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Pr x a sail saa Shee. a tial ie reer age Piy r promised so much that he was no more likely to perform it than to obtain perpetual motion; indeed, if the invention were not overstated, they would certainiy be nearer perpetual motion than they have eyer been before. Mr. Varley suggested that as the principal feature in the invention appeared to be the heating of the ma- terials, it was not impossible that it might be as great a s'ep in advance as the introduction of the hot-blast in the manufacture of iron: this of course remained to be seen.—London Mechanics’ Magazine. ILLUSTRATIONS OF MAGNETIC ACTION. The following is a partial report of a lecture recently delivered before the Royal Institution of London, by Prof. Tyndall, ‘‘On some of the Phenomena of Magnetism” :— The Crackle of Magnetized Iron.—Here is a fine permanent mag- net, competent to carry a great weight. Here, for example, is a dish of iron nails, which it is able to empty. At the other side of the table you observe another mass of metal, bent like the magnet, but not, like it, naked. This mass, however, is not steel, but iron, and it is surrounded by coils of copper wire. It is intended to illustrate the excitement of magnetism by electricity. At the present moment this huge bent bar is so inert as to be incapable of carrying a single grain of iron. I now send an electric current through the coils that surround it, and its power far transcends that of the steel magnet on the other side. It can carry 50 times the weight. It holds a 56 lb. weight attached to each of its poles, and it empties this large tray of iron nails when they are brought sufficiently near it. I interrupt the current: the power vanishes and the nails fall. Now the magnetized iron cannot be in all respects the same as the unmagnetized iron. Some change must take place among the mole- cules of the iron bar at the moment of magnetization. And one -= NATURAL PHILOSOPHY. 125 curious action which accompanies the act of magnetization I will now try to make sensible to you. Other men labored, and we are here entering into their labors. The effect I wish to make manifest was discovered by Mr. Joule, and was subsequently exammed by MM. De la Rive, Wertheim, Were Matteucci, and Wartmann. It is this. At the moment when the current passes through the coil surrounding the electro-magnet, a clink is heard emanating from the body of the iron, and at the moment the current ceases a clink i is also heard. In fact, the acts of magnetization and demagnetization so stir the atoms of the magnetized body that they, in their turn, can stir the air and send sonorous impulses to our auditory nerves. I have said that the sounds occur at the moment of macnetization, and at the moment when magnetization ceases; hence if I can devise a means of making and breaking in quick ‘succession the circuit through which the current flows, T can obtain an equally quick sue- cession of sounds. I do this by means of a contact breaker which belongs to a Ruhmkorff’s induction coil. Here is a monochord, and a thin bar of iron stretches from one of its bridges to the other. ‘This bar is placed in a glass tube, which is surrounded by copper wire. I place the contact “breaker in a distant room, so that you can- not hear its noise, The current is now active, and every individual in this large assembly hears something between a dry crackle and a musical sound issuing from the bar in consequence of its successive maenetization and demacnetization. Magnetism of the Electric Current—Hitherto we have occupied ourselves with the iron which has been acted upon by the current. Let us now devote a moment’s time to the examination of the current itself. Here is a naked copper wire which is quite inert, possessing no power to attract these iron filings. I send a voltaic current through it: it immediately grapples with the filings, and holds them round it in a thick envelop. I interrupt the current, and the filings fall. Hereis a compact coil of Copper wire, which is overspun with cotton to prevent contact between the convolutions. At present the coil is inert; but now I send a current through it: a power of attrac- tion is instantly developed, and you see that it is competent to empty this plate of iron nails. Thus we have magnetic action exhibited by a body which does not contain a particle of the so-called magnetic metals. ‘The copper wire is made magnetic by the electric current. Indeed, by means of a cop- per wire, through which a current flows, we may obtain all the effects of magnetism. “T have here a long coil, so suspended as to be capable of free motion in a horizontal direction ; it can move all round ina circle like an ordinary magnetic needle. At its ends I have placed two spirals of platinum wire, which the current will raise to brillant incandescence. They are glowing now, and the suspended coil be- haves, in all respects, like a magnetic needle. Its two ends show opposite polarities ; it can be attracted and re pelled by a magnet, or by a current flowing through another coil; and it is so sensitive that the action of the earth itself is capable of setting it north and south. Ampere’s Theory.