on the eye-piece beyond will be (if f is the principal focal distance and b the conjugate focal distance between lens and eye-piece, remem- bering that the shift must be resolved parallel to the scale ss) =( I I \G ) ée= — ——. — — SaaS et TaN Fie Ve ae |? de where the correction e is to be added to 24, and is positive for the rotating grating and negative for the stationary grating. Hence in the mean values of 2+ for stationary and rotating grating the effect of e is eliminated. For a given lens at a fixed distance from the eye-piece (b/f— 1) is constant. 172 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, 4. Data for Single Lens in Front of Grating.—In conclusion we select a few results taken at random from the notes. Grating | Line. Observed 27’. Shift. Corrected 27x. Stationary es | 132.60 | —.26 | 132.34 D, | 113.90 | —.23 | 118.67 F 98.23 —.19 98.04 Hydrogen | 87.87 —.16 87.71 Violet Rotating C 132.10 | 4.26 132.36 D, 118.45 -23 pee 97-90 1g 98.09 H. Violet _ 87.50 | 16 87.66 The real test is to be sought in the coresponding values of 2x for the stationary and rotating cases, and these are very satisfactory, remembering that a centimeter scale on wood and a vernier reading to millimeters only was used for measurement. 5. Single Focusing Lens Behind the Grating.—The lens L’, which should be achromatic, is placed in the standard behind g. The light which passes through the grating is now convergent, whereas it was divergent in §2. Hence the focal points at distances a’, a” lie in front of the grating; but in other respects the conditions are similar but reversed. Apart from signs, for the stationary grating ; 7 a a=a s—> Fs and for the rotating grating v f= 7 The correction for shift loses the factor (b/f-—1) and becomes WZ I I ar, ( Vi- wer ae) As intimated, it is negative for the rotating grating and positive for the stationary grating. It is eliminated in the mean values. 6. Data. Single .Lens Behind the Grating—An example of the results will suffice. Different parts of the spectrum require focusing. Grating. Line. 2x Shift. 2x Stationary: 6-6 ec etests Dz 118.40 + .13 118.53 WROratinoue Abr cent eee es Dz 118.65 — .13 118.52 a oie 1909.] SIMILAR TO ROWLAND’S METHOD. 173 The values of 2%, remembering that a centimeter scale was used, are again surprisingly good. The shift is computed by the above equation. It may be eliminated in the mean of the two methods. The lens L’ may be more easily and firmly fixed than L. 7. Collimator Method.—The objection to the above single-lens methods is the fact that the whole spectrum is not in sharp focus at once. Their advantage is the simplicity of the means employed. If a lens at L’ and at L are used together, the former as a collimator (achromatic) and with a focal distance of about 50 cm., and the latter (focal distance to be large, say 150 cm.) as the objective of a telescope, all the above difficulties disappear and the magnification may be made even excessively large. The whole spectrum is bril- liantly in focus at once and the corrections for the shift of lines due to the plates of the grating vanish. Both methods for stationary and rotating gratings give identical results. The adjustments are easy and certain, for with sunlight (or lamplight in the dark) the image of the slit may be reflected back from the plate of the grating on the plane of the slit itself, while at the same time the transmitted image may be equally sharply adjusted on the focal plane of the eye-piece. It is therefore merely necessary to place the plane of spectra horizontal. Clearly a’ and a” are all infinite. In this method the slide S:and D are clamped at the focal dis- tance apart, so that flame, etc., slit, collimator lens and grating move together. The grating may or may not be revoluble with the lens L on the axis a. 8. Data for the Collimator Method.—The following data chosen at random may be discussed. The results were obtained at different times and under different conditions. The grating nominally con- tained about 15,050 lines per inch. The efficient rod length ab was R=169.4 cm. Hence if 1/C=15,050 X .3937 K 338.8, the wave- length A=C.2* cm. Grating. Lines. 2a! _ 24 RranOHAGH 2524255. 0s050' D: 118.30 118.19 i SLE ae alee Dz 118.08 118.19 RYE AEMMIAENG sor SE aise «22. D: 118.27 118.16 UT ea D: 118.05 118.16 174 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, Rowland’s value of D, is 58.92 & 10°* cm.; the mean of the two values of 2% just stated will give 58.87 & 10° cm. The difference may be due either to the assumed grating space, or to the value of R inserted, neither of which were reliable absolutely to much within ty perreent: Curious enough an apparent shift effect remains in the values of 2x for stationary and rotating grating, as if the collimation were imperfect. The reason for this is not clear, though it must in any case be eliminated in the mean result. Possibly the friction involved in the simultaneous motion of three slides is not negligible and may leave the system under slight strain equivalent to a small lateral shift of the slit. g. Discussion.—The chief discrepancy is the difference of values for 21 in the single lens system (for D,, 118.7 and 118.5 cm., re- -ectively) as compared with a double lens system (for D,, 118.2 i.) amounting to .2 to .4 per cent. For any given method this dif- ference is consistently maintained. It does not, therefore, seem to be mere chance. We have for this reason computed all the data involved for a fixed grating 5 cm. in width, in the two extreme positions, Fig. 5, the ray being normally incident at the left hand and the right hand edge respectively for the method of §6. The meaning of the sym- bols is clear from Fig. 5, S being the virtual source, g the grating, e the diffraction conjugate focus of S for normal incidence, so that b=r is the fixed length of rod carrying grating and eye-piece. It is almost sufficient to assume that all diffracted rays b’ to b” are directed towards e, in which case equations (1) would hold; but this will not bring out the divergence in question. They were therefore not used. Hence the following equations (2) to (5) successively apply where d is the grating space. (1) cot 6’—(b/g+sin6)/cos 6; cot 6” = (b/g — sin 6) /cos 6; (2)) (ab / cos"; a’ =a" —V/ 92 + a: (2) sing —=cint gay (4) —sini’+sin (6+ 6')=A/d; sind=A/d; sini’ + sin (86 — 0”) =d/d; (5) cos?#’/a’ =cos*(0 + 6’) /b’; :cos* 1a” ==cos?( 6 8" )// Be. 1909.] SIMILAR TO ROWLAND’S METHOD. 175 Since 6, g, A, d, b, are given @’ and 6” are found in equation (4), apart from signs. If 6, and 6,” be the distance apart of the projec- tions of the extremities of b’ and b, b and b”, respectively, on the line +, (6) 8,’ =g+ (b—0’' ) sind—D' sin?’ 6,” =g + (b” —b) sin 6 — b” sin 1” If 8,’ and 8,” be the distance apart of the intersections of the prolongation of b’ and b, b and b”, respectively, with the line +x, 6,’ = sin (6+ 0’) (bcos 6/cos (8+ 6’) —b’) (7) 8,’ = sin (6 — @”) (b””— b cos 6/cos (6 — 6”) ) Given b= 169.4 cm., == 20° 22’, about for sodium, g—=5 cm., the following values are obtained: Get 30r, &— 192-7 cm., Di 166.01cm:, C— 1347. 2 — 4 -—— O02 OCI... 7——D—— 10:4 Cinl., tin Os Oli 7 2: A Cis, whence 6, —O2iem | 905 ==. 74 em, These limits are surprisingly wide. If, however, they should be quite wiped out on focusing, for any group of rays and symmetrical observations on the two sides of the apparatus, this would be no source of discrepancy. The effect of focusing the two parts of the grating may, in the first instance, be considered as a prolongation of b’ till it cuts x, together with the corresponding points for the intersection of b” with x. Thus the values 8,’ and 8,” are here in question and they are oo 1-7, Cre, 6,’ — 8,’ = .05 cm. whence D3 105 ei., 6,” —$, = .09 cm. are the conjugate foci for the extreme rays of the grating, respec- tively, beyond the conjugate focus of the middle or normal rays b, on +. Hence the mean of the extreme rays lies at .o7 cm. beyond 176 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, (greater 6) the normal ray and the » found in the first instance is too large as compared with the true value for the normal ray. The datum .o7 cm. may be taken as the excess of 2%, corre- sponding to the excess of angle for a grating one half as wide and observed on both sides (2%), as was actually the case. Finally, since the whole of the grating is not in focus at once a correction less than .o7 cm. for 2% must clearly be in question. This is quite below the difference of several millimeters brought out in §§ 4 and 6. To make this point additionally sure and avoid the assumption of the last paragraph, we will compute the conjugate focus of the central ray (different angles 0) on the b’ focal plane parallel to the grating and to x and on the b” focal plane parallel to +. The com- putation is simpler if the central ray is thus focused, than if the extreme rays are focused on the x plane. The distance apart will be §,/ = g — b’ cos (6+ 6’) (tan (6+ 6’) —tan6), 8,” =g — b” cos (6 — 6”) (tan 6— tan (0 — 6”) ). Inserting the results for 6, 6,', 0,”, b’, b”, g, os == 003) 0.) —— 048 Both the b foci thus correspond to large angles. Their mean, however, may be considered as vanishing on the intermediate -r plane. Thus it is clear that the effect of focusing is without influence on the diffraction angle and much within the limits of observation. It is therefore probable that the residual discrepancy in the three methods is referable to a lateral motion of the slit itself due to insufficient symmetry of the slides 44 and BB in the above adjust- ment. This agrees, moreover, with the residual shift observed in the case of parallel rays in § 8. Brown UNIVERSITY, PROVIDENCE, R. I. SHE ELECTRON METHOD OF STANDARDIZING THE CORONAS, GF “CLOUDY ‘CONDENSATION. By CARL BARUS. (Read April 24, 1909.) 1. Introductory.—Last year I published some preliminary experi- ments! in which the coronal display of the fog chamber was stan- dardized by aid of the value of Thomson’s electron, 10'°e = 3.4 electrostatic units, and of the known velocity of the ions. Later similar experiments were made in terms of the former datum and the decay constants of the ions, though this method is not here to be considered. In the experiments in question a separate leaded condenser was used to determine the ionization, while the nucleation was measured in a cylindrical fog chamber. The data, though nec- essarily rough, owing to the dampness of the room in the summer time, when used for the determination of e by aid of my earlier and independent constants of coronas, nevertheless gave a series of promising values. In the paper cited it was assumed that the whole current due to both positive and negative ions is measured. If, however, the current observed is due to negative ions, while the negative ions only were caught in the fog chamber used, as now appears probable, then the data would be (V denoting the fall of potential per second, dV’ /dr the average field, all referred to volts, N the number of nuclei (negative ions), per cubic centimeter). dV |dr 103 7 |V N 101% 1.0 40 150,000 23 i 50 185,000 we oy) 60 210,000 3.7 12 137 570,000 2 where the velocity of negative ions in a unit field of dry air is taken as v— 1.97 ‘em./sec. * American Journal of Science, XXVI., 1908, p. 87; idem, p. 324. Hida, 178 BARUS—METHOD OF STANDARDIZING [April 24, In the following experiments I have returned to the measure- ments of N in terms of e and the velocities of the ions, modifying the method by using the cylindrical fog chamber both as an electrical condenser for the measurement of current, as well as for the speci- fication of the number of ions in action by aid of the coronas of cloudy condensation. 2. Apparatus.—This consists of a cylinder of glass C, F, about 45 cm. long, 13.4 cm. internal diameter, closed at one end F and pro- vided with a brass cap C, with exhaust F and influx attachments J, in the usual way. There is a layer of water w at the bottom. The glass must be scrupulously clean within; and this is best secured by scouring with a probang of soft rubber under water, until the water adheres as an even film on shaking. The fog chamber is put to earth, as at e. The end F is perforated at h, to receive the aluminum tube ¢?’, closed at t’ and open at t, 40 cm. long and .64 cm. external diameter. Sealed tubelets of radium 17, r,...may be placed at intervals within this tube to ionize the surrounding wet air. The walls being about I cm. thick, 8 and y rays are wholly in question. Neither emanation nor a@ rays escaped the double thickness of aluminum. The tube ##’ is grasped at t by a sheath of hard rubber with an annular air space and fixed in place by a rubber cork. If care be taken to keep the tube in dry air except when in use, there is no conduction leakage of consequence. The end t, moreover, is placed in connection with a Dolezalek electrometer, by aid of a thin wire (not shown) running axially 1909. ] THE CORONAS OF CLOUDY CONDENSATION. 179 within an earthed tin drain pipe and away from the fog chamber, to escape the action of y rays as much as possible. In fact their combined effect does not exceed 2 per cent. and is determined in special measurements. The keys to the electrometer,? etc., were all placed on pillars of hard rubber and actuated by long wooden rods from a distance. So far as possible the electrical wires of the room were surrounded by earthed pipes, but it was not practicable to carry this out com- pletely so that a method of correction appears in the work below. Even when the electric lighting circuit was completely cut out, the electrostatic drift in question remained. The measurements were standardized and the electric system charged by a Carhart-Clarke cell. The radium tubelets used were as follows: No. I, 100 milligrams, strength 10,000 X No. II, t0 milligrams, strength 200,000 X No. III, too milligrams, strength 10,000 No. IV, 100 milligrams, strength 7,000 X No. V, 100 milligrams, strength 20,000 X 3. Electrical Condensers.—To give the fall of potential a suitably small value relatively to the period of the damped drop of the needle, anumber of auxiliary condensers, C’, C”, Fig. 1, are needed. It suffices, however, to measure three capacities, viz., 1. That of the cored fog chamber alone, c; 2. That of a relatively large auxiliary condenser, including the electrometer, the piped wires and the fog chamber, Pelae EY ot 3. That of a standard condenser, C’, for reference. In the present paper C’ was computed by the equation A I 16V TA(d + a’) aa! (eee awed \ We {Get a ae é -(: og (a+ d\n re + a’l\n z; )) where A is the area, d the distance apart and d’ the thickness of *The disposition of condensers C’, C”, cell, etc., earthed at e is sug- gested in Fig. 1. 180 BARUS—METHOD OF STANDARDIZING [April 24, the brass plates. Since A is equal 315 sq. cm., d=.082 cm., 2 107 em, C’ = 305.6(1 + .0784) = 330 cm. This value will suffice for the present purposes, though it needs further correction by comparison with a standard condenser, not now at hand. A special key was provided (Fig. 1) whereby C’ could be switched into the electrometer system or out of it and put to earth. Hence in a series of successive discharges CO Oe acy ite ig (CY + o)y' = (C” + Ci + By a etc., so that for m discharges, if the residual potential is V», V(C" + c= V(C" + C0), from which the total capacity C=C” + C’+c is determinable in terms of C’. The results were: Positive charge, C’ + C’ + c=1,445, 1,443, 1,422, Negative charge, C’ +C +c¢= 1,482, 1,480, Mean C 1,459, the experiments alternating from positive to negative charge, be- cause of the marked drift by the electrometer system when isolated from the cell, as already specified. To measure the small capaci- ties c, of the fog chamber, the same method with ten discharges suffices, if C’” is excluded and C” retained. Thus the data were successively found, “| Charge, 6118) 124 12!2) (ize; — Charge, ¢==10:8- FO ) Tn.) 15.5) Meany G03 iy ee Om aie) eliminating the drift in the final mean, c—11.4. Since the capacity c in terms of the effective internal radius FR, and external radius FR, the length / of the clindrical condenser may be written I OHS Aas REN a I Kes ee a 1909. ] THE CORONAS OF CLOUDY CONDENSATION. 181 the constant c furnishes a mean value for the factor on the left. The ratio of 4.6 c to the measured value of (log R,/R,)/l was .568, a reduction factor used throughout the tables below. 4. Method Pursued—lf C is equal to C’+C’+c we may write the equation for the negative ionization N (positive charge) wal FOLR, d(In V) we fn V) 6007lve at Pr ba where R,, R, and / are the effective radii and length of the con- Gensel lO e— 2 AwU—— tot Clie sec.) and, %—= tay Ci,/SeC., the velocity of the negative and positive ions in the unit field, volt/cm., in case of moist air. The factor (In R,/R,)/l is replaced by 1/2C, as specified in §3, which must here be regarded as an adequate correction for the ends and the imperfect cylindricity of the con- denser fog chamber. Similarly the equation for the positive ionization is (negative charge), Cink jake, ain") ,a(in VY’) ~ 6007lue FT ae i dt and the total ionization is therefore N+ N’. The experiments below will show that even if the fog chamber is put to earth, there is a drift towards negative potential, suffi- ciently steady to be eliminated in the mean results. Hence if V, be the effective negative potential of the wet glass envelope we may write tentatively, Fe nf ai \ a How y where Il’, is intrinsically negative. Similarly, V. d(In V’’) / Ol Z NV (: + =e a Hence if V=V', N+ N’ the total ionization is again SN Mie TahIZ4) dt K K . Direct experiments, however, show that the drift results from 182 BARUS—METHOD OF STANDARDIZING [April 24, the influx of a high permanent positive voltage. Curiously enough even when the lighting circuit is cut out, the effect remained with undiminished intensity. It will appear elsewhere, that in the absence of radium and of initial charge in the condenser, the equation I, CV, where l, for any given ionization is a constant negative quantity, applies very closely within the limits of measurable V, values. Hence in the presence of radium in the core of the cylin- drical fog chamber and a positive charge, I, + 6007 Nev/(In R,/R,) =GV. Thus in this case NV =xd(V —V,)/dt; —N’V'=.'d(—V'—YV,) /dt, and for the same / =V’, to a first approximation N+ N’=d(x« In V+’ In V’)yey-/dt, as before. If the equation for N is integrated and N/«—K, since J, —CV,, V, being intrinsically negative, Vse®(V,—VIK) 40K; Vim PV! + VIR) — VIR" where I’, and I’, are the initial positive and negative potentials. The constant l’, increases with the strength of the ionization but has a fixed value for a given ionization. 5. Data: High Ionization: Currents—The tables® investigated contain the mean potentials ’, the positive and negative logarithmic currents d(log V’)/dt (apart from the constant), the apparent nucleation N positive and N’ negative, computed from these data and additional information as to conduction leakage and effect of y rays. In most of the cases the corresponding logarithmic cur- rents due to y rays outside the fog chamber was carefully measured in the same units, by placing a short hard-rubber rod between the end ¢ of the aluminum tube, Fig. 1, and the wire leading to the electrometer. This cuts out the fog chamber but leaves the whole remaining circuit undisturbed. Similarly the leak value of d(log V')/dt in the absence of radium and due to mere conduction of moist parts is always quite negligible. Thus in the data in * The tables will be removed for brevity, as Figs. 2-4 sufficiently repro- duce the data. 1909. ] THE CORONAS OF CLOUDY CONDENSATION. 183 question for relative logarithmic currents of the order of .035, the y ray effect is .oo10, the conduction leakage smaller than .ooot. The other extreme, 1. e., the value of d(log V)/dt for the freely falling needle is about .1 in the same units. Hence it follows that if the needle falls faster than would be quite trustworthy, the auxiliary capacity selected is too small. The time interval between observations for V was 4 sec., throughout. 6. The Same: Coronas.—These results (to be given in Figs. 2a and 2) contain the data for the maximum ionizations obtainable with the radium tubelets I., II., III., [V., V. at my disposal. The corresponding corona was a large orange-yellow type, representing (in my former reductions) 506,000 nuclei in the exhausted fog chamber. I have supposed this to be equivalent to 653,000 when the fog chamber is at atmospheric pressure, seeing that the coronas are actually displaced during exhaustion; 1. e., at the maximum ionization does not coincide in the position with the largest corona on exhaustion,* but is displaced in the direction of the exhaust currents. The observation would seem to mean that exhaustion is more rapid than the reproduction of ions to restock the region of dilatation. In general this inherent discrepancy of a marked distribution of ionization increasing from end to end of the fog chamber is still outstanding. It is partially allowed for since the observations are made near the middle of the chamber where the average conditions supervene. 7. The Same: Summary.—The data given in Fig. 2a merely show the fall of potential in scale readings, in the successive observations 4 seconds apart, for positive and negative charges. Fig. 2 gives the corresponding positive and negative apparent ionizations. If the two curves between .8 and 1.2 volts be considered, the mean ioniza- tion of each is Apparent positive ions (negative charge), N= 540,000. Apparent negative ions (positive charge), N’ = 1,164,000. Total true ionization, N + N’ == 1,704,000. Total nuclei caught, 650,000. It will be seen that N + N’ is the true total ionization, positive *See papers cited; also Science, XXVIIL., p. 26, 1908. 184 BARUS—METHOD OF STANDARDIZING [April 24, and negative, if 10e==3.4. Only 65/170, or about 38 per cent., of this is actually caught in the given fog chamber on exhaustion, provided the old coronal values are corect. If, however, it is assumed that negative ions only are caught Ose S pd Gor Ga (ess during exhaustion in the fog chamber in question, then the value of the electron would be 10%e = 3.4 K 2.62 K 4 = 4.4 electrostatic units. The irregularities of the curves, Fig. 2, are due in part to fluctua- tions of the drift and in part to errors inevitable in derivations so 1909.] THE CORONAS OF CLOUDY CONDENSATION. 185 close together; but such errors necessarily compensated each other in the mean values. 10. Data: Moderate Ionization: Electrical Currents.——These re- sults were obtained by placing but one radium tubelet, No. IV., in the aluminum tube tt’ of the condenser-fog-chamber. The data were found in the same way as in the above. N=x«d(logV) /dt, as usual. Both positive and negative currents were observed in succession and the true total ionization is N-+ N’ as before. Moreover, the capacity of the condensers were widely varied, 410 to 1,459 cm., without showing serious divergences. 11. The Same: Coronas.—At a fall of pressure of 21 cm. (and somewhat below) or 66/p=.27, the nucleation was stationary and equal to N 113,000 in the exhausted fog chamber. At atmos- pheric pressure therefore 113,000 & 1.37==154,000 nuclei should have been present. The effect of a charge on the core of the con- denser did not appreciably diminish the nucleation. 12. The Same: Summary.—tThe successive observations in scale parts at intervals, 30 seconds apart, are shown in Fig. 3a, the slopes only being of interest. The apparent values of N are given in Fig. 3. All the four series show about the same drift, even though taken many days apart. The condenser effect (excessive rapidity of needle) may be considered eliminated for capacities greater than 500 cm. By averaging the ionizations between V =.6 and V=1.24 in both curves the data found are as follows: Apparent negative ions, N = 278,000. Apparent positive ions, N’ = 107,000. True total ions, N-+N’ = 385,000. Total nuclei, 180,000. Hence about 47 per cent. of all the ions were caught on exhaustion, if the values of u, uv, e, N, inserted, are correct. Supposing that negative ions only are caught in the above fog chamber, the value of the electron would be 10%e = 3.4 K 2.14 K $= 3.6 electrostatic units. 186 BARUS—METHOD OF STANDARDIZING fig. &. 2000 eae 200 cae, fee 7 eae r 40 7. [April 24, 1909. ] THE YCORONAS” OF CLOUDY CONDENSATION. 187 13. Data: Small Ionization: Electric Currents——In the next series of experiments the aluminum tube tt’, Fig. 1, was surrounded by a lead tube with walls .117 cm. thick, leaving the y rays only effective and these much reduced in intensity. The data are suffi- ciently given in the following charts. 14. The Same: Coronas.—The coronas found at a drop of pres- sure similar to the above 6//f = .300, corresponded in my tables to 46,200 nuclei in the exhausted fog chamber. Hence at atmospheric pressure there should have been 64,000. The effect of charging the core was not definite. 15. The Same: Summary.—The drop of potential in scale parts, in successive intervals 30 cm. apart, isegiven in Fig. 4a, showing how much slower the negative charges are lost than the positive charges. The apparent values of N are given in Fig. 4, to which remarks similar to those already made are applicable. There is the usual drift and the usual temporary fluctuation. If the mean data be taken between / = 1.1 and 1.4 volts, the results are Apparent positive ions, N’ = 37,000. Apparent negative ions, N = 98,000. True total ionization, N + N’ = 135,000. Total nuclei caught, 60,000. It follows, then, that about 44 per cent. of the total ionization computed from 10'°e = 3.4, u and v, is caught on condensation. If we suppose the negative ions only are caught in the above fog chamber the electron value is 6x 10" =—— 3:42.20 x. 4 —— 3.0 electrostatic units. Conclusion.—Supposing the electron value to be 10'°e = 3.4 elec- trostatic units as before, the normal velocities of the ions in wet air to be u= 1.37, v1.51 cm./sec., in the volt/cm. field, the coronal equivalent of the ions caught in the above fog chamber is in the several cases, Total ions, 1,700,000, Total nuclei, 38 per cent. 385,000, AZ pet cent. 135,000, 44 per cent. 188 BARUS—METHOD OF STANDARDIZING [April 24, When N is 1,700,000 the coronas are too diffuse for sharp speci- fication. If it is assumed that negative ions only are caught, and if the nucleations corresponding to the coronas seen in the given fog chamber be taken as developed in my earlier work, then for N + N’=~1I,700,000, 385,000, 135,000, the electron values are 10} == 4iAe 31652 ,0, electrostatic units. With regard to the two parts of this paper that need revision the first, the comparison of the computed condenser capacity C’ with a standard, is a minor matter; but the other, 7. e., the marked dis- tribution of ionization along the axis of the fog chamber, will need further inquiry. In the direction of the exhaustion the amount of ionization may vary in the ratio of more than I to 2, in a fog cham- ber of about one half meter of length; and this under conditions where there should apparently be no variations and irrespective of the production of radiation from within or from outside of the fog chamber. Brown UNIVERSITY, PROVIDENCE, R. I. THE ELECTROMETRIC MEASUREMENT OF THE VOL- TAIC POTENTIAL DIFFERENCE, BETWEEN THE TWO CONDUCTORS OF A CONDENSER, CON- TAINING A HIGHLY IONIZED MEDIUM. By CARL BARUS. (Read April 24, 1909.) 1. Introductory.—The difficulties encountered in the preceding paper (§ 4), were made the subject of direct investigation by replac- ing the fog chamber with a metallic cylindrical condenser, the core of which was an aluminum tube, 50 cm. long and .63 cm. in diameter, the shell a brass tube, 50 cm. long and 2.1 cm. in diameter, coaxial with the former. Sealed radium tubelets could be placed within the aluminum tube, or withdrawn from it. Moreover, either the outer coat or the core of the condenser could be joined in turn with the Dolezalek electrometer, the other being put to earth. The conduct- ing system now appears as follows (Fig. 1), C being the outer coat or brass shell, 4 the aluminum core and ¢ the radium tubes in the cylindrical core. Conductors are earthed at e. BB show the metallic connections with the auxiliary condensers C’, C”. E is one of the insulated quadrants of the electrometer with the highly charged needle N, E being virtually also a condenser. Masel og Veep a ee e e Hig. A Clark standard cell may be inserted for standardization, but it is otherwise withdrawn. Direct experiment showed the self charging tendencies to come apparantly from the highly charged needle N, as if positive ions were loged into the conductor EBBA for a positive needle, negative ions 189 190 BARUS—ADJUSTMENT FOR PLANE GRATING [April 24, for a negative needle. In addition to this however there is a voltaic difference, aluminum-brass, at AC when radium is in place and the medium therefore highly ionized. The latter potentials are usually negligible. These are the chief electromotive forces, the first very high (150 volts) and in a weakly ionized medium; the other low (.2 volt) but in an intensely ionized medium: thus they may produce equal currents. Other voltages such as the room potential may be operative, but their effect is secondary. If the capacities C’, C”, are successively removed the electrometer current increases proportionately, showing its origin to be directed from the needle toward the insulated or non-earthed pair of quadrants. If the ‘condenser’ metals are reversed’ (see Fic!'1)) the voltare couple is reversed. This makes it possible to obtain both the voltaic contact potential and the ionization in the condenser C, from a pair of commutated measurements. 2. Theory.—Let V, be the potential at the electrometer, V, the voltaic potential difference of the two metals of the condenser, V the potential of the insulated conductor Bb, measured by the electrom- eter. Let be the hypothetical ionization in the electrometer, N the (radium) ionization in the condenser (length /, radii R,, R,). Let C be the total capacity of the systems CBBE. Then . 6007/ Nev yam! Be IN gh caeg Beta ZC i = AV, Vn Gineyee Vv) where 4 is a constant, « and v the normal velocities of the positive and negative ions, e the charge of the electron. The needle is posi- tively charged. This may be written V=V,=—KV 7.) where for WV —=0,.K9—0;6or V =Vye=A(Vr—V)n, i. e., the current in the electrometer, observed in the absence of radium, from needle to quadrants. This is directly measurable with accuracy. It is nearly proportional to V, since V is much within i per centot V,,. The integral of this equation is, t being the time, V =(Ve/ = oa ao 1909.] SIMILAR TO ROWLAND’S METHOD. iS If now the needle is left positively charged, but the condenser metals exchanged (commutated), so that the aluminum core is earthed and the shell put in contact with the electrometer (see figure), the equa- tion becomes a OI) Vig ee Let kx==N/K and x'=WN/K’ where K’ refers to the normal MElOciny~ Of positive ions, a: Uhen if k= Vo /nl/7.. and kh’ == V./n' VK, similarly V =V.(1—kN)e™. V'=Vi(1 + RN) e-™. iiitnes potential)” —— Vat }=—=)co. Vigo iN —Ve, Vel SVN +e two equations from which both N and V’, may be found, if the limiting potentials V,, V’, and the electrometer current V are severally observed. If V’, is not obtainable, it may be computed from observations at ¢ and t, = 2t, as Vo=—(2V = V2) /7? and Va — Chr — 1) /V 2: Here however there is a difficulty as the curves begin with a double inflection not yet expained. The times ¢,==2t must therefore be estimated from the observations beyond the double inflections; or the rearward prolongation of the curve for those observations, to meet the time axis. The initial tangents may be found in the same way, but this is not necessary since their values are, respectively, Viti kN and y(n kN). 3. Data: Origin of the Electrometer Current.—The seat of the chief electromotive force in the electrometer follows from the follow- ing data, in which the capacities C, C’, C”, Fig. I, are successively removed. The currents increase in the same ratio as the reduction of capacities, E being that of the electrometer. The data are (poten- tials in scale parts where 1 cm. is equivalent to .0595 volt), V_ being the fall per second: Capacities. Vin cm, V,, in Volts, C+C4+C’+E 14 .0083 C’+C”’ +E a5 .0089 C’ +E 58 0345 E 4.3 256 192 BARUS—ADJUSTMENT FOR PLANE GRATING, [April 24, The change of voltage throughout the main contours of the curves is almost a linear variation with the lapse of time, except that at the beginning the motion is accelerated from rest as usual; for instance: Time *tisses Oo 4 8) 2) V6 20 24 28 32 Go.) sec ee | BbGAY NOMI S77) LOM ee 4 US Shes Onciae a pat Arabs loreahh 4 | OLE. 16 oR 48 64 80 96 720 4. Aluminum Tube Charged with Radium Tubelets I.V.: Data. —The air in the condenser C is now highly ionized and its voltage becomes appreciable. The data obtained are given in Fig. 2. The needle is positively charged, thus impelling positive charge toward the quadrants. In the four series of data observed the aluminum core of the condenser is twice joined to the electrometer, the brass shell being put to earth (series 1 and 4) and twice com- mutated (aluminum to earth series 2 and 3). The results are identical except that in series 3 the insulation was perhaps better, or Vq may have changed. The accelerated march of the needle from rest is obvious in both curves and is thus independent of the sign of the limiting voltage, / . It may be mere inertia, but it is of less consequence here because the initial data are not needed in the following computation. 1909. ] SIMILAR TO ROWLAND’S METHOD. 193 5. Results: Ionization, N. Voltaic Contact Potential Difference V ..—The equations Vo =V./N—V , Ni Vee may now be used to compute N and /,. The constants are numer- ically (all in scale parts, I cm. equivalent to .0595 volt), K== 20.0 <110°)") Vig —— 3 AS Vg Ae K’ = 39.7 X 10°, Va.’ =9.3, Hence N = 876,000 ions, either positive or negative, Vie —6.37 cms:, or .376 volts. * [The drift, Va, which in the above experiments was eliminated by com- mutation, was eventually traced to a defect in the electrometer. It vanishes on replacing the given instrument by another. Data since obtained for Aluminium-Copper and Aluminium-Zince condensers showed Al-Cu, Vce=.58 volts, Al-Zn, Ve=.06 volts, or Zn-Cu, .52 volts, a result, however, which varied much with the surfaces, etc.] June, 1900. Brown UNIVERSITY, ProvipENCE, R. I. PROC. AMER. PHIL. SOC., XLVIII. Ig2 N, PRINTED SEPTEMBER 3, 1909. THE ABSORPTION SPECTRA OF VARIOUS POTASSIUM, URANYL, URANOUS AND NEODYMIUM SALTS IN SOLUTION AND THE ERRECT (OF TEMPERA] TURE ON THE ABSORPTION (SPECTRA OF CERTAIN ‘COEORED* SALTS iN SOLUTION. (Piates VII. to XIV.) By HARRY C. JONES ann W. W. STRONG. (Read April 24, T1909.) (A report on part of the work on absorption spectra that is being carried out with the aid of a grant from the Carnegie Institution of Wash- ington.) OUTLINE. I, Experimental Methods. II. Absorption Spectra of Potassium Salts in Aqueous Solutions. III. Absorption Spectra of Uranyl Nitrate (under Different Conditions). (a) In Aqueous Solution. (b) In the Crystalline State. (c) As Effected by Dilution. (d) In Methyl Alcohol. (e) In Mixtures of Methyl Alcohol and Water. (f) In Ethyl Alcohol. (g) As an Anhydrous Salt. IV. The Absorption Spectrum of Uranyl Bromide, Uranyl Acetate and Uranyl Sulphate. (a) Uranyl Bromide in Water. (b) Uranyl Acetate in Water. (c) The Uranyl Bands of the Acetate. (d) Uranyl Sulphate in Water. V. The Absorption Spectrum of Neodymium Chloride in Glycerol. VI. The Absorption Spectrum of Uranyl Chloride. (a) In Water. (b) As an Anhydrous Salt. (c) The Characteristic Bands in Water. (d) As Affected by Calcium and Aluminium Chlorides. (e) In Methyl Alcohol. 194 1909.] OF VARIOUS SALTS IN SOLUTION. 195 (f) In Methyl Alcohol with Calcium Chloride. (g) In Methyl Alcohol and Water. (h) In Ethyl Alcohol. (7) The Blue-violet Band. VII. The Absorption Spectrum of Uranous Salts. VIII. An Example of the Complexity of the Problem of Explaining the Origin of Spectral Lines and Bands and the Proposed Method of Attacking this Problem. IX. Effect of Rise of Temperature on the Absorption Spectra of Certain Salts in Aqueous Solutions. (a) Uranous Chloride. (b) Copper Bromide. (c) Chromium, Calcium and Aluminium Chlorides. (d) Uranyl Chloride. (e) Neodymium Salts. (f) Erbium Chloride. X. Summary. I. EXPERIMENTAL METHODS. On account of the large number of bands in the absorption spectra of uranium and the rare earth salts, a study of the absorp- tion spectra of these salts is more interesting and more fruitful of results than the study of the absorption spectra of the ordinary colored salt like those of nickel or copper. The absorption spectra have been mapped for potassium ferricyanide, potassium ferro- cyanide, potassium chromate, potassium dichromate, the acetate, bromide, chloride, nitrate and sulphate of uranyl in water, of uranyl acetate, nitrate and chloride in methyl alcohol, and of uranyl nitrate and chloride in ethyl alcohol. Beer’s law has been tested for these salts as well as the effect of foreign substances on the absorption spectra. The absorption spectra of two uranous salts, the chloride and sulphate, have been photographed and the ab- sorption spectra of neodymium chloride in pure glycerol and in mixtures of glycerol and water have been studied. In this work the methods used by Jones and Uhlert and Jones and Anderson? have in the main been employed. The investigations on the effect of changes in temperature on the absorption spectra of solutions have been confined to different con- centrations of aqueous solutions of the chloride, nitrate, acetate, *Publication No. 60, Carnegie Institution of Washington. * Publication No. 110, Carnegie Institution of Washington. 196 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, sulphate and sulphocyanate of cobalt, the chloride, acetate and sul- plate of nickel, the chloride, sulphate and acetate of chromium, chrome alum, the nitrate and bromide of copper, uranous chloride, erbium chloride, the chloride and nitrate of przesodymium, the sul- phate, acetate, chloride and nitrate of uranyl and the chloride, bromide and nitrate of neodymium. Spectrograms are made of the absorption spectra for a given concentration of a salt, keeping the thickness of layer constant for every 15° between 0° and go° C. To make a spectrogram light from a ‘Nernst glower and from a _ spark is allowed to pass through the solution that is being in- vestigated. It is then focused upon the slit of a spectroscope—and falling then on a concave grating, the light is spread out into a spectrum on the film upon which it is photographed. The films used were made by Wratten and Wainwright of Croyden, England, and were very uniformly sensitive to light from » 2100 to » 7200. The sectional diagram (Fig. 1) will make the experimental arrangement of the apparatus clearer. NV is a Nernst glower which is arranged to slide along the rod AB. P and P’ are quartz prisms which are held by a lid L. The prism P is stationary, whereas the prism P’ can be moved by the travelling carriage E back and forth through the trough T which contains the solution whose absorption spectrum is being investigated. AB is so inclined that the optical length of the light beam from N to P’, P and the concave mirror M@ shall be constant, whatever the length of the solution between P and P’ may be. The greatest length of path PP’ used was 200 mm. The hypothenuse faces of P and P’ are backed by air films which are enclosed by glass plates cemented to the quartz prisms. Considerable difficulty was experienced in finding a cement that would adhere to the polished quartz prisms at the higher tempera- tures. For aqueous solutions baked caoutchouc was found to work fairly well. D is a brass box holding the trough 7. D is filled with oil and is placed in a water-bath whose temperature can be varied between 0° and 90° C. The path of a beam of light is then from the Nernst glower (NV) or spark to the quartz prism P’. The light is totally reflected from the hypothenuse face of this prism through the solution to P. This prism also has its hypothenuse face backed by an air-film, so that the light is totally reflected upwards to the 1909.] OF VARIOUS SALTS IN SOLUTION. 197 concave speculum mirror at M@. WM focuses the light on the slit of the Rowland concave grating spectroscope, G being the grating and C the focal curve of the spectrum. The prism arrangement was designed by Dr. John A. Anderson. oe Lo Maas Ij MIA YOUU LLL LL! With Imates ie This apparatus was found to work very well for aqueous solu- tions. Some evaporation took place at the higher temperatures, but distilled water was added in proper quantity and mixed with the solution so as to keep the concentration constant. By using troughs of different lengths it was possible to vary the length of salt solution through which the light beam passed from I to 200 mm. One inconvenience was experienced at low temperatures ; moisture would sometimes condense upon the exposed prism faces. To overcome this an air blast was directed upon these faces and this helped very materially to prevent the condensation of moisture. 198 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, II. ABSORPTION SPECTRA OF PoTASsIUM SALTS IN AQUEOUS SOLUTIONS. Most potassium salts in solution are colorless, and for this reason it is considered that the potassium atoms do not themselves absorb any light in the visible portion of the spectrum. Several colored potassium salts are known and the color of these is due in some way to the other atoms in the salt molecules. In the present work the absorption spectra of potassium ferricyanide, potassium ferro- cyanide, potassium chromate and potassium dichromate have been studied. Using a 3 mm. length of solution of potassium ferricyanide in water we find that for a normal concentration there is complete absorption of all the shorter wave-lengths of light beyond 2 4800. As the concentration is decreased the edge of transmission moves continually towards the violet. It should be noticed that the region between complete absorption and complete transmission for the more concentrated solutions is quite narrow, being less than 40 Angstrém units; thus making solutions of this salt quite good screens for absorbing light. Continually decreasing the concentra- tion we reach a 0.0156 normal solution, when a transmission band begins to appear. For a certain range of concentration there ap- pears an absorption band in the region 44200. Further decrease in concentration results in increasing transmission throughout the violet and ultra-violet. For dilutions greater than 0.00195 normal there is almost complete transmission throughout the ultra-violet. Very faint bands appear in the regions AA 2500 to 2600, AA 2950 to 3050 and AA 3200 and 3250. Several spectrograms were made, keeping the product of con- centration and depth of solution layer constant. In this case the spectrograms will be identical if Beer’s law holds. Beer’s law was found to hold according to this method of testing within the ranges of concentration over which the spectrum was mapped. The absorption of aqueous solutions of potassium ferrocyanide was investigated in the same way. A half-normal solution 3 mm. deep shows that all light of shorter wave-length than 23950 is absorbed. Keeping the depth of layer the same, it is found that 1909.] OF VARIOUS SALTS IN SOLUTION. 199 with decrease in concentration the transmission gradually moves towards the ultra-violet, and for dilutions greater than 0.0078 normal there is transmission throughout the whole spectrum. Beer’s law was found to hold. A 2-normal aqueous solution of potassium chromate 3 mm. in thickness, shows complete transmission of wave-lengths greater than 44950. Decreasing the concentration causes the transmission to move gradually towards the violet and for a 0.01 normal solution a transmission band appears at 43100, or, in other words, there appears an absorption band whose center is about 43700. As the concentration decreases this absorption band fills up, the violet edge of the transmission band gradually pushes out into the ultra-violet, and for dilutions greater than 0.0005 normal there is complete transmission throughout the spectrum. Beer’s law was found to hold for potassium chromate throughout the above ranges of con- centration, except in the more concentrated solutions between 2 normal and 0.25 normal. Potassium dichromate in water was found to have a much greater absorbing power than the solutions previously described. A one-third normal concentration absorbed all wave-lengths shorter than 45350. As the concentration is decreased the transmission extends farther and farther out into the violet. For a 0.0026 normal concentration a transmission band appears in the violet, thus giving an absorption band whose center is about A 3800. As the concen- tration is further decreased transmission becomes greater and greater in the violet and ultra-violet, and is practically complete for a 0.0006 normal concentration. Beer’s law has been tested between the above ranges of cencentration and has been found to hold. In photometric measurements of Beer’s law, the equation defin- ing the quantities to be measured is: J=J,10-* J, is the intensity of the light that enters the solution (neglecting any loss due to reflection), J the intensity of the light as it leaves © the solution, c the concentration in gram molecules of the salt per liter of solution, / the thickness of layer and A a constant if Beer’s law holds. Strictly speaking the above equation holds for mono- 200 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, chromatic light. For ordinary white light one would have to integrate this equation over the range of wave-lengths used. The equation would then have the form Ag J=/J, i, e~ Bled, Jy The quantity B is called the index of absorption and 4 the molecular extinction coefficient. If the absorption is proportionately greater in the more concentrated solutions, then Beer’s law fails and 4 decreases inversely as the concentration. From photometric measurements Settegast® and Sabatiér* con- clude that the absorption spectrum of potassium dichromate is the same as that of chromic acid, and that the absorption spectrum of potassium chromate is entirely different. This is corroborated by the present work. Settegast finds that Beer’s law does not hold for potassium chromate and potassium dichromate, the coefficient 4 decreasing with increasing concentration. Grinbaum® finds the following values of A and e where e=c/A. ' Potassium Dichromate. Value of A. Value of A. A c = .034 c¢ = .0034 509 62.4 58.0 521 28.7 26.2 538 7.24 6.2 It will be seen that the deviation here from Beer’s law is in the opposite direction from that of Settegast. Grtinbaum finds that and therefore A depends on the depth of layer. An example will be given where the same concentration was used and different depths of the solution. A Values of « for c = .0034 25 cm. layer. 12 cm. layer. 5 cm. layer. 521 .0758 0818 .0884 521 0761 .0830 .0897 Our work indicates that Beer’s law holds for all small concentra- tions and usually the deviations for concentrated solutions is very 5 Wied. Ann., 7, pp. 242-271, 1870. *C.R.\103, DD. 49-52) TSS: 5 Ann. d. Phys., 12, pp. 1004, IOII, 1903. 1909.] OF VARIOUS SALTS IN SOLUTION. 201 small. Of the potassium salts above described, only potassium chromate between 2 normal and 0.25 normal showed any consider- able deviation from Beer’s law, and in this case the absorption of the concentrated solution was greater than would be expected if Beer’s law held by about 40 Angstrom units. The present method is a very good qualitative test of Beer’s law, and gives the results for each wave-length, whereas most photo- metric methods only give integrated results over a more or less wide region of wave-lengths. III. AssorRPTION SPECTRUM OF URANYL NITRATE UNDER DIFFERENT CONDITIONS. There are two groups of uranium salts, the uranyl salts con- taining the UO, group, and the uranous salts. The uranyl salts in solution are yellow and usually crystallize from aqueous solu- tions with a certain amount of water of crystallization; for ex- ample, at ordinary temperatures uranyl sulphate crystals have the composition UO,(SO,).3H,O. The uranous salts are intensely green and are very unstable, oxidizing very easily to the uranyl condition. | Uranous sulphate crystals have the composition U(SO,),9H,0. (a) Uranyl Nitrate in Aqueous Solution. The spectrum of uranyl nitrate in water is a typical example of the uranyl salts. Using a depth of solution of 3 mm. its absorp- tion spectra was investigated between concentrations of 1.5 normal to 0.0234 normal. For the 1.5 normal solution the absorption con- sists of a band in the blue-violet and absorption throughout the ultra-violet portion of the spectrum. As the concentration de- creases the blue-violet band fills up with transmission, and the ultra-violet absorption is pushed farther and farther out into the ultra-violet. The blue-violet band is practically gone at a concen- tration of 0.5 normal, and there is almost complete transmission throughout the ultra-violet for concentrations less than 0.02 normal. During these changes in concentration a large number of bands about 50 Angstrom units wide make their appearance. Near the edge of an absorption band these bands are relatively quite clear. 202 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, As the absorption edge recedes from the uranyl bands, the general transmission is so great as almost to entirely obscure them. A, Plate I, represents the absorption spectra of an aqueous solution of uranyl nitrate of different depths of layer. The narrow and rather weak bands shown here are the uranyl bands. Twelve of these bands have been photographed. Starting at the band of longest wave-length they shall be designated by the letters a, b, c, d, etc. On account of the irregularity of the distribution of light in the spark spectrum and the small intensity of the uranyl bands, the Nernst glower was used as the source of light in the ultra-violet, and long exposures were made. A screen was used that cut out all wave-lengths greater than 4200. A represents a_ typical spectrogram of this kind. Starting with the spectrum strip at the top, the concentrations were 1.5 N, 1.1255 N, 0.75 N, 0.5 N, 0.375 N, 0.25 N, and 0.1875 N. The slit width was 0.08 mm. and the current through the Nernst glower 0.8 amperes. The spectra of wave-lengths greater than A 4300 represent the absorption of a depth of layer of 15 mm.; the spectra of shorter wave-lengths rep- resent the absorption of a depth of layer of 3mm. The upper spectrum strip represents then the absorption spectrum of a 1.5 normal solution of uranyl chloride 15 mm. thick, exposure being made I min. to the Nernst glower. It will be seen that the uranyl a band comes out very strongly. The screen was then placed in the path of light and exposure of 5 minutes made to the violet and ultra-violet beyond 4300; a solution of uranyl nitrate of 1.5 normal concentration and 3 mm. depth of cell being in the path of the beam of light. This amount of uranyl nitrate absorbed practically all the light in this region. A very short exposure was afterwards made to the spark in the region A 2600, in order to get a comparison spark spectrum in this region, so that the wave- lengths of the uranyl bands could be measured. Throughout this work a comparison spark spectrum usually containing the very strong line 4 2478.8 was photographed on each spectrum strip. In measuring the uranyl bands all measurements were made from this line as a standard, and although the absolute wave-lengths of the uranyl bands may not be correct to within 20 1909.] OF VARIOUS SALTS IN SOLUTION. 203 Angstrém units, yet their relative accuracy is probably correct to within less than 10 Angstrém units for the finer bands. The second spectrum strip from the top represents in the long wave-length end of the spectrum the absorption of a 15 mm. solu- tion of a 1.125 normal solution of uranyl nitrate exposed 1 min. to the Nernst glower. The a band appears, although not nearly as intense as in the spectrum strip above. The region of shorter wave-lengths beyond 4300 represents the absorption of a 3 mm. depth of layer of a 1.125 normal concentration exposed 5 min. to the Nernst glower. A very faint transmission is shown in the region 43700. The ultra-violet line A 2478.8 is shown in the com- parison spark spectra. The other spectrum strips were made in a similar manner, using the concentrations given above. By this method of exposing two new bands were detected in the ultra-violet. In aqueous solutions the intensities of the bands are much the same. In other solvents however and for other uranyl salts, the relative intensities of the bands change very greatly. In uranyl nitrate crystals the bands are even more closely related to each other than in aqueous solutions. The longer the wave-length of the band the more intense and wider it is as a rule. The posi- tion of the long wave-length bands in the orthorhombic uranyl nitrate crystals UOQ,(NO,),6H,O is the same as the position of the bands for an aqueous solution. The wave-lengths of the bands are as follows: a b c d e if g Water Sol. 4860 4720 4540 4380 4290 4150 4020 Deussen. ( Jones and Water Sol. 4870 4705 4550 4390 4155 40305 Sirens Crystals 4870 4705 4500-4565 4405 4275 4170 4050 h i j k l Water Sol. 3870 3790 3690 Deussen. é: J Jones and Water Sol. 3005 3815. °3710 +3605 35154 Strong: Crystals 3035 3830 (3720?) 3600 In the original film from which 4, Plate I, was made all these bands except d could be very distinctly seen. The bands of longer 204 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, wave-length are slightly wider. The i band is considerably weaker than its neighboring bands. (b) Absorption Spectrum of Uranyl Nitrate Crystals. In the aqueous solution there is no sign that the bands can be broken up. In the crystal spectrum this is not the case. The a band is narrow. The b band is also very narrow, about 15 Angstrom units wide. A very faint band appears about ) 4650. The ¢ band, on the other hand, is very wide, about 70 Angstrom units, and is probably double. The d band is about 50 4. u. wide, and the e band is about 70 Angstrém units wide and appears double. The f band is the most intense and is about 4o A. u. wide. The bands g, h, 1 and 7 keep decreasing in intensity respectively. The above description is of a spectrogram taken of a crystal in Canada balsam, and of course the width of the bands varies with the time of ex- posure and various other things. The above spectrogram showed many details, however, that other spectrograms did not. It will thus be seen that the a, b, c, d, j and k bands of the solution agree fairly well with those of the crystal, and that the crystal bands f, g, h and i are shifted towards the red with reference to the bands in the aqueous solution. (c) Effect of Dilution upon the Uranyl Bands. The effect of dilution on the position and intensity of the blue- violet, the ultra-violet and the uranyl bands of the acetate, nitrate and sulphate of uranyl in water was tried. The absorption spectra of solutions of about 1 normal and 3 mm. depth of cell was photo- graphed along by the side of the absorption spectra of the same salts of 0.008 normal concentration and 380 mm. depth of layer. The absorption consisted of the blue-violet band, the ultra-violet band and the a, b, c, 7, j7 and k bands. Between the blue-violet and ultra-violet bands there was the transmission band containing 1, 7 and k. For each of the three salts this transmission band was much weaker for the dilute solution, whereas in the cases of the sulphate and nitrate the long wave-length transmission edge of the blue-violet band was stronger for the more dilute solution. The opposite was true of the acetate solution. In the dilute solution of 1909.] OF VARIOUS SALTS: IN’ SOLUTION. 205 the acetate the bands were more intense than for the more concen- trated solution. There was no noticeable change in the position of the bands. Neither the intensity nor the position of the uranyl nitrate or the uranyl sulphate bands was changed by the above dilution. A more detailed study was made as to whether Beer’s law holds for uranyl nitrate and for the other uranyl salts. The method of taking the spectrograms is the same as that used for the potas- sium salts. Beer’s law was found to hold for dilute solutions of uranyl nitrate in water. When the concentration is greater than .5 normal the absorption is greater than it should be if Beer’s law held. (d) Uranyl Nitrate in Methyl Alcohol. In methyl alcohol the general appearance of the absorption is very similar to that of the aqueous solution; the blue-violet, the ultra-violet, and uranyl bands appearing under the same general conditions that they appear for aqueous solutions. There is a very marked deviation from Beer’s law for the more concentrated solu- tions, however; the absorption of concentrated solutions being greater than it would be if Beer’s law held. The positions of the bands are quite different from the positions of the uranyl bands of the aqueous solution, or of the crystals, as shown by the follow- ing values: a b c d e f g h 1 A 4930 4760 4610 4455 4325 4190 4070 3965 3855 (e) Uranyl Nitrate in Mixtures of Methyl Alcohol and Water. In the previous work of Jones and Anderson® it was found that in some cases (for example neodymium chloride) a salt in water had a different set of absorption bands compared with the same salt in another solvent as, e. g., methyl alcohol. When the salt is dissolved in mixtures of these two solvents, say methyl alcohol and water, it was found that as the amount of one solvent, methyl alcohol for instance, decreased the methyl ° Publication No. 110, Carnegie Institution of Washington. 206 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, alcohol bands of the salt decreased in intensity, but did not change their position in the spectrum. At the same time the water bands of the salt became more intense. In the present work it is shown that the uranyl nitrate bands in pure water and in pure methyl alcohol occupy different positions. The problem to be investigated is to find out whether in mixtures of water and methyl alcohol, the uranyl bands will show a gradual shift, or whether the methyl alcohol uranyl bands and the water bands will both exist together ; their relative intensities being proportional to the relative amounts of methyl alcohol and water. It was found that the two sets of bands exist together and that the methyl alcohol bands decrease in intensity quite rapidly with increase of water. The blue-violet band showed marked changes until the amount of water reached about 20 per cent. In this work the amount of uranyl nitrate in the path of the light was kept constant, and the only variable was the relative amounts of methyl alcohol and water. The above would indicate that uranyl nitrate in water is “ hydrated” and in methyl alcohol it is “alcoholated.” The above data indicate that the effect of “hydration” is much more persistent than that of “ alcoholation.” It is quite possible that this is due to a greater number of water molecules producing the hydration than there is methyl alcohol molecules taking part in alcoholation. (f) Uranyl Nitrate in Ethyl Alcohol. The absorption of uranyl nitrate in ethyl alcohol was mapped and the general characteristics were found to be the same as for the water and methyl alcohol solutions. A new band was found at dX 5200 which was about 50 Angstrom units wide. All the uranyl bands were very faint and wide and therefore difficult to measure. Beer’s law showed deviations similar to those found for the methyl alcohol solution. On account of the diffuseness of the bands no spectrograms were made of mixtures of water and ethyl alcohol. Following are approximately the positions of a few of the bands: a b c d e i g h 1 X% 5000 4800 4630 4475 4325 4180 4080 3970 3875 1909.] OF VARIOUS SALTS IN, SOLUTION. 207 (g) Absorption Spectrum of Anhydrous Uranyl Nitrate. When it was first discovered that the uranyl nitrate “water” bands were all shifted to the violet with reference to the bands of the other uranyl salts in water, as well as with reference to the uranyl nitrate bands in other solvents, it was thought that possibly it was more hydrated than the other salts in solution. The uranyl salts crystallize from water solutions at ordinary temperatures with the following composition: UO,(NO,),.6H,O, UO,SO,.3H,O, WOstCHe COO). 2H-O;, and UOlEL.HL©.. Lhis: fact would favor the supposition that in solution the nitrate might be more hydrated than the other salts. The fact that the absorption of the aqueous solution of the nitrate and the crystallized salt was very much the same as far as the positions of the uranyl bands is concerned, also seemed to favor this view. In this connection it was considered important to examine the absorption spectrum of the anhydrous uranyl nitrate. The salt was powdered and placed in a closed glass tube just above the slit of the spectroscope. The light of a Nernst glower was then focused upon the surface of the salt nearest the slit and an exposure of about three hours made. In this way we examine light that has penetrated a short distance into the powder and is then diffusely reflected. The absorption spectrum was found to consist of quite a large number of bands, which seem quite different in many respects from those of the solution. The following are the approximate wave- lengths: AA 4800, 4650, 4500, 4420, 4360, 4280, 4180 (broad), 4060 (broad), 3950 (broad), 3820 (broad), 3700 (narrow) and 3600 (narrow). The bands marked broad are from 50 to 60 Angstrom units wide and the narrow bands about 20 Angstrom units. If the first band is the a band, then the bands of the anhydrous salts are to the violet of the corresponding bands of the crystals and of the solution. If it is the b band the opposite is the case. On account of the smallness of the intensity of the bands it could not be settled whether A 4800 is the a or the b band. Further investigation of this point will be made. There are two difficulties to the above theory, difficulties for 208 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, which no explanation so far has been suggested. In the work on the effect of rise of temperature on the absorption spectrum it was found that the uranyl nitrate bands did not shift to the red. On the other hand, the uranyl sulphate and uranyl chloride bands were shifted to the red under the same conditions. (In these cases aqueous solutions were investigated.) If the uranyl nitrate bands owe their position to a large amount of hydration it would be ex- pected that with rise in temperature they would be shifted towards the red more than the bands of the sulphate and chloride. Another difficulty is that of the effect of dilution. The greater the dilution the greater the dissociation, and, therefore, according to the theory of Arrhenius for very dilute solutions the UO, group should exist in the ionic condition and the absorption spectrum of all the salts should be the same, 7. e., the uranyl bands should then occupy the same positions independent of the kind of salt. No effect of this kind is to be noticed, as was shown above under the division de- scribing the effect of dilution. It is intended to use much more dilute solutions in the future. IV. THE ABsorRPTION OF URANYL BroMIpE, URANYL ACETATE AND URANYL SULPHATE. (a) Absorption Spectrum of Uranyl Bromide in Water. The absorption spectrum of uranyl bromide in water was mapped and found to be very similar to that of the nitrate. The ultra-violet, blue-violet and uranyl bands appear and are affected in the same manner as the same bands of the nitrate. Beer’s law was found to hold. The uranyl bands were found to be much wider and more diffuse than in the case of the aqueous solution of the nitrate. The following are their approximate positions: a b c d e i 4880 4720 4560 4450 4280 4160 (b) Uranyl Acetate in Water, Beer’s Law. A spectogram was made to test whether Beer’s law holds for an aqueous solution of uranyl acetate between the concentrations 0.25 normal and 0.031 normal. The spectrogram showed that there was a very great deviation from the law, and in the opposite direc- 1909.] OF VARIOUS SALTS IN SOLUTION. 209 tion to any deviation hitherto found either in this work or in that of Jones and Anderson or Jones and Uhler. The absorption of the more dilute solutions was found to be proportionately much greater than for the more concentrated solutions. A similar run was made for a solution of the acetate in methyl alcohol and a deviation from Beer’s law in the same direction was found, although the amount was not so great in this case. (c) The Uranyl Bands of the Acetate. The following table gives the approximate wave-lengths of the uranyl bands of the acetate in water, in methyl and as the anhydrous powder. Bands of Uranyl Acetate. a b c d é if g h 1 In Water 4910 4740 4505 4455 4310 4160 4070 3970 3830 In Methyl Alcohol 4900 4770 4600 4460 4320 4200 4090 As Anhydrous Salt. 4910 4760 4610 4460 4330 4190 4070 3980 From this table it seems that the positions of the bands of the acetate under these different conditions is about the same. (d) Absorption Spectrum of Uranyl Sulphate. The mapping of the absorption spectrum of uranyl sulphate in water showed that it was very much like that of the nitrate in water. As in the case of the nitrate the 7 band was much weaker than the adjacent bands. Beer’s law was found to hold. The addition of a large amount of sulphuric acid was found to make the uranyl bands much sharper, but not to cause them to shift. Much more work will be done on the effect of strong acids on the uranyl bands. The following gives the wave-lengths of the sulphate bands: a b c d e€ if g h 1 y k l 4900 4740 4580 4460 4330 4200 4070 3070 3850 3740 3630 3530 V. Tue ApsorpTion oF NEODYMIUM CHLORIDE IN GLYCEROL AND MIXTURES OF GLYCEROL AND WATER. The absorption spectrum of a glycerol solution of neodymium chloride is much like that of the aqueous solution in its general PROC, AMER. PHIL. SOC, XIVIII. 192 0, PRINTED SEPTEMBER 3, I909. 210 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, characteristics, but when proper concentrations are used so as to bring out the fine bands it is found that the two spectra are entirely different. For example,‘ the aqueous solution shows a very fine band at 44274. In the glycerol there is a band that on first sight appears exactly identical with this 4274 band. However, its wave- length is about 4287, and it has two extremely fine components on each side, one at \ 4273 and one at about 4.4300. The same is true throughout the spectrum. In general, in mixtures of water and glycerol the appearances indicate that there are “glycerol” bands and “water” bands and as the amount of one solvent is increased, so are the bands cor- responding to this solvent increased in intensity. Herein lies a very large field for investigation and considerably more work is being carried on here along these lines. The above described spectrum of the glycerol solution of neodymium indicates that glycerol has a a very great influence upon the vibrations of the electrons within the neodymium atom—and that this is due to a kind of “atmos- phere” of glycerol about the neodymium atom. Jones and Ander- son showed that alcohol has a similar effect, and that the “alcohol ” bands were much less persistent than the water bands. Further 99 66 work is being done upon the relative persistence of “water,” “alco- hol” and “glycerol” bands; also on the effects of foreign sub- stances and rise of temperature upon these bands, both in the pure solvent and for mixtures of solvents. VI. ABSORPTION SPECTRUM OF URANYL CHLORIDE. The absorption spectrum of uranyl chloride was mapped tor an aqueous solution, a methyl alcohol solution, an ethyl alcohol solution, a mixture of methyl alcohol and water, a mixture of methyl alcohol and calcium chloride, and a mixture of water and aluminium chloride. (a) The Absorption Spectrum of Uranyl Chloride in Water. The absorption spectrum of uranyl chloride in water was found to be very similar in general to that of the other uranyl salts. The uranyl bands were less sharp than the bands of the nitrate and sul- phate in water. The wave-lengths of a few of the bands are as follows: 1909.] OF VARIOUS SALTS IN SOLUTION. 211 a b c d e if g 4920 4740 4560 4460 4315 4170 4025 (b) Absorption Spectrum of Anhydrous Uranyl Chloride. The absorption spectrum of the anhydrous uranyl chloride was photographed in the same way as that of the anhydrous nitrate. The bands differ considerably from the bands of the aqueous solu- tion, and one cannot tell very well whether they are identical with the corresponding a, J, c, etc., bands of the solution or not. Their wave-lengths are approximately as follows: AA 4950 (narrow), 4860, 4765, 4700, 4615, 4540, 4460, 4320, 4290, 4160, 4050 and 3940. (c) The Characteristic Bands of Uranyl Chloride. In addition to the bands already described, uranyl chloride has several remarkably fine bands in the green. These bands are not more than 5 Angstrém units wide and were first seen on spectro- grams taken upon Whatten and Wainwright red sensitive films, They appear only for aqueous solutions, and the addition of cal- cium chloride or aluminium chloride causes them to disappear. They do not appear in alcoholic solutions. Aqueous solutions of uranyl sulphate show them very faintly. The wave-lengths are approximately as follows: NA 5185, 5200, 6000, 6020, 6040 and 6070. These bands have never hitherto been noticed as absorption bands. H. Becquerel* gives quite a full set of measurements of the phosphorescent bands of various uranyl salts at room temperature and at the temperature of liquid air. Among the bands given for the double chloride of uranyl and potassium at room temperature are 4X 6070 to 6040, and AA5220 to 5193. Whether these corre- spond to the above absorption bands is quite difficult to say. Fur- ther work is being done in this direction. (d) Uranyl, Calcium and Aluminium Chlorides in Water. Spectograms were taken of aqueous solutions of a constant con- centration of uranyl chloride to which varying amounts of calcium "C. Rs t. Ot, p. 1252, 1885; pp: 459 and 621, 1907. 212 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, chloride were added. The addition of calcium chloride causes the ultra-violet, the blue-violet band and the uranyl bands to widen gen- erally. The effect upon the uranyl bands is however, very small. The effect of aluminium chloride, however, is very great. The two narrow and faint bands at 45200 only appear in the pure aqueous solution of uranyl chloride. The a band in the aqueous solution is about 60 Angstrém units wide, and is almost as intense as the band. The addition of aluminium chloride causes the band to be- come quite narrow, about 25 Angstrém units wide. A slight addi- tion of alminium chloride decreases the intensity of the band very considerably. Further increases in the amount of aluminium has very little effect. The addition of alminium also causes the bands to shift to the red; the shifts in some instances amounting to 25 Angstr6ém units. The 6 and c bands have their intensity very greatly increased by the addition of aluminium chloride; and by making the solution about 2 normal of aluminium chloride these bands are shifted about 30 Angstrém units to the red compared with the same bands for the pure uranyl chloride solution. The d, e, f, g and h bands are also increased in intensity, but are but very slightly shifted to the red. The d and e bands are widened so that they practically form a single band. (e) Absorption Spectrum of Uranyl Chloride in Methyl Alcohol. In the absorption spectrum of uranyl chloride in methyl alcohol the a, b, c, d, e, f, g, h, 1, and j bands all appear, the b and c bands being the largest and most intense. The following are the approxi- mate wave-lengths of the bands: a b c d e f g h i Uranyl Chloride in Methyl Alcohol 4930 4760 4590 4465 4345 4220 4090 3980 3860 3760 Uranyl Nitrate in Methyl Alcohol 4930 4760 4610 4460 4325 4190 4070 3070 3855 Uranyl Acetate in Methyl Alcohol 4900 4770 4600 4460 4320 4200 4090 It is seen from the above table that the uranyl bands of these three salts in alcohol occupy almost exactly the same positions. 1909. ] OF VARIOUS SALTS IN SOLUTION. 