—There is an irresistible tendency to unify in the human mind; and, in accordance with our mental constitution, we desire to reduce phenomena which are so much alike to a common be 126 ANNUAL OF SCIENTIFIC DISCOVERY. cause. Hence the conception of the celebrated Ampere that a mag- net is simply an assemblage of electric currents. Round the atoms of a magnet Ampere supposed aninute currents to circulate .inces- santly in - parallel planes ; round the atoms of common iron he also supposed them to circulate, but in all directions,—thus neutralizing each other. The act of magnetism he supposed to consist in the ren- dering of the molecular currents parallel to a common plane, as they ere supposed to be in a permanent magnet. This is the celebrated theory of molecular currents propounded by Ampere. The Lengthening of Lron by Magnetism.—lIs it a fact that an iron par is shortened by the act of magnetization? It is not. And here, us before, we enter into the labors of other men. Mr. Joule was the first to prove that the bar is lengthened. Mr. Joule rendered this lenzthening visible by means of a system of levers and a microscope, through which a single observer saw the action. The experiment has never, I believe, been made before a public audi- ence, but the instrument referred to at the commencement of this lecture, will, I think, enable me to render this effect of magnetization visible to everybody present. Before you is an iron bar, two feet long, firmly screwed into a solid block of wood. Sliding on two upright brass pillars is a portion of the instrument which you see above the iron bar. The essential parts of this section of the apparatus are, first, a vertical rod of brass, which moves freely and accurately in a long brass collar. The lower end of the brass rod rests upon the upper flat surface of the iron bar. To the top of the brass rod is attached a point of steel; and this point now presses against a plate of agate, near a pivot which forms the fulerum of a lever. The distant end of the lever is connected by a very fine wire with an axis on which is fixed a small circular mirror. If the steel point be pushed up against the agate plate, the end of the lever is raised; the axis is thereby caused to turn, and the mirror ro- tates. I now cast a beam from an electric lamp upon the mirror; it is reflected in a luminous sheaf, 15 or 16 feet long, and it strikes our screen, there forming a circular patch of brilliant light. his beam is to be our index; it will move as the mirror moves, only with twice its angular velocity ; and the motion of the patch of light will inform us of the lengthening and shortening of the iron bar. I employ one battery simply to ignite the lamp. I have here a second battery to magnetize the iron bar. At present no current is passing. I make the circuit, and the bright image on the screen is suddenly displaced. It sinks a foot. I break the circuit; the bar instantly shrinks to its normal length, and the image returns to its first position. I made the experiment several times in succession ; the result is always the same. Always when I magnetize, the image instantly descends, which declares the lengthening ¢ of the bar; always when I interrupt the current the image immediately rises. A little warm water projected against the bar causes the image to descend gradually. ‘This, I believe, is the first time that this action of mag- netism has been seen by a public audience. I have employed the same apparatus in the examination of bismuth bars ; and, though considerable power has been applied, I have hith- erto failed to produce any sensible effect. It was at least conceivable NATURAL PHILOSOPHY. 127 that complementary effects might be here exhibited, and a new an- tithesis thus established between magnetism and diamagnetism. No explanation of this action has, to my knowledge, been offered ; and I would now beg to propose one, which seems to-be sufficient. I place this large flat m agnet upon the table; over it I put a paper screen, and on the screen [ shake iron filings. You know the beau- tiful lines in which those filings arrange themselves, —lines which have become classical from the use made of them in this Institution ; for they have been guiding-threads for Faraday’s intelligence while ex- ploring the most profound and intricate phenomena of magnetism. These lines indicate the direction in which a small macnetie needle sets itself when placed on any of them. The needle will always be a tangent to the magnetic curve. A little rod of iron, freely suspended, behaves exactly like the needle, and sets its longest dimension in the direction of the magnetic curve. In fact, the particles of iron filings themselves are vir tually so many little rods of iron, which, when they are released from the friction of the screen by tapping, set their long- est dimensions along the lines of force. Now, in this bar magnet the lines of force run alone the magnet itself, and were its particles capa- ble of free motion they also would set their longest dimensions parallel to the“tines of foree,—that is to say, parallel to the length of the magnet. ‘This, then, is the explanation which I would offer of the lengthening of the bar. The bar is composed of irregular crystalline granules : : and, when magnetized, these oranules tend to set their long- est dimensions parallel to the axis of the bar. They succeed, partially, and produce a microscopic lengthening of the bar, which, suitably mag- nified, has been rendered visible to you. But can we not bring a body with movable particles within an elec- tro-magnetic coil ? We ean; and [ will now, in conclusion, show you an experiment devised by Mr. Grove, which bears directly upon this question, but the sight of which, J believe, has