213° (f) Absorption Spectrum of Uranyl Chloride and Calcium Chloride im Methyl Alcohol. In the solution of uranyl chloride in methyl alcohol the d and e bands are very diffuse, but are entirely separate. By adding cal- cium chloride a very peculiar phenomenon takes place. The d and e bands come together and as far as one can tell form a single band. At the same time the f, g and h bands shift to the red. For a solu- tion containing a .9 normal solution of calcium chloride one finds that the b and c bands have practically remained in the same posi- tion, the d and e bands have merged into one and the f, g, bands have moved to approximately AA 4260, 4120 and 4oro respectively. The de band is approximately at A 4420. (g) Absorption Spectrum of Uranyl Chloride in Methyl Alcohol and Water. A spectrogram was made of a solution of uranyl chloride of con- stant concentration in mixtures of methyl alcohol and water. A small addition of water causes a considerable decrease in the absorp- tion power of the uranyl chloride. When the amount of water has reached about 16 per cent. very little further change is produced by further increasing the amount of water. The most important effect of the addition of water is the effect upon the uranyl bands. Fora pure alcoholic solution the a and b bands appear; the b band being quite intense. Adding water causes a and b to both decrease in intensity and apparently to shift towards the violet. A spectrogram of smaller concentration shows the a, b, c, f, g, h and i bands; the solution containing 8 per cent. water the 0, c, d, e, f, g, h, 1 and j bands; the 16 per cent. water solution b, c, d, e, f, g, h,1 and 7; the 24 per cent. aqueous solution shows all these bands greatly weak- ened, and in solutions containing a greater amount of water prac- tically only the b and c bands appear, and these are very diffuse. The general effect upon the positions of the bands is quite remark- able, the b and c bands apparently being shifted to the violet with increase of water, whereas the ultra-violet bands appear to be shifted towards the red. “214 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, (h) Absorption of Uranyl Chloride in Ethyl Alcohol. The absorption spectrum of uranylichloride in the ethyl alcohol shows the uranyl bands quite strongly, although they are less intense than for the methyl alcohol solution. A very interesting resemblance has been found for the various uranyl bands of different mixtures. The absorption spectrum of a solution of uranyl chloride in ethyl alcohol has been found to be almost the same as that of a methyl alcohol solution of uranyl chloride containing a 0.9 normal concen- tration of calcium chloride or an aqueous solution of uranyl chloride and a 2 normal concentration of aluminium chloride. The positions of the uranyl bands for the ethyl alcohol solution was approximately: a b c d é f g h 1 A 4900 4750 4580 4400 4400 4250 4100 3980 3860 The relation above mentioned comes out much better in comparing the spectrograms. The values of wave-lengths thus far given does not bring this out very well on account of the difficulty of making measurements. Much more work is to be carried on along this line, and the measurements above given are to be considered as more or less of a preliminary character. (1) The Blue-Violet Band. Under the various changes above noted, 7. e., of changing the acid radicle, of changing the solvent and of adding foreign sub- stances, the position at which the blue-violet band faded away was approximately 44200. This is rather unexpected when we con- sider the very considerable effects which are produced upon the finer bands. VII. ABpsoRPTION SPECTRUM OF URANOUS SALTS IN SOLUTION. It is quite well known that by reduction the yellow uranyl salts are changed to the intensely green uranous salts. In the present work this reduction was accomplished by adding the same acid to the solution that corresponded to the anion of the salt and then putting in a metal that would produce a colorless salt. The absorption spectrum of uranous sulphate and uranous 1909.] OF VARIOUS SALTS IN SOLUTION. 215 chloride in water was found to be very similar. The absorption of the shorter wave-lengths was complete under the conditions used. The following are the approximate positions of some of the bands: A 6700, 6500, 6300, 5480 and 4900. The 6500 band was the strongest one of all, and upon increasing the depth of cell this band widened out so as to unite with the bands AA 6700 and 6300, forming an absorption band covering hundreds of Angstrom units. This is a very characteristic property of many of the uranous bands, that of widening out so as to include a very large portion of the spectrum. The uranyl bands do not change in width very greatly on increasing the depth of cell. Besides the bands described above uranous chloride shows bands at AA 4600, 4770 and 4970. The absorption spectrum of uranous chloride in methyl alcohol was found to differ very much from that of the aqueous solution. The bands at AA 4600 and 4780 appeared, closely resembling the water bands at the same position. The band 4970 in water was broken up into two bands in methyl alcohol at AA 4930 and 5030. In the alcohol a very broad band appeared at 45300, which does not appear at all in the water solution. The band at A 5580 is very similar to the water band. Weak and broad bands appear at dA 6150, 6300 and 6480, and a strong band at A6750. As the depth of the alcoholic solution is increased the widening of the bands is very different from the widening of the bands of the aqueous solution. The absorption spectrum of a mixture of calcium chloride and uranyl chloride in water was found to be very similar to that of the pure uranyl water solution. Much further work along the above lines is being carried on. VIII. AN EXAMPLE OF THE COMPLEXITY OF THE PROBLEM OF EXPLAINING THE ORIGIN OF SPECTRAL LINES AND BANDS AND THE ProposepD MeEtTHop oF ATTACK. It is a fact that investigations upon the spectral emission and absorption of bodies has been far less fruitful in extending our knowledge of the structure of the atom than had been expected. 216 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, This is largely owing to the almost infinite complexity of the struc- ture of the atom and our general ignorance of the forces that exist there. Probably the best known example is that of the uranyl group which we have been describing. Let us consider the spectral vibrations that can be produced by components that exist or may be produced from the apparently simple UO, group: (1) We have the absorption spectrum described above. At low temperatures most of these bands break up into much finer bands. (2) The uranyl salts under various methods of excitation emit a phosphor- escent spectrum of a large number of rather fine bands throughout the visible region of the spectrum. It is quite possible that this spectrum is intimately connected with that of the absorption spec- trum. (3) We have the absorption spectrum of the uranous salts which has been described above. This spectrum has been probably caused by the change of valency of the uranium atom. Uranium is known to form quite a large number of oxides and it is quite possible that for each valency of the uranium we have a character- istic spectrum. (This also is being investigated.) It is also quite probable that at low temperatures those spectra would consist of quite fine bands. (4) We have the spark spectrum and the ab- sorption spectrum of oxygen, and (5) that of ozone, which bears no relation to that of oxygen. (6) There is the exceedingly com- plex spark spectrum of uranium consisting of thousands of fine lines and also (7) the complex arc spectra. From radioactive ex- periments it is known that uranium is continually breaking down into ionium. (8) Ionium possesses the properties of a chemical atom and most likely has a spectrum of its own. This would make eight spectra. (9) Ionium breaks down into the radium and radium has a very characteristic spark spectrum, as does also (10) the radium emanation. During the various radioactive transforma- tions several a products are emitted with a velocity almost as great as that of light. It is probable that these particles are mov- ing with very great velocities in the uranium atom under ordinary conditions. (11) The a particles are known to be charged helium atoms and therefore under proper excitation would give the helium spectrum. The radium emanation breaks down into Radium A, B, C, D, Eand F. These products behave like chemical elements 1909.) OF VARIOUS SALTS IN SOLUTION. 217 and probably have characteristic spectra. (12) The final product is lead, *which has a very complex spark and arc spectra. During these transformations several electrons have been thrown off from the various products with enormous velocities. In a very large number of the above spectrum lines the Zeeman effect indicates the presencé of negative electrons and charged doublets. We thus see what an extremely complex system UO, must be and it might seem almost hopeless to entangle the mystery of its various spectra. At present we know that the arc and spark spectra problem is very complex and that we have very few methods of producing any changes in it. Practically the only method of changing the frequency of these vibrations is by applying a very powerful magnetic field or great pressure and these changes in the frequency are very small. One very important result, however, has been accomplished by Kayser, Runge, Wood and others. This work consists in separating spectrum lines into various series. A series of lines are those whose intensity and Zeeman effect vary in the same way when the conditions outside the atom are changed. The work of Wood is very important and shows that spectrum lines are due to different systems of vibrators inside the atom. By using monochromatic light of different wave-lengths he has been able to excite diffirent series of lines which constitute altogether the fluorescent spectrum of the element. Present theories of the atom usually regard the electrons and other vibrators that are the sources of arc and spark lines as being far within the atom and as affected by external physical conditions only under very special circumstances. Stark believes that these electrons may rotate in circular orbits, the locus of the centers of these orbits being a closed curve, say a circle. This system will be equivalent to a positive or negative charge according to the sense of rotation of these electrons. These electrons we will call ring electrons. Supposing these systems to be positive charges, it will require electrons to neutralize these charges. Several of these neutralizing electrons may be in the outer parts of the atom and under certain conditions might be knocked off from the atom. These easily removable electrons will be called “ valency ” electrons, of con- ’ and can exist under different conditions of “ looseness’ 218 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, nection with the atom. Most of the neutralizing electrons will probably lie far within the atom. For instance, we would expect that in the uranium atom the charged helium atoms are neutralized by negative electrons. Our theory is that the finer absorption bands of such salts as neodymium, erbium and uranium are due to vibrations of these neutralizing electrons, and that the forces acting upon these are considerably different from those acting on the ring electrons, which, in many cases, give a normal Zeeman effect. It is probable that these neutralizing electrons play the greatest role in the optical properties of bodies, such as the properties determining the index of refraction, the extinction coefficient, etc. Usually the equation of motion of such an electron is given by an equation like the following when a light wave of an electric field Ecos pt is passing by it: m a +2 2 + nx = EF cos ft. where m is the total mass (electromagnetic and material) of the electron, x - dv/dt is the damping or frictional term and n2r is the quasielastic force. It is an experimental fact as shown by the above work and the work of other investigators, that x and n? are not only functions of the electron and the atom, but that they are also functions of the physical and chemical conditions existing in the neighborhood of the atom. On the other hand, the effect on « and nm? for a ring electron, when external physical and chemical conditions are changed, is very small. It is for this reason, and the probable fact that there are relatively few neutralizing electrons, that we believe that much greater progress can be made in determining some of the properties and constitution of various interatomic systems of atoms and molecules by the study of the absorption spectra of uranium and neodymium than by a study of the arc or spark spectra of the same. The method of attacking the above problem will be to study the effect on the spectra of a body produced by changing the physical and chemical conditions about the light absorbers or emitters within as wide ranges as possible. Some of the possible changes that 1909.] OF VARIOUS SALTS IN SOLUTION. 219 can be made are as follows: Take for instance the’ uranyl group UO,. We can find the effect upon the absorption bands produced (1) by diluting the solution, (2) by changing the acid radicle to which the uranyl group is united, (3) by changing the solvent and using mixtures of solvents, (4) by adding other salts (like alumin- ium chloride), or (5) by adding acids of the same kind, as that of the salt of the uranyl group. The effect of adding foreign salts and acids at the same time and then varying the solvent, or the temperature, can also be tried. In this way a very large number of very interesting things can be tested. In most of these changes Ic will be kept constant. In the above examples the temperature (7), the external pressure (8), the electric: field (9) and the magnetic field (10) can be changed between wide limits. The latter effect is a very important one. For example, in aqueous solution neodymium salts give a large number of fine bands, in glycerol there are quite a number of new bands replacing the “water” bands, and in the alcohols there are various “alcohol” bands. At low temperatures these bands become very fine and it is quite possible to detect the Zeeman effect. Now it seems quite probable that a “glycerol”? band and an “alcohol” band that seem to replace each other as the solvent is changed are both due to the same vibrator. If the Zeeman effect is the same in both cases it would be a strong argument in favor of the above theory. A case that will soon be described is very im- portant. It was found that certain neodymium lines in a pure water solution did not have their wave-length changed when the tempera- ture was changed from 0° to 90°. If, however, calcium chloride was added, then on raising the temperature the above bands were shifted to the red. A very interesting and important investigation is whether the Zeeman effect on this band would be affected by the presence of bodies like calcium chloride. To be compared with the above changes are changes in the absorption spectra of the crystals of the salt (11) as affected by water of crystallization, or by the presence of foreign substances, or as affected by the polarization (12) or direction of passage of light through the crystal. The absorption spectra (13) of the anhydrous powder at different temperatures, etc., should be found. The 220 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, phosphorescent spectrum (14) should be studied in this connection, especially as affected by the mode of stimulation (X-rays, cathode rays, heating or monochromatic light of different wave-lengths). The temperature, electric or magnetic field could be changed about the phosphorescing body. The effect of change of state (15) should be tried if this is possible, also any possible changes of valency of the atoms (16) composing the body investigated. We shall attack the problem from all of these standpoints. After correlating the data obtained by the above named in- vestigations it is pretty certain that it will be possible to take each vibrator and trace the effects produced upon it by the above changes. It is also quite certain that we shall also know something of the nature of the vibrating system and the part that it plays in that complex body we call the atom. We shall now describe a few results obtained by changing the concentration and temperature of a solution of the chemical compound whose absorption spectrum we are studying. IX. THE EFFrect oF RISE IN TEMPERATURE ON, THE ABSORPTION SPECTRUM OF CERTAIN SALTS IN AQUEOUS SOLUTION. (a) Uranous Chloride (B, Plate VII.). To a normal solution of uranyl chloride in water was added a small amount of hydrochloric acid and zinc. The production of hydrogen reduced the uranyl to the uranous state. The same can be done in some cases by simply passing hydrogen gas through the uranyl solution. The solution was placed in the glass trough and a temperature run made as in the usual manner. The thickness of layer was I mm. The length of exposure was 50 sec. to the Nernst glower and 4 mins. to the spark, the current through the glower being 0.8 amperes and the slit width 0.20 mm. Starting with the strip nearest the comparison scale the temperatures were 8°, 17°, 33°, 48°, 62° and 73°. An exposure was also made at 80° which is not shown in the spectrogram B. At 8° a mist formed on the prisms and for this reason the spec- trum film taken at this temperature is much underexposed and the bands appear wider than at the higher temperatures. At this tem- 1909. ] OF VARIOUS SALTS IN SOLUTION. 221 perature there is complete absorption of the shorter wave-lengths to A 3650. A blue-violet absorption extends between A 4050 and A 4450. Following this band are three strong bands of about equal intensity and each almost 100 Angstrém units wide. Their wave-lengths are approximately AA 4590, 4760 and 4970. Following is a band at X 5500, a wide band from A6400 to A6630 and a rather narrow band at 2.6740. The absorption does not change very greatly until a temperature of 60° is reached. Above this temperature the increase in absorp- tion is quite rapid as the temperature rises. At 73° the ultra-violet band has widened to A 3800, the blue-violet band covers the region from A4050 to A5000. The bands Ad 4600, 4770 and 4980 at 8° have shifted slightly to the red with rise of temperature. None of the other bands seem to shift to the red at all and the broadening seems to be quite symmetrical. The band at A 5500 has become about twice as wide as it was at the lower temperatures and the two red bands have merged into one band running from 46350 to A6800. Between 73° and 80° the absorption increases very greatly. All short wave-lengths are absorbed up to A 5050. The band in the green runs from 45450 to \ 5600 and the band in the red has also widened very gfeatly, extending from 26200 to d 6800. (b) Copper Bromide (A and B, Plate VIII.). The two spectrograms showing the absorption spectra of copper bromide in water for various temperatures were made for different concentrations of the salt. A gives the absorption of a 2.06 normal solution I mm. thick and B the absorption of a 0.25 normal solution 8 mm. thick. The time of exposure to the Nernst glower was 2 mins. (current 0.8 amperes and slit width 0.20 mm.) and to the spark 6 mins. Starting with the strip nearest the comparison scale the temperatures at which exposures were made for A were 6°, 17°, Boerandiac sia fom BOP. 17°. 30",, 460°) 50°,.71-, and-35°. As the spectrograms show, the effect of change of temperature on the absorption spectrum is very marked. Above 45° the concen- trated solution did not transmit enough light to affect the photo- graphic film. 2a, JONES-STRONG—THE ABSORPTION SPECTRA [April 24, (c) Chromium, Calcium and Aluminium Chlorides (A and B, Plate TX): A, Plate IX., represents a spectrogram showing the effect of rise of temperature on an aqueous solution of chromium and aluminium chlorides. The concentration of the chromium chloride was 0.125 normal, and of the aluminium chloride 2.28 normal. The depth of layer wasgmm. The length of exposure to the Nernst glower was 4 mins. (current 0.8 amperes and slit width .20 mm.) and to the spark 6 mins. Starting with the strip adjacent to the comparison scale)the temperatures were 6, 192307 ,,51 7,00, andor 1 The most marked effect of the aluminium chloride was the pro- duction of a very pronounced unsymmetrical broadening, which does not occur when a pure aqueous solution of chromium chloride is heated. At 6° the ultra-violet band extends to A 3000, at 81° to A 3300, a much greater widening than takes place for a chromium chloride solution in water. At 6° the blue-violet band extends from 4100 to A 4600 and the yellow band from 5800 to 46200. Not only do the red sides of the blue-violet and yellow bands widen out enormously towards the red, but the short wave-length edges of these bands actually move towards the red. This effect is much more pronounced in the changes of temperature from 51° to 66° and from 66° to 81°. At 81° the blue-violet band extends from A 4150 to 45050 and the yellow band from 5900 throughout the remaining portion of the spectrum, as far as the film is sensitive. The fine chromium bands in the red do not appear. B, Plate IX., is a spectrogram, giving the absorption spectrum of a .125 normal concentration of chromium choride and a 3.45 normal concentration of calcium chloride in water at different temperatures. The length of the solution was 9 mm., the length of the exposures to the Nernst glower were for 5 min. and to the spark for 6 min. The current through the glower was 0.8 amperes and the slit width 0.20 mm. Starting with the strip adjacent to the comparison scale the temperatures at which the exposures were Made wereiO:, TOC) 20 nM 5 eelo4y and iGO a The effect of rise of temperature upon the absorption spectrum of a mixture of chromium chloride and calcium chloride is very similar to the effect on the mixture of chromium chloride and 1909.] OF VARIOUS SALTS IN SOLUTION. 223 aluminium chloride. The blue-violet and the yellow bands widen unsymmetrically and the short wave-length edges of these bands apparently moves towards the red at the higher temperatures. At 6° the ultra-violet band extends to A 2800, the blue-violet band from A 4000 to 44400 and the yellow band from A 5600 to A 6100. At 64° the ultra-violet band extends to » 3100, the blue-violet band from 4000 to A4600 and the yellow band from A 5650 to A 6300. At 80° the ultra-violet band extends to A 3250, the blue-violet band from \ 3950 to X 5000 and the yellow band from 45700 throughout the red end of the spectrum as far as the film is sensitive. (d) Uranyl Chloride (A and B, Plate X.). A spectrogram (A, Plate X.) was*made of the absorption spectrum of a normal aqueous solution of uranyl chloride, the depth of cell being 3 mm. Exposures were made to the Nernst glower for go sec., current 0.8 amperes and slit width 0.20 mm. The time of exposure to the spark was 6 min. Starting from the comparison spectrum the temperatures were 6°, 18°, 34°, 52°, 68° and 82°. At 8° the ultra-violet band extended to 3550, the blue-violet band from 4000 to 44450. The bands a, b and ¢ appeared, but the a band is very faint. The wave-lengths of the b and c¢ bands were AA 4565 and 4725. At 82° the ultra-violet band extends to 43700, and the blue- violet band from A 3950 to 44600. At this temperature only the b band appears,—a being very weak and c being completely merged into the blue-violet absorption band. The b band is located at » 4755. A spectrogram, B, Plate X., was made of a uranyl chloride water solution 0.0156 normal concentration and a depth of layer of 196 mm. Exposures were made to the Nernst gower for 30 sec., current 0.8 amperes and slit width 0.20 mm. No exposures were made to the spark except for comparison spectra. Starting with the numbered scale the temperatures were 6°, 18°, 29°, 44°, 59°, 71° and 79°. For this concentration there is a very slight temperature effect. There is a very faint transmission band between the ultra-violet and blue-violet bands. This is extremely faint and is practically un- 224 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, affected by temperature. The blue-violet band widened slightly with rise in temperature. The uranyl bands in the concentrated solution were much stronger and wider than in the dilute solution. (e) Neodymium Salts. A spectrogram (A, Plate XI.) of the absorption spectrum as affected by change of temperature was made of neodymium chloride solution in water, the concentration being 3.4 normal and the depth of layer 12 mm. The length of exposure was 2 min. to the Nernst glower, current 0.8 amperes; slit width .20 mm. The time of ex- posure to the spark was 6 min. Starting with the strip nearest the numbered scale the temperatures were 11°, 22°, 33°, 45°, 50°, 73° and 85°. An absorption band appears at about 2970 for the 11° tempera- ture, a very strong band from d 3250 to 43285 and an adjacent band from ) 3285 to 43310. At 11° a very narrow and feeble transmission band separates these two bands. At 85° the trans- mission band has weakened very much. At 11° a very strong band lies between 3490 and 23580. The band A 4274 is about 8 Angstrém units wide. An extremely narrow band appears at A 4297, d 4306 and 24324. At A 4234 is a wider and rather diffuse band, it being about 12 Angstr6m units wide. Bands at 11° lie between NA 4415 and 4470, AA 4580 and 4650, AA 4665 and 4710, AA 4740 and 4775, AN 4815 and 4835, and the very wide bands AA 5010 and 5300 and AA 5665 and 5935. Weak bands are located at 4645, A 4800, 5320, 16235, 16255, '6280, A6305 and A6380. Rather diffuse bands appear at AA 6780 and 6840, at AO850 and from A 6870 to d 6920. The effect of rise of temperature from 11° to 85° is quite noticeable, although it is not great. In the ultra-violet there is a slight increase in the general absorption. The band AA 3285 and 3310 widens slightly. The band AA 3490-3580 at 11° has widened so that at 85° it extends from A 3450 to A 3600. The band at AA 4415 and 4470 has widened but little. The group of bands from 4600 to 4800 have also widened but little. The faint diffuse bands dA 4645 and 4800 have practically disappeared. The bands AA 5010 and 5300 and \A 5665 and 5935 at 11° have widened at 85° to 1909.] OF VARIOUS SALTS IN SOLUTION. 225 XX 5010 and 5350 ahd AA 5660 and 5985. The widening of the latter band is distinctly unsymmetrical. The existence of the band A 5320 causes the band A 5010 to A 5300 to widen unsymmetrically. The bands in the region A 6300 become less sharp as the tempera- ture rises. At 11° there was considerable transmission in the region 6850. At 85°, however, this transmission disappears and there is practically complete absorption from 26760 to 46920. The very sharp bands AA 4282, 4300, 4310, 4322 and 4343 do not appear to change very much with change in temperature. On the strip taken at 73° these bands appear sharper than on any of the other strips. A spectrogram (5, Plate XI.) showing the effect of rise in tem- perature was made on a neodymium chloride solution in water of c.17 normal concentration and a depth of layer of 196 mm. The amount of neodymium chloride in the path of the light is approxi- mately the same as in the spectrogram, showing the effect of tem- perature upon a 3.4 normal concentration and a depth of cell of 12 mm. In this case the temperatures were 5°, 16°, 28°, 42°, 59°, 72° and 82°. Exposures were made to the Nernst glower for 3 mm. current 0.8 amperes and slit width 0.20 mm. Fach strip was ex- posed to the spark for 6 mm. The purpose of making this spec- trogram was to find the effect of concentration of a salt upon the changes produced by change in temperature. A description of the bands at 5° and 82° will be given. Any change between these two temperatures that takes place is a gradual one. Transmission begins at 42600. Bands appear between dd 3250 and 3300 and AA 3455 and 3575. The band 4274 is much sharper and narrower than for the more concentrated solution. The nu- merous fine bands in the region 4.4300 are very faint. The bands dA 4420 to 4460, AA 4600 to 4630, 44645, AA 4680 to 4705, AX 4745 to 4770 and 4820 have rather diffuse edges. Wide bands appear from 45020 to 5290 and from 25685 to 5920. Diffuse bands are located at 45310, A6810 and A6go00. The group in the region 6300 appear, but they are extremely faint. At 82° the general absorption has increased in the ultra-violet and has reached to about 2800. It will be noticed here that the effect of rise in temperature is greater upon this general ultra-violet PROC. AMER. PHIL. SOC., XLVIII. 192 P, PRINTED SEPTEMBER 7, 1909. 226 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, absorption in the dilute solution, than it is for the concentrated solu- tion previously described. The band AA 3455 to 3575 at 5° has widened slightly, having the limits A 3445 and 3580 at 82°, the widening being about 15 Angstrom units. This band in the concentrated solution widened 60 Angstrom units. Practically no effect of temperature is to be noticed upon the bands from A 4200 to X 4900 with rise in tempera- ture. At the higher temperatures the bands are slightly more diffuse, but this change is very small. The band XA 5020 to 5290 at 5° has widened to AA 5015 and 5285, about ro Angstrém units. The corresponding widening for the concentrated solution was approxi- mately 50 Angstrom units, although it must be noted that in the more concentrated solution this widening was mostly due to the increased absorption of the band \ 5310 at the higher temperatures. The band 25685 to 45920 at 5° has widened to AA 5775 and 5930, about 20 Angstrém units, compared with a widening of 55 Angstrom units for the more concentrated solutions. None of the other bands show any appreciable change with change in temperature. A spectrogram (A, Plate XII.) was made showing the effect of temperature upon the absorption spectrum of a 1.66 normal aqueous solution of neodymium bromide, the depth of layer being 6 mm. An exposure of 4 mm. was made to the Nernst glower, at .8 amperes and a slit width of 0.20 mm. The length of exposure to the spark was 6 mins. The temperatures of exposure, starting with the strip adjacent to the comparison spark, were 4°, 20°, 36°, 50°, 68° and (eles At 4° there is complete absorption in the ultra-violet up to 2600. A broad absorption band appears at A 2660 to » 2800 and from 2950 to A 3060. These absorption bands appear with a more or less general absorption. Bands appear at Ad 3460, 3500 and 3540. The band at 4274 is weak. Weak and diffuse bands occur at AA 4440, 4630, 4695, 4760, 4825, 5095, 5260, 6810 and 6900. Wider bands are located at AA 5116 to 5140, AA 5200 to 5240 and AA5710 to 5850. At 83° the spectrum is almost exactly the same as at 4°. The ultra-violet absorption is complete up to A3050. The bands at 43500 have increased in width slightly and the band A4274 is 1909.] OF VARIOUS SALTS IN SOLUTION. 227 _—a slightly broader. The bands that have widened appreciably are dA 5195 to 5260 and AA 5700 to 5880. The change in the absorption is greatest when the temperature is changed from 68° to 83°. Up to 68° there is practically no change in the absorption spectrum at all. A spectrogram (B, Plate XII.) showing the effect of temperature was made, using an aqueous solution of .055 normal concentration of neodymium bromide, the depth of the layer being 197.4 mm. This spectrogram was made to compare with that taken with a 1.66 normal concentration of the same salt and a depth of layer of 6 mm. The exposures to the Nernst glower lasted 90 sec. in this case, current 0.8 amperes and slit width of 0.20 mm. The length of ex- posure to the spark was 6 mins. Starting with the strip nearest to the comparison scale the temperatures of the solution were 5°, 16°, 207,42",55),.08 and 84>. At 5° there is practically complete transmission of light between d 3400 and 2600, no ultra-violet bands appearing, as was the case for the more concentrated solution. The bands AA 4445, 4693, 4760, 4825 and 5095 were somewhat sharper than they were in the con- centrated solutions. The two largest bands extended from 25200 to 45250 and from A5710 to 5850. As in the case of the more concentrated solution, so here, the greatest change in the absorption took place in the change from 68° to 84°. The ultra-violet absorp- tion increased up to A2900. The bands at A 3500 became consider- ably stronger, but they widened very little. The bands AA 4445, 4693, 4760 and 4825 are somewhat weaker than at 5°. The wide bands remained practically as wide as at 5°, 45200 to 5250 and d 5705 to 5870. This indicates a widening of about 25 Angstrom units for the latter band. For the more concentrated solution the widening of these two bands was 25 and 40 Angstrém units re- spectively. It is thus seen that in the more concentrated solutions the bands widen more with rise in temperature than they do in the less concentrated solutions. At 42° in the dilute solution there ap- pears a narrow band at A6710. This increases in intensity with rise in temperature. This band does not appear at all in the con- centrated solution. A spectrogram (A, Plate XIII.) was made of neodymium chlo- ride and calcium chloride in water. Exposures.were made for 30 sec. 228 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, to the Nernst glower, the current being 0.8 amperes and the slit width 0.20 mm. The length of exposure to the spark was 4 mins. Starting with the strip nearest the numbered scale the temperatures were6", 177, 21°40, 03) \7as andie2=. The general effect of the addition of calcium chloride is to make all the bands hazier, and to increase the transmission throughout the region of the band. At 6° there is a slight transmission throughout the ultra-violet portion of the spectrum. As the temperature is raised this general transmission is decreased, and at 82° practically no light passes through the solution of shorter wave-length than 2800. Sharp bands occur at A 3464, 43500, A 3535, 44276 and weak diffuse bands at ’ 4295, 44305, 44340, 4445, 4620, 4695, i 4760, 44825, A5095, A5130, A5225, A5260, A5320, A5710, to 5860, 6245, XO810 and A 6go0. At 82° the bands in the A 3500 region are slightly more intense than at 6°. Practically all the bands from A 4200 to 5200 have be- come much weaker at the higher temperature. This is especially true of the band \ 4276, its intensity being less than half what it is at 6°. Most of the bands are shifted to the red with reference to the same bands at 6°. For instance, A 5095 is shifted 5 Angstrém units towards the red. The bands 4695, 44760 and 24825 are all shifted to the red at the higher temperature, and especially A 4825, the shift in thise case amounting to 5 Angstrom units. In the case of these bands the shift is not an apparent one due to unsymmetrical broadening, for in this instance there is no broadening at all. The band from A5710 to A5860 at 6° has widened very unsym- metrically and has the limits 45710 to 45920. The short wave- length side is quite sharp and its position is practically independent of the temperature. The long wave-length edge is quite broad and recedes quite rapidly towards the red as the temperature is raised. The bands in the red AA 6810 and 6900 grow fainter and fainter with rise in temperature, and have practically disappeared at 82°. The band A 6245 is very weak at 6° and has disappeared at about 60°. It will thus be seen that not only does the presence of calcium chloride modify greatly the absorption of neodymium chloride, but that it changes the effects due to temperature very fundamentally. In pure neodymium chloride practically no bands decrease in in- 1909.] OF VARIOUS SAETS IN SOLUTION: 229 tensity with rise in temperature, and at present no shift has been detected. When calcium chloride is added to the solution most of the bands decrease in intensity with rise in temperature and several are shifted towards the red at the same time. Several bands dis- appear. Moreover, the band XA 6800 to 6900, although it widens, this widening is entirely on the red side, whereas for the pure neodymium chloride solution this widening always takes place on both sides of the band. A spectrogram (B, Plate XIII.) was made to show the effect of change in temperature upon a 2.15 normal aqueous solution of neodymium nitrate. The length of layer was 3 mm. The exposures were for 40 sec. to the Nernst glower, current 0.8 amperes, slit width .20 mm. The length of exposure to the spark was 6 mins. Starting with the strip nearest the comparison spark the tempera- Gines.wiere 41/17, 20, 42 565 7 and Sac. The changes in the spectrum due to this change in temperature of 80° was very slight. The NO, band extends to about » 3250 at 4°, and to about A 3280 at 84°. The bands at A 3500 became con- siderably wider and their edges'more diffuse at the higher tempera- tures. At the lower temperatures fine bands appear at XA 5210, 5225 and 5240. At 84° these bands all merge into a single band. The red band extends from 45705 to 5860 at 4°. The band at A 5820 is very faint at the lower temperatures. At 84° it is unrecognizable, At this temperature the red band extends from 45700 to 5880. The widening of this band for the concentrated solution is somewhat greater than for the dilute solution, but the effect of concentration is very slight. This is to be expected since the effect of temperature itself is so very minute. A spectrogram (A, Plate XIV.) was made of an aqueous solu- tion of neodymium bromide 1.66 normal concentration and 54.6 mm. depth of cell. The exposures were 3 mins. to the Nernst glower and 6 mins. to the spark. The current in the Nernst glower was 0.8 amperes and the slit width 0.20 mm. Starting with the strip nearest the comparison scale the temperatures were 6°, 20°, 33°, 47°, 62°, 735 and 82°. The effect of rise in temperature upon the absorption spectra of this salt was quite marked; practically all of the bands broaden- 230 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, ing and becoming more intense. At 6° the ultra-violet absorption extended to 43600. At 82° it had advanced to 3800. Very nar- row and fine bands appear at A4186, 44300, 44308, 4345, 6240, 6265, 6290, 6305, and much broader bands at X6380 and A6740. Wide bands occur at from AA 4390 to 4480, AA 4550 to 4850, AA 4990 to 5340, AA 5650 to 5950 and AX 6760 to 6930, at 6°. At 82° these bands have the following limits respectively : AA 4380 to 4500, AA 4540 to 4910, AA 4960 to 5370, AA 5620 to 5990 and AA 6730 to 6960. (f) Erbium Chloride. A spectrogram (B, Plate XIV.) was made to show the effect of rise in temperature upon the absorption spectrum of a solution of erbium chloride. For this purpose a 0.94 normal solution of erbium was used and the depth of layer was 48 mm. The solution probably contained a considerable number of impurities, so that in fact the amount of erbium was quite small. The absorption spectrum was found to change but little with rise in temperature, thus indicating a dilute solution. Exposures were made for 30 sec. to the Nernst glower and 4 mins. to the spark. The current through the glower was 0.8 amperes and the slit width 0.20 mm. Starting with the spectrum nearest the comparison scale the temperatures were 7°, ns 120" HAO, 60° ZO, and Sor At 70° the ultra-violet is absorbed to A 3950. As the temperature is raised the ultra-violet absorption increases, and at 80° it reaches d 3150. Bands from 20 to 40 Angstrém units wide occur at A 3235, 3510, 43640 and A 3785. These bands are slightly wider at 80°, but as for all the other erbium bands this widening is very small. Weak and narrow bands appear at AA4165, 4425, 4458, 4500 (strong), 4535, 4540, 4555, 4580, 4685, 4750 (30 A. u. wide), 4810, 4840, 4855, 4870 (strong and 20 A. u. wide), and 4920, » 4920 lies alongside of a fuzzy band extending from 4 4910 to » 4950. After these comes a rather wide band which for a shorter length of layer would most likely be broken up into a number of much finer bands. This band extends from A 5190 to A5250. At A5217 there runs a narrow sharp line through the fuzzier and wider band. Broad (about 30 A. u. wide) and very faint bands are located at 456030 and 25760. For greater concentrations these would prob- 1909.] OF VARIOUS SALTS IN SOLUTION. 231 ably show as finer bands. The band at 6540 is much more diffuse on the red than on the violet side; this possibly being due to a component that is not separated at this temperature. Other bands are located at AN 5365, 5380, 5425, 5445, 5505, 6410, 6440, 6495 and 6690. The general effect of rise in temperature here is to cause the lines to become slightly fuzzier and to show more of a “ washed out’? appearance. No shift due to rise in temperature was noticed. Throughout all the previous work the wave-lengths were read directly from a scale. This scale was made so as to give the wave- lengths in Angstr6m units directly. It was found in the measure- ments that the Seed films did not correspond to the Wratten and Wainwright films, when the same spark spectra on the two kinds of films were placed beside one another. This was probably due to different shrinkage of the two kinds of films on fixing, washing and drying. For this reason the wave-length measurements are not intended to be absolutely correct but only relatively so. All the temperature work was done with Wratten and Wainwright films. The relative measurements of fine bands for any spectrogram are prob- ably correct to within a few Angstrom units. X. SUMMARY. The absorption spectra of the uranyl salts contain a series of bands in the blue and violet. Twelve of these bands can usually be detected for each salt. Starting from the blue end of the series the bands are designated by the letters a, b, c, etc. These bands are usually diffuse and from 30 to 50 Angstrom units wide. The uranyl bands of uranyl nitrate in water are all farther to the violet than the uranyl bands of any other salt investigated, or of uranyl nitrate in other solvents. The uranyl absorption bands of crystals of uranyl nitrate agree with the absorption bands of an aqueous solution of the nitrate, with the exception of the f, g, / and i bands; these latter being shifted to the red in the crystal. Dilution within the ranges studied does not affect the position of the uranyl bands. Theoretically, all the uranyl salts in water 232 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, should give the bands of the same wave-lengths for very dilute solutions. The uranyl bands of the nitrate in methyl alcohol are all shifted to the red about 50 Angstroém units, with reference to the bands in water. Mixtures of water and methyl alcohol show that we have both sets of bands existing for the same solution, the “water” bands increasing in intensity as the amount of water increases. The water bands are the more persistent. This indicates the existence of a hydrate and an alcoholate of the uranyl group. In ethyl alcohol the a, b, c and d bands are shifted to the red with reference to the methyl alcohol bands. The other bands appear to have the same positions as the methyl alcohol bands. The absorption spectrum of the anhydrous salt is very complex and the bands could not be recognized. The bands of uranyl bromide in water, of uranyl acetate in water and methyl alcohol, and also of the anhydrous salt, are ap- proximately of the same wave-lengths, differing but slightly from the wave-lengths of the uranyl nitrate bands of an aqueous solution. The bands of uranyl sulphate in water are all shifted towards the red about 50 Angstr6m units, with reference to the uranyl nitrate bands in water. For both the sulphate and nitrate in water the bands are very much alike. The 7 band is very weak in both cases. Uranyl chloride bands of an aqueous solution are shifted to the red with reference to the uranyl nitrate bands of an alcoholic solu- tion. The addition of calcium chloride or aluminium chloride is found to produce very marked effects upon the uranyl chloride bands. The addition of sufficient aluminium chloride to a water solution of uranyl chloride, or of calcium chloride to a methyl alcohol solution of uranyl chloride is found to cause the d and e bands to come together, so as to form a single wide band, and to cause the other uranyl bands to shift so that the whole resulting series of bands is almost identical with the series of bands of an ethyl alcohol solution of uranyl chloride. The effect of adding foreign substances also greatly modifies the intensity of the bands. An example of this difference of action is the effect of adding aluminium chloride to an aqueous solution of uranyl chloride. The 1909.] ' OF VARIOUS SALTS IN SOLUTION. 233 a and b bands are affected entirely differently ; the a band being very much reduced in intensity and made narrower, whereas the b band becomes very much stronger and wider. A new set of fine bands in the green has been discovered in the absorption spectrum of an aqueous solution of uranyl chloride. These only appear for pure water solutions; a small amount of aluminium or calcium chloride causing them to vanish. They do not appear for methyl or ethyl alcohol solutions, and for no other uranyl salt except very faintly for the sulphate. The absorption spectrum of several uranous salts has been photographed. The spectrum is entirely different from that of the uranyl compounds. The absorption spectra of uranous chloride in methyl alcohol and in water were found to be very different. The absorption spectrum of neodymium chloride in glycerol was found to be entirely different from that of the salt in water. Mixtures of water and glycerol seem to indicate the existence of both sets of bands in the same solution. The “glycerol” bands are more persistent with reference to water bands than “alcohol” bands are. Much more work along this line is contemplated. Rise in temperature has been found in general to cause an in- crease in the amount of absorption, and to cause the absorption bands to widen. This widening of the bands may or may not be symmetrical. Some of the absorption bands of uranous chloride widen very rapidly with rise in temperature. Other bands do not widen so rapidly, and seem to be slightly shifted towards the red. In solutions containing a single salt, it has invariably been found that the bands widen with rise in temperature, and that this widen- ing is greater, the greater the concentration of the solution. The uranyl bands of aqueous solutions of the chloride and sul- phate of uranyl are shifted towards the red with rise in temperature. The intensity of the uranyl bands does not seem greatly modified by changes in temperature. The effect of rise in temperature on the absorption syectrum of a solution of a salt containing calcium or aluminium chloride is very peculiar. The bands usually broaden very unsymmetrically, 234 JONES-STRONG—THE ABSORPTION SPECTRA [April 24, and in all cases investigated, the widening has been on the longer wave-length edge. A tyipcal example is shown in Plate III. Rise in temperature causes the neodymium bands to widen slightly, but no shift of the bands has been noticed. However, when calcium chloride has been added to the neodymium solution, a rise of temperature causes many of the bands to become much less intense, and also causes some of the bands to shift to the red. In the recent work of Becquerel and others it is quite possible that the presence of various foreign bodies in the crystals along with the neodymium may have a very great influence upon the absorption spectrum. All the above conclusions must be understood to be limited to the conditions and within the ranges described in the earlier parts of this paper. PuHysICAL CHEMICAL LABORATORY, Jouns Hopkins UNIVERSITY, May, 19009. PROCEEDINGS Am. PHILOS. Soc. VOL. XLVIII. No. 192 PLATE VII is oO = @ = = - 3 = 8 & S: PROCEEDINGS Am. PHILOS. Soc. VoL. XLVIII. No. 192 PLATE VIil 60 O38 ee ee ee ce Re SS 48 50 | AG 10 Me eee co er 1G 18 | ‘Tes fh } 1 ¢ > y 1s PROCEEDINGS Am. PHILOS. Soc. VOL. XLVIII. No. 192 PLATE IX . 7 es a te i SEBS PROCEEDINGS Am. PHILOS. Soc. VOL. XLVIII. No. 192 PLATE X oo dO is 1G s bad bic 10) IX ee ee PROCEEDINGS AM. PHILOS. Soc. VoL. XLVIII. No. 192 PLATE X|l 2 a | a 8 eet | tf] be ba ADNAN A A 1 PROCEEDINGS AM. PHILos. Soc. VoL. XLVIII. No. 192 PLATE XII ; iN | x Les we YS epee * AS eT a : a 3 ; 3 4 a 4 : 3 PROCEEDINGS AM. PHILOS. Soc. VoL. XLVIII. No. 192 PLATE XIII is 10 Po — 2 til ee te — Poe PROCEEDINGS Am. PHILOS. Soc. VoL. XLVIII. No. 192 PLATE XIV sagas: | wih = es es a 0: So ERS ad OU 12 POA Re TBE i Ba PAOUAKES >; HEIR ;CAUSES AND) ERREECES: By EDMUND OTIS HOVEY. (Read April 24, 1909.) The occurrence of three earthquakes in the western hemisphere within the space of nine months in 1906-1907, all of which were attended with disastrous effects upon human life and property, at- tracted as never before the attention of the world, and particularly of the United States, and focused interest upon the science of seismology in a manner calculated to advance materially the study of movements and other physical changes in the earth’s crust. San Francisco, in April, 1906, Valparaiso, in August, 1906, and Kingston, in January 1907, attracted wide notice, but the disaster that over- whelmed Messina, Reggio and vicinity on December 28, 1908, capped the climax, and sufficient reason is apparent for the universal interest now prevailing, one manifestation of which is the present symposium. The thesis of the seismologists is that the chain of earthquake observatories that have been established in the past decade and a half should be extended and united into a network of stations covering the globe, sufficiently, at least, to furnish a com- plete record of the important vibrations propagated through the earth, indicate their places of origin and provide data for more satisfactory theories as to their causes. Great earthquakes rank with volcanic eruptions as being the most terrifying of all natural phenomena. Usually coming with no recognized warning, often happening in the night, extremely indefi- nite as to source, extent and duration, they fill the mind of the human observer with the horror of utter helplessness. They have been far more destructive to human life and property than volcanic eruptions have been, for we have the earthquake shocks of Sicily, 1693, with 60,000 victims; Yeddo, Japan, 1703 (200,000) ; Peking, 1731 (100,000) ; Lisbon, 1755 (60,000) ; Calabria, 1783 (60,000) and Messina-Reggio, 1908 (200,000); besides many others, to 235 236 HOVEY—EARTHQUAKES: [April 24, compare with the volcanic outbursts of Krakatoa, 1883, destroying 36,500 victims; Vesuvius, 1663 (18,000) ; Mt. Pelé, 1902 (29,000) and the Soufriére of St. Vincent, 1902 (1,400), other historic eruptions having entailed comparatively small loss of life. Although earthquakes have been recorded frequently throughout all historic time, seismology is one of the youngest of the sciences —it is still in its formative state. Scientific interest in the subject has indeed not been lacking, but real edvance was retarded by the fact that, up to the latter part of the nineteenth century, the causes of the phenomena were sought without rather than within the earth itself. Geology was not seriously called upon for aid in solving the problems. The modern science of seismology is generally held to have had its beginning with the publication, in 1862, of Robert Mallet’s great book upon the so-called Neapolitan, or better Basilicata, earth- quake of 1857. Mallet, however, approached his task with the pre- conceived idea that earthquakes were always caused by subterranean explosions, and his observations and deductions were warped ac- cordinigly. The science received its real start from Eduard Suess, when he published in 1874" his brilliant generalization showing the intimate association of more than forty Austrian earthquakes with the already well-known Kamp, Thermen and Murz fault lines near Vienna and postulated crustal movements as an important cause of seismic disturbances, thus combatting the “centrum” theory of Mallet and others. Suess followed this paper with a still more im- portant paper? the next year along the same lines showing the inti- mate relation of the great earthquakes of southern Italy and Sicily to the fault zones of the region. Impetus was added by the publi- cation of the illuminating treatise of Rudolph Hoernes® in 1878, in which earthquakes were first definitely classified into (1) those due to the collapse of the roofs of cavities within the earth’s crust, (2) those resulting from explosions connected with volcanic eruptions and (3) tectonic quakes, or those caused by crustal movements along fault planes or due to other effects of the action of mountain- 1“ Die Erdbeben Nieder-Oesterreichs,’ Denkschr. k. Akad. Wiss., Wien, XOX A Dth we ps Om 1874: 2“ Die Erdbeben des siidlichen Italien,” id., XXXIV., Abth. I, p. 1, 1875. 3 Jahrbuch d. k. k. Geol. Reichsanstalt, XXVIII., p. 387, Wien, 1878. 1909.] THEIR. CAUSES AND EFFECTS. 237 building forces. Many others in Europe, Japan and America have contributed to the advance of seismology, but particular mention should be made of the services of Professor John Milne, of England, whose long residence in Japan and intimate study of the earthquake phenomena of that and other uneasy regions have enabled him to contribute more than any other one person to the advance of the new science. The perfecting of instruments for the purpose of recording movements of every kind in the surface of the earth has vastly extended our knowledge of the character of earth vibrations and enhanced the value of deductions affecting the theory of earth- quakes. The instrumental study of earthquakes by means of seis- inographs, however, can hardly be said to antedate the year 1892, but within the past decade and a half the number of fully equipped earthquake stations has vastly increased, the growth having been considerably accelerated through the interest aroused by the dis- asters of the last three years. There are now in Great Britain and her colonies fifty seismographic stations equipped with the same type of instrument, while in all the world there are more than two hundred stations equipped with instruments capable of recording world-shaking earthquakes. More than half of these stations are in Europe. No large part of the surface of the globe seems to be entirely stable, but certain regions or zones are much more liable than others to the occurrence of earthquakes. If we study a map of the world upon which their location has been plotted, we find in the eastern hemisphere a broad belt of seismic activity extending from west to east through the Mediterranean Sea, Persia, the southern Himalayas and the Sumatra-Java group of islands. A branch zone stretches from the southern end of the Caspian Sea northeastward half way across Asia. This is de Montessus de Ballore’s “ Alps-Caucasus- Himalayas” belt and it has furnished more than 53 per cent. of recorded shocks. A seismic belt practically encircles the Pacific Ocean, the principal points in it being the Japanese Archipelago, Alaska, California, Southern Mexico and Central America and the *F. de Montessus de Ballore, “Les tremblements de terre,” p. 24, Paris, 1906. 238 HOVEY—EARTHQUAKES: [April 24, northern and southern Andes. This “ Circum-Pacific” or ‘“ Andes- Japan-Malay ” belt has given 41 per cent. of the quakes. In the western hemisphere in addition to a part of the circum-Pacific belt, there are the West India Islands and the mountains of Venezuela forming a seismic zone. Earthquakes mostly of volcanic origin have visited many of the islands of the South Seas. The major portions of Africa and South ‘America remain blank upon such a map, probably because little is known about their seismicity. We are in the habit of thinking of eastern North America as a region free from earthquake shocks. The impression, however, is erroneous, since New England has experienced about 250 recorded shocks since the Pilgrims landed at Plymouth, and there have been at least four great earthquakes in the eastern half of the continent within the past two and one half centuries, one on the fifth of Feb- ruary, 1663, which affected the St. Lawrence Valley over an area more than six hundred miles long and three hundred miles wide as described in the “ Jesuit Relations.”® In 1811-1812 heavy quakes occurred in the central part of the Mississippi Valley, accompanied with considerable subsidence fifty miles south of the junction of the Ohio and Mississippi Rivers. Strong shocks continued for more than a year and evidence of the sinking still persists in lakes and submerged trees. The southeastern part of the United States was the center of an earthquake shock January 4, 1843, the waves of which were felt at points at least eight hundred miles apart. In 1886 occurred the Charleston earthquake, an event still fresh in the minds of most of our population. As to earthquakes of the several classes, the falling in of the roof of a buried cavity causes slight shocks. Quakes of this kind have often been reported from certain parts of Switzerland, the Tyrol and elsewhere, but all have been local in character. It seems certain too that the blocks falling in the caverns of southern Indiana and Kentucky produced vibrations sensible on the surface, but re- ports of such have not come under my eye. Earthquakes arising from volcanic explosions or associated with eruptions form a much more important subdivision. Until within *W. H. Hobbs, “ Earthquakes,” p. 315, New York, 1908. °H. D. Rogers, Am. Jour. Sci., I., XLv., 342, 1843. 1909.] THEIR CAUSES AND EFFECTS. 239 J thirty-five years, indeed, it was the general belief that volcanic earth- quakes were by far the most numerous and destructive of all. This idea controlled and vitiated Mallet’s work, but it is now known to be erroneous, for although it is true that earthquake zones coincide in part with belts of volcanic activity, shocks are more frequent and more severe in non-volcanic regions. The severest quakes of South America have not happened around the great volcanoes; the shocks of California are evidently independent of the now extinct or at any rate dormant volcanoes of the Cascade Range; the recent (1899) great earthquakes of Alaska were in the vicinity of Yakutat Bay, at a long distance from the active vents of the Aleutian Islands or any recent volcanicity ; the earthquakes of Japan are most numer- ous and severe in the non-volcanic parts of the islands; the great disasters of the Caribbean Sea have occurred in Jamaica and at Caracas, hundreds of miles from Mt. Pelé and St. Vincent’s Sou- fricre, and have not been contemporaneous with any eruptions. On the other hand, some of the most violent of historic volcanic eruptions have been unattended by severe earthquakes or have given rise to shocks of merely local significance. The Island of Mar- tinique in the French West Indies lies within a markedly seismic zone, but the great eruptive activity of 1902-1903 was free from earthquake shocks. This fact is of particular interest, because the eruptions were of the most highly explosive character. Although, however, no vibrations were felt upon the island of Martinique and no subterranean noises were heard there, dull sounds like the boom- ing of distant cannon were heard the morning of the great eruption of May 8, 1902, at Caracas, Venezuela, 450 miles distant, south- west, where people feared that a naval battle was in progress off their coast. Similar booming was reported from St. Kitts, 200 miles northwest of Martinique and from other regions. I myself was on the island of St. Vincent, 100 miles due south of Pelé when the great eruption of June 6, 1902, occurred, and I felt several dull thuds, as if some heavy object had fallen in a neighboring room. The noises seemed to come from beneath the ground, and they were due, in all probability, to subterranean explosions or to the rushing of lava into underground cavities, somewhat on the prini- ciple perhaps of the water hammer. On the island of St. Vincent 240 HOVEY—EARTHQUAKES: [April 24, some observers, indeed, had noted, an increase of seismic shocks for a year or more before the volcano burst into violent eruption in May, 1902. The eruption itself, however, was free from earth- quakes, except apparently for the quivering of the mountain due to the uprush of steam and ejecta through the conduit, just as hap- pens in the chimney of a fire engine under full blast. The chattering vibrations thus set up in the volcano shook a narrow strip of recent beach formation from the west base of the mountain, where the declivity of the shore is considerable. Vesuvius being the volcano that has been most continually and thoroughly under observation throughout its known history, we naturally look to its records for light upon the relation between volcanic eruptions and earthquakes. When this old center, which was not known to the ancients as a volcano, renewed its activity in the year 79, the first phase was a series of earth shocks which in- creased in frequency and severity until the afternoon of August 24, when the eruption actually began. The ground is said to have rocked to and fro like the sea, but we read of no great damage as resulting therefrom even in Pompeii and Herculaneum at the very base of the mountain. The outbreak of 1631 occurred after centuries of repose and was heralded by a half year of earthquakes and terrific noises in the interior of the mountain. This history has been re- peated again and again in greater or less degree, particularly when the eruptions have been of the explosive kind. According to the report of A. Lacroix, violent earth movements shook the cone of Vesuvius during the great eruption of April, 1906, and were felt throughout much of the surrounding region. Whatever effects have been produced have been local in extent and comparatively light in degree. The eruptions of Etna usually have been accompanied by the formation of great fissures in the upper part of the cone, and the opening of these fissures has been accompanied by severe vibra- tions of the surface of the mountain, as has been vividly portrayed by Silvestri in his account of the eruption of 1879, but the shocks seldom affect the mainland of Calabria across the narrow Strait of Messina. Stromboli, the “Lighthouse of the Mediterranean,” — 1909.] THEIR CAUSES AND EFFECTS: 241 often shakes its island, but the disturbances are rarely felt in nearby Sicily. The most violent of all recorded volcanic explosions is that which took place in the Strait of Sunda, August 26-27, 1883, when the volcano of Krakatoa was blown to pieces. This outburst destroyed half the mountain and left soundings of 160 fathoms where part of the cone had formerly stood. It produced sea waves that affected tide gauges half way around the world; air waves that traveled three times around the globe before they ceased to be distinguish- able ; and it threw dust into the air to such a height that it remained suspended for months, but the earthquake shocks produced were strictly local in character and were scarcely felt at Batavia, 90 miles from the crater. Another of the great explosions of modern times was that of July 15, 1888, when the Japanese volcano Bandai-san, extinct for a thousand years, burst into sudden eruption. In the immediate vicinity of the mountain a moderately severe earthquake shock last- ing about twenty seconds was felt at half past seven in the morning. This was soon followed by additional shocks which culminated when the explosion occurred at the surface, but none was felt severely beyond a limited area. Even the eruptions of the Hawaiian volcanoes, Kilauea and Mauna Loa, which are the types of the class of “quiet volcanoes,” have sometimes been accompanied by severe local earthquakes. Many eruptions of Mauna Loa, indeed, have been recorded of which the first indication to the inhabitants of the town of Hilo only a few miles away has been the light seen at night reflected in the clouds from the streams of flowing lava. On March 27, 1868, however, there began a series of earthquakes on the southern flanks of the mountain which increased in frequency and intensity for a week and culminated in one of the most severe eruptions known in the history of the volcano, during which a great fissure opened, dis- charging vast quantities of lava that flowed to the sea. In the words of Dr. Titus Coan,’ who was on the island at the time: 7Am. Jour. Sci., I1., xtvi1., 107, July, 1868. PROC, AMER, PHIL, SOC, XLVIII. 192 Q, PRINTED SEPTEMBER 7, 1909. 242 HOVEY—EARTHQUAKES: [April 24, Meanwhile the whole island trembled and shook. Day and night the throbbing and quaking were nearly continuous. No one attempted to count the sudden jars and prolonged throes, so rapid was their succession. And even during the intervals between the quakes, the ground and all objects upon it seemed to quiver like the surface of a boiling pot. The quaking was most fearful in Kau. . . . The shocks and quiverings cintinued with different degrees of intensity until Thursday, the second inst. [April] ... when, at 4 P. M., a shock occurred which was absolutely terrific. All over Kau and Hilo the earth was rent in a thousand places, opening cracks and fissures from an inch to many feet in width, throwing over stone-walls, prostrating trees, breaking down banks and precipices, demolishing nearly all stone churches and dwellings, and filling the people with consternation. This shock lasted about three minutes. Mr. F. S. Lyman® writes as follows of his experiences at Kau during this disturbance: First the earth swayed to and fro from north to south, then from east ' to west, then round and round, up and down, and finally in every imagin- able direction, for several minutes, everything crashing around and the trees thrashing as if torn by a hurricane, and there was a sound as of a mighty rushing wind. It was impossible to stand; we had to sit on the ground, bracing with hands and feet to keep from being rolled over. The villages on the shore were swept away by the great wave that rushed upon the land immediately after the earthquake. Some observers estimated that more than 2,000 shocks occurred during this period of disturbance. In spite of the violence of this earthquake on Mauna Loa, it was quite local in extent. No damage was done in the northern half of Hawaii even by the heavy shock of April 2. This shock was felt distinctly on the island of Maui, 110 miles distant, for 90 seconds, shaking furniture, pictures and walls and causing small sea waves. At Oahu, 210 miles from the cen- trum, the shocks were slight, and though they occurred in the middle of the afternoon, most of the inhabitants of Honolulu were not aware that an earthquake had occurred. From the human standpoint, the most disastrous of the earth- quakes assigned to volcanic causes is that which occurred at Casa- micciola on the Island of Ischia, July 28, 1883. When it took place there was a large assemblage of people in the theater, which was of stone and collapsed under the shock, killing most of the audience. Only one house in the whole town was left standing and it is esti- mated that about 1,900 people lost their lives in the disaster. In ® Am. Jour. Sci., I., xtvt., 110, July, 1868. 1909.] THEIRVCAUSHS ANDI ERRECTS: 243 Naples, however, only twenty-two miles away, the shock was felt by but few people, and the seismographs in the observatory on Mt. Vesuvius did not record it at all, though the instruments at Rome and Florence showed the passage of some extremely light vibrations. The depth of the focus has been calculated at about a half mile and Casamicciola received the vertical shock. The latest eruption of Mte. Epomeo, Ischia’s great volcano, occurred in 1302. Many other instances of volcanic earthquakes might be cited, but perhaps none within historic times have been more severe than those which have been mentioned. All show extremely restricted areas of disturbance, a fact which indicates a comparatively slight depth for the origin of the shocks and a far smaller expenditure of total energy than is developed in connection with the great tectonic quakes. It must not be overlooked, however, that some earth- quakes, the origin of which is doubtful, may rightly be assigned to a volcanic origin. Furthermore, the intrusion during past geologic time of countless dikes, sills and laccoliths of igneous rock, the occurrence of which is known from exposures all over the world, must have been accompanied by sudden dislocations, causing earth- quakes. Such quakes would be of combined volcanic and tectonic origin. It cannot be asserted positively that they are not occurring at the present epoch. This brings me now to the consideration of the third and most important class of volcanoes, viz., tectonic quakes, or those which are caused by dislocations in the earth’s rock crust due to the action of mountain-building forces. Mountain regions of high geological antiquity, like the Appalachian protaxis and the Scandinavian Peninsula, have had time to adjust themselves to the crustal strains due to their elevation and hence are rarely the scene of great earth- quake shocks. In the younger mountain systems, however, such as the Apennines, the Japanese archipelago, Central America and those of California, where young strata abut unconformably against old, the adjustment to strains is still going forward, the cumulative effect being followed by sudden and irregular release of pressure, producing the vibrations which we know as earthquakes. Some of these tectonic quakes have sensibly affected enormous areas. That of Lisbon, 1755, was felt from northern Africa on the south to 244 HOVEY—EARTHQUAKES: [April 24, Scandinavia on the north and to the east coast of North America on the west, an area estimated by Baron von Humboldt at four times that of the whole of Europe. The Andean earthquake of 1868 shook severely a strip of country 2,000 miles long. The modern seismographs have given pronounced records of earth- quakes whose origin was certainly not less than 8,000 miles distant— truly world-shaking events. The depth of the origin of the shocks below the surface of the earth probably never exceeds thirty geographical miles and usually is not more than from five to fifteen miles. The geological struc- ture of the region through which the earth waves are propagated affects the rate of advance of the same earthquake in different direc- tions and produces many changes in the direction of movement and great differences in the destruction wrought upon buildings. Heavy earthquake shocks are transmitted through the earth at a greater velocity than light ones and the same shock shows different rates in different materials. In the case of distant quakes three disturbances are recorded instrumentally. The first set of waves to arrive comes on a direct course through the earth’s mass; the second set comes along the shortest route on the surface, while the third set arrives by the opposite and longest surface route. The last are comparatively feeble, and they may arrive three and one half hours behind the second set. The first set of waves, those coming through the earth, are propagated with the greatest velocity, which is practically uni- form and is about ten kilometers (6% miles) per second. These direct waves have been shown by Marvin to be longitudinal in character, and this character combined with their velocity is sup- posed to cause them to give out the musical sounds which are the premonitory rumblings of an earthquake. The second set are the surface waves due to the “ principal portion”’ of the earthquake, and the increased use of delicate instruments of measurement has led to the acceptance of 3.3 km. per second as their normal rate of propaga- tion. The determination of these various velocities leads to the conclusion that the crust of the earth is practically uniform in con- stitution to a depth of at least thirty miles. The duration of an earthquake and the number of shocks in it 1909.] THEIR CAUSES AND EFFECTS. 