hitherto been confined to Mr. Grove himself. At all events, I am not aware of its ever having been made before a large audience. I have here a cylinder with glass ends, and it contains a muddy liquid. This muddiness is produced by the magnetic oxyde of iron which is suspended mechanic- ally in water. Round the glass cylinder I have coiled five or six layers of covered copper wire; and here is a battery from which a current can be sent through the coil. First of all, I place the glass eylinder in the path of the beam from our electric lamp, and, by means of a lens, cast a magnified image of the end of the cylinder on the screen. That image at present possesses but feeble illumination. The light is almost extinguished by the suspended ee of mag- netic oxyde. But, if what I have stated regarding the lines of force through the bar of magnetized iron be correct, the particles of the oxyde will suddenly set “their longest dimensions parallel to the axis of the cylinder, and also in part set themselves end to end when the current is sent round them. More light will be thus enabled to pass ; and now you observe the effect. The moment I establish the cirewt the dise upon the screen becomes luminous. I interrupt the current, and gloom supervenes; I re-establish it, and we have a luminous dise once more. 128 ANNUAL OF SCIENTIFIC DISCOVERY. ON THE MECHANICAL THEORY AND APPLICATION OF THE LAWS OF MAGNETIC INDUCTION AND ELECTRICITY. E In a paper on the above subject read before the British Association, at its last meeting, by Mr. J. B. Thomson, electricity and magnetism were considered as a force in the same way as heat and light; and electric and magnetic induction were treated in correspondence with mechanics. ‘The summary of the author’s theories is: That the phe- momena called electricity and magnetism are two forms of force which may either be in conatus or in act. If in conatus, they are in a state of tension; if in act, then in a state of fluxion. Electricity is in co- natus when in the static form of excitation, or when the voltaic circuit is not completed; in act, when the matter highly excited is brought in contact with matter less highly excited, or when the voltaic circuit is completed. Magnetism is in conatus when the magnetic vortical sphere is held constant by a constant electric current, or by hardened steel or magnetic iron ore, so that the earth-magnetism may flow in; in act, on its electric projection and recession, or when iron or some other paramagnetic is moved through this sphere. That electric con- dution is by certain molecular movements of particular portions of mat- ter. Those wherein this movement is easily excitedtre called con- ductors, and those wherein it is with difficulty excited are called insula- tors. That magnetic conduction is by the symmetrical arrangement into a vortical sphere of spirals of a general medium, which pervades all matter, and holds it in that form for the time bemg. That par- ticular matter wherein the sphere is easily excited is called paramag- netic, and that wherein it is with more difficulty excited is called dia- magnetic. ‘That this sphere can be fixed by means of hardened steel or magnetic iron ore. That the magnetic vortical can be excited by means of spiral currents of electricity generally, and even by a tan- gent to such spiral. Also it can be induced by magnetic conduction in paramagnetics. That the magnetic force is only in a state of fluxion on the projection aud recession of this sphere. That this sphere is projected in the direction of the exciting electric current, an 1 recedes in the opposite direction. That the electric force is induced on the projection of the magnetic vortical, and also on its recession. That, consequently, for one inducing current there are two induced cur- rents ; therefore, it would appear that by induction electric excitation is multiplied. Finally, that these inductions and conversions of force are in strict accordance with the laws of mechanical motion. In con- nection with the paper an induction machine was exhibited, the chief points of novelty in which appear to be these: That it is self-acting ; the current of voltaic electricity which produces the induced current also drives the machine; that the machine can be so adjusted that the quantity and intensity of the induced current shall range from that of ten Daniell’s cells to that of 1,000, and this without employing more than three or four cells. These are valuable properties to electricians who are engaged in experiments with electricity of high or even mod- erately high tension. Besides, it is applicable to any batteries what- ever, having been used experimentally for telezraphy and for electro- depositing. For telegraphy through submarine and subterraneous cables there appears to have been a great objection to induction ma- NATURAL PHILOSOPHY. 129 chines, or rather induction coils. The objection was, that these induc- tion coils sent their electricity through the cables in sudden intense shocks, which injired the insulation of the cable. In this machine it is apparently a.continuous flow, and no spark will jump from one elec- trode to the other, unless first brought in contact, as in. batteries. When modified for electro-plating it is much more efficient than the ordinary battery ; for though it deposits the metal more slowly on any one ar- ticle, yet it deposits it much more firmly and with a better surface than the ordinary battery does, and it will deposit the same quantity on 1,000 articles at once, which enables it to deposit ten times more metal in the same time than its own exciting battery would do. The construction of the machine is apparently very simple, and will not be easily deranged or speedily worn out. ANALYSIS OF MAGNETIC STORMS. The first analysis of 177 magnetic storms, recently laid before the Royal Society, by the Astronomer Royal, Mr. G. B. Airy, is printed in alate number of the Proceedings of the Society. In regard to the physical inference to be derived from the numerical conclusions ob- tained from tables exhibiting the algebraic sum of fluctuations for each storm, the aggregate or mean for each year, and for seventeen years, the number of irregularities for each year and for the whole period, &c., Mr. Airy expresses his strong opinion that it is impossi- ble to explain the disturbances by the supposition of definite galvanic currents, or definite magnets, produced in any locality whatever. He suggests that the relations of the forces found from his investigations bear a very close resemblance to what might be expected if we con- ceived a fluid (to which, for facility of language, the name ‘‘ magnetic ether” is given) in proximity to the earth, to be subject to occasional eurrents produced by some action, or cessation of action, of the sun, which currents are lable to interruptions or perversions of the same kind as those in air and water. He shows that in air and water the general type of irregular disturbance is traveling circular forms, sometimes with radial currents, but more frequently with tangential currents, sometimes with increase of vertical pressure in the center, but more frequently with decrease of vertical pressure; and, in con- sidering the phenomena which such traveling forms would present to a being over whom they traveled, he thinks that the magnetic phe- nomena would be in a great measure imitated. Mr. Airy recommends that observations be made at five or six observatories spread over Europe, and would prefer self-registering apparatus, provided that its zeros be duly checked by eye observations, and that the adjustments of the light give suflicient strength to the traces to make them visible in the most violent motions of the magnet. : CURIOUS MAGNETIC DISTURBANCES. At a recent meeting of the Royal Society, Gen. Sabine brought to notice some remarkable magnetic phenomena recently brought to hght by his researches, namely, the difference of direction observed in disturbances of the magnetic declination at stations in England, and others beyond the Ural Mountains. ‘The days and hours at which the phenomena occur are, with slight exception, the same, and the move- 130 ANNUAL OF SCIENTIFIC DISCOVERY. ments are simultaneous, in both localities ; but the direction of the magnet indicating the disturbances is directly the reverse in Eastern Siberia of the direction in England. RESIDUAL MAGNETISM. Dr. A. Von Waltenhofen has communicated to Dingler’s Polytech- nisches Journal, an account of a curious magnetic discovery which he has recently made. It is a well-known fact that the magnetism of an electro-magnet does not entirely disappear with the cessation of the magnetizing current. Dr. A. Von Waltenhofen has, however, ob- served that the amount of this residual magnetism, as it is called, is dependent upon the manner in which the current is interrupted. If this interruption takes place suddenly, the residual magnetism is much less than when it takes place gradually. A still more interesting circumstance has been observed by him, viz: that the residual magnet- ism obtained by suddenly breaking a very strong current, is sometimes of an opposite nature to that previously existing in the electro-magnet. This fact, which he has hitherto only noticed in very soft iron, is of great interest, inasmuch as it furnishes a new and simple proof that magnet- ism is not caused by the separation of two fluids, but by the motion of magnetic molecules, to which is opposed a certain amount of frictional resistance. With much ingenuity he compares the state of each mag- netic molecule of the electro-magnet to that of a spring which is bent back. Ifthe spring be suddenly released, it will return very nearly to its orginal position, or even go beyond it. On the other hand, if it be released gradually, it will stop at a point still further removed from its original position. “LIQUID STEERING COMPASs ” AND ‘MONITOR COMPASS.” Two new forms of compass recently devised by Mr. E. S. Ritchie, of Boston, have the following construction: The distinctive pecul- iarities of the liquid compass are an air-tight metallic case within which is placed the magnetic needle, and of such size and weight as to be of very nearly the same specific gravity as the liquid in which it is intended to float. The weight is thus removed from the pivot, and friction is almost prevented; certain modifications being intro- duced to provide against tilting and other emergencies occurring during the motion of the ship. The distinctive principle of the Monitor Compass is the separation of the magnet from the card or index, so that the magnet may be elevated above the sphere of dis- turbing attraction of. the iron of the ship, while the card is brought to a convenient position to be seen by the pilot; and suspending the movable portion in a liquid so as to secure entire freedom from fric- tion, that the needle may obey the polar force, and at the same time great steadiness is secured for the card. New Form of Magnetic Needle.