245 vary indefinitely. The Charleston, San Francisco, Kingston and many other quakes lasted only from thirty to forty seconds. Milne states that the average duration of 250 earthquakes of moderate intensity recorded by instruments in Tokyo between 1885 and 1801 was 118 seconds. The first shocks are almost always succeeded by after shocks which may continue for weeks, months or even years. It has not been possible yet to determine the periodicity of shocks or to predict with any degree of accuracy the time of the occurrence of an earthquake. Some earthquake regions are subject to frequent shocks, while others experience them only at long intervals. The frequency of earthquakes, considering those of all amplitudes, is not generally realized. The globe, indeed, may be said hardly ever to be free from seismic disturbances of some kind somewhere, since the average of all recorded shocks, according to de Montessus de Ballore, is more than fifteen per day, and there are between fifty and sixty heavy shocks per year. The bare enumer- ation by this author of those occurring in 1903 alone fills a book of six hundred tabulated pages, and he has compiled the data and plotted the position of 159,781 earthquakes that have been recorded up to the end of 1903. At the same time that important quakes are the result of tectonic movements in the earth’s crust, they may themselves be the causes of more or less important changes in the surface of the earth. Sharp waves passing through mountain regions have been known to produce land slides, shatter rocks, displace larger or smaller seg- ments of cliffs, open fissures in the soil or cause subsidence in alluvial regions. Springs, brooks, rivers and lakes have been formed, altered or obliterated as a result of earthquake action. Great earthquakes have usually produced important sea waves caus- ing much destruction along the coast and, sometimes, permanent changes due to erosion and transportation of material. Several scales for the purpose of indicating the severity of an earthquake shock have been proposed. The one most commonly employed is known as the Rossi-Forel scale, which distinguishes ten degrees of intensity according to the effects produced upon human observers and structures. Another widely used scale is that which has been devised by Professor G. Mercalli. This likewise 246 HOVEY—EARTHQUAKES: [April 24, consists of ten degrees of intensity and depends upon human ob- servers and the effects upon buildings for the classification of a shock. On account of the vagueness of these series, the influence of the personal equation of the observer in placing shocks in accordance with them and the over-importance attached by them to effects upon human property, other scales have been proposed, the best of which are based upon instrumental records. Difficulties in using the latter, however, arise through the small number of instruments actually at work, and the Rossi-Forel and Mercalli scales are still found very useful, particularly in the collection of data. I shall close what I have to say regarding the subject of the afternoon by brief descriptions with illustrations of the earthquakes that occurred at Charleston, S. C., in 1886, at San Francisco in 1906, at Kingston, Jamaica, in 1907, and at Messina in 1908. THE CHARLESTON EARTHQUAKE. The most important earthquake occurring in the eastern part of North America during the historic period was that which de- vastated Charleston, South Carolina, in 1886. This was investigated under the auspices of the United States Geological Survey by Major Clarence E. Dutton and his assistants, their report being published in the Ninth Annual Report of the survey. About eight o’clock in the morning of August 27, 1886, the villagers of Summerville, 22 miles northwest of Charleston, S. C., were startled by the noise and shock of what was at first thought to be a heavy blast or a boiler explosion. The sound seemed very near, but no cause for it was learned that day. Around five o’clock the next morning the noise and shock came again and more heavily, and the idea that an earthquake had occurred became general and was strengthened by light tremors that were felt that day and the next. The affair seemed then to be over, for nothing unusual was heard or felt on the thirtieth and during daylight of the thirty-first. The noises or shocks were felt by very few people in the city of Charleston, but they were the premonitions of the great earthquake 1909.] THEIR CAUSES AND EFFECTS. 247 that began at 9:15 P. M. of the thirty-first. In the words of Dr. G. E. Manigault, a resident of Charleston, as quoted by Dutton :° Although the shocks at Summerville excited uneasiness in Charleston, no one was prepared for what followed. . . . As the hour of 9:50 was reached there was suddenly heard a rushing, roaring sound compared by some to a train of cars at no great distance, by others again to an escape of steam from a boiler. It was followed immediately by a thumping and beating of the earth underneath the houses, which rocked and swayed to and fro. Furniture was violently moved and dashed to the floor, pictures were swung from the walls and in some cases completely turned with their backs to the front, and every movable thing was thrown into extraordinary convulsions. The greatest intensity of the shock is considered to have been during the first half, and it was probably then, during the period of the greatest sway, that so many chimneys were broken off at the junction with the roof. The number was afterwards counted and found to be almost 14,000. Apparently there were two maxima, the first of ten seconds duration, the second of six, with an interval of comparative quiet of 22 to 24 seconds. The whole period to be assigned to this destructive double shock is about 68 seconds. Another observer states that four severe shocks occurred before midnight and that three others followed at about 2, 4 and 8:30 o'clock A. M.1° Afterquakes occurred for months. Twenty-seven persons were killed outright and at least 56 more died from injuries received and exposure suffered. The money value of the property destroyed was estimated for Charleston alone at between $5,000,000 and $6,000,000. Not a building wholly escaped injury. Damage to buildings was greater on the low made ground than on the natural higher parts of the city. The occurrence of visible surface waves was so definitely as- serted by so many observers and with such detail of description that the fact of their formation cannot be discredited. The pass- ing of such waves has often been included in the description of earthquakes, but their actual existence had been doubted, on account of the difficulty of explaining their origin. The amplitude of the surface waves in some parts of Charleston is estimated by Dutton at nearly or quite a foot and the average amplitude for the city at three or four inches. * Ninth Annl. Rept. U. S. Geol. Survey, p. 231. Washington, 1889. a (Op ths pe 217. 248 HOVEY—EARTHQUAKES: [April 24, Besides throwing down walls and chimneys and moving houses bodily on their foundations, the earthquake caused wooden posts and brick piers to sink vertically into the earth; compressed railroad tracks into more or less complicated curves or stretched them apart; opened innumerable fissures in the ground, and formed hundreds or craterlets at many places out of which gushed water, sand and mud in copious streams. The earthquake waves traversing Charleston were localized as coming from the northwest and from the west. The principal epicentrum was determined as being about sixteen miles northwest of the city and one mile from the little railway station at Woodstock, and a secondary epicentrum about fourteen miles due west of town. The focus of disturbance was a line or plane estimated as being ‘ twelve miles below the surface “ with a probable error of less than two miles.” The velocity of the wave motion throughout the eastern half of the United States was calculated as averaging 190 miles per minute. The intensity reached No. 2 of the Rossi-Forel scale as far away as New Orleans, Clinton, Mo., La Crosse, Wis., Saginaw, Mich., Burlington, Vt., and Boston—an extreme radius of about 1,000 miles. The Charleston earthquake is classed as a tec- tonic quake, though no evidence of faulting was apparent on the surface. (Lantern slides were shown depicting the destruction of build- ings in Charleston and vicinity and the formation of fissures and craterlets. ) THe SAN FRANCISCO EARTHQUAKE. California has always been known as a seismic region. Pro- fessor E. S. Holden has catalogued 514 shocks, 254 of which affected the region of San Francisco alone, within the period between 1850 and 1886. During the nineteenth century there were ten severe quakes; that of 1868, known as the Mare Island quake, having such a disastrous effect upon the city of San Francisco that serious doubts were entertained of the advisability of rebuilding on the same site, but these fears were soon forgotten and the city rapidly rose again. It was rebuilt, however, without much reference to the lessons that might have been learned from the experience. 1909.] THEIR CAUSES AND EFFECTS. 249 In the Sierra Nevada, forming the eastern half of the state, earthquakes are likewise frequent. In 1872 occurred the great Owens Valley quake, which was one of the most severe on record and was the result of movements producing a series of faults along a line more than 100 miles long with a throw of from ten to twenty feet. This mountain system is formed of Precambrian granites, gneisses and schists, upon which have been laid down upon the west an unconformable series of late Paleozoic and Mesozoic strata. The coast ranges, in which the earthquakes occur with far greater frequency, are composed of a granitic core against which rest ex- tensive Mesozoic and Cenozoic strata upon which are thick marine Pleistocene and recent beds. The latter are full of the fossil shells of still living species of mollusks and show that elevation is still going forward in California. The San Francisco Peninsula is traversed by at least five known lines or zones along which movement, or faulting, has occurred again and again. The principal of these zones is the San Andreas, which takes its name from an important lake through which it runs. It is likewise known as the Stevens Creek fault, as the Portola-Tomales fault or more simply as “the rift.” This zone con- tinues northwest in a slightly curved line to Point Arena and south- east to the mountains west of Hollister. This is the continuous extent of the fault, some 190 miles, but it probably extends under the ocean beyond Cape Mendocino to the north and into the moun- tains southeast of the line recently disastrously affected.1t Accord- ing to H. W. Fairbanks’? the recognized rift extends from Shelter Cove, Humboldt County, as far southeastward as the Colorado desert and is 700 miles long. Dr. Fairbanks states further that the great Tejon earthquake of 1857 was caused by movement in the same fault zone. The recurrence of horizontal and vertical movement along the northern 200 miles of this fault line caused the earthquake which at 4“ The California Earthquake of 1906,’ by David Starr Jordan and others. G. K. Gilbert, map, p. 317. San Francisco, 1907. 2“ The California Earthquake of 1906,” pp. 321-337. See also “ Report of the California State Earthquake Investigation Commission,” by A. C. Lawson, chairman, p. 48. Washington, 1908. 250 HOVEY—EARTHQUAKES : [April 24, 5:12 o’clock A. M., western time, April 18, 1906, wrought ruin or serious damage over a belt 50 miles wide and 300 miles long. The approximate position of the epifocal point of the disturbance is given by F. Omori as being in latitude 38° 15’ N. and longitude 123° W., near Tomales Bay.*? The horizontal shearing movement varied from nine to twenty feet toward the N.N.W. or the S.S.E.; the vertical movement did not exceed two feet at any locality and usually was absent, upthrow where present being on the west side of the rift. Among the effects along the line of the fault were rifting and bulging of the soil, offsetting of fences, roads and walks, splitting and overturning of trees, landslides in the mountains, wrecking of railway tunnels, spreading and telescoping of lines of waterpipe. This is the most disastrous earthquake that has visited the United States, though the chief destruction wrought was due to the fire that followed in the train of the quake rather than to the shock itself. About four hundred people are known to have lost their lives in the catastrophe, and at least $350,000,000 worth of buildings and other property were ruined by the shock or consumed by the flames. An exact statement of the pecuniary loss caused by the shock cannot be made, but the insurance companies finally agreed upon a settlement to the effect that one-fourth of the damage was due to the earthquake and three-fourths to the fire, and this esti- mate may be accepted as the best that can be made. More than four square miles of the city of 400,000 inhabitants was devastated. The main part of San Francisco lies about eight miles northeast of the fault line, and the propagation of the waves through the city was in a direction N. 76° E., nearly normal to the fault line. In general the advance of the wave motion on each side of the rift was away from it. Omori concludes that both sides of the fault line were displaced toward the N.N.W., the west side more than the east, the amount of apparent slip being merely differential. In San Francisco the chief damage was wrought upon structures built upon alluvial or made ground. High steel-frame structures which were not stiffly braced acted like inverted pendulums, causing ruin to their walls. This was illustrated in the case of the City Hall in San Francisco and the library buildings at Stanford University %“ The California Earthquake of 1906,” p. 280. 1909.] THEM CAUSES ANDTERFEFECTS: 251 and the City Hall at Santa Rosa. The main source of the earth- quake is thought to have been situated at a considerable depth below the surface (Omori). (Lantern slides were shown to illustrate the destruction of buildings in San Francisco, Santa Rosa and Leland Stanford Jr. University, and the geologic and topographic changes wrought in the surface of the ground along the line of fracture.) THE KINGSTON EARTHQUAKE. The Blue Mountains, rising 7,400 feet above the level of a sea 18,000 feet deep, form the back-bone of the island of Jamaica. They trend northwest-southeast and, according to Robert T. Hill,1* from the earliest axis of folding now apparent. Upon this have been super-imposed later east-west flexures corresponding with the crustal movements that early in the Mesozoic era determined the chief characteristics of the Greater Antilles. Charles W. Brown, reports observing “transverse faults in the Blue Mountain region which undoubtedly indicate lines along which fractures may occur.” Professor Hill assumes an east-west axis of folding with an anti- cline producing the trend of the Greater Antilles and leaving a parallel syncline coinciding with the Bartlett Deep just north of Jamaica. Such strong relief coupled with folding indicates a high state of tension in the earth’s crust. Resistance to stress is diminished on steep slopes, especially when the application of pressure to the ends of an axis is not made in the same plane, giving rise to torsional strains. Fracturing results, tending to follow old fault planes, and these fault planes were originally determined by zones of weakness in the rocks. Fracturing, as we have seen, produces earthquakes. Montessus de Ballore acquiesces in the folding postulated by Hill and embraces the Greater Antilles, including Jamaica, within the great Alpine geosynclinal. The region experiences frequent shocks and one of the most dreadful disasters of modern times occurred within it in the year 1692, when, as a result of an earthquake, the greater part of Port Royal, the capital of Jamaica, sank into the “ Bull. Mus. Comp. Zool., Vol. XXXIV., p. 164. * Popular Science Monthly, Vol. LXX., p. 385, May, 1907. 252 HOVEY—EARTHQUAKES: [April 24, ~_ sea. The city was built upon a narrow sand spit formed of the detritus brought down by rivers from the mountains of the interior or cast up by the sea. It is estimated that 2,000 people lost their lives in this disaster, when a tract of land about a thousand acres in extent sank so as to lie thirty or forty feet under water. After the destruction of Port Royal the city of Kingston was established on the gradually rising Liguanea plain across the harbor from the old capital, and it flourished for 215 years, becoming a compact city of 60,000 inhabitants. Its business portion extended along the water front and was only twelve blocks long and two wide. The city was built, however, upon unconsolidated gravels and sands —alluvial and coast deposits that gave a foundation but little more secure than the sand spit gave to old Port Royal. Hence when the earthquake of January 14, 1907, occurred, 85 per cent. of the build- ings in the city was injured or destroyed, and fire completed the ruin over ten or fifteen blocks of the business and warehouse section. The shock probably began at 3:33 P. M., though an exact state- ment cannot be made through lack of accurate standard time in the island. This defect as to time has made it impracticable to plot any coseismal lines. The first series of vibrations, the great shock, lasted 35 seconds, more or less, but the duration varied with the position of the observer. The longest period was reported from the north shore and as being go seconds. After the preliminary tremors, which were heard before they were felt, the shock was double, the first maximum being reached in about ten seconds, followed by a second and less acute climax before the vibrations ceased. The in- terval between the preliminary tremors and the main shock was almost insensible. After shocks occurred for several months. Through the city of Kingston and its immediate vicinity the earth- wave shown by the first climax passed from west to east, but three miles north of town the direction of motion was distinctly from the south, while in the Hope River valley five miles east of the city, the advance was from the northwest. The earthwave recorded by the second maximum of shock was more undulatory in character than the first and seems to have originated more to the south of the city. This direction of motion combined with the first produced a twisting counter-clock-wise movement of slender upright structures 1909.] THEIR CAUSES AND EFFECTS: 253 like statues, columns and chimneys and had a noticeable effect on buildings. According to Professor Brown: The dip of the angling cracks at Kingston points to a locus of dis- turbance much to the west of that city, while the lines of isoseismals indicate the intensity area to be in the eastern half of Kingston. . . . The only conclusion then is that the eastern end of the Liguanea plain was the nearest area to the real epicenter that by nature of material would give the greatest amplitude to the destructive epifocal waves. Further, the angle of emergence at Kingston codrdinated with the proximity of a probable epicenter together with the limited area of disturbance indicates a shallow origin of about three miles. As is demanded by theory and observed in fact the vibrations increase in violence on passing from an elastic to an inelastic medium—the destruction wrought in Messina, San Francisco and other places has been worse in the sections built upon alluvial or other loose soil than in those built upon rock, and Kingston was entirely upon such loose material. The experiences of these and other regions show that the destructiveness of an earthquake is not necessarily greatest in the epifocal area. If the locus of disturbance is in or under an elastic rock-mass and the shock is propagated into a region of inelastic loose material, the destruction in the latter may exceed that in the real epicenter. The fault which was the locus of the San Francisco quake is some miles from the city. The shock of the Kingston earthquake was not sensible on the island of Haiti to the east or on Grand Cayman to the west, but Santiago de Cuba, 120 miles to the north, felt it slightly. This in- dicates an ellipse as being the generalized form of curve for the isoseismals, with the longer axis extending approximately north and south. At Annotta and Buff Bays on the north shore of Jamaica, opposite Kingston, the destruction wrought was almost as severe as at the capital city. The inference is that renewed faulting along north-south fault lines caused the earthquake. The building construction of Kingston was as bad as the founda- tion upon which the city rested. Brick structures predominated, but for the most part it was evident that the brick had been laid dry in poor mortar. Such buildings collapsed under the shock. Those that were properly put together withstood the quake better. Wooden houses with good braces and well fastened together were not thrown 254 HOVEY—EARTHQUAKES: [April 24, down. Massive walls showed cracks from half an inch to two inches wide. The double amplitude of the wave motion of the earth is estimated at not more than one inch. Such an amplitude is small when compared with the four-inch amplitude calculated by Omori?® for the earthwave of the San Francisco (1906) quake, the 6 to 12-inch amplitude estimated by F. A. Perret!’ for the earthwave at Messina in last December’s quake, or the one foot maximum ampli- tude given by C. E. Dutton’® for the Charleston earthquake wave. These largest estimates were derived from effects in soft ground and are probably excessive. From a geological standpoint the movements causing the King- ston earthquake were less important than the changes in the earth’s surface that were produced by it. Surface evidence of the former has not yet been discovered, but the latter are quite apparent. Be- ginning in the city water front, a belt of fissuring and subsidence skirted the eastern half of the harbor and returned along the inner (northern) base of the Palisadoes. Opposite the city the zone of disturbance forked, one branch maintaining the original direction and passing through Port Royal, while the other curved north- westward touching Ft. Augusta and dying out in the River Cobre valley, eight to ten miles northwest of town. From soundings taken for Professor Brown, it was learned that “in several places along the edge of the harbor the bottom had sunk from old soundings of a fathom and a half to over six fathoms, and that on the harbor side of the base of the Palisadoes a series of step faults reached a maximum depression at the shore to the north of four fathoms.” Port Royal sank from 8 to 25 feet. The zone of disturbance was from 100 to 300 yards wide, contain- ing where exposed many fissures and craterlets out of which water, sand and mud gushed to heights of three or four feet. The fissur- ing was caused by the compression and expansion of the earth due to the passage of the earthquake wave, but the cause of the sub- sidence is not clear, for the harbor as a whole did not sink—only an encircling belt. Perhaps solution of the soft limestone where *“ The California Earthquake of 1906,” p. 307, 1907. Am. Jour. Sct., 1V., xxvu., 327, April, 1900. *® Ninth Annual Rept. U. S. G. S., p. 269. Washington, 1880. 1909.] THEIR CAUSES AND EFFECTS. 255 the ground waters enter the harbor left caverns into which the overlying material was shaken by the quake (Brown). No sea wave of importance accompanied or followed the shock. (A series of lantern slides was used to show the destruction caused in the city, the sinking of Port Royal point and the faulting, fissuring and formation of craterlets along the Palisadoes.) THE Messtna-ReGccio EARTHQUAKE. Time after time during the historic period Italy has suffered from the effects of serious earthquakes, but never before so severely as from that which occurred in Calabria and Sicily on December 28, 1908, when 200,000 human beings are supposed to have lost their lives. The cities of Messina in Sicily and Reggio in Calabria were completely wrecked, and many other villages and towns were laid in ruins or damaged throughout an irregularly elliptical district 85 miles long by 50 miles wide, extending from Pizzo, Calabria, on the northeast to Riposto, Sicily, at the sea base of Mt. Etna, on the southwest. The epifocal area was the Strait of Messina, with the epicentrum at or near the northern end of the Strait. More precisely, the longer axis of the ellipse of greatest destruction (from Ali to Palmi, about 35 miles), as shown by isoseismals, lies in the strait and runs N.N.E-S.S.W. Calabria and northeastern Sicily form a district of extreme seismicity that has been visited by several disastrous earthquakes, among which those of 1783, 1785 and 1905 stand out with prom- inence on account of their destructiveness to human life and prop- erty. Volcanic quakes have been associated with eruptions of Mt. Etna, but they have been strictly local in effect, and their influence has not been seriously felt across the Strait. All the severe shocks have originated in Calabria or under the Strait of Messina are of tectonic character, the geological structure being particularly favor- able to the production of such quakes. Forming the backbone of Calabria and extending beyond Messina in Sicily there is an elongated area of Archean gneisses and mica schists. Along this axis there occur nearly horizontal beds of Miocene age up to an altitude of 3,300 feet above the sea, while along the Strait of 256 HOVEY—EARTHQUAKES: [April 24, Messina there runs a fault with thousands of feet of throw, the uplift being upon the Calabrian side of the Strait. Movement ap- pears to be still going on along this and other fault zones, resulting in repeated earthquakes. Furthermore, the slopes into the sub- marine depths on both sides of the “toe” of Italy are very steep and therefore unstable. Toward the end of 1908 the seismic activity of the region was evidently on the increase, and noteworthy shocks were felt No- vember 5 and December 10, while F. A. Perret?® reports that at 5:20 A. M., December 27, just twenty-four hours before the occur- rence of the great shock, the seismograph at the Messina observa- tory registered an important earth movement. The observatory was wrecked by the great earthquake, but the instruments had been installed in its cellar and Dr. E. Oddone?® of the seismographic service found them intact and the records intelligible, when he reached the place January 1. These records showed that the quake began at 5:21:15 o'clock A. M., December 28, with a gentle move- ment the force of which increased during ten seconds and then diminished during ten seconds. After two minutes of calm came the great shock, lasting 30 to 35 seconds, which was recorded by seismographs all over the world. This was followed by com- paratively light shocks at 5:45, 5:53 and 9:05 o'clock A. M. of the same day, and by noteworthy quakes at 2:51 and 7:30 o'clock P. M. of the following day. For several days and even weeks minor shocks continued to occur. Some of these “ after-shocks ” were strong enough to add to the damage caused by the principal quake. According to Mr. Perret*! the intensity within the mega- seismic area was between the ninth and tenth degree of the Mercalli scale decreasing rapidly with increasing distance from the epi- centrum, and the centrum was not deeply located, being possibly fifteen kilometers (92 miles) beneath the surface. Messina was a beautiful city stretching for miles along the shore of a magnificent harbor. Lying in an advantageous position on the short cut from the Eastern Mediterranean to the Tyrrhene * Am. Jour. Sci., 1V., XXvIL, p. 321, April, 1909. Ta Nature, XXXVII., 103, January 16, 1909. a BOGHICIE Sapa seke 1909.] THEIR CAUSES AND EFFECTS. 257 Sea, the city has enjoyed prosperity for centuries, in spite of fre- quent visitation from earthquakes. The city was almost com- pletely destroyed by a shock in February, 1783, but the people seem to have learned nothing from their experience with an unstable land. The Messina of yesterday—the city does not exist to-day— was constructed of stone and rubble and old cement. The build- ings lined narrow streets and were three, four and even five stories high with massive walls. Hence when the shock came and raised and then dropped the ground for half a minute, the houses, stores, hotels, churches and government buildings were shaken into un- recognizable heaps of debris, filling the sites of the structures and obliterating the streets. The sea-wall in front of the city was partly destroyed, and the promenade along the harbor sank in places below the water. Reggio di Calabria likewise has suffered frequently from earthquakes, but until within the past few years the inhabitants had not profited by experience to put up earthquake-proof build- ings, and all the old houses in the city were demolished by this latest quake. New houses not more than ten meters (33 feet) high are said to have resisted the shocks perfectly. Throughout the Calabrian earthquake district the buildings erected since the disaster of 1905, according to the specifications of the Milan Com- mittee, are reported to be intact in spite of the severe shaking thus received, but all these are low structures. Photographs show that there was some fissuring of the ground at Messina, and it is reported that “ vast chasms’ both Messina and Reggio, but the latter statement is probably in- 5 were opened at correct. Professor G. B. Rizzo is quoted as stating?* that the sea bottom rose in some places, for he saw several boats out of water at the places where they had been anchored some distance from the original shore. The extensive breaking of telegraphic cables indicates submarine disturbance, but the fact of* any considerable change in the configuration of the sea bottom remains to be proven and can only be established by careful soundings. No changes in the coast line have occurred, as far as can be detected without an 2 Nature, Vol. LXXIX., p. 280, January 7, 1909. PROC, AMER. PHIL. SOC. XLVIII. 192 k, PRINTED SEPTEMBER 7, 1909. 258 HOVEY—EARTHQUAKES: [April 24, instrumental survey. It is stated positively that the ground sank in several places in Messina, Reggio and elsewhere, particularly along the harbor front in Messina and along the sea front and in the center of Reggio; but all the low-lying parts of the two cities were built upon unconsolidated alluvial and shore material, per- mitting, as in the earthquakes of San Francisco and Kingston, severe and destructive oscillations and displacements. As is usual with shocks occurring along or near the seacoast, 9 the earthquake was accompanied by a “tidal wave,” the sea re- treating for a considerable distance and then returning into the strait with growing force. The wave was not at all violent in the deep water of the strait and was of importance only as it came into the shallower water near shore, where it was eight or ten feet high. Its crest swept across the marina, or esplanade, bordering the harbor at Messina two or three minutes after the great earth- quake shock occurred, and some comparatively slight damage is assigned to the water. The wave was somewhat higher at Reggio than at Messina and attained its maximum on the coast south of Taormina (Perret). In Reggio the buildings on the low land along the coast were flooded. The wave injured a few boats at Syracuse near the southeastern corner of Sicily; but it was scarcely perceptible at the Island of Malta, about 165 miles south by east of Messina, where it arrived at 7:15 o'clock A. M. The sea gauge at Ischia, about 190 miles north-northwest of Messina registered maximum oscillations of 22 centimeters (8.6 inches) at 2:30 o'clock P. M. and at 8 o’clock P. M. If the former was due to the quake that destroyed Messina and Reggio at 5:25 o’clock that morning the rate of advance northward was much less than it was south- ward. (A series of slides was shown illustrating the effects of the earthquake in Messina, Reggio di Calabria and Scylla.) THE EVOLUTION AND THE OUTLOOK OF SEISMIC GEOLOGY. (PLates XV AND XVI.) By WILLIAM HERBERT HOBBS. (Read April 24, 1909.) CoNnTENTS. Part I: EvoLuTion oF SErsmMic GEOLOGY. Introduction. The Natural Development of Seismology Prevented by False Theory. The Process of Averaging in Mapping Isoseismals and Coseismals. The Evolution of the Fault-block Theory of Earthquakes. The Relation of Earthquakes to Volcanoes. The Mesh-like Distribution of Volcanic Vents. Volcanic Extrusions in Relation to Block Adjustments. A Possible Explanation of Volcanic Earthquakes. The Conditions of Strain during the Growth of Block Mountains. Part Il: Tue OvutiLook or Seismic GEOLOGY. The Ultimate Cause of Earthquakes. Earthquake Forecasts. Periodicity of Earthquake Cycles. Possibilities of Future Prognostication. Need of Expeditionary Corps. A Service of Correlated Earthquake Stations. Preparation of Maps of Fracture Systems. Maps of Visible Faults and of Block Movements for Special Earthquakes. Rate of Mountain or Shore Elevation by Quantitative Methods. Investigation of Earthquake Waterwaves. Conclusion. Part I: THe EvoLuTIon oF SEISMIC GEOLOGY. Introduction—Speaking generally, the present condition of a science is so largely the consequence of an evolution by slow stages, that if the past be reviewed the present stands revealed. Zodlogy, which began with the encyclopzedists as a descriptive science, passed into the comparative stage with the advent of Cuvier, and entered 259 260 HOBBS—THE EVOLUTION AND THE [April 24, upon its fruitful genetic period when the modern view-point was given it by Darwin. Looking back upon this evolution, we note that the order is in every way a natural one. The facts of observa- tion should first of all be assembled; they must next be compared with a view to establishing correspondences, and, finally, the explana- tion of the correspondences must be sought in genetic relationships. Of geology it may be said, that the natural order of*its evolution was exactly reversed; for the genesis of the earth and the full order of events in its history had supposedly been given to man through divine revelation. The growth of the science began, therefore, only after a measure of emancipation from the tyrrany of religious dogma had been achieved. The Natural Development of Seismology Prevented by False Theory—It may well be doubted if there is another branch of science which has been so long held in fetters by false theory as the branch of geology which treats of earthquakes. Had fate been more kind, it might have been the earliest to develop; for the seats of ancient culture were in earthquake countries, and it will hardly be claimed that the phenomena of earthquakings are not such as to attract the attention. Theories of cause do, indeed, date back before the beginning of the Christian era, the dominating one being that of Aristotle which connected the quakings with explosive sources of energy, conceiving that gases confined in subterranean cavities brought on quakings in their struggles to escape. For the times, this theory seemed to be well supported by facts, since earthquakes were generally manifested at the time of great volcanic eruptions, and volcanoes and earthquakes were common to the same countries. The Aristotelian theory of earthquakes acquired prestige from the adhesion to it of Strabo and Pliny among the ancient philosophers, and at the opening of the nineteenth century, through its adoption by von Humboldt and von Buch, who then dominated the field of geo- logical thought. The middle of the nineteenth century is a turning point in the history of nearly all sciences toward a greater exactness of ob- servation. Academic discussions in large measure gave place to careful and painstaking observation or to laboratory experimenta- tion. Yet almost at the moment when Darwin and Huxley were 1909.] OUTLOOK OF SEISMIC GEOLOGY. 261 opening a new world to students of biology, the way to progress in seismology was effectually closed through the commanding authority of a pseudo-scientific work of great compass, written by the English physicist, Mallet. Darwin’s great theory was an induction reached on the basis of extended observations and!of meditations with an open mind; Mallet, on the other hand, approached his work firmly intrenched in a preconceived notion which the facts were assiduously, though perhaps unconsciously, twisted to confirm. Assuming that Mallet’s method had been a sound one, his elaborate observations conclusively proved the fallacy of his theory; for instead of pointing to a definite centrum, his results ranged with noteworthy uniformity between depths of 10,000 and 45,000 feet. The history of science furnishes no more striking example of a great monograph wrought out with laborious scientific method and yet absolutely lacking in scientific spirit or judgment, for with a naive simplicity Mallet drew from his results the conclusion that, “the probable vertical depth of the focal cavity itself does not exceed three geographical miles, or 18,225 feet, at the outside.” Nowhere in the two bulky volumes of his report is the possibility of a non- existence of the centrum even raised. As was true of the famous fallacy of Werner concerning the origin of basalt, it was here the commanding position of the author which gave his theory its authority; and, although the impractica- bility of his method soon came to be generally recognized, the funda- mental idea was destined to survive at least half a century as the standard doctrine of seismology. It was the brilliant system of Huyghens for treating the propagation of wave motion carried over bodily to seismology, which caused it to be so warmly welcomed by physicists and elasticians, to whose care this branch of science was thereafter entrusted. As late as 1899, the depth of the imaginary origin of a particular earthquake was sought by no less than four different methods with results which ranged from 21 kilometers on the one hand to 161 upon the other, these results apparently not shaking the worker’s faith in the reality of the earthquake focus. It becomes ever more clear that men of science discover in the main those facts only which their working hypotheses indicate to be important. For this reason a theory which is largely correct, grows 262 HOBBS—THE EVOLUTION AND THE [April 24, by elimination of the false and augmentation of the true, whereas a theory essentially false yields nothing, and by discouraging effort bars the way to progress. With the aid of mathematics and by an abundance of exact observation, the more or less occult Aristotelian theory was by Mallet clothed in a modern dress and thus made respectable in the company of the modernized sister sciences. The cause of the earthquake disturbance was by the very nature of the theory hidden so deep beneath the earth’s surface as to be removed from direct observation, and was, therefore, a matter suitable only for speculation. . At the opening of the twentieth century, almost fifty years after Mallet had modernized the theory of Aristotle, authors of text- books of geology quite generally disposed of the subject of earth- quakes by a treatment of the outlines of the Mallet theory in the compass of a few pages. How generally the investigation of earth- quakes was excluded from the field of research in geology is strik- ingly shown by the activities of the United States Geological Survey, a bureau employing the largest staff of working geologists of any in the world and including in its field subjects as diverse as paleon- tology and mineral resources. In the years 1868, 1872, 1886 and 1887 earthquakes of the first magnitude wrought damage to property within the national domain, and with one exception no effort was made by the national bureau to investigate these phenomena, and but little by independent geologists. Since the intellectual shock from the California earthquake of 1906, individual geologists have begun to take advantage of this opportunity for study, even though the golden opportunity had already passed. The Process of Averaging in Mapping Isoseismals and Coseis- mals.—Aside from its occult and speculative basis, which removes it from the reach of direct observational studies, the centrum theory has yet assumed to adopt the observational method of modern sci- ence. The isoseismal and coseismal lines which belong to the Mallet conception of an earthquake centrum must be obtained through averaging the results of observation either of the intensity of the shocks or of the time of their arrival. In how far it has been nec- ‘adjust’? data in order to make the circular or elliptical curves concentric about the epicenter and represent uniformly de- é essary to 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 263 creasing values as they recede from it, one who has not compared the individual data will scarcely believe. A local intensity which is too large can be explained either by a soft or a wet basement, by an earthquake “bridge” or by probable error of observation; while one too small may be explained by an earthquake “ shadow,” by an interference of waves, etc. Many curiously anomalous data not possible of explanation on any of these grounds may be dismissed as “ earthquake freaks.” As regards time of arrival of shocks, “too early” or “ too late” data have not uncommonly been included among those which seemed a priori the most reliable. Especially good examples of such data are furnished by the studies of the Agram earthquake of 1880, the Andalusian earthquake of 1885, the Charleston earthquake of 1886, and the Indian earthquake of 1887. Out of 260 time data collected by Dutton in connection with the Charleston earthquake, 47 were Zejected as .; too early: To average the determinations of an unvarying value in order to eliminate the errors of observation and experiment, is indication of a desire to secure accuracy which must be commended as eminently scientific in its nature; but to average the values of a property the distribution of which either in space or in time is likely to be sig- nificant, is, on the contrary, one of the most pernicious, as it is one of the most common and unconscious methods. Such a practice is often condoned on the ground that the data may otherwise appear to possess an accuracy beyond what they really have; forgetting, what is far more important, that through the averaging process the data lose their most significant characters. Now that so many sciences are entering upon their quantitative stages it is important that this method be corrected. A companion fallacy to the supposed necessity for averaging data of different values is that nature in all its moods has avoided angles and straight elements in favor of the curving outline, and that in consequence results are incorrect in proportion as they bring out strong accent, or definiteness of character, or exhibit straight- ness of contour. Inno field, perhaps, has this fault been more often committed than in topographic mapping, where it has been encour- aged as tending toward accuracy. A new era is dawning, however, ! 264 HOBBS—THE EVOLUTION AND THE [April 24, and the wonderfully improved maps which have been brought out in recent years by the United States Geological Survey and by Euro- pean surveys have been secured through the elimination of the process of averaging and “rounding off” of angles. Significant character is thus taking the place of a lack of expression in the older maps. In a similar way the isoseismals and coseismals, which have assumed to represent the distribution in space and in time of the seismic activity of a district, have through averaging of results removed all true expression of seismic distribution. It is likely, however, that this method will yet, at least for a number of years, effectually retard the natural progress of seismology. The Evolution of the Fault Block Theory of Earthquakes.—It would be incorrect to state that no progress was made in seismic geology during the last half of the nineteenth century, but it would be only the truth to say that such progress as there was, was achieved in spite of and almost in defiance of the orthodox doctrine of seismology. Nine out of ten reports upon special earthquakes made during that period have included only the maps of isoseismal and coseismal lines, to which has been added a computation of the depth of the supposed origin. It is now proposed to trace the development of the tectonic con- ception of earthquakes as it has grown into the fault-block theory of the present day. To the Austrian school of geologists and to its leader, Eduard Suess, must be credited the pioneer work upon the geology of earthquakes. The discovery of the localization of heavy shocks along definite lines, or the recurrence of epicenters (surface loci of heavy shocks) along such lines, has been a characteristic of the Austrian method, which dates from a paper published by Suess in 1872. Such lines in the surface, generally approximating either to a right or to a broken line, were in some cases identified with the traces of fault planes and in others were shown with much proba- bility to be the course of such displacements. Here, then, was the first important recognition of the tectonic nature of earthquakes, and, as a consequence, the Austrian school of seismologists has since endeavored to examine earthquakes in the light of the geological structure of the affected region. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 265 It must be regarded as quite remarkable that the recognition of this fundamental fact was reached in Austria, for the opportunities offered by the Austrian field were by no means exceptional. In fact, the great surface faults which have been a feature of great earthquakes in other districts, have there been seldom observed. In New Zealand, for example, accompanying a heavy earthquake in 1856, an area of country comprising 4,600 square miles was sud- denly upraised to form a visible escarpment varying from one to nine feet in height. This event was duly described by Lyell, who, in the eleventh edition of his widely read “ Principles of Geology ” reported this and other similar cases apparently without seeing that they throw any discredit upon the centrum theory. In 18841 Gilbert, in a brief note, explained the earthquakes char- acteristic of the Great Basin of the western United States as due to the interrupted jolting uplift of the mass of the mountains by vertical thrust. The stresses tending to uplift the range aided by a fissure already in existence, accumulate until they overbalance the starting friction upon the fissure, when through movement the strain is relieved and the potential energy of the system reduced. In a later note published in 1890? he showed that during the earthquake of 1872 in the Owen’s Valley, California, the ground was moved in strips both vertically and horizontally. In 1893 Kotd, describing the great Japanese earthquake of 1891, in referring to earlier earthquake rents within the same district said: The event of October, 1891, seems to me to have been a renewed move- ment upon one of these preéxisting fissures—the Neo Valley line of fault, by which the entire region lying to the right of it not only moved actually downwards but was also shifted horizontally towards the north-west for from one to two metres along the plane of dislocation. This vertical move- ment and horizontal shifting seem to me to have been the sole cause of the late catastrophe.’ Without the aid of surface faults, Leonhard and Volz, in 1896, expressed clearly the idea that the Silician earthquake of 1895 was the result of an adjustment among orographic blocks or Schollen. Their statement was: *Amer. Jour. Sci., Vol. 27, 1884, pp. 49-53. ?Mon. I., U. S. Geol. Sur., pp. 360-362. 8 Jour. Coll. Sci., Tokyo, Vol. V., 1803, p. 329. 266 HOBBS—THE EVOLUTION AND THE [April 24, We must, therefore, regard the cause of the earthquake of June 11, 1895, as a movement of the Nimpt complex of orographic blocks, which occurred along the southern and eastern fracture margins.‘ The great Indian earthquake of 1897 was thoroughly examined from the geological side with results which seem to have afforded indication of the movement of the ground in individual blocks. This, however, was not the theory adopted by R. D. Oldham, who wrote the report upon the earthquake, apparently for no other rea- son than that it seemed to require an expansion of the affected area. In consequence, the unique hypothesis was offered that the earth- quake was due to a movement upon a thrust plane beneath the affected region. The mental attitude of Dr. Oldham is brought out in the following paragraphs from his report in modification of his choice of theory :* Though apparently the most probable this is not the only possible, hypothesis. The surface features of the Assam range, described in the last chapter, are compatible with, in some respects they suggest, the idea that these hills are what the German geologists call Schollengebirge, that is, mountains which have arisen from straight up and down thrusts, instead of from lateral compression, like the Alps and Himalayas. Jf this be so, the faults by which the fault scarps are formed would be normal faults, and so far from there having been any compression, the elevation of these hills would have been accompanied by an extension of the surface. The state of strain, too, which preceded the earthquake would have been one of tension and not compression. The mechanism of the production of this form of mountain is not prop- erly understood, and a condition of tensile strain in the crust of the earth would be still more difficult to explain, but the fact of the existence of such mountains and structures cannot be gainsaid, so the possibility of the state of tensile strain they imply must be allowed. If such is the nature of the Assam range, and of the cause of this earth- quake, there would be no thrust-plane underlying it, and the focus of the earthquake would have to be regarded as a complex one. That is to say, there would be no general focus, but a number of independent ones, along each fault, and the magnitude of the earthquake experienced would be due to the simultaneous occurrence of a number of ecarthquakes of various degrees of severity. Whether we regard the focus as a thrust-plane, or as a network of faults, it practically covered an extensive area." The hypothesis of a thrust-plane * Zeitsch. f. Erdkunde z. Berlin, Vol. 31, 1806, pp. I-21. °R. D. Oldham, “Report on the Great Earthquake of 12th June, 1897,” Mem. Geol. Surv. India, Vol. 29, 1899, pp. 165-168. ®° The italics are mine—W. H. H. * The italics are mine.—W. H. H. agnor OUTLOOK OF SEISMIC GEOLOGY. 267 is the simplest to work with, as also the most probable, and it is that which has been adopted in the following pages. As we shall see, the fundamental difficulty which stood in the way of the acceptance of the Schollen idea at the time Oldham was writing, has since been removed by the “ distant” studies of earth- quakes (see below, p. 285), and the theory of a thrust-plane, which he chose to adopt, has remained without any support in later work. Additional and important contributions toward the fault-block theory of earthquakes have crowded about the beginning of the twentieth century. In the year 1900, Yamasaki, in describing the great earthquake of northern Honshu, which occurred in 1896, gave as its cause the movement on two visible displacements which opened on opposite sides of the mountain mass.*® Two long lines of fracture were discovered by me to be the cause of the Riku-U. earthquake. . . . They lie on the two sides of the mountain axis of the Central chain, and so this earthquake offers an example of the longitudinal quakes (Liangsbeben) which but seldom occur. Thoroddsen, in a report which reached the scientific world first through a German abstract of the year 19o1,° was able to show that during each of the five heavy shocks of the South Icelandic earth- quakes of 1896, a separate block of country had been shaken. These several areas were all included in a low plain walled in by a ram- part of mountains, and with a single exception they were contiguous areas which did not overlap. Each of the heavy shocks was limited to a circumscribed area which was made evident by a mass of collapsed houses, and from this the earthquake waves were propagated outward in all directions. The ground beneath the low plain is probably separated into individual parts and the continued movement on these cross lines [across the main fissures on which the volcanoes of the island are ranged.—W. H. H.], as well as the faults between the individual parts, appear to be the causes of the many earthquakes of this district. If one studies the statistical tables of the ruined houses from each shock [given in Icelandic report—W. H. H.] it is seen that the individual areas are somewhat sharply delimited; while upon them nearly everything was destroyed, the damage outside was rela- tively small. ®N. Yamasaki, Pet. Mitt., Vol. 46, 1900, pp. 249-255, map. ° Pet. Mitt., Vol. 47, 1901, pp. 53-56. The full report had appeared in the Icelandic language two years earlier. 268 HOBBS—THE EVOLUTION AND THE ~ [April 24, Writing in 1902 Professor John Milne, who has done so much to advance seismology, gave expression to his views upon the cause of the larger and smaller earthquakes :?° The earthquakes to be considered may be divided into two groups—first, those which disturb continental areas and frequently disturb the world as a whole, and secondly, local earthquakes which usually only disturb an area of a few miles radius and seldom extend over an area with a radius of I00 or 200 miles. These former I shall endeavor to show are the result of sudden accelera- tions in the process of rock-folding accompanied by faulting and molar dis- placements of considerable magnitude, whilst the latter are for the most part settlements and adjustments along the lines of primary fractures. The relationship between these two groups of earthquakes is therefore that of parents and children. Professor Milne’s studies of “ distant’ earthquakes had revealed the fact that the world-shaking earthquakes most frequently occur upon the floor of the ocean. When a world-shaking earthquake takes place, and its origin is sub- oceanic, we occasionally get evidence that this has been accompanied by the bodily displacement of very large masses of material. For example, sea- waves may be created which will cause an ocean like the Pacific to pulsate for many hours. To indicate the grand scale of the mass movements of the crust upon the continental areas, a list of twenty-two larger disturbances was compiled by Milne and the following important conclusions drawn: If it can be admitted that world-shaking earthquakes involve molar dis- placements equal in magnitude to those referred to in the preceding list, . . . then, in the map showing the origins of these macroseismic effects, we see the districts where hypogenic activities are producing geomorphological changes by leaps and bounds. The sites of these changes are for the most part suboceanic troughs. When they occur, the rule appears to be that a sea becomes deeper, whilst a coast-line relatively to sea level may be raised or lowered. For nearly all the regions of the world where they take place we have geological and not unfrequently historical evidence that the more recent bradyseismic move- ments have been those of elevation. This elevation, however, only refers to the rising of land above sea-level, while the mass displacements seem to be accompanied by sudden subsidences in troughs parallel to the ridges where rising has been observed. In short, at the time of a large earthquake, two ” “ Seismological Observations and Earth Physics,” Geogr. Jour., Vol. 2I, 1903, pp. 2, 9, II. 1909. ] OUTLOOK OF SEISMIC; GEOLOGY. 269 phenomena are simultaneously in progress. A suboceanic trough may sud- denly subside, whilst its bounding ridge may be suddenly increased in height, and the concertina-like closing of the trough may account for the sea-waves. Dutton, in 1904,11 included in his classification tectonic earth- quakes, and by supplying data concerning the earthquake of Sonora in 1887 contributed an additional example of uplift en bloc of a mountain mass accompanied by a great earthquake. Of this range, the Sierra Teras, he says: In other words, the range seemed to have been uplifted several feet between faults on either flank. Yet the implication in the context is that these observations are hardly decisive, and in a paper read before the National Academy of Sciences in 1906” it is made clear that Dutton at this time still adhered strongly to a modified centrum view to which he had con- tributed in 1889 in his report upon the Charleston earthquake of 1886. The Dutch geologist, Verbeek, in 1905 published a catalogue of the earthquakes of the island of Ambon in the East Indian Archi- pelago, together with a full account of the heavy earthquake which caused much damage upon the island on January 6, 1898.%° His study of the distribution of the damage resulting from the latter quake brought out the fact that the shocks were largely limited to narrow zones on either side of a main fault running in a north and south direction across the island, and to similar zones about three additional faults which cross the first nearly at right angles, the stronger shocks belonging with the first mentioned displacement. Of this north and south zone he says: The terrane most disturbed, which one designates “the pleistoseismic area” does not here have the form of a circle or of an ellipse, as in the case of so many earthquakes, but that of a long band relatively straight, which shows clearly that we have here to do with a tectonic quake; now since we have shown above in the description of the geology that there is at the south of Ambon a fault which is prolonged to the north through Ambon and southward ... to the southern coast, it is altogether natural to attribute the earthquake to a new dislocation along this cleft or fault of the 1“ Rarthquakes in the Light of the New Seismology,” 1904, p. 55. 2“ *7olcanoes and Radio Activity,” Englewood, N. J., 1906, p. 5. RD. M. Verbeek, “ Description Géologique de l’isle d’Ambon,” Batavia, 1905, Pp. 300-323. 270 HOBBS—THE EVOLUTION AND THE [April 24, earth’s crust. Since the formation of this cleft, which is at least of pre- Cretaceous age, doubtless movements have often occurred which continue EVEN TOVOUT IMC Tey te In the following year the Count de Montessus de Ballore, who had already become known as a seismologist of reputation by reason of his masterly essay upon the distribution of seismicity over the globe, brought out a comprehensive work entitled “ Seismic Geog- raphy.” In this volume, as a result of the study of no less than 170,000 recorded shocks of earthquake, their distribution within each province was analyzed by new and ingenious methods of com- bination. In each case the known faults of the district under con- sideration were discussed, and so far as possible, their relation to the seismic distribution was brought out.** Much the clearest demonstration of the adjustment of por- tions of the earth’s crust as individual blocks, and here by well- demonstrated changes of level, is to be found in a paper by Tarr and Martin upon the results of earthquakes in’ Alaska in the fall of 1899.1° Some portions of the coast were found to have been elevated, and other smaller ones to have been depressed. The sea, which here cuts up the district by a number of fiords, permitted the changes of level to be measured by the height of the abandoned shore lines of 1899. In the absence of earlier soundings or of cor- rect maps, the submerged areas were determined with much less precision, though forests now below sea level bear abundant testi- mony to the local direction of the earth movement. Still older abandoned shore lines, appearing as notches above the raised beach of 1899, proved that the latest elevation is but one stage in the progressive, though interrupted, general uplift of the region. Tarr and Martin’s statement of their view is as follows: Briefly summarizing the inferences which the facts seem to warrant, we conclude that in 1899 there was a renewal of mountain growth, uplifting that part of the mountain front bordering the Yakutat bay inlet to different amounts—7 to 10 feet in the southeast side of the bay, and 40 to 47 feet on the northwest side. This uplift occurred all within a little over two weeks and mainly on a single day (September 10). It was complicated by move- 4“ Tes tremblements de terre; Géographie séismologique,” Paris, 1906, PP. 475. *“ Recent Changes of Level in the Yakutat Bay Region, Alaska,” Bull. Geol. Soc. Am., Vol. 17, 1906, pp. 290-64, pls. 12-23. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 271 ments along secondary fault lines, which produced at least three (and perhaps more) major blocks. . . . The first and largest of these blocks, . is apparently titlted upward toward the southwest. Accompanying this faulting was a minor fracturing apparently due to local adjustments in the tilted blocks. Doubtless this minor fracturing is much more common than our observations indicate, for it was discovered in more than half our expeditions into the interior when we went out of the valleys away from the sea coast. The evidence accumulated for the tectonic origin of earthquakes and their inseparable connection with the process of faulting in rock strata, has shown that seismology must be considered as a part of tectonic or structural geology—that part, namely, which is con- cerned with the recent and present-day history of the earth. So soon as this fact receives general recognition, the field of study must be added to that now explored by geologists. For their loss in this quarter elasticians will be more than compensated by the enlarged opportunities which are now offered them for studying earth waves as they are registered at a distance upon the newly devised earth- quake instruments. Recognizing, then, that earthquakes manifest the time of opera- tion of these larger mass movements of the earth’s crust which have brought about changes in level as well as changes in horizontal posi- tion in connection with faulting, it becomes necessary to place the subject em rapport with the latest that has been learned in the wide field of tectonic geology. This treatment of earthquakes as a part of tectonic geology was attempted by the present writer in two monographs published in 1907 in connection with a description of the Calabrian earthquake of 1905,1° and later, in the same year, in a treatise upon seismic geology.” Having in mind the fact that the traces of fault planes are but rarely exposed to view, and in only a small percentage of cases possible of determination from purely geological studies, the inves- tigation of the Calabrian earthquake was directed toward deter- mining whether, (1) there are lines or narrow zones of special *“ On Some Principles of Seismic Geology,” with an introduction by Eduard Suess. “The Geotectonic and Geodynamic Aspects of Calabria and Northeastern Sicily,’ with an introduction by the Count de Montessus de Ballore. Gerland’s Beitrige z. Geophysik, Vol. 8, 1907, pp. 219-362, pls. I-12. ™“ Rarthquakes, An Introduction to Seismic Geology,” New York, 1907, pp. 1-336. 272 HOBBS—THE EVOLUTION AND THE [April 24, intensity of shocks, (2) whether these are repeatedly the seat of special danger from successive earthquakes, and (3) whether such lines, if they exist, are expressed in the surface of the country as earth lineaments. The investigation showed that at the time of an earthquake the surface of the country affected is peculiarly sensi- — tized to reveal the courses of hidden faults, which, if thus made apparent, may be designated seismotectonic lines, and that strong seismotectonic lines correspond in position to the striking linea- ments of the country. In this we find a means of deriving through the study of the topography, the tectonic geology and the seismic history, an imperfect yet none the less a valuable map to display the architecture of each seismic district. It is a curious illustration of earlier misdirection of effort, that up to the year 1907 no detailed map of the fault system within an area disturbed by destructive earthquake had been attempted. The maps which best display the disposition of adjusted fault blocks were the small-scale charts by Thoroddsen and by Tarr and Martin. In the summer of 1907, at the writer’s suggestion, the expert topog- rapher and geologist, Mr. W. D. Johnson, of the U. S. Geological Survey, prepared accurate maps of the surface faults of certain areas disturbed during the Owen’s Valley earthquakes of 1872, which maps were published in part during the same year.1* The sudden changes of displacement on individual faults and the mosaic- like structure of the disturbed region were thus brought out with a clearness and accuracy never before attained. Seismological science may be said to have suitably celebrated its emancipation from the bondage of the centrum theory, when in 1907 there was published from the pen of the Count de Montessus de Ballore the most comprehensive treatise upon the subject.1s* This book recognized the adjusted fault block theory as the best avail- able working hypothesis of the science, and with a grasp of the subject which was based upon a lifetime of study, and upon a quite unparalleled knowledge of the literature, earthquakes were so treated as to make the work the one authoritative reference book of the science. *TIn the author’s “ Earthquakes,’ Figs. 23, 45 and 64. More complete maps will appear in a special monograph. #214 Science Séismologique, Paris, 1907, pp. 579. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 273 The common characteristic of all phases of the modern tectonic theory of earthquakes, the evolution of which we have now largely traced, is that the adjustments in position or attitude of sections of the earth’s crust are regarded as the proximate cause and not the effect of the shocks themselves. So far as molar movements have been recognized by the advocates of the centrum theory, they have been regarded as the direct consequence of volcanic or explo- sive shocks emanating from a deeper-seated origin. Two recent papers of a somewhat speculative nature, prepared by an astronomer, have sought the cause of earthquakes in a leakage from the bottoms of the oceans.*° The Relation of Earthquakes to Volcanoes.—As already pointed out, the earliest of the generally accepted theories of earthquakes connected them directly with volcanic action, and this idea has sur- vived in the centrum theory. The tendency of later study has been to indicate that while both betray a certain relationship to each other, this is not often of sucha nature as to call for a quick response of the one phenomenon to the other. Regions of volcanoes are sub- ject to earthquakes, yet some of the heaviest earthquakes have affected a region distant from any volcanic vents. Again, most great volcanic outbursts are inaugurated by light earthquakes, but great earthquakes produce as a rule no perceptible immediate effect upon the activity of neighboring volcanoes. Thus, for example, during the late Messina earthquake, which was so heavy about the slopes of Etna, that volcano showed no sympathetic response. Catalogues setting forth the seismic and volcanic activity within any province betray, however, certain periods of years during which both seismic and volcanic activity are at either a maximum or a minimum ; though within these periods no close time relation of the one phenomenon to the other is apparent. In short, it would appear 2 T. J. J. See, A.M., Lt.M., Sc.M. (Missou.), A.M., Ph.D. (Berol.), “ The Cause of Earthquakes, Mountain Formation and Kindred Phenomena Con- nected with the Physics of the Earth,” Proc. Am. Puiv. Soc., Vol. 45, 1907, pp. 274-414. “Further Researches on the Physics of the Earth, and espe- cially on the Folding of Mountain Ranges and the Uplift of Plateaus and Continents Produced by Movements of Lava Beneath the Crust Arising from the Secular Leakage of the Ocean Bottoms,” ibid., Vol. 47, 1908, pp. 157-275. PROC, AMER. PHIL, SOC. XLVIII. 192 S, PRINTED SEPTEMBER 7, 1909. 274 HOBBS—THE EVOLUTION AND THE [April 24, that both earthquakes and volcanic activity are different indica- tions of the operation of a more fundamental geological process— mountain formation, with its concomitant manifestation in changes of level. Going back in the direction of the ultimate cause of mountain building, we are probably correct in assuming that it is a conse- quence of the contraction of volume of the planet and the wrinkling of the outer shell, as that shell adjusts itself over the diminished volume of the core beneath. In the past much confusion has arisen from assuming that flexuring has taken place within the outermost shell of the earth, and that the faults discovered are an incident to the folding process within one and the same set of beds. Thus we have come to speak of “dip faults” and “strike faults,’ “longi- tudinal faults’ and “cross faults.” Later studies have shown that the processes of folding and of faulting within rocks take place under different conditions of load corresponding to different depths below the surface; and that, therefore, the folding which accom- panies the rise of a mountain range is so deeply buried beneath the roots of the range that it can be laid open for study only after a blanketing layer of rock some miles in thickness has been removed. Those mountains which are growing to-day—such, for example, as the Sierra Nevadas of the Pacific border of our own country—are being pushed up in blocks which are outlined by steep faults. The elevation goes on spasmodically, and each successive uplift causes a jolt which is manifested as an earthquake more or less destructive, according as the movement is of large or of small amplitude. Deep below the surface, the rising blocks of the crust rest upon arches of folds which a future generation of geologists may be privileged to study after a layer of the present surface some miles in thickness has been carried away. Those parts of the earth’s crust which are not shaken by earthquakes are, in the language of de Montessus, no longer living—they are dead. Not only are earthquakes the indication of changes in level such as accompany the process of mountain growth, but active vol- canoes are now recognized to afford evidence of the same move- ments. Wherever mountain ranges are now rapidly growing, there active volcanoes are to be found. The full significance of this fact 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 275 is only beginning to be appreciated. Fortunately this hypothesis may be fitted to the now quite generally accepted view that the earth is essentially solid throughout, and is maintained in that condi- tion at great depths below the surface by the high pressure from the superincumbent material. Now the arching of strata in the process of folding is competent to lift the load from underlying rocks, so that wherever their temperature is such that fusion would occur at the surface, a reservoir of molten lava is produced and will be brought to the surface from the action of gravity whenever a path is open for it. A reason is thus found for the presence of lava bodies at moderate distances only from the surface in those districts where the process of mountain building is in operation. The Mesh-like Distribution of Volcanic Vents—The lineal arrangements of volcanoes and the dependence of this alignment upon the existence of fissures through the crust, seems to have been one of the earliest of geological observations, so soon as the less civilized continents had been scientifically explored. In Europe the systematic arrangement of volcanoes is much less strikingly dis- played, and it was there in consequence a later discovery. The credit for having first recognized this important fact of observation is generally given to von Buch, because of his classical study of the Canary Islands. It seems probable, however, that Alexander von Humboldt, his friend and colleague in the field of geological ex- ploration, was the first to make the observation. The latter showed that the volcanoes in the Cordilleran system of South and Central America furnish striking examples of such alignment. Von Buch, in his turn, emphasized this significant relationship, but found cer- tain volcanic districts within which the alignment of vents was not apparent, and so he distinguished volcamic chains from central volcanoes. Other explorers like Dana and Darwin soon added con- firmation of a linear arrangement from the regions which they had individually visited. Dana, a member of the Wilkes Exploring Ex- pedition, brought out the lineal arrangement of the Polynesian Islands and showed that all these were alike rows of partly sub- merged volcanic peaks.2® Darwin, during his voyage on the »“ Mafual of Geology,” pp. 37, 282. 276 HOBBS—THE EVOLUTION AND THE [April 24, “ Beagle’ made observations"! which advanced the knowledge of volcanic distribution, as we shall see, very nearly to that of the present day. As early as 1825, that pioneer and master of vulcanology, Paulett Scrope, discussed the arrangement of volcanoes in the following manner :?7 The generality of volcanos have a decided linear arrangement; one vent following the other in the continuation of the same straight or nearly straight line; and when volcanos have been formed on neighbouring points out of this principal line, they are in almost all cases situated upon other rectilinear bands parallel to the first. Later Scrope expressed his doubt of the existence of v. Buch’s class of central volcanoes, for which it had been claimed no align- ment could be discovered.?? In 1844 Darwin proved the existence of neighboring parallel fissues outlined by volcanoes, and was further able to show by his studies of the Galapagos Islands that the arrange- ment of the vents there brought out the existence of a network of fissures composed of two rectangular series with the principal vents at the intersecting points.*4 The directions of the two series were northwest by north and northeast by east. Virlet d’Aoust had already discovered the same kind of structure in the arrangement of the volcanoes within the Grecian archipelago.” Inasmuch as a mesh-like disposition of volcanic vents within a network is of the first importance in its relation to the mass dis- placements which occasion earthquakes, it is pertinent to examine the more recent literature of the subject with a view to establishing its truth or falsity. The newer and more accurate methods for pre- paring maps which have been introduced since the time of Darwin, make such a review at the present time in every way desirable. There are two regions especially which have been recently carefully studied by authorities of the first rank in the field of vulcanology. I refer to Iceland, surveyed at his personal expense throughout a *“ Geological Observations on the Volcanic Islands, etc.,” 1844, pp. 140-145. “Considerations on Volcanos,” London, 1825, p. 126. 78“ \Tolcanos,” London, 1862, p. 258. *L. c., edition of 1900, p. 131. * Bull. Soc. Geol. France, Vol. 3, 1832-33, pp. 103-I10, 201-204. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 277 period of seventeen years by Professor Thoroddsen of Copenhagen, and the islands of the East Indian Archipelago, surveyed for the Dutch Government by the distinguished geologist, Verbeek. Of the Icelandic volcanic region Thoroddsen says :*° Of larger eruption fissures and crater chains I have found 87, all of postglacial origin ; . The many fissures which are common to several districts can not possibly be entered upon a map of small scale; the terrane is often so divided by clefts that both within the flat country and upon the slopes of mountains it appears to be separated into numerous narrow strips some kilometers in length. Between the numerous non-volcanic and the volcanic clefts which have poured out important streams, no difference is to be noticed; an ordi- nary cleft may suddenly become volcanic. . Where larger fissure systems cross, there are often found large 24 46 Scole of Miles. Fic. 1. Map showing arrangement of volcanoes in the western part of the Island of Java. (After Verbeek.) volcanoes, as for example the largest volcano in Iceland, Askja, with a crater of 55 sq. km. area situated at the intersection of the southland fissure running NE.-SW. and the northland one trending N.-S. “Die Bruchlinien Islands und ihre Beziehungen zu den Vulkanen,” Pet. Mitt., Vol. 51, 1905, pp. 1-5, map pl. 5. [April 24, HOBBS—THE EVOLUTION AND THE 278 C3PEqIAA IFW) ‘SJUGA DULIJOA dy} FO JUsMIASUvIIe ayI][-Ysow Surmoys eAef JO puR[sy 94} JO UOoT}Iod usojsey < Sas f2 975 a —_) - of Cy @) At | 1909. J OUTLOOK, OF SEISMIC ‘GEOLOGY. 279 With the exception of the report on Krakatoa the five mono- graphs and accompanying grand atlases which have been issued by the Geological Survey of the Dutch East Indies under the direction of Dr. Verbeek, seem to be but little known; yet they contain the results of extended and detailed surveys within one of the world’s most interesting volcanic regions.*7 Nowhere have such trustworthy data been compiled which permit of a thorough study of the arrange- ment of volcanic vents. Clearly aligned upon fissures the map of Java displays the elements in the intersecting volcano network, as may be seen from atlas drawings reproduced in Figs. 1-2. Though more accurately worked out, it does not appear that these instances of intersection of volcano rows is exceptional. Felix Fic. 3. Map to bring out the arrangement of volcanic islands and submerged volcanic peaks in the Lipari group. and Lenk?’ have explained the prominence of the mighty volcanoes of Mexico, Popocatepetl, Ajusko and Nevada di Toluca, as due to their location at the intersection of important fissures, though the warrant for this has been questioned by others. The volcanic Lipari Islands of the Mediterranean, which were formerly regarded as 7 Verbeek, “ Sumatra’s Westkust”’ (Dutch language), Batavia, 1883, 674 pp., atlas of 16 maps. Verbeek, “ Krakatau,” Batavia, 1885, 567 pp., atlas of 25 pls. Verbeek et Fennema, “ Description Géologique de Java et Madoura,” Amsterdam, 1896, two volumes, 1,183 pp., atlas of 24 maps. Verbeek, “ De- scription Géologique de Vile d’Ambon,” Batavia, 1905, 323 pp., atlas of 10 maps. Verbeek, “Rapport sur les Moluques,” Batavia, 1908. 1844 pp. atlas of 20 maps. * Zeitsch. d. deutsch. geol. Gesell., Vol. 44, 1892, pp. 303-326. 280 HOBBS—THE EVOLUTION AND THE [April 24, built up on radial fissures going out from the ruptured center of a depressed area, reveal a regular plan with the volcanic peaks and craters at the crossing points of intersecting lines, so soon as the submerged cones are brought into the problem (see Fig. 3).”° The volcanoes of Italy and surrounding waters furnish an example of a much larger network within which the vents are located at inter- secting points.*° What is true of the arrangement of ordinary volcanic cones within individual provinces, is repeated in the case of the monti- cules or parasitic cones which are built up upon the flanks of larger composite volcanoes, such, for example, as Etna.** To some extent a similar arrangement may be inferred on a far grander scale than any that has been mentioned, as in the longer trains of the volcanic islands. As long since pointed out by Neumayr, the volcanic island, St. Helena, is located at the crossing point of two long lines of widely separated volcanoes, one trending NE.-SW., and the other NW.-SE. (See Fig. 4). One of these, the well known ‘‘ Cameroon fissure,” bisects the Gulf of Guinea and includes the volcanic islands, St. Helena, Annobom, Sao Thomé, I. do Principe, and Fernando Po. On the land this fissure is continued in a striking manner by the fault bridge which ends in the Tschebitschi, 2,000 meters high, which then drops suddenly to the level of a low plain less than 200 meters above the sea. The volcanotectonic line which intersects this striking lineament at St. Helena, includes Ascension, one of the eastern cones of St. Paul’s Rocks and a conical, submerged elevation upon the sea floor, almost under the tropic of Capricorn about 800 kilometers southwest of Amboland. In addition to these two fissure directions, a third is like them strikingly characteristic of the African continent, as shown by the remarkable north and south lines of volcanoes and rift valleys in central Africa east of the Nile. To these three prevailing directions, northwest-southeast, northeast-southwest, and north-south, must be added a fourth less common direction, namely, east-west. Simmer » Hobbs, Gerlands Beitrige 2. Geophysik, Vol. 8, 1907, pp. 316-317. »” Tbid., pp. 315-316, smaller map of pl. 3. See also Suess, ~The Face of the Earth,” Vol. 1, p. 144. 5! Hobbs, J. c., pp. 348-349, pl. Io. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 281 in a noteworthy compilation®? has shown that these directions are brought out for the African continent not only in the lines of Fic. 4. Volcanotectonic lines which cross at St. Helena. volcanoes but by the fracture systems revealed in the rocks, so far as they have been studied. It is interesting to note that these 2“ Der aktive Vulcanismus auf dem Afrikanischen Festlande und den Afrikanischen Inseln,” Mitinchener Geographische Studien, No. 18, 1906, 218 pp. 282 HOBBS—THE EVOLUTION AND THE [April 24, directions are also the dominant ones in the fracture system of North America.** A number of papers of a controversial nature have appeared notably by Branca** in opposition to the view that volcanoes are aligned upon fissures, but inasmuch as they deal with districts in which the evidence is more or less equivocal they need not be con- sidered here. The problem of arrangement of volcanoes must be solved not in southern Europe nor on the Mexican plateau border, but in the volcano gardens of the world, such as Iceland or Java. Volcanic Extrusions in Relation to Block Adjustments.——Clar- ence King in his description of the area included in the Fortieth Parallel Survey,*° an area divided by vertical faults into great blocks which underwent adjustments at the close of the Miocene, has furnished a classical instance of the relation of volcanic outflow of lava to block movement. He says: Single ranges were divided into three or four blocks, of which some sank thousands of feet below the level of others. The greatest rhyolite eruptions accompanied these loci of subsidence. Where a great mountain block has been detached from its direct connections and dropped below the surrounding levels, there the rhyolites have overflowed it and built up great accumulations of ejecta. Whenever the rhyolites, on the other hand, accom- pany the relatively elevated mountain-blocks, they are present merely as bordering bands skirting the foothills of the mountain mass. There are a few instances in which hill masses were riven by dykes from which there was a limited outflow over the high summits—but the general law was, that the great ejections took place in subsided regions. The study of the great rifts of eastern Africa seems to have shown that the volcanoes which have there been built up, are simi- larly related to the sinking of the great strips of country which have caused the chief inequalities of the general surface.** The two °8 Hobbs, “ The Correlation of Fracture Systems and the Evidences of Planetary Dislocations within the Earth’s Crust,’ Trans. Wis. Acad. Sci., Vol. 15, 1905, pp. 15-20. % W. Branca, “Zur Spaltenfrage der Vulkane,” Sitzungsber. Ak. Wiss., Berlin, 1903, pp. 748-756. %“TJnited States Exploration of the Fortieth Parallel,’ Vol. 1, Sys- tematic Geology, 1878, p. 604. %® Ed. Suess, “ Die Briiche des ostlichen Afrika,” Denksch. Weiner Akad., Math. Naturw. K1., Vol. 58, 1801, pp. 555-584. 1909. ] OUDEOOK OF SEISMIC ‘GEOLOGY, 283 chains of volcanoes in Mexico as mapped by Sapper®? seem to be similarly associated with the great rift valley lying on the western border of the Mexican plateau. It is in Iceland, however, that the most extended studies have been made of the most interesting field, in which the relation has been worked out with the greatest thoroughness.** Says Thoroddsen: One gains the impression that the form of the surface has no significance as regards the volcanic force, which breaks out above upon the ridges, as well as below in the valley, yet the volcanoes are always found associated with areas which are either sinking or have sunk. The lava stream Ogmundarhraun in Krisnoik, which dates from about 1340, was poured out from two parallel clefts. The southernmost portion of this stretch of country between the clefts after the beginning of the eruption sank about 66 meters, and one side of the western fissure rose like a vertical wall with four half craters open at the brink, the other halves having sunk. At the end of the cleft is a visible dike which leads up to the row of craters. Where great fractures or faults are present in the crust, the volcanic forces have not always made a single passageway through them, but in the vicinity on parallel clefts, often upon the high fracture margin; thus one fracture line 50 km. long extends without volcanoes from Krisnoik to Hengill, at which place the north side is sunk 200 to 300 meters; parallel with this is here found above at the margin of the cliff an almost uninter- rupted series of craters which have formed not alone upon a single fissure but over several slices and small fissures running parallel to one another. A similar phenomenon is to be observed on the southern fracture margin of the peninsula of Snaefellsnes where the craters are mainly found above upon the edge of the bluff. Often, also, the reverse is the case, as for example, in the Odadahraun, where the rows of craters for the most part extend along the bases of the mountain chains, which rise as horsts from the sunken ground on either side; a like example occurs at Myvatu, although here the rows of craters occur at times above upon the ridge. In none of these cases have we evidence that the eruptions coin- cided closely in time with the earthquakes which must have accom- panied the movements of the earth strips between their bounding faults, but the relationship of the one phenomenon to the other could hardly be more clearly proven. Summing up the discussion, we note that volcanoes, no less than earthquakes, help us to find the positions of those fissures within the crust by which it is separated “Ueber die ratimliche Anordnung der Mexikanischen Vulkane,” Zeitsch. d. Deutsch. Geol. Gesell., 1803, pp. 574-577. eee Cane Be 284 HOBBS—THE EVOLUTION AND THE [April 24, into a mosaic of blocks, and that these lines of fracture may there- fore be designated seismotectonic or volcanotectomic lines or simply lineaments according as they are revealed by earthquakes, by volcano rows, or by topographic and geologic peculiarities. A Possible Explanation of “Volcanic Earthquakes.’—Writing before 1885 Suess distinguished two classes of earthquakes, the dis- location and the volcanic earthquakes, and to these Rudolph Hoernes added the type of in-caving earthquakes to cover especially some of the light shocks of the Dalmatian coast. If we were to supply a complete category of earthquakes it would be necessary to add further a type of cataract earthquakes to cover the occasional fall of limestone blocks in the Niagara cataract, as well as many other minor forms, such as blast shocks in mines, etc. In point of im- portance two classes only stand out sharply as they were originally announced by Suess, and the present writer has been of the opinion that even these may perhaps be subclasses only of a single phenome- non. The mechanics of volcanic eruption, so far as it applies to the cone, is now so well understood that we are able to connect the outflow of lava which marks the beginning of the grand stage of paroxysmal eruption in a composite cone, with the rending of the mountain and the opening of a fissure—a distinctly tectonic movement induced by the lava as it rises under the influence of gravity, aided perhaps by the expansive power of the associated steam. I believe we have been misled into supposing that the fissures which are thus opened are necessarily radial to the cone, since this would be presumed if the mass of the cone and its base- ment were throughout homogenous, with no preexisting fractures, and were acted upon by hydrostatic pressure from the central shaft only. Etna is a giant mountain rising nearly 11,000 feet directly from the sea, its diameter is more than twenty-five miles, and since the higher portions are so largely concentrated at the center, the aver- age thickness of visible volcanic ejectamenta over the base of the cone is only about one half mile. Apparently, therefore, this super- ficial layer of volcanic material may play a relatively small role in the rending of the entire mass which accompanies an outflow of lava. Sq soon as we examine the lines of parasitic craters which 1909. ] OUTLOOK OF SEISMIC’ GEOLOGY. 285 are distributed upon the flanks of the mountain, we find that the majority of these are not radial to the mass at all, but comprise a network. A notable instance of a line of craters not in radial rela- tion to the central cone is furnished by the chain of Monti Segreta, ‘ Nocella, Pizzuta, Gervasi, Arso and Difeso. Nearly parallel to this chain is that of the Monti Mazzo, S. Leo, Rinazzi, Guardiola and Albano. A map of these and other monticules upon the flanks of Etna has been already published by the writer.*® It is, therefore, not only possible, but extremely probable, that in many instances the earthquakes which so generally accompany the rending of a volcanic cone, are directly associated with the opening of, and perhaps a differential movement upon, those fractures in the basement of the mountain which are a part of the larger fracture system of the district. Lacroix has recently shown that a network of fissures appeared upon Etna in connection with the eruption of 1908.°*? The Conditions of Earth Strain During the Growth of Block Mountains.—lf we consider any circumscribed portion of the earth’s crust within which mountains are growing through the adjustment by individual blocks or compartments of the crust, it is necessary to assume that the superficies is increased during the process. Indi- vidual blocks may indeed be actually depressed as a consequence of the adjustment, but yet the average movement must be assumed to be upward rather than downward. Such a conclusion is, however, in contradiction of the generally accepted view that mountain growth comes about through a reduction of superficial area from secular cooling. This very obvious difficulty in the way of adopting the Schollen conception of mountain structure has been quite generally recognized, and we have already seen how Oldham, in seeking the cause of the great Assam earthquake, was led to reject the theory, even though the vertical faults and the differential changes in level were plainly to be observed. In the opinion of the writer, the recent study of “ distant” earth- quakes by modern seismographs has removed this difficulty in the way of a general acceptance of the fault-block theory. By extend- ® Gerland’s Beitraege z. Geophysik, Vol. 8, 1907, pp. 348-350, Pl. to. *@T eruption de l’Etna en avril-mai 1908, Revue générale des Sciences pures et appliquées. 20° année, 1900, pp. 208-314. 286 HOBBS—THE EVOLUTION AND THE [April 24, ing our knowledge of surface displacements of the earth to the floor of the oceans, it has brought us a surprise; for we have learned that to these areas, by many regarded as so stable, belong a much larger proportion of the grander movements, and by presumption of the smaller ones as well. The recent study of the ocean floor through soundings, examined with reference to the loci of suboceanic quakes, has told us, further, that though the movements upon the land are generally upward, those upon the ocean bottom, on the contrary, are downward. The so-called “origins” of the oceanic quakings are most frequently the steep borders of the great sea troughs where the greatest depths have been revealed by soundings. Now it is as impos- sible to separate the idea of molar displacements from these great disturbances as it is to avoid the conclusion that since these troughs are now the deepest bottoms, this is a direct consequence of the repeated displacements which must accompany the quakings. It has, moreover, been a general result of direct observation, that with noteworthy local exceptions the sea-coasts are to-day undergoing elevation, and that the steeper coasts face the greater depths.*° It is difficult to avoid the conclusion that the general upward movement of the margins of the continental areas and the general downward movements of the near-lying oceanic floors are inter- related as parts of one general adjustment within the outer shell of our planet. This granted, there is no difficulty in conceiving of the rise of block mountains upon the continental borders, since the increase of superficies within the affected continental region is com- pensated by a contraction of area in portions of the sea floor which in the same general period are subsiding. A rise of block moun- tains to the accompaniment of an earthquake, if our theory of cause be correct, though it calls for an expansion of the surface, should reduce the superficies of the affected region if measured on the sur- face of a sphere at its former level. A renewed and sudden com- pression of the district is thus made possible through the action of the tangential compressive stresses within the contracting shell. The writer believes that evidence of such compression has been * See, among others, G. Schott u. P. Perlewitz, “ Lothungen I. N. M. S. “Edi” und des Kabeldampfers “Stephan” im westlichen Stillen Ozean,” Arch. d. deutsch Seewarte, Vol. 29, 1906, pp. 5-11. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 287 found in the case of most large earthquakes in the behavior of rails and bridges.*? Part II: THE OUTLOOK oF SEISMIC GEOLOGY. The Ultimate Cause of Earthquakes.—No one should be deceived into concluding that because we seem to have found some evidence of the nature of the process by which the external shell of our planet undergoes its adjustment at the time of an earth shock, we have thereby discovered the ultimate cause of earthquakes. That is a far deeper problem, to which the discovery of the proximate cause is but an initial stepping stone. It is in this field that the deeper secrets lie hidden. The outlook of the science indicates two lines of effort to be followed up. These are: (1) To make practical application of the knowledge already gained, and (2) to investigate with every possible improvement in method until we have so laid bare the laws of seisms that we may forecast the time, the place and the probable severity of future earthquakes with at least as much accuracy and forewarning as is now possible in weather prediction. Earthquake Forecasts.—It is much to be feared that the science of earthquakes is to pass through a stage not unlike that in meteor- ology which ushered in the day of scientific prognostication. Judg- ing from statements which have been published, a “ Farmer’s Almanac” of earthquakes and popular earthquake prophets may be looked for as a possibility of the near future. It will be well, there- fore, to consider the nature of the earthquake forecasts which have been so widely advertised. Examined with care it is found that these, in so far as they have found any verification, apply to a single, though the most important, seismic zone, and that all are indefinite as to the time and largely so as to place. Dr. Omori, of Tokyo, after the California earthquake of 1906, made a forecast which he himself subsequent to its partial verification reported as follows :*? As to the probable position of the next great shock on the Pacific side of America I expressed my view that it would be to the south of the equator “Hobbs, “A Study of the Damage to Bridges During Earthquakes,” Jour. Geol., Vol. 16, 1908, pp. 636-653. bul Bole Ca Noli i, Nott; ps 23: 288 HOBBS—THE EVOLUTION AND THE [April 24, (that is to say, Chili and Peru), as it was very likely that the seismic activity would extend to either end along the great zone in question, and as the coasts of the countries above named are often visited by strong earth convulsions. About two months after the prediction was made occurred the Valparaiso earthquake, but at the same hour an earthquake of the same order of magnitude visited an area in the Aleutian Islands within the same seismic belt, though nearer and in the opposite direction from the one predicted. On the same grounds Lawson in a lecture read in March, 1907, said of the stretches between southern California and Central America, and between northern California and southern Alaska: These strips, I believe, will be visited before long, and then the long line of this earthquake will be complete from Chili to Alaska. The Guerrero earthquake in Mexico occurred only a few weeks later and bore out the geologist’s faith in the soundness of his hypothesis. The method upon which such predictions are based is already indicated in the quotations given. Briefly expressed it is the prin- ciple of immunity from shock for a considerable period after heavy earthquakes, combined with the conception of relief secured through- out an extended zone in sections by alternation. An extended zone on the earth’s surface is recognized to be what might be called an orographic unit; that is to say, it is all undergoing progressive though interrupted elevation. Stresses tending to produce uplift are presumably cumulative and may be of varying amounts in dif- ferent sections of the zone. ‘The resistance to movement under the strain—whether due to the rigidity, to the vice-like compression, to the absence of suitable fissure planes on which the movement might occur, to the healing of such fissures by mineral matter, or to any other causes—may be assumed to be different in different parts of the zone. Relief of stress through sudden uplift should, therefore, occur first within some one section of the zone where stresses are greatest, resistance least, or both. The earthquakes furnish abun- dant proof of the general correctness of this view. Now it is sim- pler to assume that relief having been secured in one section of the belt, a certain lowering of the potential energy of the system of 1909.] OUTLOOK OF SEISMIC GEOLOGY. 289 stresses is to be expected in the near-lying sections on either side, particularly since the shock tends to discharge the system of strain as would a fulminate. On the theory of probabilities the area next to be relieved should be the most distant, providing stress has there been accumulated for an equally long period. The third and fourth steps in the cycle of release of strain should in position be inter- mediate between the first and second on one side or the other. Later steps in the “letting down” process should affect especially the still intermediate unrelieved sections of the zone. This method, simple as it is in theory, permits of only the broad- est generalization and, as already stated, has been tested in but one zone and for one cycle of relief. This zone is the great circle belt which surrounds the Pacific Ocean, and the cycle of relief seems to have begun with the Colombian earthquake of January, 1906. Only two months after this disturbance came the Formosa earthquake, in a province between one third and one half the distance around the planet. The area of the California earthquake, which occurred a month after that in Formosa, is intermediate between the first two, though nearer the first than the second. By examination of Fig. 5, which is drawn to scale, it will be noted that the distances separating the approximate centers of these and the later disturbances in the series, generally bear out the hypothesis that each later earthquake affects an area farthest removed from those sections of the zone which have already found relief. The rapidity with which the steps in the process of securing relief have here succeeded to one another, lends strong support to the view that the zone in question should be regarded as a definite orographic unit, and that the stress-strain conditions within all except the southernmost portions were before relief began, remark- ably uniform. The planetary order of magnitude of the movements would thus seem to be clearly indicated. The section of the zone last to be relieved was, it is interesting to note, one which had been partly relieved of stress during two earthquakes six years and four years before the main cycle of relief was inaugurated. The section which separates the district of the Aleutian from that of the Cali- fornian earthquake had also been visited by earthquakes seven years and six years previous to the main cycle of relief. The portions PROC. AMER. PHIL, SOC., XLVIII. 192 T, PRINTED SEPTEMBER 7, I909. 290 HOBBS—THE EVOLUTION AND THE [April 24, of the zone in which the probability of heavy shocks is now most imminent, are the Japan-Kamschatka segment, the Peru-Bolivian segment, and the archipelago region to the southeast of Asia. Inas- much, however, as between 1899 and 1903, 29, 12 and 41 heavy shocks had been registered by seismographs from the vicinity of 7 (LL haskalyritish Columbia \ vf Segrien? Aleutians California August 17, 06 Avr! 18, 06 Guerrero April (807 Aome hortca- Jepon Segment Columbia Jan.29 06. T Wh Forrosa : W10°Ch 17, Ob Feru- Bolivia Segrnent Fic. 5. Diagram showing the distances which separated the approximate centers of areas of the series of earthquakes within the circum-Pacific zone in the years 1906-7. these three segments respectively,** the time may be long before the limit of strain may again be reached in them. The problem is thus far from simple and prediction would be extremely hazardous. It should not be forgotten that prediction of any sort has thus * Milne, Geogr. Jour., 1903, map. 1909. ] OQUTEOOK OF “SEISMIC GEOLOGY: 291 far been possible only within this circum-Pacific zone, which, at the time, is passing through a remarkable seismic history. It is little likely that any such sudden relief of strain will take place again in the same zone before a considerable period has elapsed. Yet, outside this zone and within our own country, earthquakes of the first order of magnitude have visited the lower Mississippi Valley, the coastal plain in South Carolina and the valley of the St. Lawrence during the brief period that the country has been occupied by whites. Of these sections of country, as of most others, the only safe prediction that can now be made, is that dis- tricts already visited by historical destructive shocks, as well as some others, notably New England and the Middle States, will eventually suffer from disastrous earthquakes. To the time of such visitations we have not even a clue. Periodicity of Earthquake Cycles—The “letting down” of the potential energy of the system of stresses within the circum-Pacific belt, as brought out by the events of 1906-7, is, in the writer’s belief, as regards its close sequence, an event without parallel in the history of seismic geology. Something approaching it appears, how- ever, to have been in operation within a somewhat longer period in the other great seismic belt of the globe. Making all due allowance for the fact that our quite recent study of distant earthquakes has greatly extended our horizon, it still seems necessary to conclude that the present is a time of very exceptional seismic intensity. So soon as we admit the planetary scale of these seismic dis- turbances and explain them as a result of mountain growth upon the borders of the continent, we are led to expect the existence of such maxima and minima of seismic intensity. If now we examine the history of earthquakes in those countries possessing the longest records, we find evidence in support of this view. The stronger earthquakes in Japan, which are on record for a period of fifteen hundred years, betray a strong tendency to group themselves. The 154 heavy earthquakes recorded in that country since the beginning of the fourteenth century may be divided more or less definitely into A4I groups separated by average intervals of 134 years. In Kyoto a complete record has been kept for a thousand years. Here there was a strong maximum of destructive and strong earthquakes be- 292 HOBBS—THE EVOLUTION AND THE [April 24, tween the middle of the fourteenth and the middle of the fifteenth century, this maximum period being followed by a steady decrease to a minimum in the last half of the nineteenth century. Minor fluctuations reveal an average period of 6} years, or about one half that revealed by the records for the Empire as a whole.* The natural objection which would be raised to making use of these data for basing conclusions upon the behavior of the earth as a whole, is that the maximum of intensity in Japan may well have been compensated by a minimum in a neighboring district. What we need for basing our conclusions is a world catalogue of earth- quakes extending over a sufficiently extended period. Thanks to John Milne and those who have followed his lead, we are now pre- paring such a catalogue, which is sure to permit of a definitive answer to the question of earthquake periodicity. Even within the first section of this catalogue, comprising as it does the thirteen years from 1892 to 1904, Milne believes he has made out a relatively short period with the maxima of world shaking in correspondence with the more abrupt changes in direction in the orbit of the earth’s pole. On a priori grounds it is reasonable to connect seismic dis- turbances with sudden changes in latitude, and the further data upon the pole movement and the seismic world maxima, will be scrutinized with interest. Possibilities of Future Prognostication.—It is too early to pre- dict whether more satisfactory bases for future forecasting of earth- quakes will be discovered, but the indications are certainly encourag- ing. Two, and perhaps three, lines of inquiry are already suggested. Most promising of these, is, perhaps, the study of terrestrial magnet- ism; for in a considerable number of instances, destructive earth- quakes have been preceded by periods measured in hours and some- times in days, within which the behavior of magnetographs was singularly abnormal. It seems likely that this change in magnetic conditions may sometimes be utilized as a warning signal. For solution of this problem the completion of the magnetic survey of the world, may be expected to contribute. Evidence is not lacking that fore-shocks, or rather fore-tremors, #“ Kichuchi, ‘E) 1, C. Pub, No:.10) 10904; pp.) 11-13. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 293 for they would appear to have an extremely small amplitude of vibration, are a fore-runner of most heavy earthquakes. These fore-tremors should not be confused with the preliminary tremors in the record of the distant seismograph, for they are of such small amplitude that they would probably not be registered by any instru- ments today constructed, except perhaps within the affected district itself. Our best evidence that such fore-tremors exist is furnished by the behavior of certain of the lower animals. In the opinion of the writer, such a body of evidence has now accumulated, that it can no longer be waved aside. Just as the sense of smell is so much more highly developed in the dog, for example, than it is in man, so there seems no valid reason for doubting that the detection of small motions by the lower animals may be by as much superior to the human sensibility. Dr. Omori has expressed his belief that seismographs will yet be made sufficiently sensitive to record these microscopic tremors. Just as a block tested in our experiments assumes very large deformations as it approaches rupture, so the earth structure may behave during a period which is as much longer in proportion as the time of augmenting the stresses exceeds that in our experiments. Judging from the recorded behavior of animals, it would not be surprising if the period during which warning may be possible on this basis, should prove to be a large fraction of a day, or even longer. If measurable deformation does occur as a result of the accumulated stresses long before the limit is reached, it may be possible in the case of those earthquakes particularly which result in horizontal shearing movements, to determine by frequent measurement of the distances which separate properly placed monu- ments, the approach of the strain limit. It is a subject which is at least worthy of investigation. Since the days of Perrey, who devoted his life to an attempt to find a connection between earthquakes and lunar conditions, there have been those who have sought to connect seismic and volcanic disturbances with periods of special gravitational stress due to luni- solar phases. The most recent advocate of such a connection, is Perret,*® who is so convinced that he has found the secret behind ©“ Some Conditions Affecting Volcanic Eruptions,’ Science, Vol. 29, 1908, pp. 277-287. 294 HOBBS—THE EVOLUTION AND THE [April 24, the phenomena as to have ventured to predict for the year 1908, a grand eruption of Etna.#* This eruption not having materialized, Perret has accepted the Messina earthquake as a substitute.*7 As- suming that his method is correct, it is possible to see how a period of seismic or volcanic activity might be predicted; the method, how- ever, gives no clue as to what part of the earth’s surface is likely to be thus affected. The predictions of the author of the theory have, Fic. 6. Abandoned Sea Cave to feet above water on Coast of California. (After Fairbanks.) on the whole, been less remarkable than the statements made by one of his supporters.** Need of an Expeditionary Corps—Ilt may well occasion surprise that governments have been so slow to appreciate the necessity for providing means for the investigation of earthquakes. Our own government, which has shown such commendable generosity in providing the sinews for scientific investigation, has in this particular % The World's Work, November, 1907. “ Am. Jour. Sct., Vol. 27, 1900, pp. 322-323. *SJaggar, The Nation, Vol. 88, 1900, pp. 22-23. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 295 field lagged far behind other nations. In Japan since 1892 there has been an Earthquake Investigation Committee, and whenever a destructive earthquake is reported from any part of the world, Pro- fessor Omori, the secretary of the committee and its chief expert, is despatched by his government to prepare a report upon it. Under orders from the Japanese government, he is today in the vicinity of Messina engaged in a study of the latest great disaster. While these expeditions have been of value in securing information, the time has come when with the incease of our knowledge of earth- quakes, something more than a reconnaissance survey is required. One man without assistants and without elaborate equipment, is today in no position to secure those more important data which alone can advance our knowledge of earthquakes beyond its present status. Today a scientific party should have at its disposal one or more surveying vessels—small gunboats or protected cruisers could be easily adapted for the purpose—provided with modern sounding apparatus and with a full equipment of necessary instruments. The crops of scientific workers should include skillful topographers and their assistants and all suitable instruments for preparing accurate topographic maps. The party should also include trained experts whose duty it should be, among other things, to map the distribution of the surface intensity of the shocks. An expeditionary vessel of the type described could be utilized upon occasion to study volcanic as well as seismic disturbances; such, for example, as the late erup- tions in the Windward Islands. The seismic events of the years 1906-8, would have been more than sufficient to take up the atten- tion of two surveying vessels with their corps of scientific workers.* In times of relative seismic inactivity the ships and their comple- ments could be employed to advantage in work which will be more definitely indicated below. A Service of Correlated Earthquake Observatories —In addition to the study upon the ground, which may be expected to lay bare some important laws of seismic geology, there should be installed a series of stations equipped with modern seismographs for the regis- “In a late number of the Popular ence Monthly (February, 1909) the writer has pointed out the exceptional opportunities which the recent Messina disaster has offered for study by this method. 296 HOBBS—THE EVOLUTION AND THE [April 24, tration of the distant as well as the nearer and local earthquakes. These stations should be well distributed over the national domain, and should include a number of stations of the first rank provided with the more sensitive type of pendulum adapted to the registration of distant earthquakes. A larger number of stations of lower rank should be provided with simpler instruments suited only for secur- ing full data upon the local shocks. These smaller stations should | be located with due regard to the more important seismic provinces of the country. The United States Weather Bureau already possesses suitable buildings for installing such apparatus, and the regular employees of the stations could be trained to add the care of the instruments to their other duties. In 1907 with the hearty approval of the heads of the various scientific bureaus of the govern- ment, the American Association for the Advancement of Science, upon recommendation of its Committee on Seismology, memorialized Congress upon the pressing need of such a service. A year later, the Geological Society of America passed a resolution of similar import, and in the same year, no positive result having been secured, the Committee on Seismology renewed its first memorial by a second resolution.*** Scientific research has already gone far to remove some of the greatest scourges of human existence. Of those which are char- acterized by sudden and usually unexpected visitation, are pestilence, flood, conflagration, earthquake and volcanic eruption. Of these flood and conflagration must be in part laid at the door of earth- quake disturbances, to which they have all too frequently been an almost inevitable sequel. They have, moreover, taken the larger toll of human life and property. As compared with epidemic diseases, like the plague and smallpox which repeatedly overran Europe during the middle ages, earthquakes and their consequences have been the less destructive of life. It has been estimated that in Europe, the plague alone carried off no less than 25,000,000 people. Yet medical science has discovered the mystery of the disease, and in sanitation and isolation provided the remedy. To meet the great dangers of conflagrations, which from time to time “a See also the resolution passed by the American Philosophical Society on April 24, 1909. Proceedings No. 101, p. xii. 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 297 have swept over our cities, we have as yet made only partial provi- sion, yet the remedy is known and the country does not hesitate to make an annual expenditure conservatively estimated at $25,000,000, and in addition compels its citizens to build according to approved regulations. A single earthquake has involved us in a loss of over $350,000,- 000, or nearly ten times the loss from the Baltimore fire.*° Yet the government has expended nothing in an attempt to safeguard the future by avoiding the recurrence of such disasters. In Europe within a few months an entire city has been laid in ruins with a loss of life which may reach 150,000, yet the latest information makes it almost certain that this quake was not an exceptionally heavy one, and that most of the loss of life and property might have been avoided if proper methods of construction had been adopted. It can hardly be claimed that the comparatively recent California disaster gave us our first warning of danger, for twenty years earlier the earthquake in South Carolina caused a loss of over one hundred lives, and property to the value of between $5,000,000 and $6,000,- 000. The earlier earthquakes within our territory have been far heavier and the small loss of life and property is accounted for only because the districts were at the time so thinly populated. We must not, therefore, overlook the fact that the United States is an earthquake country, and this not alone in its Pacific section. Some of our largest and most prosperous cities are almost certain to pass through their trials in the future, as Charleston and San Francisco have so recently. On February 5, 1663, almost the entire valley of the St. Lawrence and large sections of New England were visited by an earthquake, which, if the country had been built up as it is today, would have caused a disaster which it is not pleasant to contemplate. Preparation of Maps of Fracture Systems.—As we have seen, earthquakes register the movement of portions of the earth’s crust between planes of fracture. In just how far these fracture planes are present in advance of the movement, and in how far they result © The official figures kindly furnished by Professor J. W. Glover. 298 HOBBS—THE EVOLUTION AND THE [April 24, from the relief of strain at the time of the shocks, has not yet been determined. Some writers have dismissed from consideration as “secondary phenomena” most of those visible fractures which first appear at the surface during an earthquake. It seems certain, however, that many of these fractures, at least, as regards both direction and position, are dependent upon the fracture system already present in the underlying rocks; and there is, therefore, need for extended study of the fracture and fault system within the rock basement of each earthquake province. With this study might perhaps be combined the determination of the depth and the earth- quake properties of each of the overlying unconsolidated deposits. Experiments are further necessary in order to determine whether large thicknesses of such deposits are controlled by the same laws as are the thinner ones. In every district which has an earthquake history, this record should be examined to learn if possible the points, the lines, or the areas of heaviest shock. Whenever data are sufficiently complete, maps should be compared to represent the approximate distribution of surface intensity for each earthquake, and comparisons instituted. Maps of Visible Faults and Fissures and of Block Movements for Special Earthquakes.—lt has been pointed out that in the case of a single earthquake only has a map been prepared to show in detail the distribution of the surface faults and the block movements of the ground. Thirty-five years after the event which brought them into existence, these faults have been mapped in detail by Mr. W. D. Johnson, of the United States Geological Survey. It has been possible to prepare maps of portions only of the district affected, and the full results are not yet published. Within the national damain there are at least two other provinces which promise fruitful results from such a study. These are the regions affected by the Sonora earthquake of 1887, and, even more important, the country about Yakutat Bay, Alaska, so profoundly modified in its relief during the earthquakes of 1899. A scientific party with head- quarters upon a surveying vessel, such as we have described, would here find almost unequaled opportunities for securing important data. Rate of Mountain or Shore Elevation by Quantitative Methods. (syuUvqIIe TIF ) “BIUIOFI[E) jo }SBOO UO [VAD] BIS juasoid JAOGL JodfF OL YoIe VIS PUL JIVITI} JNI-IAV AA IAX 3Lv1d ZBL ON ‘INATX “1OA ‘90S “SOTIHd ‘WY SDNIGS3I00¥d r he SD dp My “ eee ‘ al LATO I toot Te a , a at we ae Le ae * a Bh MOR ees WE VC COMERS rat a Tac : a Me wr , Ube darz ‘ rf .. ah) 3 rab eae ar. ‘ ‘ ae ; q } Pasi Pa teed | 15 (sue qire yy IJV) “prlofie ye JIOd J1eou PIULOFI[V) JO jseoo UO SIPS SUNIqIYXa JUTT 8tOUS poreAdl[y AX 3Lv1d Z6L ON ‘INIATX “TOA “90S “SOTIHd ‘WY SDNIGSR00"d 1909.] OUTLOOK OF SEISMIC GEOLOGY. 299 —The studies of earthquakes during the last few years have done much to destroy the illusions of more than half a century. Since the time of Lyell, the burden of all geological instruction has been the extreme slowness of terrestrial dynamic processes. Oscillations of level described as slow and uniform warpings of the crust, had been gauged by measurement upon shores, which in the expressive language of de Montessus are dead, and where in consequence earth- quakes are seldom or never left. If movements accomplished within a week and largely upon a single day, can elevate stretches of coast over 47 feet, as was true of portions of the Alaskan coast in 1899, what modifications of our traditional theories will be required! There is a pressing need for extended studies on rising coasts to determine by some scale the rate of elevation. Now it happens that one of the most rapid of erosional processes is that accomplished by the waves as they beat upon a lee shore, and this process is one capable of fairly accurate quantitative measure- ment. The Pacific coast of North and South America, the greater part of the way from Alaska to Patagonia, has, during a recent period, been rising to the accompaniment of earth shocks. As we now understand, these uplifts have been mainly spasmodic, and the strand-lines abandoned with each successive uplift now stand revealed in a series-of steps or terraces, which, when closely examined, reveal the characteristic marks of wave action sometimes at heights of fifteen hundred feet and more (see Fig. 7, and Plates XV. and XVI.). Careful maps prepared after correlation of these strand lines throughout long distances when combined with precise studies of the rate of wave cutting, could hardly fail to shed light upon the broader problems of seismic geology. In some cases such abandoned shores now in an elevated posi- tion reveal clearly that their uplift was sudden and that no interval long enough to permit wave cutting separated it from the inaugura- tion of the present level. Thus in figures 6 and 8 are represented shores which might almost be described as fossilized earthquakes, for the evidence is clear that the elevation took place in what was essentially a single sudden stage and must have been accompanied by a great quake. Seacoasts offer the best possible data for observation and meas- 300 HOBBS—THE EVOLUTION AND THE [April 24, urement of the rate of uplift, because the level of the water can be made use of for the zero point. There are, however, other available means for investigating the rate of continental uplift. In arid and semi-arid regions, such as the Great Basin of the United States, the Fic. 7. Elevated shore on the coast of California showing marks of wave action. (After Fairbanks.) rare but violent storms cause torrents in the streams which de- bouch upon the plains from the mountain fronts, and so broad fans and aprons are there built up. Now if the uplift of the range goes on more slowly than the alluviation along its borders, the mountain front deposits will bury and hide the escarpments which are opened at the time of each successive uplift. If, on the other hand, the 1909. ] OUTLOOK OF SEISMIC GEOLOGY. 301 uplift is the more rapid, fault scarps will appear cutting the uncon- solidated deposits. Such scarps, some of them twenty feet in height, are characteristic of both the Eastern and the Western margins of Fic. 8. Elevated and present shore lines registered in notches of chalk cliff at Cape Ciro, Celebes. (After Paul and Fritz Sarasin.) the Great Basin region. From careful study of the rate of deposi- tion there is here the possibility of reaching an approximate measure of the rate of uplift. Investigation of Earthquake Water Waves——rThe great water wave which followed the famous Lisbon earthquake of 1755 was 302 HOBBS—SEISMIC GEOLOGY. [April 24, more destructive to human life than the shocks which proceeded it. The earthquake water wave which inundated the shore of Japan on June 15, 1896, destroyed human lives to the number of 29.953. Such waves have been especially destructive along the western coast of South America. The new seismology, by instrumental methods, points more and more definitely to the cause of such disturbances in the subsidence of great sections of the neighboring ocean floor; yet with the exception of relatively small waves within the Mediter- ranean, we are without observational data in the form of soundings in confirmation of this hypothesis. The bottom of the ocean is each year being charted in new areas, and we are fast accumulating data on which to base a decisive series of observations to settle this im- portant question. This will certainly be one of the larger problems for investigation in seismic geology. Conclusion.—It has been possible to indicate a few only of those directions along which effort will be directed in the early future of seismic geology. From this summary, I think it will be seen that there remain no other fields of investigation so long neglected and yet so full of promise in important discoveries, which are likely. to touch so intimately the lives and happiness of human beings. What we have already learned is much of it as yet only half learned, and we need careful experimentation on lines already marked out, so that recommendations may be made for adapting our lives to future seismic conditions. Probably nine tenths of the danger from earth- quakes can be avoided through practical methods of construction, but the relative cost of the different means of securing immunity must be carefully considered. The studies which are necessary are on such a scale that they call for generous government support, and it cannot be too strongly urged that the United States government undertake a work so clearly demanded by the situation. This sup- port should be nothing less than the foundation of a bureau for earthquake investigation, with regular appropriations sufficient to carry out studies by a system of correlated earthquake stations, and also upon the ground of each devastated region whether it be at home or abroad. University oF MICHIGAN, April 21, 1909. SEISMOLOGICAL NOTES. By HARRY FIELDING REID. (Read April 24, 10909.) (a) ConpITIONS PRECEDING AND LEADING TO TECTONIC EARTHQUAKES. There are two classes of earthquakes: Volcanic and Tectonic; the former, connected with volcanic outbursts, seem to be due to explosions or to the sudden liberation of steam; the latter are due to ruptures of the rock. It is only the latter class that we shall consider at present. Rock, like all solids, is elastic, and when subjected to external forces it suffers an elastic strain; if this strain is too great for the strength of the rock to withstand a rupture occurs; but it is never possible for a rupture to take place until the rock has been deformed or stretched beyond its elastic limit. When the rupture occurs, the two sides spring apart under the elastic forces and come to positions of equilibrium, free of elastic strains. The following experiments have been made to illustrate these conditions. Two short pieces of wood were connected by a sheet of stiff jelly 1 cm. thick, 4 cm. wide and about 6 cm. long, as shown in Fig. 1. The jelly was cut through along the line, ¢#t’, by a sharp knife and a straight line, AC, was drawn in ink on its surface. The left piece of wood was then shifted about I cm. in the direction of ¢’, and a gentle pressure was applied to prevent the jelly from slipping on the cut surface. The jelly was sheared elastically and the line took the position AC shown in Fig. 2. On relieving the pressure so that the friction was no longer sufficient to keep the jelly strained, the two sides slipped along the surface tt’ and the line AC broke into the two parts AE and DC. At the time of the slip A and C remained stationary, and the amount of the slip, DE, equalled the shift which A had originally experi- enced. A straight line, A’C’, was drawn on the jelly after the left side had been shifted, but before the jelly slipped along tt’. At the 308 304 REID—SEISMOLOGICAL NOTES. [April 24, time of the slip, the same movement took place in the neighborhood of this line, as near AC, and A’C’ was broken into two parts, A’E’ and D’C’; the total slip, D’E’, being equal to DE. A third experi- ment was tried; the left piece of wood was shifted I cm. and a straight line was drawn across it; it was then shifted a half centi- meter more and the straight line took the position A”C” in Fig. 3. When the jelly slipped along the surface, ¢t’, the line broke into the two parts, A”E” and D’’C”; the slip, D”E”, being equal to the total displacement of the left side. Two characteristics of the movement are to be noted; the total slip on the ruptured surface equalled the total relative displacement of the blocks of wood; and, at the time of the slip the blocks remain stationary, and the whole movement at that time was an elastic rebound of the jelly to a condition of no strain. These experiments illustrate as well as simple experiments could what occurred at the time of the California earthquake of April 18, 1906. Fortunately, early surveys had been made of this region which Dr. Hayford, in the report of the California Earthquake Com- mission has, for the sake of discussion, divided into two groups; L., the surveys made from 1851-65; II., those from 1874-92. A third survey (III.) was made after the earthquake in 1906-7. These surveys extended from Mt. Diablo, about 33 miles east of the fav’t, to Farallon Light House, about 22 miles west of it. They showed that between the I. and II. surveys Farallon Light House had shifted relatively to Mt. Diablo, 4.6 feet north-northwest, practically in a direction parallel with the fault-line; and between II. and III. sur- 1909.] REID—SEISMOLOGICAL NOTES. 305 veys it had shifted 5.8 feet more in nearly the same direction, dati a total shift in about 50 years of 10.4 feet. Observations in the field on the offsets of fences and roads showed that at the time of the earthquake there was a relative move- ment of the two sides at the fault-surface, amounting to something like 20 feet, and it is only reasonable to suppose that this movement was equally divided between the opposite sides of the fault. The surveys show that the actual displacement which took place between II. and III. diminished as the distance from the fault became greater; on the east side the displacement practically died out at a distance of four or five miles from the fault, and on the west side the displacement became equal to that of Farallon Light House at about the same distance from the fault. All the phenomena were in close accord with the experiments described above. The main difference consists in the fact that a straight line on the earth’s surface across the fault and at right angles to it did not break up into two straight lines, as in the experiment, but into two curved lines. We ascribe this curvature to the fact that the forces which produced the dis- placement of the ground were applied below the crust of the earth, whereas in the experiment they were applied at the outer boundary of the jelly. The elastic rebound near the fault-surface, of course, took place suddenly at the time of the earthquake; and the surveys show that between I. and II., and between II. and III. there was a relative shift of very extensive regions on opposite sides of the fault, but the surveys do not determine whether these shifts took place sud- denly at the times of the great earthquakes of 1868 and 1906, or whether they were the effect of a slow, gradual movement con- tinuing through the years. We must turn to other considerations to decide this point. In the experiments we have described the elastic rebound was greatest at the ruptured surface, became progressively less at greater distances from this surface, and the jelly in contact with the wooden blocks did not partake of the movement at all. The experiments might have been varied and instead of a slow shift of the block gradually setting up an elastic shear, we might have set up the shear suddenly; but this was not PROC, AMER. PHIL. SOC, XILVIII. 192 U, PRINTED SEPTEMBER 7, I909. ' 306 REID—SEISMOLOGICAL NOTES. [April 24, necessary to produce the phenomena which we know took place at the time of the earthquake. It seems impossible to think that the general shift was sudden; for we cannot imagine what forces could have produced a sudden displacement, amounting to four or five feet, of a portion of the earth’s surface covering thousands of square miles. But we have indubitable evidence, in the foldings of the rock common to all mountain chains, of the slow displacement of large regions to considerable distances; and unless such a displace- ment were slow enough to allow the rock everywhere to flow viscously and thus adjust itself to its new position, there would be places where the elastic stresses would from time to time be greater than the strength of the rock and ruptures would occur causing earthquakes. This view of the case is so entirely in accord with the elastic properties of rock, and with the slow movements of large regions, familiar to geologists, that it commends itself strongly without further argument; but there is a consideration which seems almost decisive in its favor. In the experiments described we saw that the relative slip at the ruptured surface was exactly equal to the total relative shift of the wooden blocks; this, of course, was independent of the slow or sudden nature of the shift. The slip on the fault- surface at the time of the California earthquake was about 20 feet; therefore the shift of the more distant regions which brought about the break must have been as great; but the surveys show that be- tween II. and III., the shift was only 5.8 feet, and between I. and II., 4.6 feet; that is, in all, only about 10.4 feet since the earliest surveys, some 50 years before the shock. We can therefore say, definitely, that the shift which set up the elastic strains which finally resulted in the earthquake, not only did not wholly take place at the time of the rupture but that even fifty years earlier it had already accumulated to about one half its final amount ; that between the I. and II. surveys it increased to about three-quarters of this amount, and that the last quarter was added between the II. and III. surveys. It is hardly possible, in view of this history not to be convinced that the shift accumulated gradually. Since the general order of events, that is, the setting up of elastic strains resulting in the rupture of the rocks which preceded 1909.] REID—SEISMOLOGICAL NOTES. 307 and caused the California earthquake, were the consequences not of special conditions but of the general properties of rock, we may make the general statement that tectonic earthquakes are caused by the gradual relative displacement of neighboring regions, which sets up elastic strains so great that the rock is ruptured; and that at the time of the rupture no displacements of large areas take place, but there occurs merely an elastic rebound, to an unstrained position, of the lips of the fault extending but a few miles on each side of it. It is not necessary of course that the slow displacement should set up a simple horizontal shear, as in the case of the California earthquake, but simply that an elastic strain of some kind should be produced by the relative displacement of adjoining regions. This may be due, for instance, to the slow sinking of a large region with the production of vertical elastic shears around its boundary, and when these shears become sufficiently strong a break will occur and the movement of the two lips will be vertical and in opposite direc- tions, thus producing a fault-scarp. The main, sinking region, however, would not suddenly drop at the time of the break; there would only be an elastic rebound around its boundaries; its own displacement having taken place slowly over a long period of time. The elastic strains might also be set up by a horizontal compression, in which case the rock would be folded upward, and when the curvature became too great it would break like a bent stick, both sides of the broken surface flying upwards under the elastic forces and leaving an open fissure between them. Examples of this kind of rupture are only known on a small scale. It is possible that the rupture may not be confined to a single surface, but may be distributed over a number of neighboring surfaces, and a small block between these surfaces may be displaced as a whole; but this must be looked upon as a minor phenomenon of the fault-zone, and is not an example of the readjustment of large blocks. (b) SomME CHARACTERISTICS OF SEISMOLOGICAL INSTRUMENTS. When efforts began to be made, some thirty or forty years ago, to produce an instrument that would record the actual movement of the ground caused by an earthquake, the object aimed at was to 308 REID—SEISMOLOGICAL NOTES. [April 24, “ce produce a “steady mass,” that is, a heavy mass that would remain at rest in spite of the movement of its support; and by recording, either directly or through magnifying levers, its movement relative to the ground, the hope was entertained that the actual movement of the ground would be obtained. But the hope was futile. Every seismograph consists essentially of two parts: a heavy mass adjusted in a greater or less degree to a condition of neutral equilibrium, and the drum or other surface on which the record is made. If the mass could be adjusted absolutely to neutral equilibrium and could be kept in that condition in spite of the movement of its support, it would remain at rest, and would record the true move- ment of the earth; but the size of the recording apparatus is limited and in order that the record should be made on it, the heavy mass must remain pretty closely in one position, which is practically in- compatible with neutral equilibrium. It was found necessary to keep the mass in stable equilibrium although the force brought into play by a small displacement might be very small. If displaced the mass would, therefore, vibrate about its position of equilibrium with a period of its own; and the record of every earthquake is the combination of the earth’s movement with that of the heavy mass; and if the period of the vibrations of the earth happens to approach that of the heavy mass, the amplitude of the latter increases greatly, and indicates a movement of the earth much larger than actually occurs. We cannot deduce the movement of the earth from the record except by a careful analysis based on the mathematical theory of the seismograph. This, fortunately, has been worked out; but, unfortunately, it is rather complicated, and it is only in compara- tively simple cases that it can be applied without very great labor. The earlier investigators also thought that all solid friction or viscous damping reduced the sensitiveness of the instrument, and that a long period of vibration increased it. Solid friction is indeed always harmful and should be reduced as much as possible, but viscous damping is a great advantage and simplifies the interpreta- tion of the record. Remembering that every earthquake consists of vibrations of many periods, a glance at figure 4 will show the great benefit of strong damping. The curves show the magnifying power of the seismograph so far as it depends upon the ratio of the 1909.] REID—SEISMOLOGICAL NOTES. 309 period of the earth’s vibration to that of the seismograph itself, and upon the viscous damping. The damping ratio is the ratio of the amplitude of successive swings of the heavy mass, when it is = [iS aeen| Le WAS A OLS SLO Lede L893 2.0 Fic. 4. Ratio of Periods ~ 9 samog SubfuSeyy allowed to swing freely. If this ratio is nearly 1:1, that is, if there is very little damping and the amplitude of the swinging mass dies 310 REID—SEISMOLOGICAL NOTES. [April 24, down very slowly, the curves show that the magnifying power for vibrations of very short period is unity; that is, the record gives the true amplitude of the earth’s motion; for vibrations of longer period the magnifying power rapidly increases, and when the ratio of the periods is unity; that is, when the period of the earth’s motion and the free period of the seismograph are equal, the magnifying power becomes extremely large. For still longer periods the magnifying power again decreases and when the period becomes very long, it becomes extremely small. Since, therefore, the vibrations of various periods are differently magnified, it is quite evident that the record of an earthquake would be greatly distorted, some vibrations being unduly emphasized, and others unduly minimized. It is just in this respect that damping is beneficial. Within limits, the in- equality of magnifying power for various periods becomes less as the damping ratio becomes greater; and when the damping is great enough to reduce the relative amplitude of successive swings in the ratio of 8:1, the magnifying power is nearly uniform for all periods less than that of the seismograph. A seismograph, damped to this amount, and with a period as long as the longest of those present in the earth’s vibrations, would give a much truer representa- tion of the earth’s movement. The advantage of a long free period is not to increase the sensi- tiveness of the seismograph but to increase the range of periods over which its sensitiveness may be maintained. Contrary to a very general belief, the magnifying power for vibrations of very short periods is not affected by the amount of damping. (c) SUGGESTIONS FOR A NATIONAL SEISMOLOGICAL BUREAU. The work of collecting information regarding earthquakes, and studying this material is so extensive that it cannot be carried out thoroughly except with the aid of the federal government. The United States is almost the only country of importance which does not give governmental aid to the study of earthquakes; and, al- though, fortunately, the larger part of this country is only subject to occasional slight shocks, extremely destructive shocks have occurred within our boundaries, and certain districts are frequently visited by earthquakes which cause much damage. The study of earth- 1909. | REID—SEISMOLOGICAL NOTES. 311 quakes is a thoroughly practical subject, and if properly prosecuted, will be of distinct benefit to the country. Let us glance, for a moment, at the special problems which a national bureau should take up. They may be enumerated as follows: 1. The collection of information regarding earthquakes in the United States and its possessions. 2. The study of the distribution of earthquakes in the United States and the preparation of maps showing this distribution and its relation to the geological structure. 3. The study of special regions, such as the California coast. 4. The prompt examination of a region which has ‘suffered a severe earthquake. 5. The collection of information regarding earthquakes under the sea, and tidal waves. 6. The study of the earthquakes of the Gulf of Mexico and the Caribbean Sea from the records of instruments around these areas. 7. The issue of monthly bulletins, giving the records of felt earthquakes and of seismographs in the United States. 8. The study and dissemination of information regarding the best methods of construction in areas subject to earthquakes. g. The theoretical study of earthquake instruments. to. Other theoretical studies. The variety of these studies requires the sympathetic cooperation of many branches of the government for their successful prosecu- tion. The Weather Bureau and the Post Office Department are especially adapted to collect information regarding felt earthquakes ; and the trained observers of the former, distributed as they are all over the country, could readily add a seismograph to the instruments under their charge and obtain important records. of distant and near earthquakes. The Navy, through its personnel and through its Hydrographic Office has especial facilities for collecting information regarding earthquakes felt at sea. The Geological Survey alone could study the relation of geological structure to the occurrence of earthquakes ; and the Coast and Geodetic Survey has on its staff able mathematicians capable of deducing the characteristics of the interior of the earth from the velocity of earthquake waves through 312 REID—SEISMOLOGICAL NOTES. [April 24, it, and of finding the answer to the question whether earthquakes produce changes in the.earth’s magnetism. In looking over the history of the various scientific bureaus of the government, we see that they were, in general, started by the Smithsonian Institution, and after their work had been thoroughly marked out and justified, they became independent. It seems not only conservative, but most practical, to follow this precedent in the establishment of a seismological bureau; for the Smithsonian is excellently adapted for prosecuting earthquake studies, and it could probably secure the hearty cooperation of all the other departments of the government more easily than could any single one of these departments. SOME BURIAL CUSTOMS OF THE AUSTRALIAN ABORIGINES. By R. H. MATHEWS, LS. (Read May 21, 1909.) Oval-shaped objects used in connection with native burials in the valley of the Darling River, New South Wales, were manufactured from burnt gypsum,’ reduced to a powder, and fine sand or ashes, well compounded with water, just as we would mould anything of the kind out of cement or plaster of paris. The necessary shape could be given to the mass while plastic and then allowing it to dry in the sun. These objects are in the shape of a large egg, varying in length from about three to nine inches, by a width of say two and a quarter inches for the smaller ones, up to double that width for the larger. (See Figs. 1, 2, 3 and 4, page 314.) They are often approximately circular in a section through the middle part, but in other cases such a section would be ovate. Some of them are flattish on one or both sides and are not unlike a cake baked in an elongated form. In a few of the flattened productions, one side is slightly concave, but whether this was intended by the maker it is difficult to say. Probably the wet mass assumed this shape when drying in the sun, because the heat would naturally cause the outer margin, which would dry first, to turn upward, simi- larly to the way a board warps toward the sun, when exposed in a free state. Nearly all the specimens I have seen were evidently manufactured in the way above described, but an occasional one consists of a piece of sandstone or shale, of a light color, found in the bush, which required but little fashioning to bring it to the required shape. An old aboriginal, of the Ngunnhalgu tribe, known as Harry Perry by the white people, told me that these kopat objects, which he * Called kopai by the natives; often erroneously written copi and kopi by the European residents of that region. 