—At a recent meeting of the Man- chester Philosophical Society, Mr. Joule exhibited a new form of magnetic needle for showing rapid and minute alterations of declina- tion. It consisted of a piece of hardened and polished watch spring, an inch long, and =}; of an inch broad suspended vertically by a fila- ment of silk. The steel was magnetized in the direction of its breadth. He remarked that Professor Thomson had long insisted NATURAL PHILOSOPHY. 131 upon the advantages which would attend the use of very small bars in most magnetical investigations, and had employed excessively minute needles in his galvanometers with great success. Dr. Joule stated his intention to fit up his needle so as to be observed by light reflected from its polished surface, or otherwise, by viewing a glass pointer, attached to the bottom of the steel, through a microscope. He believed that by the latter plan he should be able to observe deflections as small as one second of an are. Great Electro-Magnet.—Messrs. Chester, of New York City, have recently constructed an electro-magnet of unusual size, for the New York Free Academy. It is made of the purest iron. The core is four inches in diameter; its total length is five feet. The wire wound upon it is in eight separate strands, and the aggregate weight of copper is 200 pounds. The entire weight of the magnet is 650 pounds. It is arranged either to be suspended with the faces down- ward, or to be placed upright on a wheeled platform. Connected with it is apparatus for diamagnetic experiments, consisting of rotat- ing copper discs and tubes. When the magnetic force is in action the rotating disc is instantly stopped, and motion is converted into heat. The heat evolved is sufficient to cause water to boil in a cop- per tube. THE TELEGRAPH AS A METEOROLOGICAL INDICATOR. ‘¢ The electric telegraph is likely to render us henceforth a service which it has not until now been known to be capable of. For some time past it has been systematically employed, to transmit to one center meteorological observations made at a great number of widely scattered points, and to transmit from that center predictions founded on these observations; but Father Secchi, the Italian savant, now informs us that a line of telegraph wires itself constitutes a better indicator of certain kinds of meteorological changes than any other we as yet know of. All persons at all familiar with electric telegraphy are aware that currents other than those proceeding from the batteries employed are constantly passing along all lines of telegraph wires. They are derived from either the earth or the atmosphere, and are called ‘ earth-currents.’ They are subject to great variations, which Father Secchi and some of his friends have for some time past been earefully studying, with the result, among others, of finding that, whenever the earth-currents are more irregular than ordinary, bad weather invariably follows, the degree of their regularity of the earth-currents bearing always an exact relation to that of the storm- iness of the weather which they precede. We are certainly progress- ing as regards our power of forecasting meteorological changes.” ON PERIODIC CHANGES IN THE MAGNETIC CONDITION OF THE EARTH, AND IN THE DISTRIBUTION OF TEMPERATURE UPON ITS SURFACE. The following is an abstract of a very curious and interesting paper recently read before the Manchester (Eng.) Philosophical So- ciety, by Mr. Baxendall, F.R. A.S. He says:— Considerations arising out of an investigation of the irregularities which take place in the changes of some of the variable stars, led the 132 ANNUAL OF SCIENTIFIC DISCOVERY author some time ago to regard it as highly probable that the light of the sun, and also its magnetic and heating powers, might be subject to changes of a more complicated natare than has hitherto been sup- posed, and that, besides the changes waich are indicated by the great- er or less frequency of solar spots, other changes of a minor caarac- ter, and occurring in shorter periods, might also take place. in tie hope of detecting these supposed changes, the author resoived to undertake the discussion of a series of magnetical observations, aud for this purpose he selected the observations made at the Lnperial Observatory of St Petersburg, the most northern station at which hourly magnetic observations have been made for any lengthened period. Commencing, therefore, with the year 1848, the greatest and least values of the magnetic declination for every day were extracted from the observations; and, taking the differences and arranging them in order, it was found, on a careful examination, that they indicated changes of activity taking place in a period of 31 days. The daily oscillations were then arranged in a table, when it was found that out of 17 consecutive days, the amount of oscillation, on range of the magnetic needle, was whove the mean on 13 days and be- low the mean on only four days; while of the remaining 14 days, the range was below the mean on 13 days, and above on one day only. ‘The total amount of the differences for the 17 days of maxi- mum was 2; per day ; and for the 14 days of mimimum +45. On proceeding to examine the observations for the succeeding years it was found that they could not be represented by a period of 31 days. It appeared, therefore, at first sight, that the period which had been obtained for 1848 was merely accidental; but, guided partly by