313 314 MATHEWS—SOME BURIAL CUSTOMS [May 21, called mirndu, were made out of powdered kopai and a little sand or ashes, much in the way we mix up flour when making dough for baking into bread. He said that when a native of either sex died and was buried, the relatives came to the grave and placed these I 2 3 4 This picture shows three medium sized cakes and one small one, all of which are made from gypsum (kopai), as above described. I shall call them murndu, their native name in the Ngunnhalgu tribe, which occupied the country from about Wilcannia up to near Louth, being the tract from various parts of which my specimens were obtained. Fic. 1. The murndu numbered 1 in the picture, is 634 inches long, by a maximum width of 434 inches. The thickest part, at right angles to the width, is 37% inches. The weight of the article is 2 tbs. 9 oz. Fic. 2 measures 234 inches in length, by a mean thickness of 2% inches. Weight, 4% oz. Fic. 3 has a length of a little over 77% inches and its greatest breadth is 4% inches. It is oval in section, with a thickness of 3% inches. Weight, 2 tbs. 14 oz. Fic. 4 is 6%6 inches in length, with a maximum breadth of 34% inches. It has a practically circular section through the middle. Weight, 2 tbs. 8 oz. Scattered here and there through the composition of the balls are pieces of gypsum as large as gravel, showing that the mineral was not very well pulverized; a fact which does not surprise us, when we remember that the natives had to burn the gypsum in a camp fire. For the same reason the powder became mixed with small quantities of wood ashes. kopai balls on top of the mound of earth. For example, if the body - were that of an adult man, his widow would place a mirndu on the ground above his head. The deceased’s brothers would each place one or more along one side of the grave; his mother and sisters might also lay a mirndu or two on the other side; and so on. 1909. ] OF THE AUSTRALIAN ABORIGINES. 315 An old man of the Murawarri tribe informed me that in his language the kopai ball or tablet is called yirda. When a man, woman, or young person beyond the age of childhood, died, leaves were strewn over the earth covering the grave, and on top of the leaves were laid the yirda. There might be only one or two yirda deposited, or there might be more, depending upon whether the deceased had few or many friends. Mr. E. J. Suttor tells me that he has seen a dozen or more of these kopai balls lying on a native’s grave. They were put on as soon as the corpse was buried. A Ngéumba blackfellow told me that in his tribe the name of the kopai balls is dhaura. The gypsum was collected, burnt and pounded fine by the women, and the men shaped the dhaura. A resident informs me that gypsum is very plentiful on Yantara Station, near Lake Cobham, about 120 miles northwesterly from the Darling River, where tons of it could easily be obtained. Another correspondent, at Kallara Station on the Darling, states that gypsum is quite plentiful there. In fact, gypsum and pipeclay are both easily obtainable along the valley of the Darling, as well as in the hinterland, all the way from its junction with the Murray River up to Brewarrina. There is also a kind of slacked or rotted gypsum which occurs in patches, resembling slacked lime. Old Perry and others above quoted said that the object of deco- rating the grave in the way described was to induce the bo-ri or spirit of the dead person, to remain in its place of sepulture and thus prevent its roaming through the camp at night to do injury to anyone with whom the deceased might in his or her lifetime have had a feud. When the spirit saw that its owner’s death had been properly mourned for in accordance with the tribal custom, it felt more friendly towards everybody. The spirit comes up during the night and sits on top of the grave and commences licking or sucking one or more of the kopai balls. Sir Thomas L. Mitchell is the first author to mention these kopai balls. He says: It was on the summit of a sandhill where I fixed my depot on the Darling [Fort Bourke] that we saw the numerous white balls, and so many graves. The balls are shaped as in the accompanying woodcut, and were made of lime. ... A native explained one day to Mr. Larmer [a member of Sir 316 MATHEWS—SOME BURIAL CUSTOMS [May 21, Thomas’s Staff] in a very simple manner the meaning of the white balls, by taking a small piece of wood, laying it in the ground and covering it with earth. Then laying his head on one side and closing his eyes, he showed that a dead body was laid in that position in the earth, where these balls were placed above.” In root, Mr. G. Officer, of Kallara Station, described some kopai balls or cakes found at a grave on Curronyalpa run on the Darling River, about fifteen miles above Tilpa. There were thirty-nine specimens at the grave, some of which were lying on the surface, others were partially revealed, and the remainder were found by digging a little way into the sandy soil underneath. Fic. 5 is an exterior view of a kurno or widow’s cap, a being the front, or part fitting over the forehead, whilst b represents the back of the head. Owing to the unusually large number of pieces on this grave, I am inclined to believe that the greater portion of them had been car- ried from other graves in the neighborhood to this spot and hidden, for the purpose of protecting them from the vandalism of the white men, who were in the habit of carrying them away as curios. Mr. Higgins, a long resident of the Darling region, writes me that two old blackfellows had stated to him that, when the natives observed that the white people desecrated their burying places in this way, they themselves buried the kopai balls in the ground to keep them 2“ Three Expeditions into Eastern Australia” (London, 1838), Vol. L, pp. 253-4. Seven kopai balls are illustrated in the woodcut referred to. 1909.] OF THE AUSTRALIAN ABORIGINES. 317 out of sight. Possibly nearly all the specimens recovered by Mr. Officer had originally been concealed with earth, but the violent winds of that district had blown the sandy soil away and left them visible. The grave was on a sandhill about three miles back from the river and was therefore out of the way of the white men, whose principal traffic lay along the course of the stream. Helmet-shaped objects, called kurno, known to have been worn on the heads of widows as a sign of mourning, were made from gypsum, burnt and pounded fine, and mixed with water. A fiber Fic. 6 shows the interior of the cap, with the marks or impression of the net, and the size of its meshes, plainly discernible. This cap weighs 11 Ibs. 1 oz., and has been formed of kopai or gypsum in the way already de- scribed. The specimen was found on a native grave on Lower Budda run, Darling river. I am indebted to Mr. F. W. Beattie for the two photographs, which he took at my request. or rush net was first placed on the woman’s head to protect the hair, and the soft mixture applied outside until it resembled a cap, hence called “ widow’s caps” by the Europeans. The mixture was not all put on at the same time but by a series of additions extending over a few weeks. The marks of the meshes of the net are distinctly visible in the interior of some of the “caps” of this kind which have been preserved by white men. When the mourning cap had been worn 318 MATHEWS—SOME BURIAL CUSTOMS [May 21, the customary time, it was taken off and placed by the widow upon the grave of her late husband. When the deceased left a plurality of widows, each wore an emblem of mourning and disposed of it in the same way. If the net was firmly embedded in the dried gypsum, it was left in it, but if the net could be readily detached it was taken out of the cap for future use. In some cases, portions of the woman’s hair had to be cut to get the cap off. If the net was left in the cap, it rotted away, but its impression remained. (See Figs. 5 and 6, pages 316 and 317.) Sir Thomas L. Mitchell reports that on the Darling River he found ‘Casts in lime or gypsum, which had evidently been taken from a head, the hair of which had been confined by a net, as the impression of it, and some hairs, remained inside.” The same author states that, on the Murray, some distance above its confluence with the Darling, he saw some native graves with mounds of earth raised over them, on which were laid the “singular casts of the head in white plaster” which he had before seen at Fort Burke. In some cases the casts of the head were found lying beside the gypsum balls. 9 He gives illustrations of these two “ casts,’ showing also the marks of the net inside.* In 1838, Mr. Joseph Hawdon observed some skull-shaped caps, made of white plaster, which he thought was obtained by burning shells and grinding them into powder. They were laid on the grave of a native near Lake Bonnie on the Murray River. He says that inside the cap was a network of twine. Mr. Hawdon states that he also noticed a great quantity of crystallized lime or gypsum in the locality ; it was in masses some tons weight.‘ Mr. E. J. Eyre gives an example of the “ Korno, or widow’s mourning cap, made of carbonate of lime, moulded to the head.” The specimen illustrated by him weighed 84 lbs.® 5 Op. cit., Vol. L., pp. 253-254, and Vol. II., p. 113. *“ Diary of an Overland Journey from Port Phillip to Adelaide in 1838” (MSS). ®*“ Journs. Expeds. Discov. Cent. Australia” (London, 1845), Vol. IL., p.509, Plate: Ty Pig. 17. Rr es kop ae) THE AMERICAN PHILOSOPHICAL SOCIETY HELD AT PHILADELPHIA, FOR PROMOTING USEFUL KNOWLEDGE ‘ ANNOUNCES THAT IN DECEMBER, IgI1o0 IT WILL AWARD ITS MAGELLANIC GOLD MEDAL TO THE AUTHOR OF THE BEST DISCOVERY, OR MOST USEFUL INVENTION, RE- LATING TO NAVIGATION, ASTRONOMY, OR NATURAL PHILOSOPHY (MERE NATURAL HISTORY ONLY EXCEPTED) UNDER THE FOLLOWING CONDITIONS : 1. 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JosrpH Wuarron, Sc. D.; fe SULA. Minutes of ieee from May 7 to December 17, rg10 ............ xlil i Tadex ae a Bie wanes SE AREER SESS SEN 5 DOC Ae 9 alare Baie DE aOR i re ee * PHILADELPHIA eee : THE AMERICAN PHILOSOPHICAI, SOCIETY ge | Io4 SouTH FirrH STREET ine i FEB28 i913 | eee Be he at. ae Ge %: iss a, ers American Philosophical Society General Meeting—April 21-23, 1910 The General Meeting of 1910 will be held on April 21st to 23rd, beginning at 2 p. m. on Thursday, April 21st. Members desiring to present papers, either for themselves or others, are requested to send to the Secretaries, at as early a date as practicable, and not later than March 19, 1910, the titles of these papers, so that they may be announced on the programme which will be issued immediately thereafter, and which will give in detail the arrangements for the meeting. 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When the thirteen original colonies and the mother land closed in -1783 by the Treaty of Paris the civil war that had raged between them since 1775, and the United States were recognized by Great Britain as a member of the family of nations, both parties thought that, by that treaty of partition of 1783, they had arranged all the differences then existing between them. But during the cen- tury and a quarter that has elapsed since the Treaty of Paris was signed, the United States and Great Britain have been engaged in endless discussions and arguments concerning the proper interpreta- tion of that treaty. Among these mooted questions, that of the Atlantic fisheries has been a fruitful bone of contention between the two leading Anglo-Saxon powers. At length, just as so many other points of difference between these two nations have been settled in peace by a reference to international arbitration, so this question of the Atlantic fisheries is to be so arranged by referring it to the decision of The Hague International Court. This sensible and humane agreement of two great powers to refer the solution of this question to that august tribunal instead of allowing it to become a cause of war, will be another “ mile stone ” in the evolution of inter- PROC. AMER. PHIL, SOC., XLVIII. 193 V, PRINTED JANUARY 4, IQIO. 320 BALCH—THE AMERICAN-BRITISH [April 22, national arbitration. In the following paper, I have briefly con- sidered this important and live question. Great Britain and her North American colonies shared in the burdens and anxieties of the struggle that resulted in the overthrow of the French power in North America, and after the cession of Canada and the French maritime provinces around the Gulf of Saint Lawrence to the British Empire in 1763, the motherland of England and the British North American colonies had in common a large heritage in northeastern America. And the fishermen of the north- eastern colonies resorted to the Gulf of Saint Lawrence and adja- cent waters to catch their share of the rich harvest of fish that was to be found in those waters.* During the negotiations for peace at Paris in 1782 between the motherland and her revolted colonies, one of the subjects that gave much cause of trouble to the negotiators was the right to participate in the fisheries. On November 25, 1782, the British commissioners proposed to the American negotiators that the citizens of the United States should have the liberty of taking fish of every kind in all the waters of the Gulf of Saint Lawrence and on all the Newfoundland banks, and to dry and cure fish on the shores of the Isle of Sables and of the Magdalen Islands in the Gulf of Saint Lawrence, so long as those coasts remained unsettled, on “ condition that the citizens of the United States do not exercise the fishery but at the distance of three leagues from all the coasts belonging to Great Britain, as well those of the continent as those of the islands situated in the Gulf of Saint Lawrence. And as to what relates to the fishery on the coast of the island of Cape Breton out of the said gulf, the citizens of the said United States shall not be permitted to exercise the said fishery but at the distance of fifteen leagues from the coasts of the island of Cape Breton.’ By this proposition not only were American citizens prevented *Sir George Otto Trevelyan, “The American Revolution,” New York, 1899, Part I., pp. 263, 264. ? Francis Wharton, “The Revolutionary Diplomatic Correspondence of the United States,’ Washington, 1889, Vol. VI., pp. 74-76. 1909.] ATLANTIC FISHERIES QUESTION. 321 from drying fish on the shores of Nova Scotia, but also to catch fish within three leagues of the shores around the Gulf of Saint Lawrence and within fifteen leagues of the shores of Cape Breton Island on its seaward side. Thus by this last provision the British envoys wished to close to American citizens the right to fish in a part of the high seas that were then recognized as a joint possession of all mankind. These proposals were promptly rejected by the American commissioners, and on November 28, John Adams, for the latter, submitted a counter plan.2 Further parleys were held on this important question. As the Americans contended firmly for the rights of their citizens to fish on the Newfoundland banks, and Adams said he would not sign any agreement that did not secure to the American fishermen the right to catch fish in the Newfoundland and adjacent waters, the British commissioners yielded the point.‘ After numerous propositions and changes, the contending negotia- tors at length agreed on the following article that was embodied in the treaty of peace finally signed in 1783.5 Article III. It is agreed that the people of the United States shall con- tinue to enjoy unmolested the right to take fish of every kind on the Grand Bank, and on all the other banks of Newfoundland; also in the Gulph of St. Lawrence, -and at all other places in the sea, where the inhabitants of both countries used at any time heretofore to fish. And also that the inhabitants of the United States shall have liberty to take fish of every kind on such part of the coast of Newfoundland as British fisherman shall use, (but not to dry or cure the same on that island;) and also on the coasts, bays and creeks of all other of his Britannic Majesty’s dominions in America; and that the American fishermen shall have liberty to dry and cure fish in any of the unsettled bays,+harbors and creeks of Nova Scotia, Magdalen Islands, and Labrador, so long as the same shall remain unsettled; but so soon as the same or either of them shall be settled, it shall not be lawful for the said fishermen to dry or cure fish at such settlements, without a previous agreement for that purpose with the inhabitants, proprietors or possessors of the ground. Thus that treaty, that provided for a partition between the motherland and her North American colonies of the territory that they enjoyed in common, also provided for a partition in the en- * Francis Wharton, “The Revolutionary Diplomatic Correspondence of the United States,’ Washington, 18890, Vol. VI., p. 85. * Francis Wharton, “The Revolutionary Diplomatic Correspondence of the United States,” Washington, 1889, pp. 86-87. °“ Treaties and Conventions concluded between the United States of America and other Powers since July 4, 1776,” Washington, 1889, p. 377. 322 BALCH—THE AMERICAN-BRITISH [April 22, joyment of the “right” to reap the benefits of the rich fisheries around Newfoundland and in the adjoining waters that the subjects of the motherland and the colonies had won by their joint exertions and valor. And subject to the provisions of the treaty of peace as embodied in its third article, American fishermen continued to take fish in the waters around Newfoundland and the Gulf of Saint Law- rence as formerly they had fished in those same waters as British subjects. When the American and the British negotiators met at Ghent in August, 1814, to agree upon a treaty of peace to put an end to the state of war existing between their respective countries, the British commissioners said, among other things, that They felt it incumbent upon them to declare that the British Government did not deny the right of the Americans to fish generally, or in the open seas; but that the privileges formerly granted by treaty to the United States of fishing within the limits of the British jurisdiction, and of landing and drying fish on the shores of the British territories, would not be renewed without an equivalent.® A few days later the British commissioners also brought up the question of the free navigation for British subjects of the Mississippi River.’ In the following November the American negotiators in submitting a project for a treaty to their British colleagues, said, ‘ in an accompanying note that they were “not authorized to bring into discussion any of the rights or liberties’ that the United States had up to then enjoyed in the fisheries. After much sparring be- tween the two groups of negotiators as to the fisheries, the naviga- tion of the Mississippi and other points of difference, the two sides, who were both desirous of concluding peace, agreed to exclude altogether any mention of either the fisheries or the navigation of the Mississippi from the treaty of peace that they concluded at . Ghent on December 24, 1814.8 The rights of American fishermen in the northeastern American *“ American State Papers: Class I., Foreign Relations,” 1642) Viol. Mil pi7o5: *John Quincy Adams, “The Duplicate Letters, The Fisheries and the Mississippi; Documents relating to transactions of the Negotiations of Ghent,” Washington, 1822, pp. 54, 55, 184. 8“* American State Papers: Class I., Foreign Relations, 1832, Vol. III., pp. 744, 745. Washington, ” Washington, 1909.] ATLANTIC FISHERIES, QUESTION, 323 fisheries came to public notice a few months later. On June 19, 1815, the British sloop Jaseur, warned an American cod fishing ves- sel, when out in the open sea some forty-five miles from Cape Sable, not to approach within sixty miles of the coast. This act trenching on the rights of all mankind to fish in the open sea, the British gov- ernment disowned.® Lord Bathurst, however, at the same time said to John Quincy Adams that while the British government “ could not permit the vessels of the United States to fish within the creeks and close upon the shores of the British territories,’ it would not interfere with American fishermen “ in fishing anywhere in the open sea, or without the territorial jurisdiction, a marine league from Shorey 7° The question of whether or not the third article of the American- British treaty of peace of 1783—whereby American fishermen were secured fishing rights in certain of the territorial waters of Britain in North America—was abrogated by the War of 1812, was during the next few months discussed by John Quincy Adams, American Minister to Great Britain, and Lord Bathurst, British Minister of Foreign Affairs. On September 25, 1815, Mr. Adams, in a com- munication addressed to the Earl of Bathurst, argued that the treaty of 1783 was ‘ the common understanding and usage of civilized nations, is or can “not, in its general provisions, one of those which, by be considered annulled by a subsequent war between the same par- tiess. 72 On October 30 following, Lord Bathurst replied to Mr. Adams atv length: Ple said): To a position of this novel nature Great Britain can not accede. She knows of no exception to the rule, that all treaties are put an end to by a subsequent war between the same parties. ... The treaty of 1783, like many other, contained provisions of different characters—some in their own nature irrevocable, and others of a temporary nature. ... The nature of the liberty ” *“ American State Papers: Class I., Foreign Relations, 1834, Vol. IV., p. 349. ** American State Papers: Class I., Foreign Relations,’ 1834, p. 350. “American State Papers: Class I., Foreign Relations,” Washington, 1834, P. 352. “American State Papers: Class I., Foreign Relations, 1834, PP. 354, 355. Washington, bd Washington, ” Washington, 324 BALCH—THE AMERICAN-BRITISH [April 22, to fish within British limits, or to use British territory, is essentially different from the right of independence, in all that may reasonably be supposed to regard its intended duration. . . . In the third article (of the treaty of 1783), Great Britain acknowledges the right of the United States to take fish on the banks of Newfoundland and other places, from which Great Britain has no right to exclude an independent nation. But they are to have the liberty to cure and dry them in certain unsettled places within His Majesty’s territory. If these liberties, thus granted, were to be as perpetual and independent as the rights previously recognized, it is difficult to conceive that the plenipotentiaries of the United States would have admitted a variation of language so adapted to produce a different impression; and, above all, that they should have admitted so strange a restriction of a perpetual and indefeasible right as that with which the article concludes, which leaves a right so practical and so beneficial as this is admitted to be, dependent on the will of British subjects, in their character of inhabitants, proprietors, or possessors of the soil, to prohibit its exercise altogether. It is surely obvious that the word right is, throughout the treaty, used as applicable to what the United States were to enjoy, in virtue of a recognized independence; and the word liberty to what they were to enjoy, as concessions strictly dependent on the treaty itself. On January 22, 1816, the American Minister addressed a reply to Lord Castlereagh, who had in the meantime succeeded Lord Bathurst as foreign secretary. He said the treaty of 1783 was intended to arrange the whole scope of the diplomatic relations between the two nations. He said the British note admitted that treaties often contained recognitions in the nature of continuing ob- ligations; and that it admitted that the treaty of 1783 was such a treaty, except a small part of the article relating to the fisheries and the article about the navigation of the Mississippi. In searching for the answer of International Law to this differ- ence of opinion, two principal sources can be looked to—the judg- ments of courts of law and the opinions of leading international jurists. In the first class there are two judgments, one rendered by an American and the other by an English court, that sustain the American contention that the third article of the treaty of 1783 was not terminated by the War of 1812. In the case of the “ Society for the Propagation of the Gospel in Foreign Parts vs. The Town of Newhaven,” the Supreme Court of the United States, in rendering judgment, was called upon to pass on the continuance or extinguishment of treaties, especially upon that of 1783, by a subsequent war. On March 12, 1823, Mr. Justice Wash- 1909.] ATLANTIC FISHERIES QUESTION. 325 ington,'* delivered the opinion of the court. On the continuance of treaties, he held :*+ But we are not inclined to admit the doctrine urged at bar, that treaties become extinguished, ipso facto, by war between the two governments, unless they should be revived by an express or implied renewal on the return of peace. Whatever may be the latitude of doctrine laid down by elementary writers on the Law of Nations, dealing in general terms on this subject, we are satisfied, that the doctrine contended for is not universally true. There may be treaties of such a nature, as to their object and import, as that war will put an end to them; but where treaties contemplate a permanent arrangement of territorial and other national rights, or which, in their terms, are meant to provide for the event of an intervening war, it would be against every prin- ciple of just interpretation to hold them extinguished by the event of war. If such were the law, even the treaty of 1783, so far as it fixed our limits, and acknowledged our independence, would be gone, and we should have had again to struggle for both upon original revolutionary principles. Such a construction was never asserted, and would be so monstrous as to supersede all reasoning. We think, therefore, that treaties stipulating for permanent rights, and general arrangements, and professing to aim at perpetuity, and to deal with the case of war as well as of peace, do not cease on the occurrence of war, but are, at most, only suspended while it lasts; and unless they are waived by the parties, or new and repugnant stipulations are made, they revive in their operation at the return of peace. , In the case of “ Sutton vs. Sutton,” in order to decide the case at bar, it was necessary for the British High Court of Chancery to pass upon the continuance or abrogation of the treaty of 1794, be- tween America and Britain, known as Jay’s Treaty, after the War of 1812 between these two powers. Sir John Leach, Master of the Rolls in the British High Court of Chancery held: The relations, which subsisted between Great Britain and America, when they formed one empire, led to the introduction of the ninth section of the treaty of 1794, and made it highly reasonable that the subjects of the two parts of the divided empire should, notwithstanding the separation, be pro- tected in the mutual enjoyment of their landed property; and, the privileges of natives being reciprocally given, not only to the actual possessors of lands but to their heirs and assigns, it is a reasonable construction that it was the intention of the treaty that the operation of the treaty should be permanent, and not depend upon the continuance of a state of peace. * Mr. Justice Bushrod Washington. * Wharton’s “United States Supreme Court Reports,’ New York, 1823, p. 404. * Russell and Mylne’s “ Chancery Court Reports,” Vol. I., 676. 326 BALCH—THE AMERICAN-BRITISH [April 22, International publicists are not unanimous on the question whether war terminates all or every part of treaties. Formerly the weight of opinion held to the view that a state of war between two nations terminated the treaties between them im toto. To-day, however, the weight of opinion, in accordance with the trend of International Law towards the more humane goal of mitigating and lessening war, tends to the view that many treaties, either in their entirety or in part, are not abrogated by a state of war by the con- tracting states. In support of the former or English view, there is Vattel, who says :7° Les conventions, les traités faits avec une Nation, sont rompus ou annullés par la guerre qui séléve entre les contractans; soit parce qu ils supposent tacitement l’état de paix, soit parce que chacun pouvant dépouiller son ennemi de ce qui lui appartient, lui 6te les droits qu'il lui avoit donnés par des traités. Phillimore, the English jurist, maintains almost the same view.** Oppenheim, formerly of the University of London, now of Cam- bridge University, leans rather to the modern and more liberal view. He says 37° The doctrine was formerly held, and a few writers maintain it even now, that the outbreak of war ipso facto cancels all treaties previously concluded between the belligerents, such treaties only excepted as have been concluded especially for the case of war. The vast majority of modern writers on International Law have abandoned this standpoint, and the opinion is pretty general that war by no means annuls every treaty. But unanimity in regard to such treaties as are and such as are not cancelled by war does not exist. Neither does a uniform practice of the states exist, cases having occurred in which states have expressly declared that they considered all treaties annulled through war. Thus the whole question remains as yet unsettled. But never- theless with the majority of writers a conviction may be stated to exist on the following points: 3. Such political and other treaties as have been concluded for the purpose of setting up a permanent condition of things are not zpso facto annulled by the outbreak of war, but in the treaty of peace nothing prevents the victorious party from imposing upon the other party any alterations in, or even the dissolution of, such treaties. *% Emer de Vattel, “Le Droit des Gens ou Principes de la Loi Naturelle.” A Amsterdam chez E. van Harrevelt, 1775, Vol. II., p. 81. ™ Robert Phillimore, “Commentaries upon International Law,” Philadel- phia, 1857, Vol. III., p. 457, et seq. * LL. Oppenheim, “International Law,” London, 1906, Vol. II., p. 107. 1909.] ATLANTIC FISHERIES QUESTION. 327 Henry Wheaton, an American, says that all treaties are not ter- minated by war.’® Englishmen, too, holding Government positions, have thought that not all treaties were abrogated by war. Thus in February, 1765, Sir James Marriott, the advocate-general, held that the treaty of neutrality of 1686 between Great Britain and France was “a sub- sisting treaty, not only because it is revived, by a strong implication of words and facts but for that it may be understood to subsist be- cause it never was abrogated.’*° And speaking in the House of Commons in 1783, Charles James Fox gave it as his opinion that all treaties were not ended by a subsequent war between the contracting nations.”* From 1815 to 1818 Great Britain continued to maintain, in spite of the third article of the Treaty of 1783, that American fishermen had no right to fish in British territorial waters; and during those years British government vessels seized numerous American ves- sels found fishing in British waters. These seizures and the conse- quent partial stoppage of the fishing rights of the American fisher- men created much bad feeling. In order to avoid this continual cause of friction betweeh the American republic and the British empire, which kept alive and inflamed the bad feelings between the peoples of the two nations, the two governments agreed on October 20, 1818, on a convention to settle the fishery controversy on the principle of mutual con- cessions. This convention was negotiated for the United States by Albert Gallatin and Richard Rush, and for great Britain by Fred- erick J. Robinson and Henry Soylburn. The fishing rights of Amer- icans in the British territorial waters were defined in Article one that read as follows :* Article I. Whereas differences have arisen respecting the liberty claimed by the United States for the inhabitants thereof, to take, dry, and cure fish ® Henry Wheaton, “ Elements of International Law,” eighth edition, edited by Richard Henry Dana, Jr., Boston, 1866, p. 340. * George Chalmers, “ Opinions of Eminent Lawyers, on Various Points of English Jurisprudence, Chiefly Concerning the Colonies, Fisheries and Com- merce of Great Britain,’ London, 1814, Vol. II., p. 355. 4 Hansard, “ Parliamentary Debates,’ Vol. XVIII., London, 1814, p. 1147. “Treaties and Conventions concluded between the United States of America and other Powers since July 4, 1776,’ Washington, 1889, p. 415. 328 BALCH—THE AMERICAN-BRITISH [April 22, on certain coasts, bays, harbours, and creeks of His Britannic Majesty’s dominions in America, it is agreed between the high contracting parties, that the inhabitants of the said United States shall have forever, in common with the subjects of His Britannic Majesty, the liberty to take fish of every kind on that part of the southern coast of Newfoundland which extends from Cape Ray to the Rameau Islands, on the western and northern coast of New- foundland, from the said Cape Ray to the Quirpon Islands, on the shores of the Magdalen Islands, and also on the coasts, bays, harbours, and creeks from Mount Joly on the southern coast of Labrador, to and through the Streights of Belleisle and thence northwardly indefinitely along the coast, without prejudice, however, to any of the exclusive rights of the Hudson Bay Com- pany: And that the American fishermen shall also have liberty forever, to dry and cure fish in any of the unsettled bays, harbours, and creeks of the southern part of the coast of Newfoundland hereabove described, and of the coast of Labrador; but so soon as the same, or any portion thereof, shall be settled, it shall not be lawful for the said fishermen to dry or cure fish at such portion so settled, without previous agreement for such purpose with the inhabitants, proprietors, or possessors of the ground. And the United States hereby renounce forever, any liberty heretofore enjoyed or claimed by the inhabitants thereof, to take, dry, or cure fish on, or within three marine miles of any of the coasts, bays, creeks, or harbours of His Britannic Majesty’s dominions in America not included within the above-mentioned limits; Pro- vided, however, that the American fishermen shall be admitted to enter such bays or harbours for the purpose of shelter and of repairing damages therein, of purchasing wood, and of obtaining water, and for no other purpose what- ever. But they shall be under such restrictions as may be necessary to prevent their taking, drying or curing fish therein, or in any other manner whatever abusing the privileges hereby reserved to them. By this new agreement both sides gave up something, and, as they thought at the time, they also in that way expected to peace- fully adjust the whole northeastern fishery question for the future. The march of time and events have shown how far wrong the two governments were in the latter hope. And to-day what is meant by the language of the first article of that treaty is in dispute be- tween the two powers, and the fishery question remains for all practical purposes as unsettled to-day as it was before the negotia- tion of the convention of 1818. A comparison of the provisions of the Treaty of 1783 and that of 1818 in reference to the fisheries, shows that the right of Amer- icans to catch fish in the Gulf of Saint Lawrence, on the New- foundland Banks, and at all other places in the sea, remain the same. In other words, that both diplomatic agreements confirm the rights of Americans to take fish on the high seas, that is in all 1909.] ATLANTIC. FISHERIES’ QUESTION: 329 waters that are not known as territorial. But the liberty granted to American fishermen to fish within British territorial waters by the Treaty of 1783 is much curtailed by the convention of 1818. The former instrument gave to Americans the liberty to fish along the British coasts generally and “to dry and cure fish in any of the unsettled bays, harbors and creeks of Nova Scotia, Magdalen Islands and Labrador, so long as the same shall remain unsettled.” The convention of 1818 curtailed the liberty of Americans to fish in British territorial waters to the shores of Newfoundland, along its southern coast from Cape Ray to the Rameau Islands and on its western and northern sides from Cape Ray to the Quirpon Islands; to the shores of the Magdalen Islands in the Gulf of Saint Law- rence; and to the coast of Labrador from Mount Joly indefinitely to the east and the north. On June 14, 1819, the British Parliament passed an act to carry the first article of the convention of 1818, which specified the rights of Americans to take fish in the waters around Newfoundland, into effect. Everything on the fishing grounds did not run smoothly. A number of American fishing vessels were seized by the British au- thorities. Correspondence upon the subject between the constituted authorities of the two powers resulted from 1822 to 1826.2% Then for a decade, comparative quiet seems to have reigned concerning the fishery rights. In 1836, however, the legislature of Nova Scotia began to attempt to prevent American fishing vessels from catching fish in the waters adjoining the shores of Nova Scotia. First it passed a “ hovering act,” to prevent American fishing vessels from sailing within three miles of the coast; then Nova Scotia sought to exclude American fishermen from all bays, including even the Bay of Fundy, which is over sixty miles wide and nearly a hundred and forty miles long, that are bound by the shores of Nova Scotia.*4 That province also attempted to deny to American vessels the right ** Senate Executive Documents, No. 100, 32d Congress, Ist Session, Wash- ington, 1852, pp. I-55. * Senate Executive Documents, No. Ioo, 32d Congress, Ist Session, Wash- ington, 1852, p. 108. 330 BALCH—THE AMERICAN-BRITISH [April 22, of free passage through the Gut of Canso between Nova Scotia and Cape Breton.?® The British authorities based their rights to exclude American vessels from fishing in the Nova Scotia bays, no matter what their area, upon the renunciation by the United States in the first article of the convention of 1818 “to take, dry, or cure fish on, or within three marine miles of any of the coasts, bays creeks, or harbors of his Britannic Majesty’s Dominions in America” outside of those of the shores of the Magdalen Islands, the coasts of Canada and Labra- dor east and north of Mount Joly, and a part of the shores of New- foundland. To this preposterous claim of the British authorities, that ran counter to the accepted Law of Nations that had gradually opened the high seas to the vessels of all nations except within three miles of the shore and within those bays and fiords that were less than six miles wide, the American government protested. American fishing vessels were seized within the Bay of Fundy by the British authorities. Conscious that this attempt to apply territorial rights to such a large body of water, which obviously constituted a part of the high seas, was in contravention of the Law of Nations, the British government in 1845 gave up its claim as to the Bay of Fundy, stating, however, that it made this concession as to that one bay only.2® Daniel Webster, Secretary of State for America, and Lord Malmesbury for Britain, stated in 1852 the views of the two countries. In the summer of the same year, Senator Cass, in the United States Senate, spoke on this question. He illuminated the subject by referring to the last part of article one of the convention of 1818 which provided that “ American fishermen shall be admitted to enter such bays or harbors for the purpose of shelter and of re- pairing damages therein, of purchasing wood, and of obtaining water,’ and argued that this language meant the small bays into which vessels were accustomed to seek shelter from storms. Sen- ator Cass said: * Lorenzo Sabine, “Report on the Principal Fisheries of the American Seas,’ House of Representatives, Miscellaneous Documents, No. 31, 42d Con- gress, 2d Session, p. 221. *® Documents of the United States Senate, Special Session called March 4, 1853, Washington, 1853, Senate Document 3, pp. 4-8, 9-21. 1909.] ATLANTIC FISHERIES QUESTION. Do] That such was the understanding of our negotiators is rendered clear by the terms they employ in their report upon this subject. They say: “It is in that point of view that the privilege of entering the ports for shelter is useful,” etc. Here the word “ports” is used as a descriptive word, embracing both the bays and harbors within which shelter may be legally sought, and shows the kind of bays contemplated by our framers of the treaty. And it is not a little curious that the Legislature of Nova Scotia have applied the same meaning to a similar term. An Act of that Province was passed March 12, 1836, with this title: “An act relating to the fisheries in the Province of Nova Scotia and the coasts and harbors thereof,’ which act recognizes the conven- tion, and provides for its execution under the authority of an imperial statute. It declares that harbors shall include bays, ports, and creeks. Nothing can show more clearly their opinion of the nature of the shelter secured to the American fishermen.” In 1853 America and Great Britain agreed to a convention, whereby a settlement of all claims by citizens or corporations of either country against the other should be referred to a mixed commission, composed of two commissioners, one for each nation.”® . In every case where the commissioners could not agree the con-' vention provided that they should refer it to an umpire. In that way the claims arising out of the seizures by the Canadian authori- ties in 1843 of the American fishing vessel, Washington,?® while fish- ing in the Bay of Fundy, ten miles from shore, and in 1844 of the American schooner, 4rgus,°° on St. Ann’s Bank, twenty-eight miles from the nearest land, were referred for settlement to the umpire, Mr. Bates, an American by birth, residing in England where he was a member of the banking house of Baring. In both cases he awarded damages to the American owners, on the ground that in neither case were the Ametican vessels fishing in contravention of the convention of 1818. With the object of amicably adjusting the various controversial points that had arisen under the interpretation of the convention of 1818, the British government in 1854 sent Lord Elgin to America to * “ Congressional Globe,” 32d Congress, Ist Session, Appendix, Washing- ton, 1852, p. 805. 3“ Treaties and Conventions concluded between the United States of America and other Powers since July 4, 1776,’ Washington, 1889, p. 415. 9 Senate Executive Document, No. 103, 34th Congress, Ist Session, Wash- ington, 1856, p. 184. ° Senate Executive Document, No. 113, 50th Congress, 1st Session, Wash- ington, 1888, p. 59. 332 BALCH—THE AMERICAN-BRITISH [April 22, negotiate with the American government to that end. And on June 5, 1854, the Hon. William L. Marcy, the American Secretary of State, and Lord Elgin, special British envoy, concluded a treaty relating to the fisheries, commerce and navigation. By its provisions liberty was extended to American fishermen to catch fish of all kinds, ‘‘ except shellfish,” in British or Canadian territorial waters over and above the British territorial waters in which they had the right to fish by the convention of 1818.8 The treaty extended a similar liberty to British subjects of fishing in the American Atlantic territorial waters above the thirty-sixth parallel of north latitude. It provided also for reciprocal free trade between America and the British North American colonies in various articles; and prescribed certain regulations for the navigation of the Saint Lawrence River, Lake Michigan and such Canadian Canals as were necessary to an all water way communication between the Atlantic Ocean and the Great Lakes. The treaty went into effect on March 16, 1855, and, according to the notice of the United States terminated March 17, 1866. During this period friction over the fishery rights of Ameri- can fishermen reserved in British waters by the convention of 1818 were happily avoided. And upon the termination in 1866 of the reciprocity treaty of 1854, the Canadian government, for three years, granted licenses to American fishing vessels, at so much a ton, to exercise the same liberties they had obtained under the treaty of 1854. For the fishing season of 1870 the practice of granting licenses to the American vessels was stopped, and the British government no- tified the government of America that her Britannic Majesty’s gov- ernment was of the opinion that by the convention of 1818 the Amer- ican government had “ renounced the right of fishing, not only within three miles of the colonial shores, but within three miles of a line drawn across the mouth of any British bay or creek.” This com- munication continued : It is, therefore, at present the wish of Her Majesty’s government neither to concede nor for the present to enforce any rights which are in their nature open to any serious question. Even before the conclusion of the reciprocity 31 Treaties and Conventions concluded between the United States of America and other Powers since July 4, 1776,’ Washington, 1889, p. 440. 1909.] ATLANTIC FISHERIES QUESTION. 338 treaty Her Majesty’s government had consented to forego the exercise of its strict right to exclude American fishermen from the Bay of Fundy, and they are of opinion that during the present session that right should not be exercised in the body of the Bay of Fundy, and that American fishermen should not be interfered with, either by notice or otherwise, unless they are found within three miles of the shore, or within three miles of a line drawn across the mouth of a bay or creek which is less than ten geographical miles in width, in conformity with the arrangement made with France in 1839.” ... Her Majesty’s government do not desire that the prohibition to enter British bays should be generally insisted on, except when there is reason to apprehend some substantial invasion of British rights. And in particular they do not desire American vessels to be prevented from navigating the Gut of Canso (from which Her Majesty’s government are advised they may lawfully be excluded), unless it shall appear that this permission is used to the injury of colonial fishermen, or for other improper objects.” On November 25, 1870, an American vessel, the White Fawn, was seized at Head Harbor, New Brunswick, because she had bought herrings intended to be used as bait for fishing. Judge Hazen, of the vice-admiralty court of St. John’s, before whom the case of whether she was liable to forfeiture came, held that though she had bought bait within the British territorial waters, she had not actually proceeded to catch fish with it, and consequently that the seizure could not be sustained.** Previously in June, 1870, the British authorities seized in the North Bay of Ingonish, on the shore of Cape Breton Island, the American fishing vessel, J. H. Nickerson. They charged her with entering to procure bait and of having obtained it. The case came before Sir William Young in the vice-admiralty court at Halifax. In his decision November 15, 1871, while he condemned the vessel to forfeiture because she had bought bait in a British port preparing to fish, Sir William Young admitted that had she merely entered to buy bait without the intention of fishing, she would have been act- ing within her rights.*° ? On this point see Westlake, “ International Law,” Cambridge, 1904, Part I., pp. 184, 187. 5 3%“ Foreign Relations of the United States, 1870,’ Washington, 1870, pp. 419-420. *“ Award of the Fishery Commission: Documents and Proceedings of the Halifax Commission, 1877,” Washington, 1878, Vol. III., p. 3381. 5 Award of the Fishery Commission: Documents and Proceedings of the Halifax Commission, 1877,” Washington, 1878, Vol. III., p. 3395. Bis BALCH—THE AMERICAN-BRITISH [April 22, Commenting on this decision Wharton says :*° In the case here cited there ought to have been no conviction, even under the statute, unless it could have been shown that the purchase was a prepa- ration to fish within the forbidden belt, and that this was put in process of execution. Sir W. Young’s dictum on this point, therefore, cannot be sus- tained as a matter of municipal law. As a ruling of international law it is of no authority, since preparing to fish without fishing is in any view not a contravention of the treaty of 1818. But Sir W. Young’s ruling, on the merits, coincides with that of Judge Hazen, since he concedes that merely buying fish within the three miles is not a violation of the treaty. In order to eliminate the friction caused by such seizures of American vessels in the British fishing grounds, the American- Brit- ish Joint High Commission, which met in Washington in February, 1871, to negotiate a comprehensive treaty whereby “the Alabama Claims,” the chief cause of difference between the two countries, should be submitted to a satisfactory form of arbitration,*” and all other points of difference between America and England then caus- ing friction and dispute and liable to imbitter their peaceable rela- tions should be satisfactorily adjusted, took up for solution with other questions that of the northeastern fisheries. In respect to that question, the Treaty of Washington of May 8, 1871, extended facili- ties and liberty to American fishermen to take fish in the sea fisheries, and to British fishermen like facilities and liberty to catch fish in the American Atlantic sea fisheries north of the thirty-ninth parallel of north latitude.** The treaty provided for reciprocal free trade for a term of years of “ fish-oil” and the fish taken from the sea fisheries between America, and Canada and Newfoundland. As a result of the Treaty of Washington of 1871, the difficulties arising from the divergence of the views of the two governments as to the rights of American citizens to catch fish in the British North American colonial waters, were mostly, during the time the treaty was in operation, smoothed over. However, in Fortune Bay, New- foundland, on Sunday, January 6, 1878, the local inhabitants, pre- ** Francis Wharton, “A Digest of the International Law of the United States,” Washington, 1887, Vol. III., p. 53. “Thomas Balch, “International Courts of Arbitration, 1874,” 3d edition, Philadelphia, 1890. *%“ Treaties and Conventions concluded between the United States of America and other Powers since July 4, 1776,” Washington, 1880, p. 486. 1909.] ATLANTIC FISHERIES QUESTION. 335 vented from fishing by local regulations of Newfoundland, attacked some American fishermen, who, invoking the protection of the pro- visions of the treaty of 1871, prepared to fish.2® The Newfound- landers destroyed the boats and nets of the Americans. In the official correspondence that ensued, the British government argued that the treaty granted to the Americans only the right to fish in common with British subjects, and thus the former were amenable to the local Newfoundland laws and regulations. The American authorities contended that the local laws could not be allowed to regulate or prescribe the provisions of the treaty ; in addition they maintained that damages were due the American fishermen because of the violent attack on them. Eventually this dispute was adjusted by a money payment by Great Britain to the United States of £15,000 “ without prejudice to any question of the rights of either government under the treaty of Washington.”*? Ex- cept for this incident the fishing seemed to proceed smoothly until, upon the giving of due notice by the United States, the provisions of the treaty of 1871 regulating the fisheries came to an end on July 1, 1885. Asa result of informal negotiations between Secretary Bay- ard for America, Minister West for Great Britain, and Sir Ambrose Shea for Canada, it was agreed that the privileges of inshore fishing in the respective American and British waters to which the provi- sions of the treaty had applied would be continued for the whole season of 1885. In the year 1886 the Canadian authorities seized many Ameri- can fishing vessels. On May 6 of that year the Canadian steamer Landsdowne seized in Annapolis Basin, Nova Scotia, a landlocked harbor, where it would seem ridiculous to suppose that an American vessel would attempt to fish, the David J. Adams of the American fishing fleet.* She was then taken by the Canadian authorities to Saint Johns, New Brunswick, and on May to brought back to Digby, Nova Scotia, *® House Executive Documents, No. 84, 46th Congress, 2d Session, Wash- ington, 188o. * “ Foreign Relations of the United States, 1881,” Washington, 1882, p. 500. “Foreign Relations of the United States, 1886,’ Washington, 1887, pp. 341-346, 373-380, 396-404. PROC, AMER. PHIL. SOC., XLVIII. 193 W, PRINTED JANUARY 4, IQIO. 336 BALCH—THE AMERICAN-BRITISH [April 22, without any explanation or hearing being given to her captain. At Digby, a paper, which was alleged to be the legal precept for her capture and detention, was nailed to her mast. But this alleged writ was placed so high that it could not be read. The Canadian authorities refused the requests of both the captain of the vessel and of the American Consul General to be allowed to detach this paper in order to learn its contents Neither would the captain of the Landsdowne tell the American Consul General the ground upon which he had captured the American vessel. After many vigorous protests by Secretary Bayard and Minister Phelps to Lord Rose- berry, the British Foreign Secretary, Sir Lionel Sackville West, the British Minister at Washington, communicated to Mr. Bayard a minute of the Canadian privy council that agreed that the condemna- tion proceedings against the David J. Adams should be stopped for the alleged violation of the fishery statutes, provided that the owners of the vessels would agree that they would not base upon this discontinuance a claim for damages or expenses. This minute of the Canadian privy council was practically an avowal that the seizure of the David J. Adams had been made without good or suffi- Clenipicatlsea On October 7, 1886, a little before midnight, the American fish- ing vessel, Marion Grimes, arrived seeking refuge from a storm at sea, at the outer harbor of Shelbourne, Nova Scotia.*? She an- chored about seven miles from the port of Shelbourne, no one leav- ing her until six o’clock the next morning. She then hoisted sail and stood out to sea. As soon as she had started, however, the Canadian cruiser Terror sent a boat’s crew to arrest the Marion Grimes. Captain Landry of the American vessel, was then forced to proceed to Shelbourne to appear before the collector of customs there. In spite of the fact that the customs house was closed during the night, that the storm proved he had merely sought a haven of refuge from its violence, that he had stayed a very short time and that the Marion Grimes was equipped only for deep sea fishing, Captain Landry ““ Foreign Relations of the United States, 1888,” Washington,*1889, Part ep coz! *“ Foreign Relations of the United States, 1886,” Washington, 1887, pp. 362-370. 1909.] ATLANTIC FISHERIES QUESTION. 337 was fined $400. This fine was imposed chiefly by the insistence of Captain Quigley, commander of the Terror. Captain Landry then applied to Mr. White, the American consular agent. Owing to the importance to the success of the venture of the Marion Grimes that she should not be detained, Mr. White at once telegraphed the facts of the case to Mr. Phelan, the American Consul General at Halifax. Mr. Phelan took the matter up with the assistant commis- sioner of customs at Ottawa, who replied the fine could not be re- duced, but that the $400 could be deposited at Halifax, to await a de- cision in the case. Mr. Phelan made the deposit at Halifax and tele- graphed to Captain Landry he was at liberty to take his vessel to sea. On October 11, Captain Landry, whose vessel had by that time been held up four days, telegraphed to Consul General Phelan that ‘ the custom-house officers and Captain Quigley” refused to let him go to sea. The next morning the consul general called on the col- lector of Halifax to learn if the order to release the Marion Grimes had been issued, and was told such an order was sent, “ but that the collector and the captain of the cruiser refused to obey it, for the reason that the captain of the seized vessel hoisted the American flag while she was in custody of the Canadian officials.” Mr. Phelan telegraphed this news to the assistant commissioner at Ottawa, ‘ and received a reply dated October 12 that the “ collector had been instructed to release the Grimes from customs seizure. This depart- ment has nothing to do with other charges.’’ The same day the col- lector of customs at Halifax sent a dispatch to the collector at Shel- bourne to release the Marion Grimes, in which he said that “ this de- partment (customs) has nothing to do with the other charges. It is the department of marines.” What happened concerning the hoisting of the American flag by the captain of the M/arion Grimes over his vessel was thus told by Secretary Bayard in a dispatch to Minister Phelps: On October 11 the Marion Grimes, being then under arrest by order of local officials for not immediately reporting at the custom house, hoisted the American flag. Captain Quigley who, representing, as appeared, not the revenue, but the marine department of the Canadian administration, was, with his “cruiser” keeping guard over the vessel, ordered the flag to be hauled down. This order was obeyed; but about an hour afterwards the flag was again hoisted, whereupon Captain Quigley boarded the vessel with an armed 338 BALCH—THE AMERICAN-BRITISH [April 22, crew and lowered the flag himself. The vessel was finally released under orders of the customs department, being compelled to pay $8 in addition to the deposit of $400 above specified. For this insult to the American flag, Secretary Bayard demanded an apology, and December 7, 1886, the British Minister at Washing- ton, under instruction from the Earl of Iddesleigh, British Secre- tary of Foreign Affairs, communicated to the American government a communication from the government of the Dominion of Canada apologizing for the hauling down of the flag of the Marion Grimes by Canadian officials.** Owing to this harassing of American fishermen in Canadian territorial waters, under the guise that they transgressed the Can- adian customs regulations, the American Congress on March 3, 1887, approved an act whereby power was given to the president to retal- lage upon the Canadians. Negotiations, with a view to arrange an amicable settlement were continued by the American and the British governments.*® Finally a convention was agreed upon at Washington, February 15, 1888, subject to ratification by the American Senate, the Canadian Parlia- ment and the Newfoundland Legislature.*® This convention provided that the width of exclusively territorial bays, wherein American fishermen were excluded from taking fish by the Treaty of 1818, should be extended from six miles from shore to shore, according to the well-recognized and established custom of International Law, to a distance of ten miles from land to land. Thereby the extent of Canadian and Newfoundland terri- torial waters from which American fishing vessels were barred was increased. In addition, the convention restricted American fisher- men from fishing in specifically named bays, such as the Baie des Chaleurs in New Brunswick, and Fortune Bay in Newfoundland, that varied in width from ten to twenty-one miles from shore to ““ Foreign Relations of the United States, 1886,” Washington, 1887, pp. 491, 492. * Senate Executive Documents, No. 113, 5oth Congress, rst Session, Wash- ington, 1888, pp. 56-65, 112-1109. ** Senate Executive Documents, No. 113, 50th Congress, rst Session, Wash- ington, 1888, pp. 127-142. Joseph I. Doran, “ Our Fishery Rights in the North Atlantic,” Philadelphia, 1888, pp. 54-67. 1909.] ATLANTIC: FISHERIES -QUESTION. 339 shore. In that way the extent: of territorial waters from which American fishermen were excluded under the treaty of 1818 was still further extended. The convention guaranteed free passage to American fishing vessels through the Gut of Canso,** a right to which they were entitled by the Law of Nations. The convention also provided a right of refuge to American fishermen in Canadian ports fleeing from the danger of storms—a right to which all sea- faring men are entitled in the ports of all civilized countries—and, when the American vessels needed to make repairs, the privilege to land their catch and tranship it to America. In view of the very great advantages that were given by this convention to Canada and Newfoundland in exchange for rights which American fishing vessels already possessed under the Law of Nations without any grant by treaty from either Canada or New- foundland, the American Senate very properly refused August 21, 1888, to confirm the convention, and so it failed to become a treaty. During the latter part of 1890 and the beginning of 1891, Secre- tary Blaine for America and Sir Julian Pauncefote for Great Britain held numerous parleys concerning the fishery question as between America and Newfoundland. Their negotiations finally re- ‘sulted in a convention known as the Blaine-Bond Convention, since Sir Robert Bond, the Newfoundland premier, inspired the negotia- tions of the British Minister.4* This convention was to last for five years from the date it should go into operation, and might thereafter be renewed from year to year. It provided that Amer- ican fishing vessels entering Newfoundland waters should have the privilege of buying bait on the same terms as Newfoundland fish- ing vessels. Also it was agreed that American fishing vessels should “ have the privilege of touching and trading, selling fish and oil, and procuring supplies in Newfoundland, conforming to the harbor regulations, but without other charge than the payment of such light, harbor and customs dues as are or may be levied on New- * Senate Executive Documents, No. 113, 50th Congress, 1st Session, Wash- ington, 1888, p. 135. John Westlake, “International Law,’ Cambridge Univer- sity Press, 1904, Part I., p. 193. *°“ Convention between the United States of America and Great Britain, for the Improvement of Commercial Relations between the United States and Her Britannic Majesty’s Colony of Newfoundland.” This unratified agree- ment is known as the Blaine-Bond Convention. 340 BALCH—THE AMERICAN-BRITISH [April 22, foundland fishing vessels.” The convention provided for a recipro- cal free exchange of various American and Newfoundland products. To make the convention operative the plenipotentiaries agreed that it should be subject to ratification by the American Senate and Her Britannic Majesty, and that it should “take effect as soon as the laws required to carry it into operation shall have been passed by the Congress of the United States on the one hand, and the Imperial Parliament of Great Britain and the provincial legislature of New- foundland on the other.” Owing to a vigorous protest from the Canadian government, the British imperial government in a memo- randum addressed on May 21, 1891, by the British Legation at Washington to the State Department, notified the American govern- ment that it could not agree to ratify the convention, “unless pari passu with the proposed Canadian negotiations.” A joint commission of two experts, one named by each govern- ment, to examine and report upon the subject was agreed upon in 1892; and the commission reported early in 1897. The northeastern fisheries question was included in the work submitted for adjustment to the American-British Joint High Com- mission that met and organized for business at Quebec, August 23, 1898. Owing to thé Joint High Commission being unable to come to a satisfactory agreement concerning the eastern frontier of the Alaska lisiére, which was then in dispute between the American re- public and the British empire, the Joint High Commission adjourned in. March, 1899, without having arranged the fisheries or any other of the questions submitted to it.*® In 1895 and again in 1898 Canada unsuccessfully sought reciproc- ity herself. Secretary of State Hay and Ambassador Herbert took up at Washington the discussion of the fisheries as between America and Newfoundland and finally agreed on November 8, 1902, upon a new convention, known after the American Secretary of State and the Newfoundland premier who inspired the negotiations of the British Ambassador, as the Hay-Bond Convention.*° ® Thomas Willing Balch, “The Alaska Frontier,” Philadelphia, 1903, pp. 162, 168. ° Senate Executive Documents, No. 49, 57th Congress, 2d Session. “A Convention with Great Britain, signed at Washington on November 8, 1902, for the Improvement of Commercial Relations with Newfoundland.” 1909.] ATLANTIC FISHERIES QUESTION. 341 As in the case of the Blaine-Bond Convention of 1891, the Hay- Bond Convention of 1902 provided that the American fishing ves- sels should fish in the Newfoundland waters subject to the local Newfoundland regulations regulating Newfoundland fishing vessels. The convention also provided for reciprocal free trade concessions, whereby Newfoundland gained vastly more than she gave.*? The Hay-Bond Convention remained in the Senate Committee on Foreign Relations unacted on, for three years. On June 15, 1905, the Newfoundland government enacted an act intended to hamper the American fishing vessels in their lawful occupation of taking fish under the provisions of the first article of the Treaty of 1818.°?. In the autumn of 1905, Premier Bond notified Secretary Hay of certain concessions he was willing to have inserted in the Hay-Bond Convention in the form of senate amendments. After these amendments were added by the Committee on Foreign Rela- tions, the Senate as a whole made further changes that it was so clear would not be satisfactory to Newfoundland, that the conven- tion as amended was never brought to a vote in the Senate and so never became a treaty. In view of the probable serious interference by the Newfound- land authorities with the American fishing vessels in taking fish in those territorial waters of Newfoundland on the southern coast of Newfoundland from Cape Ray eastward to the Rameau Islands, and up along the western coast of the island from Cape Ray and round on the north coast to Quirpon Islands as guaranteed to them by the Treaty of 1818, Mr. Root, the American Secretary of State, wrote on October 19, 1905, to Sir Mortimer Durand, the British Ambassador at Washington, an expression of some of the views held on the fisheries question by the American government. Reas- serting once again the view of the American government of the right of American fishing vessels to fish in the treaty waters unham- pered by the local regulations of Newfoundland, he said:°° ** Speech of Senator Henry Cabot Lodge, April 2, 1903. 2 Supplement to the American Journal of International Law,’ James Brown Scott, chief editor, January, 1907; “An Act of Newfoundland Respect- ing Foreign Fishing Vessels,” p. 22. %“ Foreign Relations of the United States,” 59th Congress, Ist Session, 1905. House Documents, Vol. I., Washington, 1906, p. 491. 342 BALCH—THE AMERICAN-BRITISH [April 22, Any American vessel is entitled to go into the waters of the treaty coast and take fish of any kind. She derives this right from the treaty (or from conditions existing prior to the treaty and recognized by it) and not from any permission or authority proceeding from the government of Newfoundland. Secretary Root also called Sir Mortimer Durand’s attention to the evident hostile animus of the colony of Newfoundland towards American fishing vessels as shown by the “ Foreign Fishing Act” enacted the previous June by the Newfoundland government. The provisions in that act that gave authority to Newfoundland officials to search any foreign fishing vessel in any of the territorial waters of Newfoundland and upon finding any bait or fishing ap- parel to arrest and bring the vessel into port, Secretary Root pointed out were a clear and palpable infringement of American rights under the Treaty of 1818 in the treaty waters. Secretary Root also referred Sir Mortimer Durand’s attention, as a result of the New- foundland legislation that prohibited the sale of bait by the New- foundlanders to American fishing vessels, to the unrest and pro- found dissatisfaction existing among the local population living along the shores of or near the “ Bay of Islands” on the west coast of Newfoundland with the resulting situation and the risk of serious violence resulting therefrom. To these observations of the American Secretary, the British Ambassador in reply enclosed in a note of February 2, 1906, to Mr. Reid, the American Ambassador at London, a memorandum of Sir Edward Grey, the British Foreign Secretary.®® In this memorandum the British government replied that the privileges of fishing “ con- ceded” by the Treaty of 1818 in some of the territorial waters of Newfoundland were “ conceded, not to American vessels, but to in- habitants of the United States and to American fishermen.” The British memorandum reasserted the old view enunciated by Earl Bathurst, that by the Treaty of 1818 “a new grant to inhabitants of the United States of fishing privileges within the British Jurisdic- tion” was made. In the memorandum it was further maintained that “ American fishermen ” could not claim to exercise the right of *“ Supplement to the American Journal of International Law,” January, 1907, p. 22. ®° “ Supplement to the American Journal of International Law,” October, 1907, P. 355. 1909.] ATLANTIC FISHERIES QUESTION. 343 fishing within the territorial waters of Newfoundland “on a footing of greater freedom than the British subjects ‘in common with’ whom they exercised it under the convention. In other words, the American fishery under the convention is not a free but a regulated fishery, and, in the opinion of His Majesty’s government, American fishermen are bound to comply with all colonial laws and regulations, including any touching the conduct of the fishery, so long as these are not in their nature unreasonable, and are applicable to all fish- ermen alike.” The British note went on to argue that all American and other foreign vessels sojourning within British territorial waters should obey the local law, “ and that, if it is considered that the local jurisdiction is being exercised in a manner not consistent with the enjoyment of any treaty rights, the proper course to pursue is not to ignore the law, but to obey it, and to refer the question of any alleged infringement of their treaty rights, to be settled diplomati- cally between their government and that of His Majesty.” In reply to Secretary Root’s contention that the Newfoundland foreign fishing-vessel act of June 15, 1905, was directed against American fishing vessels so as to interfere with their rights in the treaty waters the British memorandum maintained that that act, especially the first and third sections, upon which Secretary Root had largely based his complaint, was not aimed at the rights of American ves- sels in particular. The memorandum referred to the seventh section of the act, as safeguarding “the rights and privileges granted by treaty to the subjects of any state in amity with His Majesty.” And then the British note went on to admit that “the possession by in- habitants of the United States of any fish and gear which they may lawfully take or use in the exercise of their rights under the con- vention of 1818 cannot properly be made prima facie evidence of the commission of an offense, and, bearing in mind the provisions of section 7, they can not believe that a court of law would take a dif- ferent view.” Nevertheless, this was an admission by the British Foreign Office that the act was so framed that the Newfoundland officials could, through legal processes, so harass and “ hold up” an American fish- ing vessel that her trip would be rendered unprofitable, as hap- pened in many cases during the latter eighties in the ports and terri- 3044 BALCH—THE AMERICAN-BRITISH [April 22, torial waters of Nova Scotia, for example in the case of the Marion Grimes. As a result of the views expressed by Secretary Root in his letter of October 19, 1905, the Newfoundland government repealed the act to which he objected and enacted on May 10, 1906, a second act relating to fishing in her territorial waters by foreigners.°® The new act was drawn so as to avoid for American fishing vessels the two special provisions against which Secretary Root had complained, but at the same time new provisions that were added gave the power to obstruct and harass American vessels in their fishing ventures should it become advisable. To the views of the British government as expressed in its memo- randum of February 2, 1906, Secretary Root replied in an elaborate and able letter on June 30, 1906, addressed to the American Am- bassador at London, Mr. Reid, by whom it was communicated to Sir Edward Grey.** Secretary Root protested in this letter against the possible inferences suggested in the memorandum that the New- foundland government has the right to require of any American captain entering the treaty waters or any port of the colony to fur- nish evidence that all the members of his crew are inhabitants of the United States. and the Secretary of State denied the assertion that the colony of Newfoundland has the right irrespective of any agreement on the subject, between the parties to the Treaty of 1818, America and Great Britain, to interfere through local legislation with the American fishing vessels in the exercise of their fishery rights under the Treaty of 1818. In previous correspondence regarding the construction of the Treaty of 1818, the government of Great Britain has asserted, and the memorandum under consideration perhaps implies, a claim of right to regulate the action of American fishermen in the treaty waters, upon the ground that those waters are within the territorial jurisdiction of the colony of Newfoundland. This government is constrained to repeat emphatically its dissent from any such view. The Treaty of 1818 either declared or granted a perpetual right to the inhabitants of the United States which is beyond the sovereign power of England to destroy or change. It is conceded that this right is, and forever °°“ Supplement to the American Journal of International Law,” January, 1907, p. 24. ** Supplement to the American Journal of International Law,” October, 1907, p. 364. 1909. ] ATLANTIC FISHERIES OQUESRION, 3845 must be, superior to any inconsistent exercise of sovereignty within that terri- tory. The existence of this right is a qualification of British sovereignty within that territory... . For the claim now asserted that the colony of Newfoundland is entitled at will to regulate the exercise of the American treaty right is equivalent to a claim of power to completely destroy that right. As a result of this vigorous exchange of views between the America and the British government, a modus vivendi, with the object of avoiding any clash between the American fishermen and the Newfoundland authorities or inhabitants during the fishing season of 1906-07, was concluded early in October, 1906, at Lon- don, between the two governments that were parties to the Treaty of 1818.°° The British government agreed to the use of purse seines, and the shipment of Newfoundlanders by American vessels outside the three-mile limit. On the other hand the American gov- ernment waived the right of American vessels to take fish on Sun- day, and agreed that they would pay lighthouse dues, and where possible comply with the local customs regulations. The provisions of the Foreign Fishing Vessels Act of 1906 of Newfoundland, and the objectionable first and third sections of the Act of 1905 were not to apply to American vessels. With this agreement in force, the fishery of 1906-07 was happily accomplished without unto- ward incident. At the beginning of September, 1907, a new modus vivendi to apply to the next fishery season was agreed to by the two interested nations.®® This new modus vivendi was practically the same in its provisions as that of the previous season, except that the American government made a further concession of waiv- ing the use of purse seines. In July, 1908,*the modus vivendi of the previous year was renewed for the fishery of 1908—'o9.°° In order to finally settle this vexatious dispute between the American republic and the British empire over the Atlantic fisheries question, in January, 1909, the two Powers at a conference held in Washington agreed to refer the matter to the decision of The Hague *“ Supplement to the American Journal of International Law,” January, 1907, Pp. 27-31. °“ Supplement of the American Journal of International Law,” October, 1907, PP. 375-377. ° « Supplement of the American Journal of International Law,” October, 1908, pp. 327-328. 346 BALCH—THE AMERICAN-BRITISH [April 22, International Court. At this conference, America was represented by Secretary of State Root, and the British empire, by Ambassador Bryce, who was aided by Mr. Aylesworth and Mr. Kent respectively for the Dominion of Canada and the Colony of Newfoundland. In deciding upon the American-British Atlantic fisheries dispute The International Court at The Hague will be called upon, accord- ing to the terms of the Root-Bryce Treaty of January, 1909, to give its decision upon first the right of American fishing vessels under Article I. of the Treaty of 1818 to take fish in the bays and gulfs, more than six miles wide; whether the rights retained to inhabitants of the United States by the Treaty of 1818 concluded between Amer- ica and Great Britain, two sovereign States members of the family of nations, can be regulated at will by the legislation of either Great Britain herself or one of her colonies or whether all changes or reg- ulations applicable to the treaty can only be made by a mutual agree- ment between the original high contracting parties, the American republic and the British empire; and also, whether the inhabi- tant of the United States have the liberty under Article I. of the Treaty of 1818 to take fish in the territorial waters along that part of the southern coast of Newfoundland which extends from Cape Ray to the Rameau Islands, or along the western and northern coast of Newfoundland from Cape Ray to Quirpon Islands or in the territorial waters of Canada around the Magdalen Islands? By an agreement, expressed in two letters exchanged on January 27, 1909, between Secretary Root and Ambassador Bryce, the right of American vessels to pass through the Gut of Canso and to take fish in the Bay of Fundy are not to be submitted for decision to the International Court at The Hague. While the right of “innocent passage” by American vessels through the Gut of Canso will not be submitted to The Hague Court, yet the raising of that point by Canada in the past is too illumi- native of the whole fishery question to pass it over without notice. About 1839 the point was raised by the authorities of Nova Scotia that the Gut of Canso,*! a passage of salt water connecting the Atlantic Ocean and the Gulf of Saint Lawrence that passed * Senate Executive Documents, No. 100, 32d Congress, Ist Session, Wash- ington, 1852, pp. 73-74. 1909.] ATLANTIC FISHERIES QUESTION. 34 between the Province of Nova Scotia and the neighboring island of Cape Breton, a part of the colony of Nova Scotia, was not a free passage to American vessels, because the Gut of Canso, which at some points was only a mile wide, belonged as territorial waters to Nova Scotia. Though this attempt to lay a claim to close the Gut of Canso as a free highway of the sea to American vessels was not seriously pushed at the time, the effort to claim the right to close it to American vessels was renewed in the Bayard-Chamberlain Con- vention of 1888.°? In that instrument Canada proposed to guaran- tee to American fishing vessels the free passage through the Gut of Canso. But Canada was thereby undertaking to concede to Amer- ica what already belonged to America as a right by the Law of Na- tions. Not only in 1888 but long before that it was a well-estab- lished principle of International Law that passages of the sea con- necting two large bodies of water, were open to navigation by ves- sels of all powers. Westlake, who for twenty years held the chair of International Law in Cambridge University, and for six years was one of the English members of The Hague International Court and to-day is in the forefront of international jurists, in speaking of the right of passage through straits, says :°° If the strait connects two tracts of open sea, as the Gut of Canso between Cape Breton Island and the mainland of Nova Scotia, or the Straits of Magellan and the other passages in the extreme south of America, the lawful ulterior destination is clear, and there is a right of transit both for ships of war and for mechantmen. Many other authorities can be cited to the same purpose, but in view of this clear statement by Westlake, who, together with Holland of Oxford, is one of Great Britain’s leading living authori- ties on questions of International Law, it does not seem worth while. The attempt at various times to include within the jurisdiction of Canada and Newfoundland bays and gulfs more than six miles in width, such as the Bay of Fundy and the Baie des Chaleurs, for instance, is an attempted restriction on the freedom of the high seas. * Senate Executive Documents, No. 113, 50th Congress, 1st Session, Wash- ington, 1888, p. 135. * John Westlake, “International Law,” Part I., “ Peace”; Cambridge, 1904, Pp. 193. 348 BALCH—THE AMERICAN-BRITISH [April 22, Ever since the famous argument between Grotius and Selden as to whether the high seas should be free to the vessels of all the world or whether parts, greater or smaller as the case might happen to be, of the high seas should be subject to the jurisdiction of one nation, the verdict of the world has leaned more and more towards the view of the famous Hollander.** Practically all international jurists are agreed now that the high seas are free and that the terri- torial waters of a nation only extend to three miles from land and over those bays or portions of them that are not more than six miles across from shore to shore. The learned Belgian jurist, Mr. Justice Nys, a member of the Court of Appeals of Brussels and of The Hague International Court, thus sums up the question of the freedom of the high seas. He says :© La haute mer, la pleine mer, la mer pour employer la désignation usuelle, est libre. Elle n’est pas susceptible de possession et de propriéte a cause de sa nature physique, de la mobilité et de la fluidité de ses flots, de l’étendue sur laquelle devrait s’appliquer la sanction des ordres ou des prohibitions; elle ne peut tomber sous le droit de police, de suprématie, d’empire d’un ou de plusieurs Etats a cause de l’egalité juridique des membres de la société internationale. Oppenheim who now sits as successor to Westlake, by whom he was chosen, in the chair of International Law at Cambridge Univer- sity, holds that many enclosed seas that are connected with the ocean by passages less than six miles in width are as free to navigation * Le Comte de Garden, “ Traité Complet de Diplomatie,” Paris, 1833, Vol. I., pp. 402-404. A. G. Heffter, “Le Droit International de l'Europe; Qua- trieme édition Francaise, augmentée et annotée par F. Heinrich Geffcken,” Berlin and Paris, 1883. F. de Martens, “Traité de Droit International,” traduit du Russe par Alfred Léo, Paris, 1883, Vol. I., pp. 491-494. Alphonse Rivier, “ Principes du Droit des Gens,” Paris, 1896, Vol. I, pp. 236-237. Hannis Taylor, “A Treatise on International Public Law,” Chicago, 1901, pp. 290-294. John Westlake, “International Law,’ Cambridge, 1904, Part I., pp. 160-163. Ernest Nys, “ Les Origines du Droit International,” Paris and Brussels, 1894, pp. 379-387; “Le Droit International, Les Principes, les Théories, les Faits,” Paris and Brussels, 1905, Vol. II., pp. 135-138. L. Oppenheim, “ Inter- national Law,’ London, 1905, Vol. I., pp. 300-306. George B. Davis, “ Ele- ments of International Law,’ New York, 1908, p. 57 et seq. *® Ernest Nys, “Le Droit International, Les Principes, les Théories, les Faits,” Paris and Brussels, 1905, Vol. II., p. 134. 1909. ] LEAN ISH RIES OuUESPON. 349 for the vessels of all nations as any part of the ocean. He says:* The enclosure of a sea by the land of one and the same state does not matter, provided such a navigable connection of salt water as is open to vessels of all nations exists between such sea and the general body of salt water, even if that navigable connection itself be part of the territory of one or more riparian states. Wheras, therefore, the Dead Sea is Turkish and the Aral Sea is Russian territory, the Sea of Marmora belongs to the open sea, although it is surrounded by Turkish land and although the Bosphorus and the Dardanelles are Turkish territorial straits, because these are now open to merchantmen of all nations. So, too, Hudson’s Bay is a part of the high seas, for the en- trance to that large interior sea to the vessels of all nations is through Hudson Strait that is much more than six miles wide. It is only within territorial waters that a state can by its legisla- tion restrict vessels of other nations from doing all those things that the vessels of all nations can properly do upon the high seas. What are the territorial waters of each state? Phillimore, judge of the British High Court of Admiralty, says :* The limit of territorial waters has been fixed at a marine league, because that was supposed to be the utmost distance to which a cannon-shot from the shore could reach. The great improvement recently effected in artillery seems to make it desirable that this distance should be increased, but it must be so by the general consent of nations, or by specific treaty with particular states. The three-mile limit as the extent of the territorial waters of nations along their sea front, except where a modification has been made by treaty between the contracting parties, is to-day universally recognized. With the aim of bringing about a universal change in the extent of the territorial belt of waters along the sea front of nations, the Institute of International Law in March, 1894, after careful con- sideration and weighing the arguments pro and con, gave it as its opinion that the belt of territorial waters along the coast line of each nation should be extended from three to six miles from low water.®* *®T. Oppenheim, “ International Law,” London, 1905, Vol. I., p. 307. *% Sir Robert Phillimore, “Commentaries upon International Law,” second edition, London, 1871, Vol. I., p. 237. Phillimore was a member of Her Majesty’s Privy Council and judge of the High Court of Admiralty. The first edition of this volume appeared in 1854. 8 Charles Calvo, “ Le Droit International,’ Paris, 1896, cinquiéme edition, Vol. VI., p. 67. 350 BALCH—THE AMERICAN-BRITISH [April 22, And that in the case of bays the line from headland to headland that should show where the open sea ended should be twelve miles across, except in those cases where immemorial usage had consecrated a greater distance. In view of the modern development of arms and the more rapid means of communication and the vast expansion of commerce, this would seem to be a most admirable change in the universally existing recognition of the extent of territorial waters. But the Institute of International Law is a body of gentlemen learned in the Law of Nations and not a congress of representatives from all the nations of the earth with plenary powers to change the Law of Nations for the best interests of mankind. Consequently, however advisable the recommendation of the institute may be, it cannot change the extent of territorial waters unless the nations of the world agree. And America has not joined in any such agreement. But even if the American government had joined the governments of other nations to double the extent of the territorial belt of water, yet such an agreement would not alter the extent of the rights of American fishermen to catch fish in the Bay of Fundy, the Baie des Chaleurs and other smaller bodies of water as defined in the first Article of the Treaty of 1818. The limit of the area over,which American fishing vessels can take fish along the coasts of the maritime provinces of the Dominion of Canada and New- foundland, is limited only by the recognized three mile limit, except that in the treaty waters American vessels have rights to catch fish that the vessels of other nations do not possess. In addition to attempting to offer to America the right for Ameri- | can fishing vessels to navigate the Gut of Canso and also to curtail the area over which they possess the right to catch fish in the high seas close to the shores of Canada and Newfoundland, both Canada and Newfoundland have sought by various local legislation to so hamper American fishing vessels in their just rights to take fish as to make their occupation unprofitable. The aim of all these various attempts of Canada and Newfound- land to nullify the privileges of American fishing vessels as de- fined by article one of the Treaty of 1818 has been to force America to grant to Canada and Newfoundland favorable trade reciprocity. But the contracting parties to the Treaty of 1818 were neither Can- 1909.] ALUAN TIC PISHERIES QUESTION: 351 ada nor Newfoundland. The contracting parties to that treaty were the American republic and the British empire. Of what use would it be for these two sovereign members of the family of nations to agree solemnly by treaty to define the respective rights of their sub- jects in the Atlantic fisheries, if power was reserved to either party by local legislation to completely nullify the plain and evident intent of the treaty which recognizes that American fishing vessels pos- sessed in those waters certain rights and privileges to catch fish that the fishing vessels of all other nations do not possess under the ordinary Law of Nations. As Vattel justly says, treaties are sacred contracts between nations.*® The Brazilian jurist Calvo, after quoting in full the text of article one of the Treaty of 1818, says of the purpose of this article :*° Rien dans cet article ne permet d’inférer que la Grande-Bretagne ait conféré aux Etats-Unis le droit de péche. Ceux-ci n’ont fait que renoncer a certains privileges, ce qui implique, de la part de l’Angleterre, que ces privi- léges existaient et que les Etats-Unis ont uniquement cédé une fraction de leur droit souverain. La Grande-Bretagne n’a pas dit aux Etats-Unis: “ Venez seulement pour chercher un abri ou faire de l’eau ou du bois,” mais les Etats- Unis disent a la Grande-Bretagne: “ Nous, les proprietaires en commun de ces pécheries consentons a ne pas prendre de poissons et a ne pas les secher ou les saler dans certaines limites, et 4 ne pas abuser d’ailleurs de privileges qui nous sont concédés.” And he goes on to say :** Jamais loi municipale ne saurait prévaloir sur une convention internationale. The uselessness for members of the family of nations to make certain agreements by formal treaty, if those agreements could be nullified by the local legislation of a colony or province or state of a party to the treaty contract seems self-evident. In the constitution of the United States provision is made to insure the maintenance of ® Vattel, “Le Droit des gens,” Paris and Lyons, 1820, Vol. II., p. 25. “Charles Calvo, “Le Droit International Théorique et Pratique,” cin- quiéme édition. Vol. I., Paris, 1896, pp. 486-487. ™ Charles Calvo, “Le Droit International Théorique et Pratique,” cin- quiéme édition, Paris, 1896, Vol. I., pp. 487-488. PROC. AMER. PHIL. SOC,, XLVIII. 193 X, PRINTED JANUARY 5, IQIO. 352 BALCH—THE AMERICAN-BRITISH [April 22, international treaties entered into by the American federal govern- ment. Article sixth of the American Constitution says: All treaties made or which shall be made, under the authority of the United States shall be the supreme law of the land; and the judges in every State shall be bound thereby, anything in the constitution or laws of any State to the contrary notwithstanding. The chief powers of Europe at the London conference in 1871, on January 5, adopted, as the Russian jurist de Martens tells us, this principle :” The plenipotentiaries of the North German Confederation, Austria- Hungary, Great Britain, Italy, Russia and Turkey, to-day assembled en confé- rence, recognize that it is an essential principle of the Law of Nations that no power can liberate itself from the engagements of a treaty, nor modify its stipulations except with the consent of the contracting parties obtained by means of an amicable arrangement. Thus Great Britain has affirmed the sanctity of treaties in a for- mal manner. Very properly America maintains that any modifica- tion of the rights of American fishing vessels under the Treaty of 1818, whether by amendment to that treaty or by police or maritime or customs or other regulation, can only be accomplished by agree- ment between the two parties to the contract known as the Treaty of 1818, the governments of the United States of America and of the British empire. Were an opposite doctrine recognized by the Hague International Court, what would become of the validity of many international treaties in force to-day between the nations of the earth. At the bar of the Hague International Court the United States of America will appear to defend the maintenance and sanc- tity of international contracts known under the generic name of treaties. ™ For the argument of the strict constructionists see William E. Mikell, “The Extent of the Treaty Making Power of the President and the Senate of the United States,” University of Pennsylvania Law Review and American Law Register, 1900, pp. 435-458, 528-562. For the argument of the loose constructionists see Chandler P. Anderson, “The Extent and Limitations of the Treaty Making Power under the Con- stitution,” The American Journal of International Law, July, 1907, pp. 636-670. See also the exhaustive treatise of Charles Henry Butler, “ The Treaty- making Power of the United States,’ New York, 1902. EF. de Martens, “ Traité de Droit International,” traduit du Russe par Alfred Léo, Paris, 1883, Vol. I., p. 546. 1909. ] ATLANTIC FISHERIES QUESTION. 353 All through the negotiations relating to the fisheries question since the treaty of partition of 1783, the British empire and her two colonies of Canada and Newfoundland have sought to cut down the rights assigned by the partition treaty of 1783 to American citizens to catch fish in the territorial waters adjoining the Gulf of Saint Lawrence and the adjoining regions. Some of those rights America consented in the formal Treaty of 1818, concluded with the British imperial government, to give up. But not satisfied with the substan- tial gains then obtained, both Canada and Newfoundland through one subterfuge or another, have again and again tried to obtain more concessions from America by offering a shadow, as guarantee- ing the right, for example, for American fishing vessels to navigate the Gut of Canso, for a reality. As in the case of the Alaska fron- tier where Canada’s land claims grew greater with the passing of the years, so in this fisheries dispute the position of America on the one hand, and of Great Britain, Canada and Newfoundland on the other hand, is well summed up in the words with which Count Nessel- rode, nearly ninety years since, contrasted the positions of the Musco- vite and the British empires when they were discussing their Russo- British American frontier : Ainsi nous voulons conserver, et les compagnies angloises veulent acquerir. THE BURNING BUSH AND THE ORIGIN OF JUDAISM. Bye JAIUIL, JEUNE Ie. (Read April 23, 1909.) Last autumn four members of our Society were invited by the German Emperor to attend the first performance of Friedrich Delitzsch’s Sardanapal at the Royal Opera in Berlin. The climax of this historical pantomime, which is based on Lord Byron’s tragedy Sardanapalus and a ballet of Paul Taglioni,* is the great pyre in the last scene, on which Sardanapalus burns himself with his queen, his attendants, and his treasures. The whole stage is full of fire; but, of course, nothing is burnt. The blaze is pro- duced by steam with reflected red light. In the same way you see the stage full of fire in the last scene of Richard Wagner’s musical drama Die Walkiire. \Wodan passes through the flames, but he is not scorched. The black cloud over Mount Vesuvius has a fiery aspect at night, but this is merely the reflex of the fiery lava within the crater. The pillar of smoke over a volcano consists chiefly of steam and ashes. Volcanic eruptions are often not central, but lateral. The great eruption of Mont Pelé in the northern part of the island of Martinique, on May 8, 1902, was a lateral eruption. In the case of Mount Etna, lateral eruptions are more frequent than eruptions from the central crater. There are several hundred parasitic craters on the flanks of Mount Etna, especially on the southern side, in the zone between an altitude of 1,000 and 2,000 meters. This region is wooded. The volcano is covered with trees up to an altitude of 2,200 meters, and shrubs grow up to 2,500 meters. If there should be in this region a cloud of steam over a lateral crater, the shrubs around it might seem to be afire without being consumed. This, I *Compare Sardanapal. Grosse historische Pantomime in 3 Akten oder 4 Bildern, unter Anlehnung an das gleichnamige Ballet Paul Taglioni’s neu bearbeitet von Friedrich Delitzsch (Berlin, 1908). 304 1909.] HAUPT—THE BURNING BUSH 355d think, is the great sight (Exodus, iii., 3) which Moses observed on the Mountain of God about 1200 B. c. . Mount Sinai is generally supposed to be a mountain on the so-called Sinaitic Peninsula between the Gulf of Suez and the Gulf of Akaba. The majority of scholars believe that the Mountain of the Law was the present Jabal Mtisd (the Mountain of Moses) which is the highest point of this barren peninsula in the south, rising to a height of 7,362 feet ; but the two famous Egyptologists Richard Lepsius and Georg Ebers claimed this distinction for the Jabal Serbal in the northwest, which is 6,731 feet high. Mount Sinai, however, cannot be located on the Sinaitic Penin- sula; it was a volcano in the land of Midian on the northeastern shore of the Red Sea. Midian is not the name of an Arabian tribe ; it denotes the Sinaitic amphictyony, 7. e., the league of worshipers of JHvH? in the neighborhood of Elath, the Edomite port at the north- eastern end of the Red Sea. Midian is derived from the old Sumerian word din which means in Arabic not only judgment, but also religion. Law and religion are intimately connected in the East. The Jewish religion is known as the Mosaic Law. In the New Testament the Jewish theologians are called Jawyers.? The Arabic term fakih denotes a scholar versed both in jurisprudence and theology. Midianite is not a name like Arabic, but a term like Islamic. Priest of Midian means a priest of the Sinaitic amphictyony. The name of Moses’s father-in-law was Jethro, which may be connected with the name of the Egyptian sun-god, Ra, which we find also in Potiphera‘ and Potiphar (for Petiphro; compare Jether for Jethro). In the original tradition, Moses was the son-in-law of a priest of On or Heliopolis, the city of the sun-god. Moses’s Egyptian wife is contemptuously referred to (in Numbers, xii., 1) as the Ethiopian *For Juvy (i. e., Jahvéh or Yahwdy, not Jehovah) see the notes on the translation of the Psalms, in the Polychrome Bible, page 164, line 4. The first syllable of Janven should be pronounced like the jah in Hallelujah. Compare Matthew, xxii. 35; Luke, vil., 30; x., 25; KI AGe SLi exten 3: It might be well to add that publican means toll-gatherer. Sinner = unortho- dox; compare John, vii. 40. 396 HAUPT—THE BURNING BUSH [April 23, woman, 7. ¢e., the negress.* Afterwards this tradition was trans- ferred to Joseph (Genesis, xli., 45). Moses is not a proper name, but a title meaning Deliverer. He was an Edomite, but the son-in-law of an Egyptian priest of Helio- polis, near the western end of Goshen where the Edomite ancestors of the Jews lived before the Exodus. According to Acts vii., 22, Moses was learned in all the wisdom of the Egyptians. If we bear this in mind, we can appreciate the remarkable state- ment in Deuteronomy, xxiii., 8 (which was written about 690 B. Cc.) : Thou shalt not abhor an Edomite, for he is thy brother; thou shalt not abhor an Egyptian, for thou wast a stranger in his land. The children that are begotten of them shall enter into the congregation of Juvu in their third generation. The Edomites were not enemies of their brethren in Jerusalem at the time of Nebuchadnezzar (about 586 B.c.) but they were unfriendly disposed toward the Jews at the time of Judas Mac- cabeus (about 164 B.c.). Both Moses and David were Edomites. Moses established the Jewish religion, David founded the kingdom of Judah. Moses corresponds to Mohammed, David to Omar. The Levites were Edomite priests. According to Exodus, ii., 1, Moses’s father belonged to a priestly family (béth Jéwi) and Moses’s mother was the daughter of a priest (bath léwi).° Jewish monotheism is derived from Egypt. Monotheism can have originated only in a highly civilized country as a reaction against excessive polytheism. About 1350 n.c. Amenophis IV. of Egypt endeavored to supersede the old polytheistic religion by the * Compare Jeremiah, xiii., 23 and my paper The Aryan Ancestry of Jesus (Chicago, 1909) page 9= The Open Court (April, 1909) page 201. The admixture of African blood in the Semitic race may be tested by the new sero-diagnostic methods (based on deviation of the complement— whereby the phenomenon of hemolysis is inhibited) which were discussed by H. Sachs at the 39 congress of German anthropologists, held at Frank- fort, Aug. 4, 1908. Compare Max Seber, Moderne Blutforschung und Abstammungslehre (Frankfurt am Main, 1909) page 44. See also, below, page 365, note 44. °A léwi (for lawi) is a méréh; Arab. dlwa is equivalent to Heb. horah. In Exodus, iv., 14; Judges, xvii, 7 léwt evidently means priest. For éth before bath léwi see Haupt, The Book of Esther (Chicago, 1908) page 18, line 6. 1909.] AND THE ORIGIN OF JUDAISM: 357 exclusive worship of the Sun.* He prohibited the cult of Amon and of all other gods; their images were destroyed, and their names erased from the walls of the temples and other public buildings. After his death, however, a reaction set in, and his innovations were abolished.*. But some priests of this monotheistic cult may have survived in Heliopolis, and Moses’s father-in-law may have been one of them. Hobab is not a proper name, but a term for father-in-law.® Jethro, the hdbab of Moses, was attached to the Edomite clan Reuel. JHVH was an Edomite god. The meaning of the name is He who causes to be. In Exodus, ii, 14 we must read instead of the meaningless ehyéh ashér ehyéh, | am that I am: ahyéh ashér thyéh,® I cause to be what is.1° The old name of this god of the Edomites was Esau, which is a dialectic form of the Hebrew word ‘Oseh (for ‘adsai) Maker. The Jews are the descendants of the Edomite worshipers of JHvH,'? who were united under the leader- ship of David about 1000 B.c. David belonged to the Edomite clan Ephrath in one of the fertile valleys about Hebron. He was not a native of Bethlehem, neither was any son or descendant of David ever born at Bethlehem. *An uncle of Amenophis IV. was high-priest in Heliopolis; see Zeit- schrift der Deutschen Morgenlandischen Gesellschaft, vol. \xiii., page 247, line 29. Userkaf, the first king of the Fifth Dynasty, is said to have been high-priest of Heliopolis prior to his accession to the throne (about 2680 B. C.). Compare below, page 368, note 59. “Compare the notes on the translation of Joshua, in the Polychrome Bible, page 4o. *In the Targum Jerushalmi ii. we find (Deuteronomy, xxvii., 13) the feminine habibthd, lit. the beloved, for the Heb. héthénth, mother-in-law. * The pronunciation yihyéh is incorrect. We say Israel, not Yisrael. Con- trast the dissertation of Erich Ebeling, Das Verbum der el-Amarna- Briefe (Berlin, 1909) page Io. This would be in Assyrian: usdbSa sa ibdsi; in Arabic: ukduwinu ma yakunu. ™ The majority of them were Edomites, but they comprised also Horites, Canaanites, Ishmaelites, Moabites, Hittites, Amorites, Philistines, Egyptians, and Ethiopians, 7. e., a mixture of Asiatic, African, and European elements. For the Philistines compare the Proceedings of the Society of Biblical Archeology, vol. xxxi. (London, 1909) page 233. Even the Phenicians may have come from Europe. Herodotus, who states (i., I; vii, 89) that the Phenicians were originally settled on the Red Sea, confounds the Phenicians with the Jews. 358 HAUPT—THE BURNING BUSH [April 23, Judah (Yéhtidah) is not the name of an Israelitish tribe, but a feminine collective to yéhddéh, he confesses.1* King of Judah is originally a title like the Islamic Commander of the Faithful. The worship of JHVH was introduced in Israel by David (about 1000 B.C.) after he had conquered the northern confederation of Israel- itish tribes; but after the death of Solomon (about 930 B.c.) the Israelites relapsed into their former idolatry.13 The Israelites have vanished ; they survive only, mixed with numerous foreign elements, including a considerable percentage of Aryan colonists,’* in the Samaritans whose number is now reduced to 170 souls. The Israelites were not in Egypt, but the Edomite ancestors of the Jews were in Egypt (about 1230 B.c.) under the reign of Merneptah,’®> whose name appears in the Old Testament as Me- nephtoah.1® At that time the Israelites were settled in Palestine, “The relation between the participial form mddéh, confessor, and the old imperfect form yéhédéh, he confesses, is the same as the connection between the modern Jewish name Meyer (Heb. Me’ir) and the old name Jair (Heb. Yair) which appears in the New Testament as Jairus. * Compare the translation of Joshua, xxiv., 2. 14. 23, in the Polychrome Bible, and the Notes, page gt, lines 3-6; also Genesis, xxxv., 2; xxxi., IO. “In the second half of the eighth century B.c. the Assyrian kings sent Babylonian colonists from Babylon and Cutha to Samaria; they also trans- ferred there Aryan colonists from Hammath and other Galilean cities; see Orientalistische Literaturzeitung, vol. xi., columns 237-230. * Canon Cheyne notes in his Encyclopedia Biblica, col. 1182, below, that thirty years ago Mr. Baker Greene (Hebrew Migration, pp. 37. 117. 199. 310) brought the passage in the Anastasi papyrus (vi. 4, 14, where a high official asks permission for the entrance into Egypt of tribes from the land of Aduma) into connection with the settlement of Hebrew tribes, such as the Josephites and, as he thought, the Kenites——The Josephites, however, were not in Egypt. The ancestors of the Israelites came from the pasture grounds south of Haran in Mesopotamia, and invaded Palestine from the northeast ; whereas the ancestors of the Jews, who had sojourned in Egypt, came from Elath, at the northeastern end of the Red Sea, and invaded Pales- tine from the south. The Israelites settled in Palestine about B.c. 1400; the Jews came about the end of the eleventh century. Compare below, page 366, line 8. *® Heb. ma‘yan mé nephtéh (Joshua, xv., 9; xviii, 15) does not mean The fountain of the waters of Nephtoah, but The Fountain of Me(r)neptah. The modern name of this place is Liftad. In this village, about two miles northwest of Jerusalem, there is a large fountain, the waters of which are collected in a great walled reservoir of very early origin. The locality is undoubtedly ancient. See Cheyne’s Encyclopedia Biblica, col. 3394. 1909.] AND THE ORIGIN OF JUDAISM. 359 in the region of Mount Ephraim. At the time of Gideon (about 1100 B. Cc.) the Israelitish peasants in Palestine were idolaters, while the invading Midianites were worshipers of JHvH. The legends of the ancient Israelites have been subsequently conformed to Judaic standards, just as the traditions of South Arabia have been systematically altered by the followers of Mohammed. The names of the ancient Israelitish gods in the old legends were afterwards replaced by the “ Angel of Juvu”* or JuvH.1® Gideon’s name Jerubbaal® shows that he was not a worshiper of JHVH. If the Midianite bedouins had not been defeated by the Israelitish peasants, they would have conquered Palestine from the east. As they were repulsed at that time, they afterwards invaded Palestine from the south. It is possible that in the time of Gideon the son of an Israelitish herdsman was sold by Midianitish Ishmaelites (or Ishmaelitish Midianites)*° as a slave into Egypt, where he afterwards attained a prominent position. But the statement that this happened to the ancestor of Ephraim and Manasseh is a later modification of the original tradition. As the Israelites never were in Egypt, the official historians tried to create the impression that Ephraim and Manasseh had been born in Egypt, and that the Israelites had been from the beginning worshipers of JHvu. The story of Joseph seems to have been influenced in some respects by the ancient Egyptian poetic autobiography of Sinuhet (about 2000 B.c.). Lifta = Nephtah; change of | and m is not exceptional: the modern name of the Biblical Shunem is Silem; on the other hand, Bethel is now known as Beitin, and Jezreel as Zer‘in. Talmudic tarnégél, rooster, is the Sumerian dar-lugallu, king of the variegated birds (chickens). Compare J. Hunger, Babyl. Tieromina (Berlin, 1909) p. 42. ™Wellhausen remarks in the notes on the translation of the Psalms, in the Polychrome Bible, page 176, line 36: Judaism has turned the heathen gods into angels, commissioned by JHvH to govern the various nations. *® Compare, e. g., Genesis, xxxi., II. 13; also xvi., 11. 13; Judges, vi., 11. ® The name Jerubbaal means Baal requites, rewards. The Hebrew verb rub or rib, to strive, to sue, means originally to retaliate, to try to obtain redress. It has recently been shown that we have the same verb in the name of Sennacherib, Assyr. Sin-ahe-ribé, O Moongod give brothers as a reward! Gideon’s god was Baal-bérith (Judges, viii., 33) 1. e., the Baal of ,Oracular Decision. Also sefr hab-bérith (Exodus, xxiv., 7) means not the Book of the Covenant, but The Book of (Oracular) Decision(s). “ Compare Judges, viii, 24; Genesis, xxxvii., 25-28. 360 HAUPT—THE BURNING BUSH [April 23, Also Balaam was a prophet of JHvuH, while the Israelites, who were to be cursed by this Edomite seer, were idolaters. In Num- bers xxiii., 7 we read that Balaam came from Aram, from the great mountain? in the east, 7. ¢., Mount Sinai in the neighborhood of Elath, on the northeastern shore of the Red Sea. This Aram is not Syria, but the Koranic Jramu which we find in the 89™ sura in connection with the Adites. Jramu (or Aramu) denotes the region southeast of Elath. Balaam is identical with Lokman the Wise. Lokmdn is a translation of Balaam.”* Both names mean Devourer. The name of Balaam’s father is Be‘ér, and Lokman’s father was called Ba‘tir. Lokman was born at Elath; élath or él6th means tall trees, including palms, and there is a large grove of palm-trees near Elath. In Judges, i., 16 Elath is called The City of Palm-trees. In the Koran the Midianites of Elath are called achabu-'l-atkati, the People of the Grove. Aikat is an adaptation of Ailat, the Arabic name of Elath. Just as Midian is not a tribal name, but the ancient term for the Sinaitic amphictyony, so the Adites, referred to in the Koran, are not a tribe, but a religious confederation. Arab. ‘ad is the collective to ‘ddah, custom, usage, institution, a synonym of sunnah which may be connected with Sinai; it is originally a desig- nation of the Worshipers of JHvH, as are also Midian and Jehudah, the prototypes of the later Congregation (Heb. kahdl and ‘edah). Hid, the name of the prophet who was sent to the Adites, is but a shortened form of Jehudah. Shu‘aib, the Arabic name of Jethro, means small tribe.?* ** The mountains = the great mountain; compare the notes on the trans- lation of Ezekiel, in the Polychrome Bible, page 157, line 22. = Similarly Nazareth is a translation of the older name of this Galilean town, Hinnathon or Hittalon, mispointed Hannathon and Hethlon, which means Seclusion; see my paper The Ethnology of Galilee in the Transactions of the Third International Congress for the History of Religions (Oxford, 1908) vol. i., page 303, line 3. The original form of the name Nazareth may have been Nacdrath with final ¢ as in Zarephath = Sarepta (Assyr. Caripiu). Compare Heb. méthé mispar, or méthé mé‘dt, or ha-méat mikkél hé-ammim (Genesis, xxxiv., 30; Deuteronomy, iv., 27; vii. 7; XXvi., 53 Psalm, cv., 12). For the Adites compare the new Enzyklopedie des Islam, edited by Houtsma and Schade, page 128. 1909.] AND THE ORIGIN OF JUDAISM. 361 Mount Sinai, the sacred mountain of Midian, must have been a volcano. When the Edomite ancestors of the Jews came to Mount Sinai after the exodus from Egypt, there were thunders?* and lightnings, and a thick cloud upon the mount, and the voice of the trumpet exceeding loud. . . And Mount Sinai was altogether on a smoke ... and the smoke thereof ascended as the smoke of a furnace, and the whole mount quaked greatly. This passage (Exodus, xix., 16. 18) describes a volcanic eruption accompanied by earthquakes and thunderstorms. The voice of the trumpet (or rather ram’s horn)*® denotes the subterraneous roaring, rumbling, and thundering accompanying a volcanic eruption or earthquake. Homer (JI. xxi., 388) uses trumpeting for thundering.2° We use blare not only of a sound like that of a trumpet, but also of a loud or bellowing noise. We speak of the blare of trumpets and the blare of thunder. In Babylonian omen tablets the blare of thunder is compared to the voices of various animals: rams, asses, horses, hogs, lions, dogs, rats, chickens and other birds, etc.2* Pliny (i1., 193) says that earthquakes are preceded or accompanied by a terrible noise which resembles either a murmuring, or a roaring, or the shouting of men, or the clangor of arms (praecedit vero comita- turque terribilis sonus, alias murmuri similis, alias mugitibus aut clamort humano armorumque fragori). A Winchester physician said of the recent seismic shocks in Virginia at the beginning of this month (April, 1909): I felt two earthquake shocks. They were like the boom of heavy cannon fired in quick succession, and were followed by a loud roaring and rumbling. The earth trembled, and my house swayed perceptibly. In the same way the walls of Jericho, which were excavated a * Lit. voices; the plural is intensive; compare above, page 360, note 21. Thunder was regarded as the voice of God. * See the cuts in the Appendix on the Music of the Ancient Hebrews in the translation of the Psalms, in the Polychrome Bible, page 222; compare the translation of Joshua, page 63. **Compare also the various uses of Lat. fremitus, sonitus, strepitus; Greek kAayyy, Krbmoc, Bpduoc, etc. See my paper on the Trumpets of Jericho in the Vienna Oriental Journal, 1909. *See J. Hunger, Babylonische Tieromina nebst griechisch-rémischen Parallelen (Berlin, 1909) page 168. 362 HAUPT—THE BURNING BUSH [April 23, year ago by the Deutsche Orient-Gesellschaft,?® were destroyed by an earthquake accompanied by shouting and horn-blowing, i. e., roaring and rumbling. The idea that the walls of this ancient im- pregnable fortress fell down owing to the shouts of the Israelites and the horn-blowing Israelitish priests*® is a later embellishment. Similarly, Sodom and Gomorrah were destroyed by a tectonic earthquake. This was discussed more than ten years ago by the German geologist Blanckenhorn, in his book on the Dead Sea and the Destruction of Sodom and Gomorrah (Berlin, 1908).*° Also the explanation of the Pillar of Salt was given long ago. At the southwestern end of the Dead Sea there is the so-called Moun- tain of Sodom, consisting of crystallized rock-salt. From the face of it great fragments are occasionally detached by the action of the rains, and appear as pillars of salt, advanced in front of the general mass. Such pillars (or pinnacles) have been often noticed by travelers. Lieutenant W. F. Lynch described one which was about 40 feet high, cylindrical in form, and resting on a kind of oval **See No. 39 of the Mitteilungen der Deutschen Orient-Gesellschaft (Berlin, 1909). * Compare the translation of the sixth chapter of the Book of Joshua in the Polychrome Bible and the Notes, on page 62. The failing of the waters of the Jordan, as described in Joshua, iii, 16 (compare the Notes on page 60) may have been due to a landslip some 16 miles north of Jericho, near Ed-Damieh (the ancient Adam, or rather Adamah, south of the mouth of the Jabbok) where the valley of the Jordan contracts to a narrow gorge. Canon Cheyne states in his Encyclopedia Biblica, col. 2400, that minor landslides still occur in that region, and a large one might again dam up the Jordan, and let it run off into the Dead Sea, leaving the bed temporarily dry. An Arabic historian relates that on Dec. 7, A.D. 1266, in the neighborhood of Ed-Démieh, a lofty mound, which overlooked the river on the west, fell into the water and dammed it up for several hours. Compare Diener, Die Katastrophe von Sodom und Gomorrha tm Lichte geologischer Forschung in the Mittheilungen der K. K. Geographi- schen Gesellschaft in Wien, 1897, pp. 1-22; also Cheyne’s Encyclopedia Biblica, col. 1047. For the fire (Genesis, xix., 24. 28) following the earth- quake, note Genesis, xiv., 3. 10 (the region was full of slime pits, i. e., bitumen springs). From the Lord out of heaven (Genesis, xix., 24) is a subsequent addition; rained does not necessarily mean that the brimstone and fire came out of heaven; compare Psalm Ixxviii, 27. The Cologne Gazette of April 27, 1909, reported that during the recent earthquake at Lisbon, on April 23, 1909, boiling water, smoke, and sulphureous dust were ejected from several large fissures.—There are sulphur springs in the region of the Dead Sea. 1909.] AND THE ORIGIN OF JUDAISM. 363 pedestal, some 50 feet above the level of the sea. A picture of it is given in Lynch’s Narrative of the U. S. Expedition to the River Jordan and the Dead Sea (Philadelphia, 1850) page 308.91 Canon Driver, of Christ Church, Oxford, says (in Hastings’s Dic- tionary of the Bible) : It is probable that some such pillar, conspicu- ous in antiquity, gave rise to the story of Lot’s wife. The late Professor Edward Robinson, of Union Theological Seminary, New York, remarked in his Biblical Researches (vol. ii., page 108) that during the rainy season such pillars were constantly in the process of formation and destruction. The other day my little girl, who is but 12 years old, was read- ing some of the numerous clippings which denounced my allusion to the destruction of Sodom and Gomorrah and raised the question how I could explain the Pillar of Salt.*? She said, How could Lot see that his wife became a pillar of salt? If he had looked back, he would have become a pillar of salt. The meaning of the original text in Genesis, x1x., 26 is undoubtedly that as soon as Lot’s wife looked back, she became a pillar of salt. Ina Philadelphia paper a correspondent stated, I had overlooked the comma. There were no commas in the original text.’ The majority of the readers of the Bible do not realize that the title-page of the Authorized Version contains the statement translated out of the original tongues and with the former translations diligently compared and revised, by His Majesty's special command. In Exodus, xxiv., 17 we read: The sight of the glory of Juvu was like devouring fire** on the top of the mount in the eyes of the Israelites. According to Exodus, xiii., 21, JHvH was before them by day in a pillar of a cloud, and by night in a pillar of fire.** The modification that this pillar of smoke or fire preceded them on their march in the wilderness is a later embellishment suggested by ** Compare my paper on Jonah’s Whale in the Proceedings of the Amer- ican Philosophical Society, vol. xlvi., page 162, note 3. *T alluded to it in a paper on the location of Mount Sinai, which I read at the annual meeting of the American Oriental Society, New York, April 16, 1909. Compare also Deuteronomy, iv., 24. 36; ix., 3; Psalm, xcvii., 3; Hebrews, xii., 29. * Compare Genesis, xv., 17. 364 HAUPT—THE BURNING BUSH [April 23, the custom of carrying at the head of a caravan, in a cresset mounted upon a long pole, a beacon-fire, the blaze of which served as a guiding-light at night, while the smoke signaled the direction during the day. According to the Priestly Code (which was compiled by Jewish priests during the Babylonian Captivity about 500 B.c.) the cloud was over the Tabernacle by day, and by night fire beaconed there.*® But originally the cloud was on the top of Mount Sinai, and at night it had a fiery aspect. Sinai means covered with senna shrubs.*® This seems to be the older name of the Mountain of JHvu. MHoreb, which is equivalent to Mont Pelé, i.e., Bare Mountain,*" is a later name.*® The top of the mountain may have been bare after the eruption observed by the Hebrews after their exodus from Egypt.*® The volcano may have been dormant for centuries*? when Moses saw the first flame of fire out of the midst of the bush, 7. e., a clump of senna shrubs. The famous Arabian geographer and historian Abulfeda (who died in A. D. 1331) says: Opinions differ with regard to Mount Sinai. Some say, It is a mountain in the neighborhood of Elath; others, A mountain in Syria. According to some, sind denotes the stones of the mountain; according to others, the shrubs thereon.*! Sanda’ is the Arabic name for senna, and sina means small stones, i. e., the lapilli of the volcano. In Exodus, xix., 13 the Hebrews are warned ® See Haupt, The Book of Canticles (Chicago, 1902) page 22 = The American Journal of Semitic Languages, vol. xvili., page 212; compare Haupt, Biblische Liebeslieder (Leipzig, 1907) page 22. % Cassia angustifolia. This shrub, which is more than six feet high, is found on the shore of the Red Sea. The best senna leaves (folia sennae) come from Arabia. % Horeb may also be interpreted to mean making bare or Destroyer (Arabic harib). In several passages (Exodus, iii, 1; xvii, 6; xxxiii., 6; i. Kings, xix., 8) Horeb represents a later addition. The name Horeb does not occur before the 7 century B.C. ° The top of Mount Etna, which is now bare, was wooded in the six- teenth century. © Mount Vesuvius seemed to be extinct from 1500 to 1631; it was covered with trees and shrubs, the cattle browsed within the crater; but on Dec. 16, 1631, there was a terrific eruption which destroyed some 3,000 men. “The Arabic text (p. 69 of the Paris edition) reads: wa-téru Sinda *htdlafit fihi, fa-qila: huwa jdbalun bi-qirbi Ailata, fa-qila: sind’u hijaratuhu, wa-gila: Sajarun fihi. Mount Sinai is called also téru Sinina. 1909.] AND THE ORIGIN OF JUDAISM. 365 against drawing too near to the mountain, inasmuch as any man or beast might be killed by a volcanic bomb or the lapilli ejected from the volcano. The universal interpretation of this passage (which we find also in the New Testament, Hebrews xii., 20) that men or beasts that disregarded this prohibition were to be executed by being stoned or shot with an arrow, is grotesque. No Hebrew ever shot a domestic cow with an arrow. There is a mountain in the neighborhood of Elath, known as the Jabal an-Nir, the Mountain of Light, or Jabal al-Barghir, a modification of barghil, which denotes a region near the water or between cultivated land and the wilderness. The Arabs say that the Lord spoke to Moses on that mountain. There is also a Jabal Harb,™ southeast of Elath, which is 7,218 feet high. It is situated near the eastern shore of the Red Sea, about lat. 28° N., west of Tabtk, north of Ziba on the Red Sea, on the route of the pilgrims from Egypt to Mecca. We ought to send an expedition to Akaba to find out whether these two mountains are extinct volcanoes and covered with senna shrubs.** Systematic explorations of this volcanic region of the cradle of Judaism would no doubt yield most striking results. I am inclined to think that not only the Edomite ancestors of the Jews came from that region, but also the Semites who invaded both Babylonia and Egypt. The aborigines of Egypt must have been a negroid race,** but Semites must have invaded the valley of the Nile in the prehistoric period. Some of these Semitic invaders, “ My attention has been called to the fact that A. H. McNeile, The Book of Exodus (London, 1908) p. cv. states: Horeb must... be located .. on the east of the Gulf [of Akaba]. And it is worthy of notice that in modern maps a Jabal Harb is situated on the east of the Gulf, a little south of lat. 28°. : *“We ought to disinter also the ancient capital of Galilee, at the hot springs (Hammath) south of Tiberias, and the traditional home of Abraham, Ur of the Chaldees, the present Mughair. I have been advocating excava- tions at Mughair for more than 25 years. Dr. John P. Peters states in his work on Nippur (vol. ii., page 300): I have seen no mound which seemed easier and safer to excavate, or promised richer results than Mughair. “See my paper The Aryan Ancestry of Jesus, page 9, note *; compare the Zeitschrift der Deutschen Morgenlaindischen Gesellschaft, vol. \xiii., page 250, lines 24-30. See also above, page 356, note 4. 366 HAUPT—THE BURNING BUSH [April 23, it may be supposed, came over land, across the isthmus of Suez, and founded the northern kingdom of Egypt in the Delta. Others came across the Red Sea, near Koseir,** and established the Southern Kingdom in Upper Egypt. The northern and the southern king- doms were afterwards united by Menes, about B.c. 3300, just as David united his southern kingdom with the northern kingdom of Israel about I000 B. Cc. The Israelites may have originally lived with their Edomite brethren on the northeastern shore of the Red Sea, but they must afterwards have sojourned for some time in Mesopotamia*® before they settled in Palestine. They may be a branch of the Semites who had invaded Northern Babylonia and had afterwards gone to Assyria.*7 The Edomite ancestors of the Jews invaded Palestine from the south prior to B. c. 1000, but the Israelites must have come to Palestine from the northeast (probably through Rakkah on the Euphrates, Palmyra, and Damascus )** prior to B. c. 1400, and settled first in the northern region of the country east of the Jordan, 1. e., Bashan and Gilead.*® If the Israelites sojourned in Mesopotamia, we can understand the points of contact between the Israelitish law- book®® in Exodus, xxi., 2—xxii., 17 and the Code of Hammurapi (B.c. 1958-1916).5* The Decalogue (Exodus, xx., I-17) repre- *“On the western bank of the Nile, at Nakadah and al-Ballas, about five days’ journey from Koseir, there are some of the earliest settlements in Egypt. Compare also the Proceedings of the Society of Biblical Archeology, vol. xxxi. (London, 1909) page 210, line 4. ** Probably on the pasture-grounds south of Haran, between the Eu- phrates and the Chaboras. Compare above, page 358, note 15, and Genesis, Xi) 28. 130s Mxive 04s LO) 3exvils 43s) oRVAIRY Si) sem), GS exccITC eee Deuteronomy, xxvi.,5. The Hebrew term for Mesopotamia, Ardm-Nahardaim, means The Arameans of the Great River, i. e., the Euphrates; see Haupt, The Book of Nahum (Baltimore, 1907) page 31. ‘In Genesis, x., 11 the Authorized Version renders correctly in the margin: he went out into Assyria. oe Rakkah means bank, shore; Palmyra=Tadmor (for Titmur): palmy, abounding in palms; and Damascus seems to be a contraction of Ddar-maski well-watered region. See my paper on the Ethnology of Galilee (cited above, page 360, note 22) and the Zeitschrift der Deutschen Morgenlaindischen Gesellschaft, vol. xli., page 195, line 9; also Orientalistische Literaturzeitung, vol. x., col. 306; vol: xii, col. 214, note 15, * Compare Genesis, xxxi., 21. 47; Deuteronomy, i., 4, etc. ® Compare above, page 359, note 19. See next page. 1909.] AND THE ORIGIN OF JUDAISM. 367 sents the quintessence of the old moral and religious precepts,®? which was probably extracted by the prophets®* in the seventh cen- tury, after Israel had fallen in B.c. 721, and which was afterwards still more concentrated by Jesus.** According to later Judaic tradition, Abraham came from Ur of the Chaldees, and went afterwards to Egypt (Genesis, xii., 10). The same source states that Abraham had an Egyptian concubine (Genesis, xvi., 1). The object of such statements as we find, e. g., in Genesis, xliii., 32, is to emphasize the fact that the Egyptians, among whom the Edomite ancestors of the Jews sojourned for some time, considered themselves superior to the forefathers of the Israelites. Genesis, xxvii., 36 (compare xxv., 33) explains how it happened that the Israelites in the north possessed a higher civili- zation than their Edomite brethren in the south. The Israelites were peasants ; the Edomites, on the other hand, semi-nomadic shep- herds. Sons of Leah means cowboys; Sons of Rachel, shep- herds.» The statement that Joseph, the father of Ephraim and Manasseh, was a Son of Rachel, must be viewed in the same light as the tradition that the Israelites were in Egypt (compare above, page 359, line 19). The ancient Egyptians called themselves Worshipers of Horus, the god of light. This deity may be ultimately identical with the god of the Sinaitic volcano. Harr is the Arabic term for volcanic regions. In the Old Testament we find harerim in Jeremiah, xviti., 6. Nahor, which was originally the name of an Aramaic deity, can hardly be connected with Horus.*® 5 Compare the Johns Hopkins University Circulars, No. 163 (June, 1903) page 50; A. H. McNeile, The Book of Exodus (London, 1908) page xlvii; Ed. Meyer, Geschichte der Altertums, vol. i., part 2 (Stuttgart, 1909) page 450. Compare Exodus, xxii., I7—xxili., Io. 8 See my paper The Religion of the Hebrew Prophets in the Transactions of the Third International Congress for the History of Religions (Oxford, 1908) vol. i., p. 270. * See Matthew, xxii., 40; vii., 12; compare Romans, xiii. 9. °° Heb. leah = cow, rachel=ewe. See my paper on Leah and Rachel in the Zeitschrift fiir die alttestamentliche Wissenschaft, Vol. xxxix. (Giessen, 1909), pp. 281-286. ° For Horus in Old Testament names see Cheyne’s Encyclopedia Biblica, col. 3304, § 81. PROC. AMER. PHIL. SOC., XLVIII. 193 Y, PRINTED JANUARY 5, IQIO. 368 HAUPT—THE BURNING BUSH [April 23, Every statement with regard to prehistoric periods is, of course, more or less conjectural. But I adhere to the principle that the probably right is preferable to the undoubtedly wrong. The possi- bility cannot be denied. It is even possible that the Sumerians are Egyptian emigrants of the pre-Semitic population of Egypt, who left their native land after the double Semitic invasion across the isthmus of Suez and the Red Sea near Koseir. The Sumerians may have come from Egypt to Southern Babylonia through the Persian Gulf. This would explain the legend of Oannes*’ and several remarkable points of contact between Egyptian culture and Babylonian civilization. There is even a racial resemblance between the Sumerian heads of Telloh and the head of the famous statue of the Egyptian scribe in the Louvre or the head of the well-known wooden statue known as the sheikh al-balad.°** We have, of course, no mathematical evidence for the prehistoric periods of Arabia, Egypt, and Babylonia. But so much is certain: Jewish monotheism is derived from Egypt,®® and the sacred moun- tain of the Edomite ancestors of the Jews was a volcano near the ancient Edomitic port of Elath at the northeastern end of the Red Sea. The Burning Bush on the Mountain of God as well as the miraculous passage of the Hebrews through the Red Sea® are not legendary, but historical. 7 See Zimmern’s remarks in E. Schrader, Die Ketlinschriften und das Alte Testament (Berlin, 1903) page 535. See the plates in Ed. Meyer, Sumericr und Semiten (Berlin, 1906) and Aegypten zur Zeit der Pyramidenerbauer (Leipzig, 1908). °° We can trace the beginning of the solar monotheism of ancient Egyptian theology to the Fifth Dynasty (2680-2540 B.c.). Horus was gradually superseded by Ra, just as JHVH was substituted for Esau. Compare above, page 357, note 6. ° The Edomite ancestors of the Jews may have crossed the Red Sea at the small peninsula, 75 miles (120 kilometers) south of the northern end of the modern Suez Canal, between the larger and the smaller basins of the Bitter Lakes which formed at that time the northern end of the Red Sea. Mayjor- General Tulloch observed that under a strong east wind the waters of Lake Menzalah, at the northern end of the Suez Canal receded for a distance of several miles. In the same way the water northeast of this peninsula may have been driven by a strong east wind (Exodus, xiv., 21) into the larger basin of the Bitter Lakes, while the water in the shallow lower basin receded at low tide. Although the Bitter Lakes and the Red Sea are now connected 1909.] AND THE ORIGIN OF JUDAISM. 369 I believe that the Deliverer was a historical person. But we need not believe that Moses and Aaron, Nadab and Abihu, and seventy of the elders of Israel saw God (Exodus, xxiv., 10). The author of the Fourth Gospel says (John, i1., 18): No man hath seen God at any time. Deuteronomy, iv., 12, states: The Lord spake unto you out of the midst of the fire; ye heard the voice of the words, but saw no similitude; only ye heard a voice. But Jesus told the Jews according to St. John, v., 37: Ye have neither heard His voice at any time, nor seen His shape. only by the*modern Suez Canal, the tide extends to the southern end of the Bitter Lakes. The present northern end of the Gulf of Suez is prac- tically dry at low tide. Pi-hahiroth (Exodus, xiv., 2) should be read Pi-haherith, 1. e., the mouth (fz) of the canal (ha-hérith = Assyr. heritu) connecting Lake Timsah (north of the Bitter Lakes) with the Nile. See my papers on the crossing of the Red Sea and the palm-grove on the Red Sea in Peiser’s Orientalistische Literaturzeitung, vol. xii. (Leipzig, 1909) columns 245 and 250. Further details concerning the statements made in the present paper may be found zbid., in my articles on the birth-place of David and Christ; the ancestors of the Jews; MHobab,. father-in-law; the name JHVH (cols. 65, 162, 164, 211) and especially in my paper on Midian and Sinai, pp. 506-530 of vol. Ixiii. (Leipzig, 1909) of the Zeitschrift der Deutschen Morgenlandischen Gesellschaft. THE VERTEBRATES (OF fin CAYUGA AIG BASEN. N.Y: (From the Department of Neurology and Vertebrate Zodlogy, Cornell University.) With Four Mapes. By HUGH D. REED anp ALBERT H. WRIGHT. (Read October 1, 1909.) INTRODUCTION. This paper is based mainly upon the records made by members of this department since the opening of the university in 1868; our personal observations have extended over the last twelve years. For valuable notes, helpful criticism and material assistance we are indebted to Professors B. G. Wilder, T. L. Hankinson and E. H. Eaton and to Messrs. G. S. Miller, Jr, L.A. Puertes; A: A. Allen G. C. Embody and John Vann. Many others have aided in various ways and acknowledgments are made in the proper places. The paper includes all the vertebrates known by us to occur in this basin. Each record is based upon specimens taken within our limits. In cases of doubt as to identification the specimens have been submitted to specialists in the group. The only previous publications which deal specifically with the vertebrates of this region are: “ Fishes of Cayuga Lake,” by B. G. Wilder, published in the Weekly Ithacan for June 25, 1875, “ Notes on the Fishes of Cayuga Lake Basin,” by Seth E. Meek, published in the Annals of the New York Academy of Sciences, Vol. IV., 1899, and “ The Lake and Brook Lampreys of New York, Especially those of Seneca and Cayuga Lakes,” by S. H. Gage, in the “ Wilder Quar- ter-Century Book,” 1893. There are numerous other publications which contain notes upon the vertebrates of this basin, particularly the birds and reptiles, to which reference will be made elsewhere. 370 PLATE XVII No. 193 PROCEEDINGS Am. PHILOS. Soc. VOL. XLVIII. Bd mall L Bis J —FSuda's : I St ot 2 Cascg rats ~ = i Sead ~ i - | < , ” . | ZF 4 ie s (the m0 Tk. , 5 mast 2 ‘ Mone I}, = & = Stang! SS eee a ovartanns Si HH. 4 —— 8] Picasauc fire et 41 Pawd\) x Turkey Hilt iy i 3 sy .S.S. 43 Ch ae Map of Ithaca and Vicinity. i a4) PLATE XVIII PROCEEDINGS Am. PHILOoS. Soc. VoL. XLVII!. No. 193 Relief Map of the Ithaca Quadrangle. PROCEEDINGS Am. PHILOS. Soc. VoL. XLVIII. No. 193 PLATE XIX Skaneateles A nt yt " Hains iil yh Sea Level — hii: HARA LAE yt WL HP i U LiMn, Hy ii g, i ae i 5 a UA? Kao — tail rm ice) As Wit a & ° % + om o a — - - be ° ily MLL SERA EHTEL RE a es i 3 x tn - Tit AIAMAR AANA (tae aR ALO i's gi < ° - ro) -_ WHA White \{: iv Cc i \ p\ ath if g < 2 a Hy Uy lle Rn, < I \ Canandaigua Cross-section of the Finger Lake Region. Rik ra eh i rae ; ; ay ie if ra A nie ; hh ‘ae ta) cay ie ie Me a fee Ve my eal les «, ‘< 7h \ Sag a 7 5 | aS ie A = 7 : , y ope eu W E H BD) ‘ m wosppy ora Yong eA tue wwe Steg re Is ‘ sume \o SEIS, is 096 © o2 4 sey 'S Tr vY su94 PIeUY3, = at = Svoospuowwey 49 "mpwoen) =e z Vase, Sue 4 HOQUUE) pen Binqeveunes 4. aves 07 oe oneBieuS © 19 ver vue © oe S =| ugpeeG euuensy © s0u08 won nies Boves 19 ies 2 my end\epueved N O aojoleovens dip "SG vow %" hog at + Stel 4, i 7 Polen . if ‘ I\ | auYt VOVGNONO MYOA MAN 1VYLNAD weiibves a0 ° NOIS3y 3yv1 SHL SO dvVW xX 3Lvid E61 “ON “INIATX “OA “90g "SOTIHd “Wy SDNIG33900Nq 1909.] PAE CAYUGA LAICE BASIN, 7N: (Ye 371 The Maps.—The map of the Ithaca region (Pl. XVII) is from Dudley’s “The Cayuga Flora.” It shows this region in more detail than the general map. A small portion of the southern end of the basin is shown in a photograph (Pl. XVIII) of a relief map made by William Stranahan from the U.S. Geological Survey sheets. It gives a very accurate idea of the gorges and general surface carving in the southern portion of the basin. It is through the courtesy of Mr. Stranahan and the authorities of the Cornell University Library that we are able to reproduce it here. Plate XIX represents a cross- section of the finger-lake region, showing the comparative depths and altitudes of lake levels and the altitude of intervening land. The lakes are represented in section at their deepest points, the land as indicated by the lines A, B, C on the figure in the lower left-hand corner of the plate. The distance between the lakes is not propor- tional to the elevation. Plate XX is a map of the lake region of central New York based primarily upon the map published by Pro- fessor Dudley in his flora of the basin. It has been modified in many particulars in order to adapt it to the needs of the present paper. The modifications are based largely upon the maps of the U. S. Geological Survey and in a minor degree upon personal obser- vations. The number accompanying the name of a town or hill indicates its altitude above sea level. The altitudes are taken from bench marks so far as they are given. In other cases the altitude given is that of the contour which passes through the center of a town or indicates the top of a hill. The Lake Basin.—Cayuga is the largest of a series of approxi- mately parallel lakes in central New York which extend in a north and south direction. They are long and narrow, virtually deep river valleys, and consequently have been very appropriately des- ignated the “ Finger Lakes.” The basin as delimited in this paper (Pl. XX) comprises about 1,600 square miles. Throughout the greater part of this area only the actual catchment basin has been included, but, in the northern portion, the limits as we have set them are, to a certain degree, arbitrary. It includes a portion of the Clyde and Seneca rivers and the large Montezuma marshes which cover an area of 45 square miles. The greatest length of the basin is about 65 miles, extending 372 REED-WRIGHT—THE VERTEBRATES OF [October 1, from the source of Butler Creek southward to the source of the Cayuga inlet near North Spencer. The width gradually increases from 12 miles at Montezuma to Taughannock Falls, where it sud- denly broadens to about 30 miles because of a finger-like extension along the course of Fall Creek. The length of the lake is usually estimated at thirty-eight miles, its breadth from one and a half to three miles. In appearance, therefore, it resembles a great river; indeed it is said to occupy a part of a preglacial river channel of which the Neguaena* valley was the continuation. The height of the lake above mean tide is 383° feet, the greatest depth found by numerous soundings of the Cornell University Engineering Department was 435 feet at a point directly off Kidder’s Ferry. In the section between Myers Point and Sheldrake Point it is in many places over 400 feet deep. On account of its depth its waters are comparatively cold far into the summer, and rarely become so chilled in winter as to admit of the formation of ice over the deeper sections. From one half to two thirds of the middle section usually remains open, but in the winter of 1884-5 the lake was frozen over before the middle of Feb- ruary and the ice did not break up till the first week in April. There is a tradition that this occurs about once in twenty years (Dudley)? Data collected from various sources show that this tradition has some foundation in fact. Since the beginning of white settlements in this basin, soon after the Revolutionary War, the lake has frozen over seven times and the intervals have been, with one exception, from eighteen to twenty years. During the winter of 1836, ice cov- ered the lake throughout its extent but was apparently very thin, for in an article under the caption “ Cayuga’ written in 1846 the writer observed that this condition lasted for a day or two only. Prior to 1836, the lake had been frozen twice but nothing is known concerning the dates further than that the intervals were about twenty years—probably about 1816 and 1796. During March and April, 1856, ice ten inches thick closed the entire lake. At many points teams were driven across. The Ithaca Weekly Journal of March 12, 1856, contains the following note: Cayuga Lake is frozen over completely from one extreme to the other. The like has not been known for over twenty years (1836) : * Now called the Inlet valley. * The average level as given by the U. S. Geological Survey is 381 feet. * Dudley, William R., “ The Cayuga Flora, Part I.: A Catalogue of the Phzenogamia Growing without Cultivation in the Cayuga Lake Basin,” Bul- letin of the Cornell University (Science), Vol. II., 1886, Andrus and Church. ithaca Nee *Ithaca Daily Chronicle, Dec. 22, 1846, Vol. I., no. 140. 1909. ] THE CAYUGA LAKE BASIN, N. Y. 373 During the last half of February and the first of March, 1875, ice thirteen inches thick covered the entire lake. On February 15, 1884, the lake again froze over completely and remained so until April 4. Since this date Cayuga has frozen from end to end but once and then during February, 1904. In certain places the ice was 22 inches thick. The shallow water at either end of the lake is frozen over usually by the middle of December and remains in this condition until the middle of March or the first of April. Dudley further observes: The temperature of the lake unquestionably influences the development of vegetation in its immediate vicinity. Plants on its shores are usually a week later in the spring than in the neighboring ravines and the warm valley about Ithaca, and a week earlier than on the distant hills; and during the first half of November, the blue flowers of Aster levis and the white plumes of Aster sagittifolius still remain in considerable abundance, while they have long ago matured and faded near Ithaca. Proceeding southward from the gently sloping shores near Cayuga Bridge the banks become gradually bolder, until in the vicinity of Levanna the first cliffs appear on the eastern shore. Between Willets and Kings Ferry these reach their culmination in the “ High Cliffs”; but stretches of lofty, pre- cipitous, or more or less broken declivities occur on both shores until within a few miles of the southern extremity. At intervals, especially near the mouth of some stream, are low, half-sandy points which yield many rare plants. Near Ithaca, and about two miles from the lake, the great valley forks, the main portion continuing to the right of South Hill, a preglacial valley of erosion extending southwardly to Waverly in the Susquehanna Valley. The other portion on the left of South Hill is similar to the first and forms the present Six Mile Creek and White Church Valleys, and opens into the Sus- quehanna at Owego. These deep valleys penetrate and cut through the great dividing ridge between the St. Lawrence or Great Lake hydrographic system to which our streams and smaller lakes are tributary, and the Susquehanna system, and are parallel to similar valleys east and west of us. The head- waters of the streams occupying them, i. e., the summits between the two systems are usually very near the crossing of the dividing ridge. (Dudley.) Hydrographic Areas.