conclusions drawn from his variable-star investigations, and partly by the high degree of improbability that the results for 1848 could be due to mere accident, the author was led to think that the period he had found for 1848 might be variable, gradually diminishing for a series of years, and afterward gradually increasing, to diminish again when it had completed its cycle of change. Assuming, there- fore, that in every year periodic changes took place in the magnetic activity of the sun, the author proceeded to determine for each year the most probable approximate value of the period, and he obtained a series of values gradually diminishing till 1556, when the period was only about 23 days, and aiterward rapidly increasing until, in 1859, it amounted to about 32 days. A glance at these results at once sug- gested the idea that the variable period thus found was in some way connected with, and dependent upon, the great solar-spot period, the minimum value occurring in the year of minimum frequency of the solar spots, and the maximum values in the years when the spots were most humerous. Several series of thermometrical observations were now examined for indications of periodical changes in the element of mean daily temperature, and it was found that they exhibited, with unexpected distinctness, changes in this element occurring also in a variable period, the range of variation being, however, somewhat less than in the case of the magnetic element, although the times of maximum and minimum were almost exactly the same. The maximum and minimum values were respectively 31 and 234 days. 4 NATURAL PHILOSOPHY. 133 A table is given showing the number of days included in the maxi- mum and ininimum portions of eaca mean period for the years 1848 to 1850, and the number of exceptional days, or those on which during the maximum part of the period the temperature was below, and during the minimum part above, the mean value. From this table it appears that out of a total number of 165 days of maximum, only 14 were exceptional; and out of a total of 1643 days of minimum, the number of exceptional days was only 16. The mean gives a ratio almost exactly as 1 to 11. Coasideriag that the values of the period in the different years are only approxunate, this result may be re- garded as affording satisfactory proot of the existence of a variable period of temperature. At St. Petersburg the average temperature of the warmer half of the period is not less than 3° greater than that of the cooler half; and as this difference of temperature is repeated at least 12 times in every year, it must necessarily exercise a poweriul modifying influence over many meteorological phenomena. Another period of change having a mean duration of rather over 18 months, is then referred to. The author was first led to it froma discus- sion of the Greenwich Magnetical Observations, for the years 1848 to 1859; and it has been confirmed by the results of a discussion of tem- perature observations, made at Brussels in Kurope, and at Yakoutsk, in Asia. It is obvious that this period will, at times, interfere sensi- bly with the shorter one, and it is probable that some of the cases which have been called exceptional may be due to this interference. With regard to the probable cause of the variability of the short period the author suggests the following hypothesis: Ist. That a ring of nebulous matter exists differing in density or constitution in different parts, or several masses of such matter forming a discontin- uous ring, circulating round the sun in a plane nearly coincident with the plane of the ecliptic, and at a mean distance from the sun, of about + of the radius of the earth’s orbit. 2d. ‘That the attractive force of the sun on the matter of this ring is alternately increased and diminished by the operation of the forces which produce the solar spots, being greatest at the times of minimum solar-spot frequency, and least when the spots are most numerous. 3d. The attractive force being variable, the dimensions of the ring and its period of revolution round the sun will also vary, their maxi- mum and minimum values occurring respectively at tie times of maximum and minimum solar-spot frequency. In reference to the nature of the varying attractive force, it is not improbable that the matter of the supposed ring may be highly dia- maenetic, and being much nearer to the sun than any of the known planets, of much greater bulk and lightness, and being subjected to a much higher temperature, it will be very sensibly affected by the changes which take place in the magnetic condition of the sun; and when interposed between the earth and the sun, it may act not only by reflecting and absorbing a portion of the light and heat which would otherwise reach the earth, but also by altering the direction of the lines of magnetic force. The changes of temperature at the sur- face of the earth will thus be due partly to differences in the amount of heat received from the sun, and partly to changes in the move- 12 134 ANNUAL OF SCIENTIFIC DISCOVERY. ments of the great currents of the air produced by alterations in the earth’s magnetic condition. Ii the larger part of the difference of temperature is due to the latter mode of action, we might expect that during the warmer half of the period the mean direction of the wind at any given station would be sensibly different from that during the cooler half; and also, that the epochs of maximum and minimum temperature