—A glance at a hydrographic map of the state will reveal the existence of seven river systems, only two of which lie within the province of this paper, namely: the Oswego, of which the Finger Lakes are a part, and the Susquehanna. The latter has in New York a catchment area of 6,267 square miles and comes into very close relation with the Oswego system through the numerous inlets of the Finger Lakes where the origins of many 374 REED-WRIGHT—THE VERTEBRATES OF [October 1, of the streams of each system are very close, in a few instances with actual water connection. The close relation existing between the Finger Lakes and the Susquehanna system is most marked in the tributaries of Cayuga Lake. Sixmile and Wilseyville creeks arise about three miles apart with a considerable elevation intervening, but within the upper three miles of their respective courses, they approach within three fifths of a mile of each other at precisely the same level with no high land between. Buttermilk creek arises one fourth of a mile from Michigan creek and three tenths of a mile from Danby Creek, all at an elevation of 1,100 feet. Taughannock Creek arises in the same marsh with a tributary of Cayuta Lake at an elevation of 1,300 feet. The inlet of Cayuga Lake arises one and one half miles from Spencer Creek at the same elevation and in the same stretch of marshy area. The west branch of the Inlet at its source is one fifth of a mile from Cantor creek in Pony Hollow. Sixmile Creek and the west branch of the Owego Creek rise in the same marsh at an altitude of 1,280 feet. The west branch of the Owego Creek also comes into close relation with Fall Creek through the tributaries of Dryden Lake. These examples serve to show not only the poSsibility of recent connections but in the case of several streams of the two systems an actual connection at the present time. The sources of Sixmile and Wilseyville creeks are so close that they are connected for lim- ited periods during flood times. Professor R. S. Tarr has expressed to us the belief that before the region was settled and the dense virgin forests cleared away, many of the streams of the Cayuga and Susquehanna systems, with present close relations, were actually connected in the heavily wooded swamps. The outlet of the Finger Lakes is the Seneca River, which con- stitutes the principal component of the Oswego system. The stream itself is about fifty miles long and according to the U. S. Geological Survey has a drop of only twenty feet which accounts for its slug- gish, meandering and marshy course. It receives the drainage of a little more than three thousand square miles of territory. 1909. ] THE WAVUGA LAKE BASIN, Nee 375 The following is a table of the elevations, and area of water and of catchment basins of the Finger Lakes taken from Rafter :° Elevation in Area of Water Area of Catchment Lake, Feet. in Square Miles. Basin in Square Miles. Canandaigua, so4.5s: 686 18.6 175 Kee uilka ah eisvevsleavanieiic esas 720 20.3 187 Sem e Cane retecto veatens oisie 444 66.0 707 Gay gay teat mac resets 381 66.8 1593 Owwascomineanaecaseen 710 12.4 208 Skaneateles) <24.05 2). 867 12.8 73 OEISCO! ailashe cress ieeveitee 784 3.0 34. Thus it appears that Cayuga has a slightly greater water area,® a decidedly greater catchment basin and a lower level (Pl. XIX) than any of the other Finger Lakes. The catchment basin is larger than the combined basins of the other six lakes. The usual fluctua- tion between high and low water in Cayuga is not great. Upon this point Rafter observes (p. 112): According to figures given in the Eleventh Annual Report of the State Board of Health of New York it appears that the maximum fluctuation of Cayuga Lake for a long series of years has been 7.56 feet, although this large fluctuation may be possibly partly due to work done by the state in cutting out the channel of the Seneca River for the purpose of draining the Mon- tezuma marsh. Ordinarily, the fluctuation of Cayuga Lake does not exceed between 2 and 3 feet. From March 4, 1887, to December 2 of that year, the lake fell 2.93 feet. By way of illustrating how these great natural reservoirs tend to prevent floods, it may be mentioned that the configuration of Cayuga outlet with relation to Clyde River is such that frequently, when there are heavy rainfalls in the catchment area of the Clyde River, Cayuga Lake being at the same time at a low level, the entire flood flow of Clyde River is dis- charged into Cayuga Lake without affecting Seneca River below the mouth of the Clyde River at all. It is undoubtedly due to this fact that fall floods on Oswego River are almost entirely unknown. The evaporation of the Oswego River catchment area is exceedingly large—about 28 inches—whence it results that the run-off from a mean annual rainfall of from 36 to 37 inches does not exceed about 9 or Io inches. During the winter of 1908-9 the lake level fell 1.25 feet below the mean level (383 feet), the lowest it had been for twenty years. *Rafter, George W., “ Hydrology of the State of New York,” Bull. 85 of the New York State Museum, 1905, p. 216. *Much greater if the forty-five square miles of the Montezuma marshes are included. 376 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, The principal tributaries of Cayuga Lake are: Cayuga Inlet, Six- mile Creek, Cascadilla Creek, with a combined catchment area of 173 square miles, Salmon Creek, with a catchment area of 90 square miles, and Taughannock Creek, with a catchment area of 60 square miles. In their upper courses all these streams follow broad and gently sloping preglacial valleys without waterfalls. All, however, except the inlet, have cut a mile or more of post-glacial channel just before entering the lake valley. Here the channels are narrow and deep and the descent sudden, forming the gorges and waterfalls so characteristic of the tributaries of Seneca and Cayuga lakes. The fall of these streams in the last two miles (more or less) is be- tween four and five hundred feet. What is said here of the princi- pal tributaries applies to most of the streams entering Cayuga lake. In this connection Professor Dudley wrote: There remains but one other feature to mention in this general review. Nothing in the physical aspect of this region strikes the stranger as more characteristic than the so-called gorges or ravines found in the first great bench above the lake and valleys, wherever a creek or even a brook descends to the lower level. The true gorges are probably, without exception, of recent or post-glacial origin; the walls are frequently of perpendicular or overhang- ing rock from fifty to two hundred feet or even much higher, as in Taughan- nock and Enfield ravines. Within these great chasms are usually falls or cascades, some of them exceedingly beautiful and of considerable height. The Life Zones—The Cayuga Lake basin is, in the main, typi- cally Transitional, although in certain localities there is a trace of the Upper Austral and Canadian. All of the nine species of mam- mals, which, Miller’ observes, “ will serve to identify any part of the Transition zone in New York,” are found within the basin. These forms are: Southeastern red squirrel, Sciurus hudsonicus loquax. Southern flying squirrel, Sciuropterus volans volans. Northern pine mouse, Microtus pinetorum scalopsoides. Naked-tailed mole, Scalops aquaticus. Hairy-tailed mole, Parascalops brewer. Northeastern chipmunk, Tamas striatus lysteri. Bonaparte’s weasel, Putorius cicognam. Big brown bat, Vespertilo fuscus. 7 Miller, Gerrit S., Jr., “ Preliminary List of New York Mammals,” Bull. of the New York State Museum, Vol. VI., No. 29, 1890. 1909.] THE CAYUGA LAKE, BASIN, N.Y. 377 Of the eastern birds which find their northern breeding limit in the Transition zone, nineteen out of the twenty-two mentioned by Miller breed in this basin. Bob-white, Ruffed grouse, Mourning dove, Yellow-billed cuckoo, Whip-poor-will, Least flycatcher, Baltimore oriole, Towhee, Grasshopper sparrow, Indigo bunting, Rough-winged swallow, Northern loggerhead shrike, Yellow warbler, Parula warbler, Long-billed marsh wren, Catbird, Brown thrasher, Wood thrush, Blue bird, They are: Colinus virginianus. Bonasa umbellus umbellus. Zenaidura macroura carolinensis. Coccysus americanus. Antrostomus vociferus. Empidonax mimmus. Icterus galbula. Pipilo erythrophthalmus. Ammodramus savannarum aus- tralis. Passerina cyanea. Stelgidopteryx serripennis. Lanius ludovicianus migrans. Dendroica estiva. Compsothlypis americana usnee, Telmatodytes palustris. Dumetella carolinensis. Toxostoma rufum. Hylocichla mustelina. Stalia sialis. Of the ten eastern birds which find the southern limit of their breeding range in the Transition zone of New York, six breed in this basin: Pied-billed grebe, Purple finch, Nashville warbler, Chestnut-sided warbler, Chickadee, Veery, Tachybaptus podiceps. Carpodacus purpureus. Vermivora rubricapilla. Dendroica pensylvamca. Penthestes atricapillus. Hylocichla fuscescens. In the higher hills and in the upper parts of the gorges at the south end of the basin there is an unmistakable tinge of the Cana- PROC. AMER. PHIL. SOC,, XLVIII. 193 Z, PRINTED JANUARY 6, IgIo. 378 REED-WRIGHT—THE VERTEBRATES OF [October 1, dian zone. In these localities are found five of the ten Canadian mammals characteristic of this zone in New York. They are: Canadian white-footed mouse, Peromycus maniculatus gracilis. Common red-backed mouse, Evotomys gapperi gapperi. Woodland jumping-mouse, Nape@ozapus insignis. Northeastern mink, Putorius vison vison. Smoky shrew, Sorex fumeus. Of the sixteen more characteristic Canadian birds breeding in New York, the Blackburnian and Magnolia warblers breed upon these hills. Associated with this assemblage of Canadian forms are others which, while not characteristically Canadian, may be con- sidered northern forms. Such are: Slate-colored junco, Junco hyemalts. Nashville warbler, Vermivora rubricapilla. Black-throated blue warbler, Dendroica cerulescens. Black-throated green warbler, Dendroica virens. Water-thrush, Seturus noveboracensis. Canadian warbler, Wilsoma canadensis. Winter wren, Nannus hiemalis. Hermit thrush, Hylocichla guttata pallasiu. In about the same degree in which a trace of the Canadian zone is found in the higher portions of the basin there is a trace of the Upper Austral in the lowlands about the head and outlet of the lake. In these places are found such of the characteristic birds of the Upper Austral zone as breed in New York, viz., Louisiana water-thrush, Seiurus motacilla. Yellow-breasted chat, Icteria virens. ; Hooded warbler, Wilsonia citrina. Carolina wren, Thryothorus ludovicianus. Tufted titmouse, Beolophus bicolor (one specimen). In the same localities with the above are found species which reach their northern breeding limit in the Transition zone in New York having.a wider breeding range to the southward, viz.: Barn owl, Aluco pratincola. 1909.] THECCAYUGA LAKE BASIN, Noy: 379 Red-bellied woodpecker, Centurus carolinus. Rough-winged swallow, Stelgidopteryx serripennis. Orchard oriole, Icterus spurius. A few Lower Austral forms, as the glossy ibis, the egret and the turkey vulture, have been taken in Montezuma marshes during the summer season. In the lowlands about the head of the lake, particularly the Renwick marshes, there remain throughout the winter a number of transients and summer residents. They are: Kingfisher, Ceryle alcyon. Flicker, Colaptes auritus luteus. Meadow lark, Sturnella magna. Song sparrow, Melospiza melodia. Swamp sparrow, Melospiza georgiana. Winter wren, Nannus hiemalis. Long-billed marsh wren, Telmatodytes palustris. Robin, Planesticus migratoria. The localities where the more southern birds are found breeding and where a few summer residents pass the winter are the alluvial flood plains which constitute the According to Dudley a few very rare plants belong to these levels, ce sheltered spots”? of the basin. among them the more southern species. Meteorology.—The basins of Canandaigua, Keuka, Seneca and Cayuga lakes constitute a meteorological subdivision of the state termed the Central Lake region. On the north this subdivision meets the Ontario region. Lakes Owasco and Skaneateles are con- sidered as within the meteorological subdivision known as the East- ern Plateau which lies to the east and southeast of the central lakes. The Seneca lake basin, except for a small portion of its northern extremity, lies wholly within the Central Lake region while that of Cayuga is not only continuous with the Ontario region in its north- ern extremity but its southeastern portion projects for a considerable distance into the Eastern Plateau. The normal annual temperature of the Central Lake region dif- fers only slightly from that of the Ontario and to the extent of about three degrees only from the Eastern Plateau. The normal temperature for each of the three regions computed from the nor- 380 REED-WRIGHT—THE VERTEBRATES OF [October 1, mal annual temperatures for eleven years, 1891-1901, is: Ontario 47.5°, Central Lakes 48.3°, Eastern Plateau 45.9°. Thus it appears that the Central Lake region is .8° warmer than the Ontario and 2.4° warmer than the Eastern Plateau. The extent to which the lake modifies the climate of the basin, if any, is still to be determined. Dr. W. D. Wilson, of Geneva, in comparing the influence of the lakes upon Ithaca and Geneva,’ states that the northerly winds in winter are warmed by their passage up the lake valley, which they follow more or less closely, and cause the temperature in the vicinity of Ithaca during this season to stand’ 3.3 degrees higher than it otherwise would. According to E. C. Turner the observations made at Ithaca prior to 1897 substantiate Dr. Wilson’s views and moreover indicate that they apply to the whole of the central lake region. The normal monthly temperature for Ithaca compiled from data collected from 1875 to 1905 follows: JESTBEDAY Soon bocce ode 24.1 nil ys Sees yoterperes: ona eeetevers 70.6 eDitiaryi .ccteiniice ses. 25.1 PANTSUITS aneeisere ciate ences 68.2 Micirchiy-erarectcretacraa 31.9 Septembetaysnneceer os 60.6 ANP Ella tols 2 a haere ors es 44.2 OctobereGas Geniscne ass 49.5 IME RP ato peaene dined oe eo C 57.0 INovembercencsceenee 37.6 ITO Uae rate, tetera ery 66.2 Decembenere-- ese 28.4 The sum of daily heat units above 32 degrees is 14,317, com- piled from a table of normal daily temperature for 33 years and the average normal daily temperature of the six hottest weeks is 70.4 degrees. According to Turner, from 1879 to 1893 the average date of the latest freezing temperature was May 6, the extremes being April 9 and May 29. The average date of the first freezing temperature in the fall was October 10, the earliest being September 26, while in one year 32 degrees was not reached until October 31. A table of the latest spring and earliest fall killing frosts from 1900 to 1907 at three stations in the basin follows: Ithaca. Romulus. Auburn. 1900. May 7-Oct. 20 May 10-Oct. 20 May 6-Oct. 16 rgo1. April 12-Oct. 28 Oct. 18 April 12-Oct. 6 8See Turner, E. T., Eighth Annual Report of the New York Weather Bureau, Assembly Documents, Vol. 25, 1897, p. 440. 1909.] 1902. 1903. 1904. 1905. 1900. 1907. Pie "CAYUGA LAKE BASIN, IN. ax: Ithaca. May May May May May May 1o-Oct. 2—Oct. 12-Oct. 2-Oct. 21—Oct. 12-Oct. Romulus, May 15-Oct. 15 May 2-Oct. 25 April 22-Sept. 22 May 3-Oct. 26 May 21-Oct. 8 May 21-Oct. 9 Auburn. May 14-Oct. 10 May 2-Oct. 24 April 22-Sept. 22 May 2-Oct. 23 May 21-Oct. 8 May 21-Oct. 9 The average precipitation for the Central Lake region is slightly less than that for either the Great Lake or Eastern Plateau. The mean annual precipitation for these regions compiled from precipi- tation data for the years 1891 to 1902 is: Great Lakes 35.65 inches, Eastern Plateau 40.8 inches, Central Lakes 34.46 inches. The nor- mal monthly precipitation at Ithaca compiled from the last twenty- nine years follows: January February March ec ee) a\(w) 9) |b),e1 0 50\(e) 0) oie ve) |e|\e)6 2.16 in UJitstliygeeevees 1.87 in August... 2.44 in September 2.29 in October 3.43 in November 3.88 in December ale," e! ‘e)(e! ser #1 6 e114) :0 Waa wee 27 cyte 3.24 in. TA eae 2.83 in. 3.17 in. From 1900 to 1907 there have been from 150 to 185 rainy days each year. For the same period the annual snowfall (unmelted) has varied from 46.4 to 75.8 inches, the average being 63.6. One of the striking features of the region about Ithaca is the small per- centage of clear days, as the following table will show: Cloudy LOOOR eis aaa Ace 174 LOOM AR testes ne es I7I 1007) # Rasiclrict Cite 149 TOOSM ctrtehstseo cies: 195 TOOA He ceteris «ccs 180 TOO Her ae cdetvay aes erats 148 LOOOM mete seis cies 164. OOP ver ies nee ees 163 Partly Cloudy. 109 126 I51 98 II5 126 Q2 140 Percentage of Clear. Clear Days. 82 22.4 68 18.6 65 17.8 72 19.7 71 19.4 QI 24.9 109 20.8 62 16.9 Based upon average hours of sunshine from 1900 to 1903 R. G. Allen derived 49 per cent. as an annual mean of sunshine, or a monthly mean of 189 hours of sunshine. The average of mean relative humidities at Ithaca from 1900 to 382 REED-WRIGHT—THE VERTEBRATES OF [October 1, 1907 is 77 per cent., based upon readings taken at 8 A.M. The range for these years being from 73 to 80 per cent. The total movement of wind in miles varies from 62,556 to 79,- 172. The maximum velocity ranges from 36 to 54 miles per hour in the period from November to March. The prevailing direction of the wind for the past eight years has been northwest. Besides the general winds there are local currents or night winds particularly in the southern portion of the basin. Concerning these Dr. W. M. Wilson® writes: The night wind commonly sets in two or three hours after sunset, first as a light breeze, but gradually increasing in strength until a velocity of about eight miles per hour is reached. This current has its origin on the hillsides at the southern end of the lake and flows northward down the channels of the two principal streams which form the inlet, converging into the main depression at the head of the lake. The flow of the current as it moves northward over the level surface of the lake is augmented by the cool cur- rents which join the main stream through the numerous gorges and water courses entering the valley from either side. Along the western shore at the southern end of the lake, where the densely: wooded slopes cool the air near the surface, the flow of the cool breeze down the water courses towards the lake often continues throughout the day. The night breeze is usually stronger, but the day breeze as it comes from the depths of the woods is delightfully refreshing. The meteorological conditions of the Cayuga basin and more particularly those about Ithaca are thus commented upon by Gar- FIOte st” In spring, summer and autumn precipitation is preceded twelve to forty- eight hours by southeast winds and falling barometer, and the barometer gen- erally falls to 29.90, or below, in spring and summer, and to 29.95, or below, in autumn before precipitation begins. In winter southerly winds precede pre- cipitation, but the winds shift more quickly and the signs of precipitation are not so well defined as in other seasons; precipitation begins in this season with a falling barometer and when the barometer has fallen to 30 or below. On account of the position of this station on the hillside and above the lake, diurnal winds are noticeable, especially during the warm months. When not influenced by passing storms these winds come as a gentle east to southeast breeze by night and by day a northwest wind having a velocity of two. or three times greater than the day breeze. When, instead of shifting to the *Wilson, W. M., “New York Section of the Climatical Service of the Weather Bureau in codperation with Cornell University,’ August, 1906, p. 59. *® Garriott, Edward B., “ Weather Folk-lore and Local Weather Signs,” U.S. Department of Agriculture, Bull. 294 of the Weather Bureau, p. 93. 1909.] Tie CAYUGA, LAKE BASIN, (Ni Ye 383 northwest in the early morning, the wind continues from the southeast and begins to increase in force, the approach of a storm is indicated. While rain begins most frequently with falling barometer, the heaviest rainfall often comes, especially in the warmer months, after the turn of the barometer from falling to rising. Richard’s registering hygrometer shows that in spring and summer the humidity sometimes decreases before rain, but rapidly increases after rain begins; in spring rain begins with relative humidity from 50 to 98 per cent., and in summer it may be as low as 50 per cent. one hour before rain begins. In autumn the effect of day and night seems greater than the influence of passing storms, and rain will begin with relative humidity as low as 50 per cent. one hour before rain. In winter there is usually an increase in humidity from one half to four hours before rain, and dry snow will begin with relative humidity as low as 40 per cent. Cirrus clouds are reliable indications of precipitation in all seasons, but are liable to be obscured by lower clouds of local formation in the colder portion of the year. These clouds appear moving from the west in the spring and winter, from the northwest in summer, and from the southwest in autumn, twenty-four to thirty-six hours before precipitation begins. Special characteristics of clouds have not been noted except in connection with cirrus clouds. Frost is likely to damage fruit or other crops in May and September. Heavy frost is generally preceded by high barometer, low temperature and humidity, very high wind and clear weather. The Fishes of the Basin —The fish fauna of the basin comprises 65 species distributed among 21 families, as follows: Petromyzonide ......... 2 species. Umbride ............... I species. Acipenseridze. js. asna-ce I fs EES OCIG G2 sor. srshayetetere cashes 2 os Lepisostetdze. 2:0) 6. dsc ss I # Peeciliiidces ae sneha I cH PNT TT a Verepere cies Sete ores exe I “ Gasterosterdceyy aemae sri: I y Sileret des Wetec ei a woes 5 5 Percopsidae ass acme. I ‘i CGatostomida eee aee: 4 os Athenmnidas Serie se cee I 6 Cyprinidae co s%.5s sos 19 i CGentranchidceme eerie: 7 . Aietiillitdceg esos cere I % Rencidzaaanasae meee 7 s Glupeidzewerieo ea sncises I te SemmmiGks ssooocoasoocer I i Salmomidcewe Mian cute si. aes 5 *s Gatti deeiesnciseinee aioe teens Be hee Gaclidzaune sentry eee I species. As yet too little is known of the fish fauna of the finger lakes to draw any definite conclusions concerning the general distribution of species or the relation of these faunas to others. Lake Cayuga and Seneca River have water connection with Lake Erie and the Hudson River through the Erie Canal; with Lake Ontario both through river and canal (Oswego) ; with the Susquehanna system through several 384 REED-WRIGHT—THE VERTEBRATES OF [October 1, of the southern tributaries at certain periods of the year. It is pos- sible, therefore, that these lakes may receive species from all three sources. Of the 65 species found in the basin 19 are common to the Ontario and Susquehanna basins although frequently varying in abundance. A table follows: Susquehanna. Cayuga. Ontario, Exoglossum maxillingua, very common, common, uncommon. Semotilus bullaris, very common, rare, uncommon. Erimyzon sucetta oplongus, very common, uncommon, uncommon. Esox reticulatus, common, common, rare. Catostomus nigricans, very common, rare, common. Hybopsis kentuckiensis, common, rare, common. Chrosomus erythrogaster, common, Tare; uncommon. Percina caprodes zebra, | common, rare, common. Lota maculosa, rare, uncommon, common. Several of the basses are common to all three basins but the in- troduction of these species from one place to another renders them of no comparative value. Twenty-one species are common to the Cayuga and Ontario basins. Two species, Cottus gracilis and Notropis procne, are com- mon to the Cayuga and Susquehanna basins. There are in the Cay- uga basin four species which do not occur in either the Ontario or Susquehanna. One of these.is the smelt, Argyrosomus osmeri- formis, confined to the interior lakes of New York. The others, Notropis umbratilis, Notropis anogenus and Lepomis cyanellus, are most common in the northern portion of the basin and doubtless found their way hither through the Erie Canal from Lake Erie. It appears that the fish fauna of the Cayuga basin bears the stamp of Lake Ontario with just a trace of the Susquehanna and Erie basins. There is a possibility that species which seem to have found their way here from the Erie and Susquehanna basins were introduced along with game fishes or from bait pails. Observations made in Monroe Co., New York, by A. H. Wright™ indicate that fishes find their way eastward through the Erie Canal. Amphibia.—One of the characteristic features of our vertebrate fauna is the relative abundance of amphibian species and individuals, particularly in the southern portion of the basin. In this respect the * Wright, A. H., MS., “The Fishes of Monroe Co., New York.” 1909.] THE: CAYUGA LEAKE BASIN, (Navy: 385 basin is similar to the mountains of Pennsylvania. The seventeen species are distributed among the following families: eT OPEUG Let ya's fayainrss%—1 sve Ne oe ET. species: />)Pleurodelida © 22...15.4. 502% I species. Ambystomide .......... I Bithonideey ye ciesrone ates I rs Plethodontidz ....6....% 5 e Ply bidet ark ts UA Matecoreisveters 2 a Desmognathide ........ I a3 Ramidee ye nic sacineanin clears 5 oe Reptilia —Twenty species of reptiles are known within our limits. The lizards are represented by a single specimen of the Ground Liz- ard, Leiolopisma laterale, found just northeast of Caroline on the divide between Sixmile Creek and a branch of the Susquehanna. Twelve species of snakes are known, three of which are now very rare. The rattlesnake so far as we know is met with only occasion- ally in the region about McLean, while the blacksnake and pilot snake are confined to the extreme southern portion of the basin near Newfield and Danby. There are seven species of turtles, representing four families as follows: MeTONYENIGEE® (esp chess esses I species. Kainosternidé :.......... I species, se @lrely rides. ..cisrarsiaysie atei~'s i, Emiydidee: so. ac ean sees 4 Only three of the seven species, the snapping turtle (Chelydra ser- pentina), Agassiz’s painted turtle (Chrysemys marginata), and the wood tortoise (Clemmys insculpta) are found distributed throughout the basin. The other four are confined to the extreme northern por- tion. The musk turtle (Terrapene odorata), a species fairly widely distributed east of the Mississippi, was first found in this basin in the fall of 1908 and proved to be common in the Seneca River near the Erie Canal. The Soft-shelled turtle (Aspidonectes spimifer), a species of more northern and western distribution, is very rare at the south end of ‘the basin but found fairly common about Montezuma. The Speckled tortoise (Clemmys guttata) is widely distributed in central and eastern United States but in this region is confined to the vicinity of the Junius Ponds north and west of Waterloo. Muhlenberg’s turtle (Clemmys muhlenbergiu), a spe- cies limited in its range to eastern Pennsylvania, New Jersey and the Hudson Valley, is the only more eastern form found here aside from those of wide distribution. 386 REED-WRIGHT—THE VERTEBRATES OF [October 1, Birds.—The birds that have been recorded for this region com- prise 257 species distributed among 51 families as follows: Colymbidze, )Sacoe. ser cer 3 species. Gavil daewoo anteaters 2 * PAN Feria beety Vana ia near aun BUA I f Weanidzeors! misma cecvrss ait: 9 s Procellanidsctyane cere cee I i iPhalacrocoracidee)). see. 2 4 IRelecanidcemee cena oceee I 2 TACO ESI aa at ores bc 33 ~ ifoyabYatsetims bes ine ain sar allet er I ny JANSHGKEN (a be cp RNR eo Wat 6 i Grid eee ceive nie I a Healt ewig mee ae yeti 6 mA Phalaropodidz 3....@/.2- 3 te Recurvirostride ......... I es Scolopacidccmeperercncr at 20 ss @haradnritder Se eeee ene 4 ke Aphivizidceyije sj aeieeseiiets « I =: Odontophoride ......... I i INGMEVETICED Gon noovooceuT I oe Columbide ee a -see een 2 Cathantidcegescmner osteo I g IBAbIKEOMNGED Goggacussooecc 9 a IPRICOMNGES SoocdcadooouDS 3 se Bandvomidzeesceeaeeaecet I f ANikerstormiake, 556u5d5e00n00 I ee Turdide Strigidz Cuculide Alcidinidee ici deer ree hice ener h pee Caprimulgidze/jsnssees Micropodide Trochilidz Tyrannide Alaudide Corvide Icteridz Fringillidz Tanagride Hirundinide Bombycillidze Laniidz Vireonide Mniotiltide Motacillidze Mimide Troglodytide Certhiide Sittidee Paride Sylviidee Q species. OOM HONE ONCN EC Ly Ga Cuncy ey 2 Cele jolla eheisisie ey @Lal,e) ee [e!e)\e (elie) prelate. ioe CEO DARD cmt pach) @hev0/\0: eevee) ie lo,et sie CC ec Ce a) ee Slope] eJeliate! chels\io diellse oe 0) e\je/.0) 0 \s)\e 6) 6.0 0 \elelere eo teheleve!ele)elele oe .ce 0,000 CMC NM tet 8 species. 2 “e The following tables show the seasonal status of each species that has been found inthe lake basin. PERMANENT RESIDENTS. Bob-white, Ruffed grouse, Red-tailed hawk, Red-shouldered hawk, Barn owl, Long-eared owl, Short-eared owl, Barred owl, Screech owl, Great horned owl, Hairy woodpecker, Downy woodpecker, Red-headed woodpecker, Prairie horned lark, Blue jay, Crow, Goldfinch, Song sparrow, White-bellied nuthatch, Chickadee. 1909.] THE CAYUGA LAKE BASIN, Ni Ye 387 TRANSIENT VISITANTS. Holboell’s grebe (sometimes in winter ), Horned grebe (sometimes in winter), Common loon (sometimes in winter), Bonaparte’s gull, Common tern, Red-breasted merganser (a few regularly in winter), Mallard (a few regularly in winter), Gadwall, Baldpate, Green-winged teal, Blue-winged teal, Shoveller, Pintail, Lesser scaup duck (sometimes in winter), Ring-necked duck, Buffle-head (sometimes in win- ter) Ruddy duck (sometimes in winter ), Great blue heron, Black-crowned night heron, Knot, Pectoral sandpiper, Least sandpiper, Red-backed sandpiper, Semipalmated sandpiper, Sanderling, Greater yellow-legs, Yellow-legs, Solitary sandpiper, Black-bellied plover, Semipalmated plover, Broad-winged hawk (found breed- ing in 1890), Duck hawk, Pigeon hawk, Osprey, Yellow-bellied flycatcher, Alder flycatcher (breeds locally), Rusty blackbird, Nelson’s sparrow, Acadian sharp-tailed sparrow, White-crowned sparrow, White-throated sparrow, Junco in winter; breeds locally), Lincoln’s sparrow, (uncommon Fox sparrow, Northern loggerhead shrike, Blue-headed vireo (found breed- ing in 1893), Black and white warbler (breeds locally), Nashville warbler (breeds locally), Tennessee warbler, Parula warbler (breeds locally), Cape May warbler, Black-throated blue (breeds locally), Myrtle warbler, warbler Magnolia warbler (breeds lo- cally), Cerulean warbler (breeds on Howland Island), 388 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, Bay-breasted warbler, Hooded warbler (breeds locally), Black-poll warbler, Wilson’s warbler, Blackburnian warbler (breeds Canadian warbler (breeds locally), locally), Titlark, Black-throated green warbler Red-breasted nuthatch (some- (breeds locally), times in winter), Pine warbler (breeds locally), Golden-crowned kinglet (some- Palm warbler, times in winter), Water-thrush (breeds locally), Ruby-crowned kinglet, Connecticut warbler (fall only), Gray-cheeked thrush, Mourning warbler (breeds lo- Olive-backed thrush (found breed- cally), ing in 1890), Yellow-breasted chat (breeds Hermit thrush (breeds locally). locally), SUMMER RESIDENTS. Black duck (a few found regu- Bald eagle, larly in winter), Sparrow hawk, Wood duck, Yellow-billed cuckoo, Bittern, Black-billed cuckoo, Least bittern, Belted kingfisher (sometimes in Green heron, winter), King rail, Yellow-bellied sapsucker (not Virginia rail, common at this season), Sora, Flicker (sometimes in winter), Florida gallinule, Whip-poor-will, Coot, Nighthawk, Woodcock, Chimney swift, Wilson’s snipe (not common at Ruby-throated hummingbird, this season), Kingbird, Spotted sandpiper, Phoebe, Killdeer, Wood pewee, Mourning dove, Least flycatcher, Marsh hawk, Bobolink, Sharp-shinned hawk, Cowbird, Cooper’s hawk, Red-winged blackbird (a few in winter), 1909. ] Meadow lark (a few in winter), Baltimore oriole, Bronzed grackle, Purple finch, Vesper sparrow, Savannah sparrow, Grasshopper sparrow, Chipping sparrow, Field sparrow, Swamp sparrow (sometimes in winter), Towhee, Rose-breasted grosbeak, Indigo bunting, Scarlet tanager, Purple martin, Cliff swallow, Barn swallow, Tree swallow, Bank swallow, THE ‘CAYUGA LAKE BASIN, SNi) ¥. 389 Rough-winged swallow, Cedar waxwing (irregularly in winter), Red-eyed vireo, Warbling vireo, Yellow-throated vireo, Chestnut-sided warbler, Oven-bird, Louisiana water-thrush, Maryland yellow-throat, Redstart, Catbird, Brown thrasher (uncommon at this season), House wren, ‘ Long-billed marsh wren, Wood thrush, Veery, Robin (a few regularly in winter), Bluebird. WINTER RESIDENTS. Herring gull, Merganser, Redhead, Canvasback, Greater scaup duck, Golden eye, Old-squaw, Scoter, White-winged scoter, Surf scoter, Canada goose (more common as a transient), Rough-legged hawk, Pine grosbeak, Red crossbill, White-winged crossbill, Redpoll, Pine siskin, Snow bunting, Tree sparrow, Northern shrike, Winter wren (found breeding in 1878), Brown creeper. 390 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, Or RARE OCCURRENCE. Red-throated loon (winter), Hudsonian curlew (transient), Brunnich’s murre (winter), Golden plover (transient), Kittiwake (winter), Turnstone (transient), Iceland gull (winter), Turkey vulture (summer), Ring-billed gull (transient), Goshawk (winter), Fork-tailed gull (winter), Saw-whet owl (winter), Least tern (transient), Snowy owl (winter), Common cormorant (transient), Hawk owl (winter), Double-crested cormorant (tran- Arctic three-toed woodpecker sient), (winter ), White pelican (transient), Red-bellied woodpecker (sum- Barrow’s golden-eye (winter), mer), King eider (winter), Olive-sided flycatcher (transient), Greater snow goose (winter), Orchard oriole (summer), Brant (winter), Lapland longspur (winter), Whistling swan (transient), Leconte’s sparrow (transient), Glossy ibis (summer), Dickcissel (summer), Egret (summer), Philadelphia vireo (transient), Whooping crane (transient), Worm-eating warbler (transient), Yellow rail (transient), Golden-winged warbler (sum- Red phalarope (transient), mer), Northern phalarope (transient), Tufted titmouse (summer), Wilson’s phalarope (transient), Orange-crowned warbler (tran- Dowitcher (transient), sient), Stilt sandpiper (transient), Yellow palm warbler (transient), White-rumped sandpiper (tran- Carolina wren (summer), sient), Short-billed marsh wren (tran- Hudsonian godwit (transient), sient), Willet (transient), Wheatear (fall), Long-billed curlew (transient), Avocet (fall). ACCIDENTAL VISITANTS. Black-capped petrel, Evening grosbeak, Blue goose, European green-winged teal. 1909.] PE CAYUGA LAKE BASING Na Ye 391 CATALOGUE, OF) SPECIES: A. Class CYCLOSTOMATA. is Order Hi YPEROARITA: 1. Family PerromMyzonip%. The Lampreys. 1. Petromyzon marinus unicolor (De Kay). Lake lamprey. Abundant in the lake, where they are very destructive to the larger fishes because of their parasitic habits.12 They are found in great numbers in the lake inlet during the spawning season, which occurs between May 25 and the middle of June. There is, how- ever, considerable variation in this respect according to the season. In 1900 the crest of the spawning season occurred during the last days of May. In 1902 active spawning continued until June 7, while in 1903 spawning was over entirely by June 1. Larve of various sizes are found at all seasons buried in the mud and sand bars below the spawning grounds. Transformation occurs from the last of August to the middle of October. The latest record of transforming individuals is that of three specimens taken October 16, 1907. In one of these transformation was just beginning. Judging from the different sizes of larve found at a given season the larval period is of about four years duration. 2. Lampetra wilderi Jordan and Evermann. Brook lamprey. Common in the inlet, where they may be found in abundance during the spawning season, which occurs during the middle of May beginning, according to Professor Gage’s observations, about the eighth of the month and lasting until about the twentieth. The maximum period averages near the middle of the month. This species is not parasitic at any stage in its life-history. It probably takes no food in the adult stage. 2 See Gage, S. H., op. cit.; also Surface, H. A., “Removal of Lampreys from the Interior Waters of New York,’ Report of the New York Fisheries, Forest and Game Commission, 1808, pp. 191-243. 392 REED-WRIGHT—THE VERTEBRATES OF [October 1 B. Class PISCES. Il. Order ‘*CHONDROSTETL. 2. Family AcIPENSERIDZ. The Sturgeons. 3. Acipenser rubicundus Le Sueur. Lake sturgeon. Rare. A large specimen of this species, now in the collection of Cornell Univer- sity, is reported as being from Cayuga Lake. Mr. Seth Green informs me that sturgeons have occasionally been taken in Cayuga Lake; but, so far as he knows, they have never been found in any other of the small lakes of central New York. I copy the following letter of recent date from Mr. H. V. Kipp, of Montezuma, N. Y.: “ There have not been any sturgeons taken from Cayuga Lake since 1880, but quite a number before that date, and the largest known weighed 35 pounds.” (Meek.) On June 4, 1905, a specimen four feet long and weighing forty- two pounds was taken at Sheldrake by Dr. L. A. Gould and on December 3, 1908, a specimen (C. U. 5130) weighing fifty pounds was caught in the Seneca and Cayuga canal near Montezuma by William Ferrei and George Wildner. These are the only records of the sturgeon since Meek’s list was published. it) Order LEPIDOSTEL 3. Family Lepisosteip®@. The Gars. 4. Lepisosteus osseus (Linnaeus). Long-nosed gar. Rare. ‘Occasionally taken from the north end of the lake. Not as numerous as they used to be” (Meek). There are in the Cornell University Museum seven specimens taken at the south end of the lake as follows: June 17, 1877, in the lower course of Fall Creek. June 13, 1894, from shallow water at the head of the lake. June 8, 1896, in Fall creek about one half of a mile from the mouth. March 26, 1899, from the lake near Ithaca. April 17, 1899, from the lake near Ithaca. May 28, 1900, from shallow water at the head of the lake. August 12, 1908, from the lake near Ithaca. Most of the speci- mens taken here are small, still showing the dark lateral band. 1909.] See sCAVUGA, LAKE BASING NaN: 393 IV. Order HALECOMORPHI. 4. Family Amimp#. The Bowfins. 5. Amiatus calva (Linnaeus). Bowfin. Abundant. Meek recorded this species as Ithaca” ‘ “seldom taken near and “not common at the north end of the lake.” During recent years the bowfin has increased so rapidly in numbers that it has become a serious pest. In shallow water during the month of August hundreds may be seen in rowing a quarter of a mile. Foster Parker, of Union Springs, reports that he has repeatedly seen them capture and swallow the young of marsh birds. V. Order NEMATOGNATHI. 5. Family Strurip#. The Catfishes. 6. Ictalurus punctatus (Rafinesque). Spotted catfish. Rare. Only two specimens have been recorded; one eleven inches long was taken on hook and line near the mouth of the inlet by Mrs. R. J. Ashdown July 10, 1902; the other, ten inches long, was taken in the same locality August 25, 1908. 7. Ameiurus natalis (Le Sueur). Yellow cat. There is one specimen (No. 888) in the collection of Cornell University taken from the lake September 27, 1877. This is prob- ably the specimen referred to in Meek’s list: “I have seen but one specimen of this species from the lake. It was taken a few years ” ago. 8. Ameiurus vulgaris (Thompson). Long-jawed cat. The collection of Cornell University contains two specimens of this species taken from the lake; one November 7, 1885, the other February 16, 1886. g. Ameiurus nebulosus (Le Sueur). Common bullhead. Abundant in the lake and all of its tributaries. In the larger streams it is found above the falls. 10. Schilbeodes gyrinus (Mitchill). Tadpole cat. Common throughout the lake along muddy shores and in the streams, below falls, over a muddy bottom. PROC. AMER. PHIL. SOC., XLVIII. 193 Z, PRINTED JANUARY 6, I9QIO, 394 REED-WRIGHT—THE VERTEBRATES OF [October 1, Vi sOrder PEECLOSPONDYEL: 6. Family Catostomip&. The Suckers. 11. Catostomus commersonii (Lacépéde). Common white sucker. Abundant throughout the basin both above and below falls. 12. Catostomus nigricans Le Sueur. Hog sucker. There is a specimen in the U. S. National Museum from Cayuga lake. Mr. Richard Rathbun writes: “The specimen is among the Museum’s earliest collections and is not accompanied by complete data.” 13. Erimyzon sucetta oblongus (Mitchill). Chub sucker. This species occurs throughout the lake although much more abundant at the north end. 14. Moxostoma aureolum (Le Sueur). Red horse. Common at the north end of the lake and taken occasionally at the south end. Meek recorded this species as M. macrolepidotum. Specimens recently taken and the specimen in the collection of Cor- nell University are all clearly aureolum. 7. Family Cyprinip#. The Minnows. 15. Chrosomus erythrogaster (Rafinesque). Red-bellied dace. One specimen taken July 13, 1901, by T. L. Hankinson near Ithaca in a cold brook which is tributary to Fall Creek. 16. Pimephales notatus (Rafinesque). Blunt-nosed minnow. Abundant at both ends of the lake and in the sluggish portions of the streams below the falls. 17. Semotilus bullaris (Rafinesque). [Fall fish. Two specimens have been recorded. One taken from the lake, January 24, 1891, and another from Beaver Brook near McLean May 21, 1902. 18. Semotilus atromaculatus (Mitchill). Creek chub. Found throughout the basin as the most common minnow. In the streams above falls it is the most common fish. aa 19. Abramis crysoleucas (Mitchill). Roach. Common in all sluggish waters over a muddy bottom. It has not been found above falls. 1909.] THE, CAYUGA LAKE BASIN, Nia. 395 20. Notropis anogenus Forbes. Black-chinned minnow. “Quite common in the canal near Montezuma” (Meek). It has been taken several times in fairly large numbers at the mouth of Fall Creek and in the lower course of Sixmile Creek. 21. Notropis cayuga Meek. Cayuga minnow. Common in the lake and the lower course of tributaries. It has not been found above falls. 22. Notropis heterodon (Cope). Varying-toothed minnow. Common in the south end of the lake and the lower courses of streams where the water is sluggish. It appears to be uncommon at the north end of the lake. The only record we have for that region is twenty specimens taken in the Canoga marshes, June 24, tgot. In 1885 J. H. Comstock and S. E. Meek took several speci- mens from Beaver Creek near McLean. This is the only record of its occurrence above the falls. 23. Notropis blennius (Girard). Straw-colored minnow. Found only at the north end of the basin in sluggish water. 24. Notropis procne (Cope). Swallow-tailed minnow. Not common. It has been taken several times in the lower courses of Sixmile and Renwick creeks. 25. Notropis hudsonius (De Witt Clinton). Spot-tailed minnow. This species was found for the first time in this basin on April 25, 1908. It was taken in large numbers with a minnow seine in a slough at the Needham Biological Station in the Renwick marsh. 26. Notropis whipplii (Girard). Silverfin. Common in the lower courses of all the streams at the south end of the basin. In the fall of 1903 several specimens were taken from Eddy pond in Cascadilla Creek above a series of falls which aggre- gate about 400 feet. This is the only place where the species has been fourtd above falls. Its presence here is probably to be ac- counted for by the following: Mr. Wilbur Genung during the sum- mer of 1903 stocked a mill pond, situated at the source of Casca- dilla Creek, with fishes taken from an ice pond on the lowlands near Ithaca where this species is common. Specimens of this were undoubtedly among other species taken and later, when the dam 396 REED-WRIGHT—THE VERTEBRATES OF [October 1, went out during a flood, found their way to Eddy pond between which and the site of the dam there are no falls. 27. Notropis cornutus (Mitchill). Red fin. Abundant throughout the basin. 28. Notropis atherinoides Rafinesque. Rosy minnow. Rare. Meek took one specimen in Sixmile Creek and a few at Montezuma. Two specimens were taken near the mouth of Fall Creek November 23, 1906, and another at the Needham Biological Station April 25, 1908. 29. Notropis umbratilis lythrurus Jordan. Blood-tailed minnow. Meek records one specimen taken from a small stream near the Montezuma dry dock. 30. Rhinichthys atronasus (Mitchill). Black-nosed dace. Common in the southern portion of the basin and as far north as Ludlowville. At present there is no evidence of its occurrence at the north end of the lake. It is found both above and below falls. 31. Hybopsis kentuckiensis (Rafinesque). Horny head. The only record we have of this species is that of Meek: “A few specimens taken from Montezuma only.” 32. Exoglossum maxillingua (Le Sueur). Cut-lip minnow. Common. Found in all streams below falls in clear water. 33. Cyprinus carpio Linnaeus. Carp (introduced). Abundant in the lake and in a few of the streams. This species was first noticed in the lake about 1889. Four or five years prior to this date three different persons had constructed ponds and stocked them with carp. One was at Newfield in a tributary to the inlet, a second was in a small tributary to Fall Creek six or seven miles from the lake and a third was at Ludlowville in a tributary of Salmon Creek. In 1888 all three of these ponds gave way during a heavy flood and in the following year carp began to be in evidence in the lake and have increased rapidly to the present time. 1909.] REE CAYUGA LAKE: BASIN) NEOY: 397 Vil Order ARODES: 8. Family AncuILtip&. The True Eels. 34. Anguilla chrysypa Rafinesque. Common eel. Common in the lake and the larger streams and ponds. The largest specimen taken in the basin of which we have any record is one caught in the lake May 29, 1893, which measured three feet in length. One caught off Kidder’s Ferry a few years ago is said to have measured five feet. Vi ‘Order [SOSPOND YE. g. Family CLupeip&. The Herrings. 35: Pomolobus pseudoharengus (Wilson). Alewife, saw-belly. One of the most abundant fishes in the lake where it has been known since 1872. In the spring from the first of May to the mid- dle of August they die in great numbers and are washed ashore. During the summer of 1907 dead individuals were much more abundant than in the three preceding years. Many persons in the region of Cayuga lake attribute the presence of the alewife here to its introduction by Seth Green who, accord- ing to Dr. H. M. Smith,'* disclaimed any responsibility for their presence in Lake Ontario, but we have been unable to find any statement concerning Cayuga Lake. Dr. T. H. Bean" is of the opinion that they have come hither of their own accord, for he writes: As to their presence in Seneca and Cayuga lakes, New York, we have ground for believing that they have, of their own accord, penetrated thus far into the interior of New York State. Mr. Fred Mather writes that he has seen alewives go up the canal locks at West Troy and Professor H. L. Smith, of Geneva, who first noticed them in the neighborhood of Seneca Lake in June, 1868, states that the canal was opened at about that time and thinks that they might come into the New York lakes from the Chesapeake or Delaware Bays through Elmira and Painted Post. * Smith, H. M., “Report on the Fisheries of Lake Ontario,” Bull. U. S. Fish Com., 1892, p. 188. * Bean, T. H., “ The Fisheries and Fishery Industries of the United States,” Section I., Natural History of Aquatic Animals, Washington, 1884, p. 590. “ Fishes of New York,” Bull. 60, New York State Museum, p. 200. | 398 REED-WRIGHT—THE VERTEBRATES OF [October 1, Mr. John Diltz, of Ithaca, for many years a fisherman, and Mr. E. C. Stillwell, now of Ithaca but formerly a ferryman at Kidder’s both state that the alewife was introduced about 1872. Mr. John Vann tells us that they were introduced purposely as food for the lake trout. 10. Family SAtmMontip&. The Salmons and Trouts. Coregonus clupeiformis (Mitchill). Common whitefish. “T have seen no specimens of this species from the lake of which it is however undoubtedly an inhabitant”? (Meek). Various re- ports have been received of whitefish taken from the lake but we have never seen one that was of this species. Mr. John Vann states that all of the so-called whitefish brought to his notice have proved to be ciscoes. We do not believe that it is found here, the fact that it has been introduced notwithstanding. 36. Argyrosomus osmeriformis (H. M. Smith). New York smelt Still taken in fairly large numbers but not as common as for- merly. Old fishermen tell us that it has never been abundant since the introduction of the alewife. Prior to that time, according to their statements, it was very abundant. 37. Salmo fario Linneus. Brown trout (introduced). This species of trout is found in considerable numbers in the lake inlet, Enfield, Sixmile and Taughannock creeks. During the last season a very large specimen was caught in the reservoir in Sixmile Creek. 38. Salmo irideus Gibbons. Rainbow trout (introduced). Fairly common in the lake inlet and its tributaries. Mr. Vann has seen individuals make their way up over the low falls in Enfield (Greek: 39. Cristivomer namaycush (Walbaum). Lake trout. Common in the deeper portions of the lake. They have appar- ently increased in numbers within the past few years. Mr. Vann has observed that they follow the alewives into shallow water in the spring. During the late spring and summer months many in- dividuals, dead from lamprey wounds, are picked up from the sur- face of the lake. Occasionally one is found not quite dead and with the lamprey still clinging. 1909.] THE CAYUGA EAKE BASIN, (NY: 399 40. Salvelinus fontinalis (Mitchill). Brook trout. Common in suitable streams throughout the lake basin. Dur- ing the summer of 1908 many of the younger individuals perished because of the long draught which dried many of the smaller streams. Pe Order HAPLOMI: 11. Family UMpripa. The Mud Minnows. 41. Umbra limi (Kirtland). Mud minnow. This species has never been taken at the south end of the lake. Meek took it in small numbers at Montezuma and Cayuga. 12. Family Esocipa#. The Pikes. 42. Esox reticulatus (Le Sueur). Eastern pickerel. Common throughout the basin. Many individuals from this region approach very closely the characteristics of Esox vermicula- tus. 43. Esox lucius Linnzus. Northern pike. Common throughout the basin. - 13. Family Paeciriup#. The Killifishes. 44. Fundulus diaphanus (Le Sueur). Gray-back. Abundant in the lake, marshes, flood lands and the lower courses of the streams. X. Order HEMIBRANCHII. 14. Family GasterosTEID&. The Sticklebacks. 45. Eucalia inconstans (Kirtland). Brook stickleback. Common in standing water and pools both on the flats and up- lands above falls. XI. Order ACANTHOPTERI. 15. Family Percopsip#. The Trout Perches. 46. Percopsis guttatus Agassiz. Trout Perch. Common. Found in the south end of the lake and the lower courses of the streams. At the breeding season, which occurs dur- ing the first two weeks in May, they are abundant in the shallow sloughs of the marshes. 400 ) REED-WRIGHT—THE VERTEBRATES OF [October 1, 16. Family ATHERINIDZ. The Silversides. 47. Labidesthes sicculus (Cope). Brook silverside. “Not found near Ithaca. Several specimens taken from a small stream which empties into the canal a few rods south of Montezuma” (Meek). It is now found to be common at the south end of the lake over a muddy bottom along shore and in the lower courses of streams. 17. Family CENTRARCHIDZ. The Sunfishes. 48. Pomoxis sparoides (Lacépede). Calico bass. Common at the south end of the lake. During the late summer and early fall of 1906 the young of the species was abundant in the lower course of Fall Creek and its tributaries. 49. Ambloplites rupestris (Rafinesque). Rock bass. Common. The young are abundant in the lower courses of all streams throughout the basin. It is not found above falls except in Eddy pond in Cascadilla Creek where its presence is probably to | be explained in the same way as Notropis whipplii. 50. Apomotis cyanellus (Rafinesque). Green sunfish. No specimens of this species have been recorded from the lake basin in recent years and never from the south end. Meek found a few near Montezuma. 51. Lepomis pallidus (Mitchill). Bluegill. Meek found it in small numbers at Montezuma. None have been recorded from other localities in the basin. 52. Eupomotis gibbosus (Linnzeus). Pumpkin seed. Abundant throughout the basin. It spawns during the whole of June and first part of July. 53- Micropterus dolomieu Lacépéede. Small-mouthed black bass. Common. Meek recorded this species as not found by him at the south end of the lake where it is now common. During late sum- mer and early fall the young are found abundantly in the lower courses of the streams tributary to the lake. By the last of August the young vary between four and five centimeters in length and by December have attained a length of from six to seven centimeters. 1909.] TEE CAYUGA TAKE “BASINS: Nir. 401 54. Micropterus salmoides (Lacépéde). Large-mouthed black bass. Common in the lake. Young of this species are found in sum- mer and fall along with those of the former species. Specimens obtained in the streams in December average between seven and eight centimeters in length. 18. Family Percip#. The Perches. 55. Stizostedion vitreum (Mitchill). Wall-eyed pike. Found in the lake but not common. 56. Stizostedion canadense (Smith) Sauger. Found in the lake in about the same abundance as the preceding species. 57. Perca flavescens (Mitchill). Yellow perch. Abundant throughout the basin. It spawns during the first of April. 58. Percina caprodes zebra (Agassiz). Manitou darter. Rare. Two specimens have been recorded in this basin; one May 27, 1907, in Fall Creek near the mouth and one July 18, 1907, in the inlet about four miles from the lake. 59. Boleosoma nigrum (Rafinesque). Johnny darter. One specimen taken in Renwick brook on the flats April 21, 1900, by T. L. Hankinson and C. O. Houghton. 60. Boleosoma nigrum olmstedi (Storer). Tessellated darter. Common in the lake and tributaries below falls. 61. Etheostoma flabellare Rafinesque. Fan-tailed darter. Common. Found in localities along with the preceding species. 19. Family SERRANID#. The Sea Basses. 62. Roccus chrysops (Rafinesque). White bass. Two specimens of this species have been taken from the lake basin; one from the inlet April 18, 1877, and one April 15, 1896. 20. Family Cortina. The Sculpins. 63. Cottus ictalops (Rafinesque). Blob. Common at both ends of the lake in cold water. The eggs are 402 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, deposited in masses attached to the under side of stones where they are guarded by one of the parents. 64. Cottus gracilis (Heckel). Miller’s thumb. Not common but found throughout the basin. 21. Family Gapip#. The Cods. 65. Lota maculosa (Le Sueur). Burbot. Not common. Found only in deep water. C. Class AMPHIBIA. XII. Order PROTEIDA. 22. Family Proreipz. The Mud Puppies. 66. Necturus maculosus Rafinesque. Mud puppy. Abundant in the lake and the lower courses of the inflowing streams. They have been taken in the inlet three miles from the lake. XML: + Order URODELA: 23. Family AMBYSTOMID. 67. Ambystoma punctatum (Linnzus). Spotted salamander. Common throughout the basin. Depending upon the season, egg- laying begins the last of March or the first of April immediately after emerging from hibernation. The earliest date March 13, 1903. Transformation of the larva begins the last of July or about four months after the eggs are laid. From this time to the middle of Sep- tember transforming individuals may be found. 24. Family PLETHODONTID. 68. Hemidactylium scutatum Tschudi. Four-toed salamander. Not common. The first specimens recorded were obtained near Ithaca in the valley of Sixmile Creek by H. W. Norris in April 18809. No other specimens were found in this basin until October 22, 1905, when twenty-one specimens were found on Larch Hill, two miles south of Ithaca on the east side of the inlet valley. They were all found under stones or about the bases of stumps in the open. * Gage, S. H., “ Notes on the Cayuga Lake Stargazer,” The Cornell Review, November, 1876, p. 91. 1909.] THE CAYUGA LAKE (BASIN, Ni Ye 403 69. Plethodon erythronotus (Green). Red-backed salamander, gray salamander. Common. Found usually in dry places under stones or any object which will furnish cover. They appear from hibernation the last of March or the first of April. The earliest date upon which they have been recorded in the spring is March 17, 1903. The latest date on which they have been observed in the fall is November 1, 1903. The eggs are deposited during June and July, under logs, loose bark or in decaying wood, in bunches of from seven to twelve. Each egg is attached by a slender cord to a common focus and the whole cluster is attended by the female. The young transform im- mediately after hatching. There is every possible gradation be- tween the red-backed and gray forms.*® During the summer of 1908 a pure red individual was found at Chautauqua, N. Y. 70. Plethodon glutinosus (Green). Slimy salamander. Common but limited to certain localities. Found usually in moist humus, manure piles, damp moss banks and decaying vegeta- tion. Its breeding habits are not known. 71. Gyrinophilus porphyriticus (Green). Purple salamander. Common. Found in all cold springs and streams flowing through gorges or ravines. They remain in the larval stage for a period of two years, at least. The only record of transformation which we have obtained is a specimen 11.5 cm. long found March 14, 1903, in which the larval characteristics have almost entirely disap- peared. A female taken May 12, 1906, with mature eggs in the ovaries and what appeared to be a larva not long after hatching taken from a cold brook June 29, 1901, are the only clues we have to the breeding habits. 72. Spelerpes bislineatus (Green). Two-lined salamander. Common in and about cold swift brooks. The breeding habits have not been observed in this locality. *® Reed, H. D., “A Note on the Coloration of Plethodon cinereus,’ Am. Nat., Vol. 42, 1908. 404 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 25. Family DESMOGNATHID&. 73. Desmognathus fusca (Rafinesque). Dusky salamander. One of the most abundant salamanders in the lake basin. It is found under most any sort of object which will furnish cover in wet and marshy places along the cooler streams. The maximum period of egg-laying is July. The eggs are laid in clusters joined by a slight cord to a common focus but not attached to extraneous objects as in the case of Plethodon erythronotus. The female at- tends the eggs and is found usually with the body partly encircling them. The larve transform from September to December, when they are from 18 to 20 millimeters long. 26. Family PLEURODELID2. 74. Diemictylus viridescens Rafinesque. Vermilion-spotted newt. The most abundant salamander found in the lake basin. The adult is found in every pool, pond, ditch and stretch of standing water. Individuals in the red land stage are common on the woods under dead leaves and decaying bark and wood. The eggs are de- posited singly upon the leaves of aquatic plants from April to June. Larve begin to transform to the red land stage in August, continuing until September. Some individuals pass the winter in the larval stage. After two and one half or three years the red land form assumes a viridescent coloration and becomes permanently aquatic.'* xix Order SALTEN TTA: 27. Family Buronip&. The Toads. 75. Bufo americanus Le Conte. American toad. Abundant. The average date of emergence from hibernation is April 15. The earliest recorded date is March 19, 1903. They proceed immediately to the water where the eggs are deposited. The maximum period of egg-laying is between April 20 and May 30, although stragglers continue to spawn until July. The larval period lasts for about sixty days, the tadpoles beginning to transform about the last of June. The latest fall record for this species is October 20, 1900. ™See Gage, S. H., “Life-history of the Vermilion-spotted Newt,’ Am. Nat., 1801, p. 1084. 1909.] TEE \CAVUGAWAIGE, BASIN TING (Ye 405 28. Family Hytipa. The Tree Frogs. 76. Hyla versicolor Le Conte. Common tree toad. Abundant. It appears from hibernation the last of April or very first of May. The eggs are laid the first of June in bunches of from four to twenty-five, which float at the surface either attached to vegetation or free. Transformation begins the first of August making the larval period of from fifty to sixty days duration. The latest fall record for this species is October 25, 1905. 77. Hyla pickeringii (Holbrook). Peeper. Abundant. It emerges from hibernation the last of March. The height of the egg-laying season is April although individuals are found depositing their eggs as early as the last of March. The eggs are attached singly to vegetation beneath the surface of the water. Sometimes they are found in bunches of from four to twelve. Transformation begins the middle of July at the end of a larval period of from go to 100 days duration. The latest fall record is October 30, 1901. 29. Family Ranipm. The Frogs. 78. Rana pipiens Schreber. Leopard frog. The most abundant anuran throughout the basin. They come out from hibernation the last of March or the first of April. The eggs are seldom deposited before April 10 from which date active spawning continues for about four weeks. The tadpoles begin to transform the middle of July, about 100 days after the eggs are laid. The latest fall record is November 18, 1906. 79. Rana palustris Le Conte. Pickerel frog. Common. The average date of its appearance in the spring is April 13. In some seasons it has been found to emerge the last of March. The eggs are deposited in bunches attached to submerged twigs and grasses. As a rule egg-laying does not begin until the last of April. They may be distinguished from the eggs of other frogs of this region by their decided yellow color. The tadpoles transform the last of July, about 90 days after the eggs are deposited. The latest fall record for the species is November 1, 1902. 405 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 80. Rana clamata Daudin. Green frog. Common. It appears from hibernation the middle of April. The eggs are not laid until the first of June, through this month, July and a part of August. The eggs are deposited in a frothy film which floats at the surface of the water. The larval period is of about thirteen months duration transformation beginning the middle - of the July of the following year in which the eggs are laid. The latest fall record is November 1, 1902. 81. Rana catesbeiana Shaw. Bull frog. Common. This is the last one of the frogs to emerge from hiber- nation, never appearing before the middle of May. The eggs are laid the last of June and the first of July in an irregular sheet or film attached to sticks or twigs near the surface of the water. The larval stage lasts for a period of two years, the tadpoles transform- ing in July and August of the second year following hatching. 82. Rana sylvatica Le Conte. Wood frog. Common. It appears in the spring, the last of March or the first of April. Egg-laying begins almost immediately. The young trans- form the last of June about go days after the eggs are laid. The latest fall record is November 1, 1906. D. Class REPTILIA. XX. Order OPHIDIA, 30. Family CoLusrip#. The Harmless Snakes. 83. Diadophis punctatus (Linnzus). Ring-necked snake. Common. The earliest date upon which it has been observed in the spring is April 19, 1900. The latest fall date is October 16, 1905. 84. Liopeltis vernalis (Harlan). Smooth green snake. Not common. De Kay, however, records it as common at the north end of the lake in the marshes. The latest fall record is Octo- ber 20, 1906. 85. Bascanion constrictor (Linnaeus). Black snake. Formerly common. Now confined to the region about New- field and Danby in the southern portion of the basin. 1909.] REE, CAYUGA LAI BASIN Ni Ye 407 86. Coluber obsoletus obsoletus Say. Racer. Rare. Only four specimens recorded for the basin. Two of these were taken June 14, 1883, one during the summer of 1889 and the fourth, a specimen five feet long, was captured alive at New- field in August, 1899. 87. Lampropeltis doliatus triangulus (Boie). Milk snake. Common throughout the basin. 88. Lampropeltis doliatus collaris (Cope). One specimen taken June 16, 1903. So far as we know this is the first record of this variety for the state. The specimen agrees with Cope’s figure and description and with a specimen of collaris taken at Danville, Ill. 89. Natrix sipedon (Linnzus). Water snake. Abundant throughout the basin, especially in the marshes where on clear days they are found coiled on stools of dead sedges. go. Storeria occipitomaculata (Storer). Red-bellied snake. Common throughout the basin under logs, pieces of bark and dead leaves along hillsides and dry places. In the fall they are seen in the open upon lawns, roads and walks. The earliest spring record is March 18, 1903. The latest fall record is October 21, 1906. gi. Thamnophis saurita (Linneus). Ribbon snake. Common, especially in the lowlands and moist meadows. The earliest spring record is March 19, 1905. The latest they have been seen in the fall is October 30, 1901. 92. Thamnophis sirtalis sirtalis (Linnzus). Striped garter snake. This is the most abundant snake in the basin. They appear in the spring about the first of April and are abroad until the last of October. 31. Family CrotaLtipz. The Pit Vipers. 93. Crotalus horridus Linnzus. Common rattlesnake. Formerly abundant. They are still met with about McLean. 408 REED-WRIGHT—THE VERTEBRATES OF [October 1, MXM Order LACERTIELS: 32. Family Scincip@. The Skinks. 94. Leiolopisma laterale (Say). Ground lizard. One specimen (No. 3550) taken at Caroline April 23, 1892, by Wee terry tand L.A. Puertes: Oy Order MESTUDINATAS 33. Family TrRionycHip%. The Soft-shelled Turtles. 95. Aspidonectes spinifer (Le Sueur). Common soft-shelled turtle. Common at the north end of the lake. -A few specimens have been taken at the south end. 34. Family CHELypRID&. The Snapping Turtles. 96. Chelydra serpentina (Linnzus). Snapping turtle. Common. Found in all marshy places. The earliest spring record is April 13, 1906. The eggs hatch the first of October. On October 3, 1883, twenty-four specimens were found that had just hatched. A few were still in the nest but the larger number were in line moving towards water. 35. Family KinostErNID#. The Musk Turtles. g7. Terrapene odorata (Latreille). Musk turtle. Common in the Seneca river and marshes about Montezuma where it was first found by A. A. Allen and J. T. Lloyd, September 24, 1908. 36. Family Emypipa. The Pond Turtles. 98. Chrysemys marginata (Agassiz). Agassiz’ painted turtle. Abundant throughout the basin. On January 25, 1906, a single individual was observed swimming under the ice on a pond near Ithaca. The same day 150 were taken by fishermen at the head of the lake. This early emergence from hibernation was due to the extremely mild winter up to that date and the unusually warm week of January 25. On the same date this species was observed along the southern shore of Lake Ontario. 1909.] THE CAYUGA-LAKE BASIN, Nery: 409 99. Clemmys muhlenbergii (Schoepff). Muhlenberg’s tortoise. For the present this species must be considered rare. Thus far only three specimens have been taken; one on June 15, 1877, near Ithaca, and two at Junius, May 26, 1906. The specimen taken near Ithaca was kept alive for a time and on July 20 deposited eggs in the sand of the terrarium. 100. Clemmys insculpta (Le Conte). Wood tortoise. Common throughout the basin in wooded regions along water courses. tor. Clemmys guttata (Schneider). Spotted turtle. The only records of this species are from Junius in the extreme northwestern portion of the basin where it is common. E. Class AVES. XXIII. Order PYGOPODES. The Diving Birds. 37. Family Cotympip#. The Grebes. 102 (2).1* Colymbus holboelli (Reinhardt). Holboell’s grebe. Not an uncommon transient during April and November. A few are found regularly in winter. The latest spring record for this species in the basin is May 25, 1907. ‘They are seldom taken at the south end of the lake. 103 (3). Colymbus auritus Linnzus. Horned grebe. Common transient from April 1 to May to and occasionally taken in winter. In the spring they become common about the mid- dle of April and all have disappeared by May 10. They appear in the fall the first of October, gradually increasing in numbers until November throughout which they are common. 104 (6). Tachybaptus podiceps (Linnzeus). Pied-billed grebe. A common transient and an uncommon but regular summer resi- dent in the marshes at the north end of the lake. In the spring they appear April 1 and are common throughout the month. In the fall they become common the first of October and continue so until Nov- ember 1. The latest fall record is a young female taken Novem- The number of the species in “ Check-list of the American Ornitholo- gists’ Union.” PROC, AMER. PHIL. SOC,, XILVIII. 193 BB, PRINTED JANUARY 7, IQIO. 410 REED-WRIGHT—THE VERTEBRATES OF [October 1, ber 15, 1897. In a collection of birds made at Ithaca about fifty years ago are several immature specimens ranging in size from just hatched to birds two-thirds grown. In the spring of 1909 a nest was found in the Renwick marshes. 38. Family GAviupa. The Loons. 105 (7). Gavia immer (Brunnich). Common loon. Common transient. They appear in the spring from April 14 to May 20, being the most common the very last of April. On April 28, 1908, Mr. L. A. Fuertes reported a flock of 50 off the mouth of Taughannock Creek. All of our fall records of this species occur between October 29 and November 29. Audubon mentions this species as breeding on Cayuga Lake in 1824. 106 (11). Gavia stellata (Pontoppidan). Red-throated loon. Rare. There is a specimen of a male in the collection of Cornell University taken on Cayuga Lake at Ithaca, November 4, 1875, by Dr. M. J. Roberts. Another specimen was taken at Sheldrake a few years ago by Jacob Cram. It was identified by L. A. Fuertes, who states that it was probably killed in November, 1880. 39. Family Atcip#. The Auks. 107 (31). Uria lomvia (Linneus). Brtinnich’s murre. Occasionally seen in recent years. The first record for Cayuga Lake was a specimen reported in 1854 by William Hopkins of Au- burn.t® On December 14, 1895, a specimen was shot and is now in the possession of H. G. Wilson, of Ithaca. On December 16 of the same year two more specimens were killed. According to our records they did not appear again until the fall of 1899 when in Nov- ember a female was obtained. Eaton?® mentions them as on “ Cay- uga Lake, winter of 1899.” The next record was a specimen taken at Ithaca December 19, 1901 by T. L. Hankinson. Since that date we have no knowledge of this species on the lake. ® Hopkins, William, Proc. Boston Soc. Nat. Hist., Vol. V., p. 13, July, 1854. * EFaton, E. H., “ Birds of Western New York,” Proc. Rochester Acad. Sci., Vol. IV., pp. 1-164. 1909.] THE | CAVUGA CAKE BASING (Nix: 411 XXIV. Order LONGIPENNES. The Long-winged Swimmers. 40. Family Larip#. The Gulls and Terns. 108 (40). Rissa tridactyla (Linnzus). Kittiwake. A specimen was reported by William Hopkins in 1854. 109 (43). Larus leucopterus Faber. Iceland gull. A specimen was taken on Cayuga Lake by L. A. Fuertes during the winter of 1896-7 and another was brought in by a fisherman March 17, 1897. 110 (51). Larus argentatus Pontoppidan. Herring gull. Common winter resident. It is abundant during the spring and fall. They appear in the fall the first of September and leave in the spring about May 25 the latest record being June 2, 1906. III (54). Larus delawarensis Ord. Ring-billed gull. Foster Parker, of Cayuga, has a specimen taken on the lake a few years ago. 112 (60). Larus philadelphia (Ord). Bonaparte’s gull. Transient. Common in spring, rare in fall. It is found in the spring from April 20 to May 25 and is usually common during that period. On June 14, 1908, a flock of eleven individuals was reported at the south end of the lake and on July 24 of the same year L. A. Fuertes reported a single individual from Cayuga at the north end of the lake. In the fall this species is found occasionally in October and November. 113 (62). Xema sabinei (Sabine). Fork-tailed gull. One specimen taken at the north end of the lake about 1887 by Foster Parker. It is now in the collection of E. H. Eaton. 114 (70). Sterna hirundo Linnzus. Common tern. Regular, though not common, transient through May and the first of June. Mr. L. A. Fuertes reports a specimen the latter part of April 1898 and two adults near the mouth of Fall Creek at Ithaca, July 6, 1908. The only fall record of this species is a single ind- vidual reported by L. A. Fuertes the last of August, 1907. 412 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 115 (74). Sterna antillarum (Lesson). Least tern. Mr. F. R. Rathbun** recorded two specimens taken on Cayuga Lake. 116 (77). Hydrochelidon nigra surinamensis (Gmelin). Black tern. Not an uncommon spring migrant during the last half of April and the first of May. Foster Parker has found them nesting on old musk rat houses in the Cayuga marshes. L. A. Fuertes took a speci- men August 28, 1900, at Ithaca, and reported three others seen at the same time. XXV. Order TUBINARES. The Tube-nosed Swimmers. 41. Family PRocELLARIID«&. Shearwaters and Petrels. 117 (98). Astrelata hasitata (Kuhl). Black-capped petrel. There was a specimen in the collection of L. S. Foster, number 759, taken in Cayuga Co., early in September, 1893. XXVI. Order STEGANOPODES. The Totipalmate Birds. 42. Family PHALAcRocorAcip2. The Cormorants. 118 (119). Phalacrocorax carbo (Linnzus). Common cormorant. A specimen was reported by William Hopkins as taken by him at Auburn. 119 (120). Phalacrocorax auritus (Lesson). Double-crested cor- morant. Rare. An adult male was taken November 16, 1875, by Dr. J. M. Roberts. A second specimen was taken September 29, 1905, at Au- rora, N. Y., and is now in the collection of Wells College. An im- mature specimen was obtained at Ithaca, August 2, 1906, by L. A. Fuertes. 43. Family PELECANID&. The Pelicans. 120 (125). Pelecanus erythrorhynchos Gmelin. White pelican. There are two records of this species for Cayuga Lake. A specimen was obtained by Mr. Cave in 1876, concerning which Mr. J. W. Beal?? writes as follows: Rathbun, Frank R., “ A Revised List of the Birds of Central New York,” p. 41, Auburn, N. Y- “? Beal, J. W., American Naturalist, Vol. I. (1867), p. 323. 1909.] THE CAMUGA) LAKE BASIN: NEw; 415 Sometime during the spring of 1864, near a marsh on Cayuga Lake, two large birds were seen for several weeks, but one of them left a few days before the other was killed. None of the hunters had ever seen anything of the kind about here before. It proved to be a specimen of the white or rough-billed pelican (Pelecanus erythrorhynchus Gmelin), in good condition, and its wings measured fully eight feet from tip to tip. In the late summer about 1888 Foster Parker killed a specimen which is now in the New York State Museum. XXVIII. Order ANSERES. Lamellirostral Swimmers. 44. Family ANatip#. The Ducks and Geese. I2I (129). Mergus americanus Cassin. Merganser. Common winter resident from the middle of October to the last of April. The latest spring record is April 27, 1907, upon which date they were still common. 122 (130). Mergus serrator Linnzus. Red-breasted merganser. Common transient and found in small numbers during the winter. It is not common after April 25 and the latest date upon which they have been recorded in the spring is May 25, 1907. 123 (131). Lophodytes cucullatus (Linnzus). Hooded merganser. Common transient from the last of March to the last of April. Foster Parker reports it as breeding occasionally in the Montezuma marshes. In the fall individuals are common from the middle of October to the middle of November. 124 (132). Anas platyrhynchos Linneus. Mallard. Common transient during March and April and again in October. It is sometimes found in winter and Foster Parker reports it as breeding in the marshes at the north end of the lake. They first appear in the fall about the middle of September and remain as late as the last of November but are most common in October. 125 (133). Anas rubripes tristis Brewster. Black duck. Common transient and regular but not common in winter. It breeds regularly and in fair numbers in the Canoga and Montezuma marshes. 414 REED-WRIGHT—THE VERTEBRATES OF [October 1, 126 (135). Chaulelasmus streperus (Linneus). Gadwall. Common transient the latter part of March and the entire month of April. They appear in the fall the last of September and remain until the very last of October. The latest fall record is a male killed November 20 at Cayuga. This species is not common at the south end of the lake. 127 (136). Mareca penelope (Linnzeus). European Widgeon. Mr. F. S. Wright of Auburn has a specimen killed on Cayuga lake in the spring of 1881. It is an adult male in full plumage. Foster Parker reports that several have been killed at Cayuga. 128 (137). Mareca americana (Gmelin). Baldpate. Common transient from March 23 to April 26, the bounding dates of our records. In the fall they appear during the last week of September and remain until the first of November. The latest date upon which they have been recorded in any numbers is October 22, 1905. 129 (138). Nettion crecca (Linnzus). European teal. Accidental. A male was shot by Will Canfield at Cayuga, April 10, 1902. The specimen was identified by E. H. Eaton. 130 (139). Nettion carolinensis (Gmelin). Green-winged teal. Common transient during April and October. Arrivals are to be noted the last of September but it is most common during October. This species is very rarely found in winter. 131 (140). Querquedula discors (Linnzus). Blue-winged teal. Common transient during April and in the fall during the last half of September and throughout October. It formerly bred in fairly large numbers in the marshes at the north end of the lake. 132 (142). Spatula clypeata (Linnzus). Shoveller. Common transient. It is not often found at the south end of the lake. 133 (143). Dafila acuta (Linneus). Pintail. Transient during the last of March and the first of April and in the fall during October and the first half of November. 1909.] Die CAYUGA LAKE BASIN, ‘No Y: 415 134 (144). Aix sponsa (Linnzus). Wood duck. Summer resident but not as common as formerly. It still breeds in small numbers at Cayuga. During the summer of 1907 a pair nested in the woods of the Renwick marshes at Ithaca. 135 (146). Marila americana (Eyton). Red head. Common transient and regularly present in winter. In the spring it is common from the middle of March throughout April. In the fall it is found during October and November. 136 (147). Marila vallisneria (Wilson). Canvas-back. Common transient and a regular winter visitant in smaller num- bers from the middle of November to the last of March. 137 (148). Marila marila (Linneus). American scaup duck. Winter resident from the first of October to the very last of April. It is more common during migration. 138 (149). Marila affinis (Eyton). Lesser scaup duck. Common transient. A few are occasionally found in winter. They arrive in the fall the first of October and remain until the middle of November. In the spring they are to be found from April 1 to June 24, the latest date. 139 (150). Marila collaris (Donovon). Ring-necked duck. Usually a rare transient. Foster Parker reports it as common during the spring of 1905 at the north end of the lake. 140 (151). Clangula clangula americana (Bonaparte). Golden-eye. Common winter resident from November 1 to April I. I41 (152). Clangula islandica (Gmelin). Barrow’s golden-eye. Rare. One specimen, an adult female, taken at Cayuga by L. A. Pnoertesy December, 20; 1906: (Coll), of L.A. F..no0.) 1523.) 142 (153). Charitonetta albeola (Linnzus). Buffle-head. Common transient. It appears in the spring from the middle of April to the last of May. In the fall arrivals from the north appear usually the second week in October and remain until the last of November. 143 (154). Harelda hyemalis (Linnzus). Old-squaw. Common transient and not uncommon in winter. They arrive the middle of October and remain until the first of May. 416 REED-WRIGHT—THE VERTEBRATES OF [October 1, 144 (162). Somateria spectabilis (Linneus). King eider. “A mounted specimen of an adult male, taken on Cayuga lake, is now in the barroom of the Cornell House at Trumansburg, N. Y.” (L. A. Fuertes). On November 3, 1908, at Cayuga four individuals, three females and an immature, were shot from a flock of twenty. 145 (163). Oidemia americana Swainson. Scoter. Common transient and uncommon winter resident. The earliest fall record is a specimen shot October 13, 1885. 146 (165). Oidemia deglandi Bonaparte. White-winged scoter. Common winter resident from October 3 to May 1. 147 (166). Oidemia perspiciliata (Linnzus). Surf scoter. Uncommon. We have no spring records of this species. The earliest date upon which it has been recorded in the fall is that of a specimen shot by L. A. Fuertes, October 13, 1906. 148 (167). Erismatura jamaicensis (Gmelin). Ruddy duck. Common transient in the fall from October 1 to November 1. It is occasionally taken in the spring but much less common at this season. 149 (169a). Chen hyperborea nivalis (Forster). Greater snow goose. Two young were killed near Ithaca during the last of March, TO70.7° 150 (169.1). Chen cerulescens (Linnzus). Blue goose. Two specimens, male and female, were killed a few years ago on Cayuga Lake by Foster Parker. They are now in the New York State Museum. 151 (172). Branta canadensis (Linnzeus). Canada goose. Common transient and an occasional winter resident. They are common in the spring from March 10 to May 7. In the fall this species begins to arrive from the north about October 1 and is pres- ent until December 1. The latest record of what appeared to be migrating flocks is December 9, 1907. Forest and Stream, Vol. 7, p. 283. 1909.] THE CAYUGA, LAKE: BASEN, Ni ¥- 417 152 (173a). Branta bernicla glaucogastra (Brehm). Brant. Rare. No specimens of this species have been recorded from the lake basin in recent years. Foster Parker has in his possession a specimen shot on Cayuga Lake a few years ago. From the Auburn List?* we quote the following: One shot on Cayuga Lake, N. Y., near the railroad bridge by Mr. Charlie Traverse. The same was identified by Mr. Greene Smith—Horace Silsby, in Auburn Daily Bulletin of December, 1877. An adult male received from Cayuga Lake, November 26, 1878, which was also shot near the railroad bridge by Mr. David Copeman. 153 (180). Olor columbianus (Ord). Whistling swan. Rare. Two specimens were shot by Foster Parker a few years ago and another is recorded by Fowler, Wright and Rathbun? from the Seneca River. On March 16, 1908, a flock of 118 individuals was reported from the north end of the lake. According to Father Raffeix swan were common on the lake in the days of the Jesuits for he writes :*° “It [Cayugal abounds in swan and geese all winter.” XXVIII. Order HERODIONES. The Heron-like Birds. 45. Family Inipiwa. The Ibises. 154 (186). Plegadis autumnalis (Hasselquist). Glossy ibis. William Hopkins recorded a specimen from Cayuga Lake in 1854. There are two specimens in the possession of Foster Parker taken on the Seneca River in 1902. F.S. Wright shot one specimen and saw three others on Howland Island in May, 1902. On May 27, 1907, two males and two females were shot at Cayuga by Foster Parker. 46. Family Arpeip&. The Herons. 155 (190). Botaurus lentiginosus (Montagu). Bittern. Common summer resident. It nests in every marsh of any size throughout the basin. The average date of spring arrival is April 15, the earliest, March 28, 1908. Nesting begins the middle of May *« A Revised List of Birds of Central New York,” collected and pre- pared for publication by Frank R. Rathbun, Auburn, N. Y. * Ornithologist and Odlogist, Vol. 7, p. 133. *6 Father Raffeix, “ Relations for the Year 1671-72,” Quebec edition, p. 22. 1 . 418 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, and continues for the rest of the month. Young in the nest are found from the first to the middle of June. They depart for the south the first of November. 150 (191). Ixobrychus exilis (Gmelin). Least bittern. Common summer resident. The average date of spring arrival is May 15, the earliest May 9, 1908. The active period of nesting extends from May 20 to June 10. Young are found in the nest from about June 8 to June 25. We have no records of this species in the fall later than September Io. 157 (194). Ardea herodias Linnzus. Great blue heron. Common spring and fall transient and summer resident at Mer- idian, N. Y., at the north end of the basin. The average date of spring arrival is March 28, the earliest, March 18, 1890. In the fall they appear at the south end of the basin the last of July, the earliest record being a specimen taken July 18, 1889, by L. A. Fuertes. We have no records indicating that this species remains aiter November I. 158 (196). Herodias egretta (Gmelin). Egret. This species was recorded in 1854 by William Hopkins. Foster Parker has in his collection a specimen shot at Cayuga but without record or recollection of date. 159 (201). Butorides virescens (Linnzus). Green heron. Common summer resident. The average date of spring arrival is May 2, the earliest, April 18, 1906. Nesting begins about May 10 and continues until the middle of July. On July 11, 1906, four nests were found, one containing four eggs and the others, young birds which left the nest upon approach. This species leaves in the fall about the last of September, the latest record being October 2, 1902. 160 (202). Nycticorax nycticorax nevius (Boddaert). Black- crowned night heron. Never common but a regular spring and fall migrant. In the former season our records extend from May 11 to June 2, in the latter from July 14 to October 29. 1909.] are CAYUGA LAKE, BASIN rN -Y: 419 POX Order PALUDICOLZ:.” ‘The Cranesand Rails: 47. Family Gruipz. The Cranes. 161 (204). Grus americana (Linnzus). Whooping crane. “Several years ago a specimen was killed on Cayuga Lake— I'rank A. Ward” (Eaton, 1901). 48. Family Ratiip#. The Rails. 162 (208). Rallus elegans Audubon. King rail. Not an uncommon summer resident in the marshes at the north end of the basin. There is but one record of this species at the south end of the lake, an adult male shot November 29, 1901. 163 (212). Rallus virginianus Linnzus. Virginia rail. Common summer resident in all the marshes throughout the basin. The average date of spring arrival is May 1, the earliest, April 24, 1904. They nest the last half of May and throughout June. The earliest date for nest is May 18, 1905. The latest date upon which nest and eggs have been found is July 9, 1906. They are abundant throughout September and the first half of October. All have usually departed by November 1. 164 (214). Porzana carolina (Linnzus). Sora. Common summer resident throughout the basin. The average date of spring arrival is May 1, the earliest, April 14, 1908. About the middle of October this species becomes exceedingly abundant and usually all have left by the last of the month. The nesting period is the same as for the preceding species. 165 (215). Coturnicops noveboracensis (Gmelin). Yellow rail. Mr. F. S. Wright, of Auburn, reports that two or three have been taken at the north end of the lake. One of them was a male shot at Meridian, N. Y., in 1897. 166 (219). Gallinula galeata (Lichtenstein). Florida gallinule. Fairly common summer resident in the marshes at the north end of the lake where it arrives the last of April. Ralph and Bagg?‘ 7 Ralph, William L., and Bagg, Egbert, “ Annotated List of the Birds of Oneida County, N. Y., and Its Immediate Vicinity,” Trans. of the Oneida Historical Society, Vol. I11., p. tor, 1886. 420 REED-WRIGHT—THE VERTEBRATES OF [October 1, recorded this species as very common in the marshes of Seneca River where they bred in great numbers. In recent years it has not been recorded near Ithaca. E. H. Eaton informs us that C. J. Pennock saw a female with young in the Renwick marshes in July, 1879. Cornell University has recently come into the possession of a collection of birds made near Ithaca in 1850. Among the skins is one of an adult male and one of a young individual in first plumage. 167 (221). Fulica americana Gmelin. Coot. Common transient the last of April and the first of May and an occasional summer resident in the marshes at both ends of the lake. On May 25, 1907, a nest containing five eggs was found in the west marsh at Ithaca. On June 1 it contained ten eggs and on June 9, when it was last visited, the number was the same. During October this species is very common and departs usually by the last of the month. XX! Order LIMICOLAL, The Shore ‘inds. 49. Family PHALARopopipa. The Phalaropes. 168 (222). Phalaropus fulicarius (Linnzus). Red phalarope. Rare transient visitant. William Hopkins reported a specimen in 1854. In the collection of Cornell University there is a specimen of a male killed on Cayuga Lake October 18, 1885, by E. H. Sar- gent. 169 (223). Lobipes lobatus (Linnzus). Northern phalarope. In the collection of E. H. Eaton are two specimens, male and female, taken at Montezuma in 1895. In the collection of Cornell University is a specimen taken at Ithaca in 1850. 170 (224). Steganopus tricolor (Vieillot). Wilson’s phalarope. One specimen, a young individual, was obtained by L. A. Fuertes at Ithaca’ in the tallvor 1692. 49a. Family Recurvirostrip&. The Avocets and Stilts. 170a (225). Recurvirostra americana Gmelin. Avocet. One specimen (C. U. 5219) was taken at Renwick, September 16, 1909, by Mr. A. A. Allen. 1909.] (LE wCAMUGA SL ARE BASIN, IN. Y. 421 50. Family Scotopacip&. The Snipe. 171 (228). Philohela minor (Gmelin). Woodcock. Summer resident in moist areas throughout the basin. They arrive in the spring the last of March and leave in the fall during the first two weeks of November. The woodcock is slowly in- creasing in numbers about Ithaca. Mr. John Vann tells us that in the fall of 1908 all the individuals of several localities succeeded in migrating without any loss from shooting. He attributes the in- crease partly to the growth of cover in the uplands where they are found during the fall.: 172 (230). Gallinago delicata (Ord). Wilson’s snipe. Common transient between April 12 and May 20. In 1908 one was recorded on April 3. They are most abundant during the latter part of April. Our autumn records fall between September 22 and November 18. The downy young were found at Meridian, N. Y., by E. G. Taber and F. S. Wright states that it is a rare breeder in the marshes at Cayuga. 173 (231). Macrorhamphus griseus (Gmelin). Dowitcher. There is a specimen in the collection of Foster Parker taken on Cayuga lake but without other data. From August 18 to 26, 1908 Foster Parker shot one and saw five others. 174 (233). Micropalama himantopus (Bonaparte). Stilt sandpiper. Foster Parker shot a specimen at Cayuga October 10, 1907, in a flock of red-backed sandpipers. August 25, 1908, E. H. Eaton took a specimen at Cayuga and two more on September 20. On Sep- tember 28, 1908, A. A. Allen and J. T. Lloyd shot a specimen at the north end of the lake. 175 (234). Tringa canutus Linnzus. Knot. Two specimens were shot at Cayuga by Foster Porker, August 30, 1908. Mr. E. H. Eaton and Mr. L. A. Fuertes report them as frequently seen at Cayuga in the fall. It is altogether probable that this species is not an uncommon transient. 176 (239). Pisobia maculata (Vieillot). Pectoral sandpiper. Common transient at the north end of the lake but rare at the south end. L.A. Fuertes has taken one specimen at Ithaca on each 422 REED-WRIGHT—THE VERTEBRATES OF [October 1, of the following dates: During the fall of 1892, August 13, 1899, and October 12, 1890. 177 (240). Pisobia fuscicollis ( Vieillot). _White-rumped sandpiper. One specimen taken at Montezuma October 12, 1906, by L. A. Fuertes. 178 (242). Pisobia minutilla (Vieillot). Least sandpiper. Common transient. Most common in spring from May 7 to 27. The latest fall record is October 12, 1906. Regarding the time of first appearance in the fall we have no data. 179 (243a). Pelidna alpina sakhalina (Vieillot). Red-backed sand- piper. Common transient being most abundant in the fall during October. 180 (246). Ereunetes pusillus (Linnzus). Semipalmated sand- piper Common transient. In the spring they are found all through May. In the fall they appear August 20 and leave November 1. They are most common during the first half of October. 181 (248). Calidris leucophea (Pallas). Sanderling. Specimens are frequently taken at both ends of the lake. It appears to be a fairly common transient in both spring and fall. 182 (251). Limosa hemastica (Linneus). Hudsonian godwit. “ A rare spring and autumn migrant” (Auburn List). A speci- men was taken at Ithaca about November 5, 1878, by C. J. Pennock and mounted by R. B. Hough. 183 (254). Totanus melanoleucus (Gmelin). Greater yellow-legs. Transient. Fairly common from April 30 to May 20. It is com- mon in the fall during October. 184 (255). Totanus flavipes (Gmelin). Yellow-legs. Common transient from May Io to June 1, the earliest spring date being April 28, 1908. It is common in the fall during October. The latest fall date is November 10, 1900. 185 (256). Helodromas solitarius (Wilson). Solitary sandpiper. Common transient from April 28 to May 20 and July 14 to Sep- 1909.] THE, GAYUGA (LAKE -BASIN, Ny: 423 tember 20. The average date of spring arrival is May 1, the earliest date being April 28, 1905. 186 (258). Catoptrophorus semipalmatus (Gmelin). Willet. “A regular migrant. Three secured in the fall of 1876” (Au- burn List, p. 33). This species has not been recorded in recent years. 187 (261). Bartramia longicauda (Bechstein). Upland plover. The only record of this species which we have is a pair found breeding by Foster Parker during the summer of 1907. In the Auburn List (p. 33) it is spoken of as not an uncommon summer resident. 188 (263). Actitis macularia (Linnzus). Spotted sandpiper. Common summer resident. The average date of spring arrival is April 24, the earliest, April 20, 1906. The active nesting period is from May 20to June 15. L.A. Fuertes reports that he has found nests with eggs as late as July 26 (1900). 189 (264). Numenius americanus Bechstein. Long-billed curlew. “A regular but somewhat rare migrant ” (‘‘ Auburn List,” p. 23). Not recorded in recent years. 190 (265). Numenius hudsonicus Latham. MHudsonian curlew. “Occurs irregularly during the migration. One specimen pre- served in the collection of the Phoenix Sportsman’s Club at Seneca BallsNe Yer(s Auburn Mist,-p.24). ‘cherens.a specimen (C. U; 1158), in the collection of Cornell University taken at Union Springs in 1882. 51. Family CuHarapriup#®. The Plovers. 191 (270). Squatarola squatarola (Linnzus). Black-bellied plover. Regular transient in the fall and occasionally in spring. On October 14, 1899, L. A. Fuertes shot a specimen at Ithaca which constitutes the only record for the south end of the basin. Mr. A. A. Allen and Mr. J. T. Lloyd reported it common at the north end of the lake on September 26, 1908. Our fall records all occur between September 20 and October 30. 192 (272). Charadrius dominicus Muller. Golden plover. The only record of this species is a specimen taken by E. H. Eaton and L. A. Fuertes at Cayuga, October 29, 1907. 424 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 193 (273). Oxyechus vociferus (Linnzus). Killdeer. Common transient and not uncommon summer resident from March 12 to November 15. It is most abundant in the fall. 194 (274). Agialitis semipalmata Bonaparte. Semipalmated plover. Transient. Uncommon in the spring, fairly common in the fall from August 15 to September 30. 52. Family Apurizip#. The Turnstones. 195 (283a). Arenaria interpres morinella (Linneus). Turnstone. Mr. L. A. Fuertes took a specimen at Ithaca June 3, 1906 and Foster Parker reports several taken at Cayuga. XXXI. Order GALLINA. The Gallinaceous Birds. 52a. Family OpontopHorip&. The Quail. 196 (289). Colinus virginianus (Linnzus). Bob-white. Common permanent resident. It is very scarce all along the eastern part of the basin. 53. Family Terraonip#. The Grouse. 197 (300). Bonasa umbellus (Linneus). Ruffed grouse. Common permanent resident. All of our nesting records fall between April 20 and May 15. XXXII. Order COLUMB2. The Doves. 54. Family Cotumpipa. The Pigeons. 198 (315). Ectopistes migratorius (Linnzus). Wild pigeon. Formerly abundant. None have been recorded here since 1892 when “A few were seen in Ithaca—L. A. F.” (Eaton, p. 32). 199 (316). Zenaidura macroura carolinensis (Linneus). Mourn- ing dove. Common summer resident. The average date of spring arrival is April 1, the earliest, March 8, 1890. Nest building has been found to begin as early as April 15 and eggs have been found until June 1909.] THE CAYUGA LAKE BASIN, N.Y. 425, 18. In the Renwick marshes they nest in colonies varying from three or four to a dozen pairs. The nests are frequently only a few feet apart, built upon stumps, brush piles, logs and heaps of debris. XXXII. Order RAPTORES. The Birds of Prey: 55. Family CatuHartip#. The American vultures. 200 (325). Cathartes aura septentrionalis (Wied). Turkey vulture. Mr. C. J. Hampton saw eight individuals hovering above a rank woodchuck on July 1, 1900, at Cosad, N. Y. One specimen was shot. On June 20, 1908, Mr. J. T. Lloyd reported one from the Renwick flats at Ithaca. 56. Family Buteonip2. The Hawks and Eagles. 201 (331). Circus hudsonius (Linneus). Marsh hawk. Common summer resident. The average date of spring arrival is March 27, the earliest being March 25, 1906. They remain in Autumn until the last of October, the latest fall record being Octo- ber 28, 1908. The only nesting records of this species which we have are: a nest and eggs found May 27, 1904, and a nest with five young found June 29, 1906. 202 (332). Accipiter velox (Wilson). Sharp-shinned hawk. Common summer resident and occasionally taken in winter. It is common from the last of March until the first of November. The only breeding record is a nest of young which took wing on July 16, 1906. 203 (333). Accipiter cooperi (Bonaparte). Cooper’s hawk. Common summer resident, more abundant in the fall. The aver- age date of spring arrival is March 25, the earliest, March 17, 1907. They remain in the fall until November 1. 204 (334). Astur atricapillus (Wilson). Goshawk. Uncommon winter visitant. A specimen was taken near West Candor, November 26, 1907, by C. S. Gridley. Mr. Fuertes reports that he sees one or more every winter. It is recorded in the Auburn List as an “uncommon winter visitor.” PROC. AMER. PHIL. SOC., XLVIII. 193 CC, PRINTED JANUARY 7, IQIoO. 426 REED-WRIGHT—THE VERTEBRATES OF [October 1, 205 (337). Buteo borealis (Gmelin). Red-tailed hawk. Common resident species. 206 (339). Buteo lineatus (Gmelin). Red-shouldered hawk. Common resident species and more common in winter than the preceding species. The earliest nesting date recorded is April 26, 1905. 207 (343). Buteo platypterus (Vieillot). Broad-winged hawk. Uncommon summer resident. The earliest spring record, March 16, 1906. 208 (347a). Archibuteo lagopus sancti-johannis (Gmelin). Rough- legged hawk. Regular but not common winter visitant from Jan. I to April 1. 209 (352). Haliaetus leucocephalus (Linnzus). Bald eagle. Not common permanent resident. It is more frequently seen in the spring and fall. It bred formerly near Crowbar point and still breeds in the vicinity of Union Springs. 56a. Family Fatconipa. The Falcons. 210 (350). Falco peregrinus anatum (Bonaparte). Duck hawk. Rare transient during spring and fall. 211 (357). Falco columbarius Linneus. Pigeon hawk. Uncommon transient. 212 (360). Falco sparverius Linneus. Sparrow hawk. Common summer resident from March 15 to November 15 and occasionally taken in winter. 56b. Family PANDIonip#. The Fish Hawks. 213 (364). Pandion haliaétus carolinensis (Gmelin). Osprey. Common transient during May and October. Several are seen every year during the summer months but we have no evidence that they nest within the basin. The average date of spring arrival is April 12, the earliest, April 5, 1901, 1902 and 1906. Migrants begin to arrive in the fall about September 20. They are common from the last of September to the middle of October. The latest fall record is a female killed October 25, 1899. 1909.] GEE, CAYUGA) TAKE” BASIN; ING Y. 427 57. Family ALuconip#. The Barn Owls. 214 (365). Aluco pratincola (Bonaparte). Barn owl. The barn owl has been recorded within the basin at various intervals since 1880 at which time Foster Parker reports one taken at Cayuga. On December 13, 1885, one was taken at Auburn by F. J. Stupp. Another was taken by L. O. Asbury September 23, 1900, at Sennett and on December 1, 1904, a specimen was shot near South Danby. Mr. Samuel Tisdel, of Ithaca, has in his possession a mounted specimen taken near Ithaca in the fall of 1907. He states that during the fall of that year three others taken near Ithaca were brought to his shop to be mounted. On June 6, 1908, A. A. Allen and J. T. Lloyd saw one in the Renwick Marshes. November 27, 1908, one was killed in Michigan Hollow in the extreme southern portion of the basin. There is little doubt that this species is in- creasing in the lake basin. 58. Family Stricipz. The Owls. 215 (366). Asio wilsonianus (Lesson). Long-eared owl. Common permanent resident. The only breeding record which we have is a nest containing eggs found April 9, 1905. 216 (367). Asio flammeus (Pontoppidan). Short-eared owl. A resident species. Common in summer at the north end of the basin, uncommon in the southern portion. 217 (368). Stryx varia Barton. Barred owl. Uncommon resident. 218 (372). Cryptoglaux acadicus (Gmelin). Saw-whet owl. Rare. ‘“ Adult male taken July 18, 1878. Two specimens re- ceived, taken in Cayuga Co., April 14, 1877, and November, 1878” (“ Auburn List,” p. 27). A female was taken at Sennett January 25, 1904, by Charles Lyon and one was taken at Ithaca January 16, 1905, by aes Allent.and \J. i. Lloyd: 219 (373). Otus asio (Linnzus). Screech owl. Abundant permanent resident. 220 (375). Bubo virginianus (Gmelin). Great horned owl. Uncommon permanent resident. 428 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 221 (376). Nyctea nyctea (Linnzus). Snowy owl. Irregular winter visitant. In the collection of Cornell University are three specimens from this basin taken as follows: winter of 1878 at Aurora, December 12, 1890, at Covert, February 22, 1902 at Newfield. 222 (377a). Surnia ulula caparoch (Miller). Hawk owl. The only record of this species is a male taken by L. O. Ash- bury at Conquest, November 23, 1902. Two birds were seen and one captured. XXXIV. Order COCCYGES. The Cuckoo-like Birds. 59. Family Cucutip®. The Cuckoos. 223 (387). Coccyzus americanus (Linnzus). Yellow-billed cuckoo. Common summer resident. The average date of spring arrival is May 10, the earliest, May 6, 1905. 224 (388). Coccyzus erythrophthalmus (Wilson). Black-billed -Cuckoo. Common summer resident. The average date of spring arrival is May 9, the earliest, April 24, 1904. 60. Family ALcepInip&. The Kingfishers. 225 (390). Ceryle alcyon (Linnzus). ~ Belted kingfisher. Common summer resident. On December 23, 1874, a female was taken at Ithaca and on January 15, 1905, one individual was seen near an open stream in the Renwick wood at Ithaca. The average date of spring arrival is April 4, the earliest, March 17, 1907. It is common in the fall until the middle of October. By the 25th of this month all have usually disappeared. XXXV. wOrder PICI. The W eodpeckers: 61. Family Picipa. The Woodpeckers. 226 (393). Dryobates villosus (Linnzus). Hairy woodpecker. Common resident species. 4 1909.] THEY CAYUGA LAKE BASIN, N:. Y¥- 429 227 (394c). Dryobates pubescens medianus (Swainson). Downy woodpecker. Common permanent resident. The active season of nesting is from May 10 to June 15. The earliest record of nesting is May 6, 1904. Our earliest record of young on the wing is June 9, 1904. 228 (400). Picoides articus (Swainson). Arctic three-toed wood- pecker. An occasional winter visitant. Specimens were taken at Ithaca during the winter of 1895-6 and on November 1, 1901, by L. A. Fuertes. A female was taken October 19, 1901, at Sennett by L. O. Ashbury. 229 (402). Sphyrapicus varius (Linneus). Yellow-bellied sap- sucker. Common transient and “reported as breeding in Cayuga, Yates and Oneida Counties” (Eaton). The average date of spring ar- rival is April 10, the earliest, March 30, 1908. They become com- mon the last of April and the first of May. The latest date upon which individuals have been seen at Ithaca is May 26, 1900. Usu- ally all have left by May 15. They appear in the fall from Sep- tember 20 to November 1. The latest fall record is one seen Nov- ember 27, 1908. 230 (406). Melanerpes erythrocephalus (Linnzus). Red-headed woodpecker. Rare in winter but becomes common about May 5. The only nesting records which we have are eggs found June 13, 1903, and May 16, 1907. 231 (409). Centurus carolinus (Linnzus). Red-bellied wood- pecker. Rare. There are in the collection of Cornell University three specimens taken near Ithaca. One in 1850, another in 1858 and a third taken by L. A. Fuertes in November, 1894. Mr. G. C. Em- body took a female in a small swamp just north of Auburn, March 4, 1808. 232 (412a). Colaptes auratus luteus Bangs. Northern flicker. Common summer resident and occasionally present in winter. 430 REED-WRIGHT—THE VERTEBRATES OF [October 1, Migrants begin to arrive the last of March from which time it is common until October 20. Frequently many are seen as late as the first of December. XXXVI. Order MACROCHIRES. The Goatsuckers, Swifts and Hummingbirds. 62. Family CaprRiMuLGIDA. The Goatsuckers. 233 (417). Antrostomus vociferus (Wilson). Whip-poor-will. Common summer resident in the basin from May 1 to September 1. In the region about Ithaca it is very uncommon. The latest that it has been observed in the fall is October 7, 1907. The earliest spring record is April 29, 1906. 234 (420). Chordeiles virginianus (Gmelin). Nighthawk. Common summer resident. The average date of spring arrival is May 109, the earliest, May 15, 1900. 63. Family Micropopip%. The Swifts. 235 (423). Chaetura pelagica (Linneus). Chimney swift. Abundant summer resident. The average date of spring arrival is April 23, the earliest, April 19, 1889. Nests with eggs are found from May 20 to July 5. Usually all have departed in the fall by October I. 64. Family Trocuinip®. The Hummingbirds. 236 (428). Archilochus colubris (Linnzus). Ruby-throated hum- mingbird. Common summer resident from May 10, the average date of spring arrival, to September 10. Nesting dates all fall between May 23 and July 21. The crest of the nesting season is between June 15 and 30. XXXVII. Order PASSERES. The Perching Birds. 65. Family Tyrannipz. The Flycatchers. 237 (444). Tyrannus tyrannus (Linneus). Kingbird. Common summer resident. The average date of spring arrival is May 6, the earliest, May 3, 1902. They nest the very last of May and during June. 1909.] TEE sCAVUGA (LAKE? BASIN, \Ne Y: 431 238 (452). Myiarchus crinitus (Linnzus). Crested flycatcher. Common summer resident. The average date of spring arrival is May 4, the earliest, May 1, 1900. Nesting begins the last of May and lasts through June. 239 (456). Sayornis phoebe (Latham). Phceebe. Abundant summer resident along the streams and lake shores. The average date of spring arrival is March 20, the earliest, March g, 1899. During the first half of October they depart for the south, latest record being October 19, 1902. Nesting begins April 20 and continues through May and June. The earliest nesting record is April 13, 1901. The latest date for eggs is a nest found June 21, 1gOO. 240 (459). Nuttallornis borealis (Swainson). Olive-sided fly- catcher. Rare. A specimen was taken in Fall creek gorge by L. A. Fuertes May 11, 1905. G. C. Embody took a male at the north end of the lake May 30, 1808. 241 (461). Myiochanes virens (Linnzus). Wood pewee. Abundant summer resident. The average date of spring arrival is May 13, the earliest, May 1, 1900. They nest throughout the month of June. 242 (463). Empidonax flaviventris Baird. Yellow-bellied fly- catcher. The definite records are three specimens, two males and one female taken at Ithaca by R. B. Hough on May 20, 1882, and several taken in the vicinity of Waterloo and reported by E. H. Eaton. A few are reported seen each year between May 15 and June Io. 243 (4662). Empidonax traillii alnorum Brewster. Alder fly- catcher. Uncommon transient and rare summer resident. The average date of spring arrival is May 14, the earliest, May 4, 1905. The yellow-bellied and the alder are the last flycatchers to arrive in the spring, the latter loitering along into June. In 1906 it was found until June 9 in the willow and alder thickets along the west side of the Renwick marshes. L. A. Fuertes reports it as breeding at Cay- 432 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, uta, N. Y., just outside the Cayuga basin on the southwest. A. A. Allen and J. T. Lloyd found a nest containing two eggs on June 16, 1908, at Ithaca. 244 (467). Empidonax minimus Baird. Least flycatcher. Abundant summer resident. The average date of spring ar- rival is May 4, the earliest, May 1, 1906. Abundant everywhere ex- cept the denser wooded areas. 66. Family ALAupIp&. The Larks. 245 (474). Otocoris alpestris (Linnzus). Shore lark. It is reported by Mr. Fuertes that the shore lark was formerly common in this basin. It is now replaced by the prairie horned lark. A few are, however, still found in winter. Mr. G. C. Embody took two specimens at Auburn. 246 (474b): Otocoris alpestris praticola Henshaw. Prairie horned lark. Permanent resident although not common during December and January. They become common about the first of February. This species is the first of our Passerine birds to nest. On April 7, 1904, a nest was found at Trumansburg which contained one egg and two young. Dating back fourteen days, which, according to Bendire is the period of incubation, the eggs must have been laid not far from March 20 to 23. On April 20, 1902, there was taken at Ithaca a young individual which had just left the nest. On April 6, 1906, young just beginning to fly were seen. In 1907 Mr. A. A. Allen found on April 3 a nest containing eggs and on April 4 another nest in which the eggs hatched April 10. The young of this nest were killed by a very heavy snow storm a few days later. 67. Family Corvip#. The Crows and Jays. 247 (477). Cyanocitta cristata (Linneus). Blue jay. Common permanent resident. It is now rarely seen in the vicin- ity of Ithaca except for a short period during the spring and fall. It has not been known to nest in this immediate vicinity since 1889 when a pair built in a small grove of oaks on the Cornell Campus. 1909.] THE CAYUGA LAKE BASIN, N. Y. 433 In all other portions of the basin they are fairly common. At En- field on May 5, 1907, A. A. Allen found a nest containing five eggs. 248 (486a). Corvus corax principalis Ridgway. Northern raven. “Formerly not uncommon at the north end of the basin. The last reported was one, seen by Foster Parker in 1880, pursued by a number of crows.” (Eaton). 249 (488). Corvus brachyrhynchos C. L. Brehm. Crow. Common permanent resident. Nests containing eggs are most commonly found from April 10 to 20. In 1903 a nest containing eggs was found on April 3. The latest record of nest and eggs is May 16, 1900. 68. Family Icrerip. The Blackbirds and Orioles. 250 (494). Dolichonyx oryzivorus (Linnzus). Bobolink. Common summer resident. The average date of spring arrival is May 4, the earliest, April 30, 1900. By July 10 they are gathered in large flocks in the marshes where they remain through August and the first of September, at about the middle of which they depart for the south. 251 (495). Molothrus ater (Boddaert). Cowbird. Abundant summer resident. The average date of spring arrival is March 28, the earliest, March 14, 1899. Eggs are found from May 5 to June 15. The maximum period of egg-laying is the last half of May. The pheebe, the vireos, redstart and yellow warbler are the most common victims of the cowbird’s parasitic habits. 252 (498). Agelaius pheniceus (Linnzus). Red-winged blackbird. Common summer resident and found regularly in small numbers in the marshes during winter. Migration begins about March Io. The earliest record is a large flock of males in full song, seen Feb- ruary 22, 1902. The earliest record of nesting is May 12, 1906. The most active breeding period is from the middle of May to the first of June. Young are on the wing by June 5. During the first two weeks of July this species collects in large flocks in the marshes where they remain until the last of November. Flocks containing hundreds are seen migrating all through November. So far as they have been observed at Ithaca they follow the inlet valley towards the south. 434 REED-WRIGHT—THE VERTEBRATES OF _ [October 1, 253 (501). Sturnella magna (Linnzus). Meadow lark. Common summer resident and found regularly in small num- bers in winter. The average date of the spring arrivals is March 17, the earliest, March 4, 1906. They remain common until the last of October. 254 (500). Icterus spurius (Linnzus). Orchard oriole. Rare. On May 30, 1898, G. C. Embody took a male at Cayuga. On May 27, 1899, Burdett Wright found a pair nesting at Monte- zuma. A male was taken at Ithaca, May 3, 1890, by L. A. Fuertes. who saw a pair at Ithaca, June 7, 1902. A male in song was found May 18, 1908, in the Inlet valley just south of Ithaca and in the same locality A. A. Allen and J. T. Lloyd found a nest which contained four eggs and one young. 255 (507). Icterus galbula (Linnzus). Baltimore oriole. Common summer resident. The average date of spring arrival is May 3, the earliest, April 30, I900 and 1905. They nest from May 10 to June 1. 256 (509). Euphagus carolinus (Muller). Rusty blackbird. Common transient. It arrives usually the last days of March. The earliest date is March 18, 1901. It is common from April 15 to 30 but small flocks are seen until May 15. 257 (5110). Quiscalus quiscula aeneus (Ridgway). Bronzed grackle. Common summer resident and occasionally found in winter. The average date of spring arrival is March 14, the earliest, March 4, 1906. Nesting begins the last half of April and continues through- out May. By May 25 large numbers of young are on the wing; dur- ing the first week in June this species begins to collect in flocks and resort to common roosts. 69. Family Frrincitt1p#. The Sparrows. 258 (514). Hesperiphona vespertina (W. Cooper). Evening gros- beak. Accidental visitant. During the winter of 1890 when it was so common in New England it appeared here in fairly large numbers 1909.] PE CAYUGA (LAKE BASING NEY. 435 from January 22, when first seen, to March 28. They were not seen again until April 11, 1904, when L. A. Fuertes shot a pair on the Cornell Campus. On December 8, 1906, Mrs. A. T. Kerr reported one which she saw on Cornell Heights. j 259 (515). Pinicola enucleator leucura (Miiller). Pine grosbeak. An irregular winter and spring visitant but never common. In 1890 it was reported by L. A. Fuertes on January 23. Since that date it has been recorded as follows: 1904 on January 7, April 26 and 29 and May 5. In 1905, April 20. In 1906, March 5. 2600 (517). Carpodacus purpureus (Gmelin). Purple finch. Common summer resident from March 22 to November 10. It is occasionally seen in winter. It nests during May and June. The latest date of nest and eggs is June 21, 1905. 261. Passer domesticus (Linneus). English sparrow. Abundant. 262 (521). Loxia curvirostra minor (Brehm). Red crossbill. An irregular visitant. Although commonly seen during March and April they are frequently present during late spring and sum- mer. In 1889 L. A. Fuertes reported them on June 16. In 1900 T. L. Hankinson saw a flock of 30 individuals on May 30 and again on July 15. On August 7 of this year another flock was seen. In 1906 a flock of ten were seen on the Cornell Campus from June 21 to 24. In 1907 they were first seen on May 27 and continued com- mon until June 24. In 1908 they were seen daily from June 10 to 16. 263 (522). Loxia leucoptera Gmelin. White-winged crossbill. Rare winter visitant. During the winter of 1907 this species was more common in the basin than in any year since records have been kept.) Specimens were frequently taken and seen from January 5 to the first of March. ‘The last specimen recorded that year was one killed at Taughannock Falls, March 4. November 15, 1882, a fe- male was taken at Ithaca. L.A. Fuertes took a specimen at Ithaca, February 8, 1906. 264 (528). Acanthis linaria (Linnzus). Redpoll. An irregular winter visitant but usually common when present. There are no records of their occurrence before January in any year. 436 REED-WRIGHT—THE VERTEBRATES OF [October 1, There is a specimen of a female in the collection of Cornell Univer- sity taken at Ithaca in January, 1876, showing that they were present that winter but no notes to indicate whether or not they were com- mon. On January 10, 1879, a male was killed by R. B. Hough. They were reported by E. H. Eaton as common that winter in Cay- uga Co. In 1904 they were common all through January, February and March on the twenty-ninth of which L. A. Fuertes shot a speci- men from a large flock. In 1907 they were common from January 13 to March 24. In 1909 the first individuals appeared January 5 and were common everywhere in the southern portion of the basin until February 1. 205 (529). Astragalinus tristis (Linnzus). Goldfinch. Permanent resident although more or less irregular in winter. They become common in the spring from the tenth to the fifteenth of April. The breeding plumage begins to show about April 20 and is complete about the middle of May at which time the males are in full song. Nests and eggs are commonly found during July. 206 (533). Spinus pinus (Wilson). Pine siskin. An uncommon winter and a common spring visitant from the last of April to the middle of May. The latest spring record is May 30, 1907. ‘The earliest winter record is a specimen taken January 20, 1890. 207 (534). Plectrophenax nivalis (Linnzus). Snow bunting. Common winter resident being most common from January to March. In the fall they arrive the last week in October and remain until the middle of March. The latest date is March 26, 1890. 268 (536). Calcarius lapponicus (Linneus). Lapland longspur. Rare. Mr. Fred Allen took a specimen near Auburn during the winter of 1876 and Mr. Charles Lyon took a male near Auburn, March 3, 1899. 269 (540). Pocecetes gramineus (Gmelin). Vesper sparrow. Common summer resident. The average date of spring arrival is March 28, the earliest, March 23, 1903. The active breeding period is May and June. The earliest record of nest and eggs is April 25, 1900, the latest, July 23, 1900. This species remains in the fall until the last of October. The latest fall record is November 27, 1908. 1909.] (/0THE. CAYUGA LAKE BASIN: Ni ¥. 437 270 (542a). Passerculus sandwichensis savanna (Wilson:). Sav- annah sparrow. Common summer resident. The average date of spring arrival is April 6, the earliest, March 23, 1905. About July 25 this species begins to collect in flocks which become numerous the first of Octo- ber. All have left usually by the middle of the month. 271 (540). Ammodramus savannarum australis Maynard. Grass- hopper sparrow. Common summer resident. The average date of spring arrival is May 2, the earliest, April 26, 1905. 272 (548). Passerherbulus lecontei (Audubon). Leconte’s sparrow. One specimen was shot in the Renwick marshes by L. A. Fuertes, October 11, 1897. 273, (549.1). Passerherbulus nelsoni (Allen). Nelson’s sparrow. The numerous specimens taken since 1900 justify the conclu- sion that this species is a common visitant during the fall migration from the middle of September to the first of October. They have always been found in the rushes close to the water where they skulk and run in a fashion very suggestive of a mouse. When flushed they rise for a moment and disappear again much as a wren. 274 (549.1a). Passerherbulus nelsoni subvirgatus (Dwight). Aca- dian sharp-tailed sparrow. Uncommon but regular fall visitant. It arrives the very last of September or first of October, about a week later than the Nelson’s sparrow and remains for a period of from 12 to 15 days. Neither this nor the preceding species has ever been taken in the spring. The definite records are skins, which are now in the collection of L. A. Fuertes and that of Corne]l University, taken between September 26 and October 12. 275 (554). Zonotrichia leucophrys (Forster). White-crowned sparrow. Common transient. The average date of spring arrival is May 4, the earliest, May 2, 1907. It remains until May 20 becoming com- mon from the tenth to the fifteenth of the month. It is common in the fall during the very last of September and the first half of Octo- 438 REED-WRIGHT—THE VERTEBRATES OF [October 1, ber. The latest record is October 28, 1908. A single individual was seen in the marshes at Ithaca, February 24, 1906. 276 (558). Zonotrichia albicollis (Gmelin). White-throated spar- row. Common transient. The average date of spring arrival is April 17, the earliest, April 13, 1903. They become common the last week of April and remain until May 20. The latest record is May 23, 1908. In the fall they appear about September 20 and are common throughout October. The latest record for the fall is November 4, 1908. 277 (559). Spizella monticola (Gmelin). Tree sparrow. Common winter resident. They arrive October 1 and remain common until April 25. Wilder, of Ithaca; N: ¥... Discussed by Dr: E. A. Spitzka. “Some Conditions Modifying the Interpretation of Human Brain Weight Records,” by Dr. H. H. Donaldson, of Philadelphia. “Some Notes on the Modification of Color in Plants,” by Prof. Henry Kraemer, of Philadelphia. Discussed by Prof. Harshberger, Prof. Hobbs, Prof. W. T. Hewett and Prof. Kraemer. “Comparative Leaf Structure of the New Jersey Strand Plants,” by Prof. John W. Harshberger, of Philadelphia. Discussed by Prof. Wilder and Mr. Harrison S. Morris. “The Composition of Chrysocolla,’ by Prof. Harry F. Keller, of Philadelphia. Vili MINUTES. [April 24, “The Chemical Work of the U.S. Geological Survey,” by Frank Wigglesworth Clarke, of Washington. “Recent Work on the Physics of the Ether,” by Paul R. Heyl, of Philadelphia. (Introduced by Prof. Harry F. Keller.) “Effect of Bleaching Powder Upon Bacterial Life in Water,” by Prof. William Pitt Mason, M.D., of Troy, N. Y. Discussed by Prof. Kraemer and Dr. W. J. Holland. “The Detonation of Gun Cotton,” by Prof. Charles E. Munroe, of Washington. On motion it was ordered that a telegram conveying the Society’s good wishes and great regret at his absence from the meeting be sent to Prof. Simon Newcomb. To this telegram a reply was re- ceived from Prof. Newcomb thanking the Society for its kind greet- ings which he highly appreciated. Afternoon Session—2.30 o’clock. Wi.iiAM B. Scott, LL.D., Vice-President, in the Chair. “South American Fossil Cetacea,” by Dr. Frederick W. True, of Washington. Discussed by Prof. W. B. Scott. “The Destruction of the Fresh Water Fauna of Western Penn- sylvania,” by Dr. Arnold E. Ortman, of Pittsburgh. “The Stratigraphic Position of the Oolitic Iron-Ore at Blooms- burg, Pa.,” by Gilbert van Ingen, of Princeton. (Introduced by Prof. W. Bs Scott) ALBERT A. MICHELSON, LL.D., Vice-President, in the Chair. “Machines and Engineering in the Renaissance and in Classical Antiquity,” by Prof. Christian Htlsen, of Rome Italy. (Intro- duced by Dr. W. W. Keen.) “On the Extent and Number of the Indo-European Peoples,” by Prof. Maurice Bloomfield, of Baltimore. ““A Mechanical Device for the Tabulation of the Sums of Numerous Variable Functions,’ by Prof. Ernest W. Brown, of New Haven. “The Burning Bush and the Origin of Judaism,” by Prof. Paul Haupt, of Baltimore. 1909. ] MINUTES. ix “On Certain Generalizations of the Problem of Three Bodies,” by President Edgar Odell Lovett, of Houston, Texas. “ Penrose’s Graphical Method for Orbit Determination,” by Prof. Eric Doolittle, of Flower Observatory, Philadelphia. Evening Session. WittiaM W. KEEN, LL.D., President, in the Chair. Commemoration of the Centenary of Charles Darwin's Birth (February 12, 1809) and the Fiftieth Anniversary of the Publica- tion of the “Origin of Species” (November 24, 1859). The following addresses were delivered: “Personal Reminiscences of Charles Darwin and of the Recep- tion of the ‘ Origin of Species.” by His Excellency, the Right Hon- orable James Bryce, British Ambassador at Washington. “The Influence of Darwin on Natural Science,” by Prof. George Lincoln Goodale, of Cambridge. “The Influence of Darwin on the Mental and Moral Sciences,” by Prof. George Stuart Fullerton, of New: York. Attention was called to the fact that there were two members of the Society still living who were friends and colaborers of Charles Darwin—Sir Joseph Dalton Hooker and Dr. Alfred Russell Wal- lace, and it was ordered that on the occasion of this Commemoration the Society transmit by cable to them its greetings and congratula- tions on the general acceptance of the views in the elaboration and promulgation of which they took an active and effective part. Saturday, April 24. Executive Session—10 o’clock. Atsert A. Micuetson, LL.D., Vice-President, in the Chair. Candidates for membership were balloted for, and the tellers reported the election of the following: Residents of the United States. Louis A. Bauer, Ph.D. (Berlin), Washington, D. C. Marston Taylor Bogert, New York City. Hermon Carey Bumpus, Ph.D., New York City. Alexis Carrel, M.D., New York City. x MINUTES. [April 24, Edwin Brant Frost, Williams Bay, Wis. Robert Almer Harper, Ph.D., Madison, Wis. William Herbert Hobbs, Ph.D., Ann Arbor, Mich. A. V. Williams Jackson, Ph.D., LL.D., Yonkers, N. Y. John Frederick Lewis, Philadelphia. Abbott Lawrence Lowell, Boston, Mass. William Romaine Newbold, Ph.D., Philadelphia. Charles Bingham Penrose, M.D., Ph.D., Philadelphia. William Howard Taft, Washington. Charles Richard Van Hise, M.S., LL.D., Madison, Wis. Victor Clarence Vaughan, M.D., Sc.D., LL.D., Ann Arbor, Mich. Foreign Residents. Francis Darwin, M.A., F.R.S., Cambridge, Eng. Hermann Diels, Ph.D., Berlin. Emil Fischer, Ph.D., M.D., Berlin. Friedrich Kohlrausch, Ph.D., Marburg. Wilhelm Pfeffer, Ph.D., Leipzig. Morning Session. AuBert A. Micuetson, LL.D., Vice-President, in the Chair. Prof. Robert William Wood (elected 1908) and Dr. Louis A. Bauer, a newly elected member, were admitted into the Society. The following papers were read: “On the Remarkable Changes in the Tail of Comet C. 1908 (Morehouse), and On a Theory to Account for these Changes,” by Prof. E. E. Barnard, of Yerkes Observatory, Williams Bay, Wis. Discussed by Prof. M. B. Snyder, Prof. Michelson, Dr. George F. Becker and Prof. Ernest W. Brown. “The Past History of the Earth as Inferred from the Mode of Formation of the Solar System,” by Dr. T. J. J. See, of U. S. Naval Observatory, Mare Island, Cal. “ The Linear Resistance between Parallel Conducting Cylinders,” by Prof. A. E. Kennelly, of Cambridge. “Vacuum Effects in Electrical Discharge around a Right Angle in a Wire,” by Prof. Francis E. Nipher, of St. Louis. “ The Ruling of Diffraction Gratings,” by Prof. Albert A. Mich- 1909.4 MINUTES. xi elson, of Chicago. Discussed by Prof. Robert W. Wood, Prof. M. B. Snyder and Prof. Doolittle. “On an Adjustment for a Plane Grating similar to Rowland’s for the Concave Grating,” by Prof. Carl Barus, assisted by M. Barus, of Providence. “The Electron Method of Standardizing the Coronas of Cloudy Condensation,” by Prof. Carl Barus, of Providence. “The Electrometric Measurements of the Potential Difference between two Conductors of a Condenser containing a highly Ionized Medium,” by Prof. Carl Barus, of Providence. “Solar Activity and Terrestrial Magnetic Disturbances,” by Dr. L. A. Bauer, of Washington. Discussed by Prof. Kennelly and Dr. Bauer. “The Effect of Temperature on the Absorption Spectra of Cer- tain Solutions,’ by Prof. Harry C. Jones, of Baltimore. (Intro- duced by President Ira Remsen.) “The Specific Chemo-Therapy of the Protozoal Diseases,” by Dr. Simon Flexner, of the Rockefeller Institute for Medical Re- search, New York. “The Unsuspected Presence of Habit-Forming Agents in Bever- ages and Medicines,’ by Dr. Lyman F. Kebler, of Washington. (Introduced by Dr. Harvey W. Wiley.) Discussed by Dr. E. A. Spitzka and Dr. Kebler. Afternoon Session—2.30 o’clock. Witu1aM B. Scott, LL.D., Vice-President, in the Chair. Prof. William Herbert Hobbs and Mr. Abbott Lawrence Lowell, newly elected members, were admitted into the Society. The following papers were read: Symposium on Earthquakes. “ Tntroduction—Classification—Discussion of Volcanic Earth- quakes—Description, with illustrations, of the Charleston, S. C., and Kingston, Jamaica, Disasters,” by Prof. Edmund O. Hovey, of New York. (Introduced by Prof. W. B. Scott.) “The Present Status and the Outlook of Seismic Geology,” by Prof. William H. Hobbs, of Ann Arbor, Mich. Xil MINUTES. [May 21, “Conditions Leading to Tectonic Earthquakes—Instruments used in the Study of Earthquakes—Suggestions for a National Seis- mological Bureau,” by Prof. Harry F. Reid, of Baltimore. (Intro- duced by Prof. W. B. Scott.) These three papers were discussed by Profs. Michelson, William Morris Davis, W. H. Hobbs, H. F. Reid and W. B. Scott. The following preamble and resolutions were presented and unanimously adopted: Whereas, Earthquakes have been the cause of great loss of life and property within the territory of the United States and its posses- sions, as well as in other countries, and Whereas, It is only through the scientific investigation of the phenomena that there is hope of discovering the laws which govern them, so as to predict their occurrence and to reduce the danger to life and property, and Whereas, Such investigations can be successfully conducted only with the support of the general government, be it, therefore, Resolved, That this Society urge upon Congress the establish- ment of a National Bureau of Seismology, and suggest that this bureau be organized under the Smithsonian Institution with the active cooperation of the other scientific departments of the govern- ment and that this bureau be charged with the following duties: (a) The collection of seismological data. (b) The establishment of observing stations. (c) The organization of an expeditionary corps for the investi- gation of special earthquakes and volcanic eruptions in any part of the world. (d) The study and investigation of special earthquake regions within the National domain. And Resolved, That copies of these resolutions be transmitted to the President, to the President of the Senate, to the Speaker of the House of Representatives, and to the Secretary of the Smithsonian Institution. 1909.] MINUTES. Xili Stated Meeting May 7, 19009. Witt1am W. KEEN, LL.D., President, in the Chair. Dr. Charles B. Penrose, Mr. John Frederick Lewis and Prof. William Romaine Newbold, newly elected members, were admitted into the Society. Letters accepting membership were read from: Louis A. Bauer, Ph.D. (Berlin), Washington, D.C. Marston Taylor Bogert, New York. Hermon Carey Bumpus, Ph.D., New York City. Alexis Carrel, M.D., New York City. Edwin Brant Frost, Williams Bay, Wis. a. V= Walliams) -Jackson, Ph.D: Lap) Yonkers, Ni. Y: John Frederick Lewis, Philadelphia. William Romaine Newbold, Ph.D., Philadelphia. Charles Bingham Penrose, M.D., Ph.D., Philadelphia. William Howard Taft, Washington. Charles Richard Van Hise, M.S., LL.D., Madison, Wis. Victor Clarence Vaughan, M.D.,Sc.D., LL.D., Ann Arbor, Mich. A letter was received from Dr. Alfred Russell Wallace, thank- ing the Society for its kind greetings sent when celebrating Darwin’s — centenary. (See page ix.) The decease was announced of Mr. Andrew Mason, at New York, on April 28, 1909, aged 80. Dr. Alexander Graham Bell read a paper an “ Aérial Locomo= tion,’ which was discussed by Mr. A. E. Lehman and Prof. M. B. Snyder. Stated Meeting May 21, 1909. Mr. H. La Barre Jayne, Treasurer, in the Chair. Letters accepting membership were read from: Francis Darwin, M.A., F.R.S., Cambridge, Eng. . Hermann Diels, Ph.D., Berlin. Emil Fischer, Ph.D., M.D., Berlin. Friedrich Kohlrausch, Ph.D., Marburg. Wilhelm Pfeffer, Ph.D., Leipzig. A letter was received from Sir Joseph Dalton Hooker expressing X1V MINUTES. [May 21, his thanks for the Society’s greeting conveyed by cablegram on the occasion of the commemoration of the centenary of Charles Darwin. (See page ic.) An invitation was read from the Massachusetts Institute of Technology inviting the Society to be represented at the inaugura- tion of Dr, Richard C.’Maclaurin as’ President; on June 7.) )@na motion the President was authorized to appoint such a representative. The decease was announced of Dr. C. Newlin Peirce, at Phila- delphia, on May 16, 1909, aged 80. “ Mr. R. H. Mathews read a paper on “Some Burial Customs of the Australian Aborigines.” Stated Meeting, October 1, 1909. Witii1am W. KEEN, M.D., LL.D., President, in the Chair. Mr. James Christie, elected to membership in 1908, was admitted into the Society. A letter accepting membership was received from Prof. Robert Ai iarper: Invitations were received: From the University of Geneva to be represented at the Cele- bration of the 350th Anniversary of the foundation of the University. From the President and Fellows of Harvard University to be represented at the inauguration of Abbott Lawrence Lowell, LL.D., as President of Harvard University. The decease was announced of the following members: Dr. Aristides Brezina, at Vienna, on May 25, 1909, et. 62. Dr. Edward Everett Hale, at Roxbury, Mass., on June 10, 1909, zt. 87. Prof. Simon Newcomb, at Washington, on July 11, 1909, et. 74. Dr. Henry C. Chapman, at Bar Harbor, Me., on September 7, 1909, zt. 64. Dr. Anton Dohrn, at Naples, on September 26, 1909, zet. 68. The following papers were presented: “The Vertebrates of the Cayuga Lake Basin, N. Y.,” by men 1909. ] MINUTES. XV D. Reed and Albert H. Wright. (Communicated by Prof. Burt G. Wilder.) “Further Notes on Ceremonial Stones, Australia,” by R. H. Mathews. Stated Meeting, October 15, 19009. WILLIAM W. KEEN, M.D., LL.D., President, in the Chair. The decease was announced of Prof. Otto Donner, at Helsing- fors, on September 17, 1909. Dr. Randle C. Rosenberger read a paper on “ Typhoid Carriers.” Stated Meeting, November 5, 1900. Wituiam W. KEEN, M.D., LL.D., President, in the Chair. Invitations were received: From the College of Physicians of Philadelphia, inviting the Society to be represented at the dedication of its New Hall. From the XVIIth International Congress of Americanists to be represented at the Congress to be held first at Buenos Aires from May 16 to 21, 1910, and then in the City of Mexico in the following September. The decease was announced of: Henry Charles Lea, LL.D., at Philadelphia, on October 24, 1909, zt. 84. Hon. William Butler, at West Chester, Pa., on November 3, LQOOs iy S77: Mr. Harrison S. Morris read an obituary notice of Mr. Joseph Wharton. Dr. W. B. Cannon read a paper on “The Correlation of the Gastric and Intestinal Digestive Processes and the Influence of Emotions upon Them.” Mr. John C. Willis, Director of the Royal Botanic Garden, Co- lombo, read a paper on “ The Vegetation of Ceylon.” Stated Meeting, November 19, 1909. WILLIAM W. KEEN, M.D., LL.D., President, in the Chair. Prof. C. L. Doolittle read a paper on “ Halley’s Comet.” xvi MINUTES. [November 19, Prof. Edward C. Pickering was elected a Vice-President to fill the unexpired term of the late Prof. Simon Newcomb. Stated Meeting, December 3, 1900. WILLIAM W. KEEN, M.D., LL.D., President, in the Chair. An invitation was received from the president of the Eighth International Zoological Congress to send delegates to the Congress to be held at Graz, Austria, from August 15 to 20, 1910. Prof. E. P. Cheyney read a paper on “ The Court of Star Cham- ber in the Time of Queen Elizabeth and the Early Stuarts.” Stated Meeting, December 17, 1909. WILLIAM W. KEEN, M.D., LL.D., President, in the Chair. The decease was announced of M. Serge Nikitin, at St. Peters- burg, on November 18, 1909. The Annual Address of the President was delivered by Dr. William W. Keen. Dr. Edward Meyer, of Berlin, read a paper entitled “ The Story of the Wise Ahikar.”’ INDEX. A Absorption spectra of certain solu- tions, effect of temperature on, 194, Xi Aérial locomotion, xiii Ahikar, story of the Wise, xvi Air, exploration of the upper, by means of kites and balloons, 8, v Australian aborigines, burial customs of, 313, xiv B Bacterial life in water, effect of bleaching powder upon, viil Balch, Edwin Swift, Why America should re-explore Wilkes Land, 34, vi, vil Thomas Willing, The American- British Atlantic Fisheries Ques- tion, 319, vi Barnard, remarkable changes in the tail of Comet C, 1908 (More- house), x Barus, adjustment for a plane grat- ing, 166, xi —— electrometric measurement of the voltaic potential difference be- tween the two conductors Ola condenser, I80, xi electron method of Gt alanain ing the coronas of cloudy conden- sation, 177, xi Bauer, solar activity and terrestrial magnetic disturbances, xi Bell, aérial locomotion, xiii Beverages and medicines, forming agents in, xi Blair, exploration of the upper air by means of kites and ballons, 8, v Bloomfield, extent and number of the Indo-European peoples, vill habit- Bogert, coal tar products and their application in the arts and medi- cine, v, vi Brain weight records, some condi- tions modifying the interpretation of human, vii Brains of two white philosophers and two obscure negroes, vii Bright, some aspects of the question of English speaking, iv Brown, device for tabulation of the sums of numerous variable func- tions, vili Bryant, voleanic formations of Java, vi Bryce, personal reminiscences of Charles Darwin and the reception of “The Origin of Species,” iii, xi Burial customs of the Australian aborigines, 313, xiv Bush, The Burning, and the origin of ‘Judaism, 354, vill C Cannon, correlation of the gastric and intestinal digestive processes and the influence of emotions upon them, xv Carter, evolution of the city of Rome from its origin to the Gallic Catastrophe, 1209, vi Cetacea, South American fossil, viii Cheyney, The Court of Star Cham- ber in the time of Elizabeth and the early Stuarts, xvi Chrysocolla from Chile, 65, vii Clarke, chemical work of the U. S. Geological Survey, viii Coal tar products and their applica- tion in the arts and medicine, v, vi College of Physicians, invitation to dedication of its new Hall, xv Color in plants, modification of, vii Comet C, remarkable changes in the tail of, 1908 (Morehouse), x Condenser, electrometric measure- ment of the Voltaic potential dif- ference between the two conduc- tors of a, 1890, xi Conklin, the world’s debt to Darwin, HLXVIU ——appointed Delegate to N. Y. Academy of Sciences, iv Coronas of cloudy condensation, 177, i: Cylinders, linear resistance between parallel conducting, 142, x XVi11 Xvili D Darwin, centenary of, and 5oth An- niversary of publication of “the Origin of Species,” ix —— — Invitation tromuN. Yo Acad— emy of Sciences to, iv influence of, on the mental and moral sciences, 7xv, 1x —— — — natural sciences, rv — personal reminiscences of, and of the reception of “The Origin of Species,” 1, ix the world’s debt to, xaxxviit Device for tabulation of the sums of numerous variable functions, viii Digestive processes, the correlation of the gastric and intestinal, and the influence of emotions upon them, xv ‘Diplomatic life usage, v Donaldson, some conditions modify- ing the interpretation of human brain weight-records, vii Doolittle, Charles L., Halley’s Comet, XV —— Eric, Penrose’s graphical method for orbit determination, ix and diplomatic E Earth, past history of the, as in- ferred from the mode of forma- tion of the solar system, I19 Earthquakes, their causes and ef- fects, 235, xi ——, symposium on, xi, xii Election of members, ix —— of Officers and Councillors, iii Electrometric measurements of the potential difference between two conductors of a condenser, 1890, xi English speaking, some aspects of the question of, iv Ether, recent work on the physics of the, vili F Fauna, destruction of the fresh- water, in western Pennsylvania, 90, Vili Fisheries question, the American— British Atlantic, 319, vi Flexner, specific chemo-therapy of the protozoal diseases, xi Fullerton, influence of Darwin on the mental and moral sciences, rxv, ix INDEX. G Geology, seismic, the present status and outlook of, 250, xi Gilman, obituary notice of Daniel Coit, lxit, v Goodale, influence of Darwin on the natural sciences, xv, 1x Grating, an adjustment for a plane, 166, xi Gratings, the ruling of diffraction, x Greetings and congratulations cabled to Sir Joseph Dalton Hooker and Dr. Alfred Russel Wallace, ix Gun cotton, detonation of, 60, viii H Halley’s Comet, xv Harshberger, comparative leaf struc- ture of the strand plants of New Jersey, 72, vii Harvard University, invitation to in- auguration of its President, xix Haupt, Lewis M., the nation and the | waterways, 5I, vi Paul, The Burning Bush and the origin of Judaism, 354, vili Heyl, recent work on the physics of the ether, viii Hindu Idea, iv Hirst, obituary notice of R. A. F. Penrose, Iviii Hobbs, the present status and out- look of seismic geology, 259, xi Hooker, acknowledgment of greet- ings, xili —— greetings cabled to, ix Hovey, earthquakes, their causes and effects, 235, xi Hiilsen, machines and engineering in the renaissance, viii and congratulations I Indo-European peoples, viii van Ingen, stratigraphic position of the Oolitic iron-ore at Blooms- burg, Pa., viii International Congress of American- ists, invitation, xv International Zoological invitation, xvi Irish race, Prof. Mahaffy on, iv Iron-ore, stratigraphic position of the Oolitic—at Bloomsburg, Pa., viii Congress, INDEX. | Jackson, mithraism and manechzism, vi Jones and Strong, effect of tempera- ture on the absorption spectra of certain solutions, 194, xi Judaism, origin of, and The Burn- ing Bush, 354, viii K Kebler, the unsuspected presence of habit- forming agents in beverages and medicines, xi Keen, recent surgical progress, vi Keller, new variety of chrysocolla from Chile, 65, vii Kennelly, linear resistance between parallel conducting cylinders, 142, x Kraemer, delegate to N. Y. Acad- emy of Sciences, iv —., modification in color plants, vii L Leaf structure of the strand plants of New, Jersey, 72, vii Lovett, certain generalizations of the Problem of Three Bodies, 111, ix M Machines and engineering in the re- naissance, etc., vill Mahaftfy, the Irish race, iv Mason, effect. of bleaching powder upon bacterial life in water, viii ——, purification of water supplies by use of hypochlorites, 67 Massachusetts Institute of Technol- ogy, invitation to inauguration of its President, xiv Mathews, burial customs of the Aus- tralian aborigines, 313, xiv , ceremonial stones used by Aus- tralian aborigines, i, 460, iil, xv Meeting, General, vi ——, Special, iv ——., Stated, iii Members deceased: . Boye, Martin Hans, v Brezina, Aristides, xiv Butler, Hon. William, xv Chapman, Henry C., xiv Dohrn, Anton, xiv Donner, Otto, xv Frazer, Persifor, vi Hale, Edward Everett, xiv Hough, George E., iv xix Lambert, Guillaume, v Lea, Henry C., xv Mason, Andrew, xiii Moore, James W., v Newcomb, Simon, xiv Nikitin, Serge, xvi Patterson, Robert, v Peirce, C. Newlin, xiv Penrose, Richard A. F., iii Platt, Charles, iv Wahl, William Henry, vi Wharton, Joseph, iv — elected: Bauer, Louis A., ix Bogert, Marston Taylor, ix Bumpus, Hermon Carey, ix Carrel, Alexis, ix Darwin, Francis, x Diels, Hermann, x Fischer, Emil, x ~Frost, Edwin Brant, x Harper, Robert Almer, x Hobbs, William Herbert, x Jackson, A. V. Williams, x Kohlrausch, Friedrich, x Lewis, John Frederick, x Lowell, Abbott Lawrence, x Newbold, William Romaine, x Penrose, Charles Bingham, x Pfeffer, Wilhelm, x Taft, William Howard, x Van Hise, Charles Richard, x Vaughan, Victor Clarence, x presented, viii, x, xi, xiii, xiv Membership accepted, xili, xiv Meyer, the story of the Wise Ahikar, xvi Michelson, the ruling of diffraction gratings, x Mithraism and Manichaeism, vi Morris, obituary notice of Joseph Wharton, lax Munroe, detonation of gun cotton, 69, viii N Nation and the waterways, 51, vi Natural sciences, influence of Dar- win on, ix Newcomb, Simon, telegram of sym- pathy sent to, viii Newell, the conservation of water resources in the western United States, v New York Academy of Sciences, in- vitation to Darwin Centenary, iv Nipher, vacuum effects in electrical discharge around a right angle in a wire, x DO.4 INDEX. 0) ee notice of Daniel C. Gilman, cM, V R. A. F. Penrose, /viii, iv Joseph Wharton, lrxi, xv Orbit determination, Penrose’s method for, ix Origin of Species, commemoration of 50 5oth anniversary of publication @ Otimadn destruction of the fresh- water fauna in western Pennsyl- vania, 90, viii P Penrose, R. A. F., obituary notice of, lviti, iv Photography, the solgram system of color, iv Pickering, elected Vice-President, Xvi Plants, comparative leaf structure of the strand, of New Jersey, 72, vii President’s annual address, xvi Pritchett, delegate to N. Y. Academy of Sciences, iv Protozoal diseases, xi R Reed and Wright, the vertebrates of the Cayuga Lake Basin, N. Y., 370, XIV Reid, seismological notes, 303, xii Rome, the evolution of the city of, 120, vi Rosenberger, typhoid carriers, xv S) See. the past history of the earth as inferred from the mode of forma- tion of the solar system, 110, x Seismic geology, 250, xi Seismological notes, 303, xii Solar activity and terrestrial mag- netic disturbances, xi South, the solgram system of color- photography, iv Star Chamber, Court of, in the time of Elizabeth and the early Stuarts, xvi Stones, ceremonial, used by the Aus- tralian aborigines, i, 460, 1, iii by Temperature, effect of, on the ab- sorption spectra of certain solu- tions, 194, xi Three Bodies, generalizations of the problem of, III, iii, viii Tower, diplomatic life and diplomatic usage, V True, South American fossil cetacea, viii Typhoid carriers, xv U U. S. Geological Survey, chemical work of the, viii University of Geneva, invitation to 350th anniversary, xiv Vv Vacuum effects in electrical dis- charge around a right angle in a wire, x Vegetation of Ceylon, xv Vertebrates of the Cayuga Lake Basin Ne ay., 9370 Vice-President elected, xvi Volcanic formations of Java, vi Ww Wallace, acknowledgment of greet- ings, xill greetings and congratulations cabled to, ix Water resources, the conservation of, in the western United States, v supplies, purification of, by use of hypochlorites, 67 Waterways, the Nation and the, 51 Wharton, Joseph, obituary notice of, lexi, XV Wilder, brains of two white philoso- phers and of two obscure negroes, Villines Wilkes Land, why America should * reéxplore, 34, vi, vii Willis, vegetation of Ceylon, xv ry fs OM bare op Witt