would not be the same at all parts of the earth’s surface. Both of these conclusions are borne out by the results given in the paper. Thus at St. Petersburg, in 1859, the mean direction of the wind on maximum days was S. 04° W., and on minimum days S. 73° _W. or 19° more to the west of South; and at Sitka, on the Northwest Coast of North America, in 1851, the mean direction on maximum days was S. 32° W., and on minimum days 8S. 56° W., the difference being 24°. As striking instances of the differences in the epochs at distant stations, it may be stated, that in 1859 the epoch of maximum at St. Petersburg corresponded precisely with the epoch of minimum at Madras; and that at Pekin, in 1801, the epoch of minimum was exactly coincident with the epoch of maximum at Sitka. Changes in the amount of heat received from the sun, sufficient to produce the variations of temperature observed at any given station, would no doubt affect the movements of the great currents of the at- mosphere, though not to the extent indicated by the observations; but it is difficult to conceive that they could produce the differences in the epochs which are tound to take place. We may therefore fairly conclude that the action of the supposed ring of nebulous matter is principally of a magnetic, and but slightly of a thermal character. Adopting, for the present, the maximum and minimum values of the temperature period as being determined with greater accuracy than those of the magnetic period, the greatest and least values of the sidereal period of revolution of the ring will be 29-12 and 22-08 days respectively. From these numbers we find that the greatest distance of the ring from the sun is 0°185, the radius of the earth’s orbit being taken as unity; the least distance, 0-154; and the mean 0°169. Taking Mr. Hind’s value of the mean distance of the earth from the sun, namely, 91,528,600 miles, we have: Greatest distance of the ring, 16,921,000 miles; least distance of the ring, 14,068,000; mean distance of the ring, 15,494,500; and the range of movement to and fro in a radial direction, 2,853,000 miles. ‘he greatest attractive force of the sun on the ring being taken as unity, the least will be 0°691. The difference is therefore nearly } of the maximum amount. It will be evident that this difference may be regarded as a measure of the forces which are concerned in the production of the solar spots. The results of the elaborate invesugations of the motions of the planet Mercury, made by Leverrier, led that accomplished mathematician to attrioute a certain unexplained excess in the motion of its perihelion to the action of a disturbing body circulating round the sun within the orbit of Mercury ; and, froin a discussion of the probable mass of the disturbing body, he concluded that it could not be concentrated in a single pla.et, and that it consisted of a ring of small bodies similar to that which is known to exist between the orbits of Mars and Jupiter; and it is re- marka le that the mean distance, which he seemed to regard as the most probable, is precisely that which the author has found for the ring of NATURAL PHILOSOPHY. 135 nebulous matter, whose existence he has assumed to account for the phenomena described in his paper. ‘This unexpected and unlooked-for agreement between results arcived at from considerations and by nethods so totally different, seems to establish the existence of this ring with quite as much certainty, as the results of the profound researches of Adams and Leverrier established the existence of Neptune before that planet had been actually seen. ‘This ring, however, owing to its proximity to the sun, may never be seen, and, like the dark companions of Procyon and Sinus, it may only be nom to us through its action on the other bodies of the system of which it forms a part. Should future rese ches place its existence beyond doubt, this will, it 8 -believed, be the first instance in which the conclusions of physical astronomy have been eon- firmed by the results of an investigation of magnetical and meteorologicil phenomena. Whether, however, “the hypothesis which the author has ventured to put forward be accepted or not, it is now very evident that observations of solar phenomena merit a much larger share of attention than has ever yet been devoted to them. It has long been suspected that the same causes which produce the spots on the sun’s disc must in some way have an important influence on the phenomena of our own atmos- phere. ‘The facts now given, convert this suspicion into a certainty ; and it is per haps, not too much to say, that meteorology can never take a as a true science while our knowledge of the sun remains in its present imperfect state. Moreover, there is s little doubt, that many question® of high physical interest depend for their solution upon our obtaining a more intimate acquaintance than we yet possess with the operations which are going on in the great center of our system. TELEGRAPHING BY MAGNETO-ELECTRIC MACHINES. We copy from the Washington Chronicle the following Sea a tion, apparently furnished by the well-known electrician, Dr. Page :— «The introductory report of the Patent Office for 1863 ventured upon the following anticipation: ‘It is not too much to say that the days of telecraphing by the galvanic battery are numbered, and that the magneto-electric machine will erelong take its place for this as well as for many other purposes.’ At that time it was well known that the magneto- electric machine was successfully working Beards- lee’s dial telegraph; but we’witnessed, on a recent evening, the ex- traordinary feat of working the Morse telegraph, between Washing- ton and New York, with one of Beardslee’s little magneto- electric machines, occupying space less than a cubic foot. The correspond- ence was kept up over the People’s Line with perfect freedom for more than an hour, and the Morse operator rattled off the messages as if he were perfectly at home. The sound of the instrument is musical, differiny from that of an ordinary receiving magnet. The Commissioner's Report alludes to the firing of eunpowder through the distance of one hundred miles by means Sof this little machine, but on the night in question we fired gunpowder in New York, a distance of two hundred miles, and the operators there fired ounpowder in Washington with perfect ease by the same little machine used to work the teleeraph. It was@ perfect success, and one of the most inter- esting and splendid achievements of modern science. If the Atlantic 136 ANNUAL OF SCIENTIFIC DISCOVERY. cable is ever laid, this seems the power destined to work it. Surely, ‘the days of the galvanic battery seem to be numbered.’ ‘* The invention above referred to is thus described by Commission- er Holloway in his Report :— “¢Conspicuous among the inventions which have received the sane- tion of letters patent is a magneto-eleciric telegraph, now in extensive use in the United States Army for field purposes, and elsewhere for or- dinary telegraphic purposes. This is a signal triumph in electro- mechanics, for by the motive power of a small magneto-electric ma- chine, occupying less than a cubic foot, a dial or index telegraph is operated through great*distances, from 5 to 200 miles, with the pros- pect of greater and indefinite extension. It was found with the Atlan- tic telegraph, in 1858, that alternating, or to and fro currents, were indispensable to its operation, and the magneto-electric machine of the telezraph before us has the peculiar movement of normal to and ro currents in rapid succession, without any extra contrivance for their production, this condition growing out of the very arrangement® of the magnetic poles and helices. The operators for this telegraph require no training, and any person who can read can telegraph. For the Morse telegraph two or three years of training are required. It is not liable to piracy by tapping, as is the Morse telegraph, and may be justly regarded as the inauguration of a new era in telegraphy, by disfensing with the cumbersome, uncleanly, unhealthy, and inconstant galvanic battery as the motive power, and the introduction of a simple and economical telegraph, adapted with equal facility to domestic and public purposes. It is not too much to say, that the days of tele- graphing by the galvanic battery are numbered, and that the magneto- electri¢ machine will erelong take its place for this, as well as for many other purposes. “¢ Another highly mteresting development in magneto-electric science is the discovery and application of a new mode of ignition for pur- poses of blasting with powder. Hitherto torpedoes and other powder blasts, fired by electricity, have depended upon the ignition of a very fine platinum wire. When this had to be done through long circuits, or at great distances, very large and expensive galvanic batteries were required, owing to the great diminution of the quantity of electricity. It was proved by experiments made at the Capitol many years since, that 150 pairs of Grove’s battery were necessary to ignite powder by the finest of platium wires placed in the telegraph circuit between Bal- timore and Washington, a distance of 40 miles. By means of the new discovery, powder has been fired through the distance of 100 miles by means of a little magneto-electric machine, occupying less than a cubie foot. This astonishing achievement has been accomplished by means so simple that electricians will wonder as much, if not more, than the uninitiated. It is done by a pencil-mark. The stroke of a common black-lead pencil on a block of wood is substituted for the platinum wire, and this disintegrated conductor, as it may be called, is so in- tensely ignited by the magneto-electric current as to set fire to the wood. ‘‘The application of this ingenious device within a suitably-pre- pared cartridge, will be hailed as one of the,most valuable contribu- tions to mining and engineering operations of the present day.” NATURAL PHILOSOPHY. 137 PROGRESS OF TELEGRAPHIC CONSTRUCTION, While citizens of the United States are engaged upon the great enter- prise of constructing a line of telegraph to Europe via Behring’s Straits and the Amoor, the British government are pushing their great project of connecting London and Calcutta with the electric wire, toa speedy conclu- sion. ‘Telegraphic communication has existed for two or three years be- tween London and Constantinop'e, and about the same time ago a cable was laid down through the Red Sea, between Suez and Aden, a distance of 3,000 miles, intended to complete the link between Europe and India, but it subsequently failed. Recently, however, a cable has been success- fully submerged through the Persian Gulf, which with the exception of 160 miles of land line, between Diwanyeh, on the Euphrates, and the Shat-el-Arab, the western termini of the Persian Gulf cable, completes the through telegraphic communication from the Thames to the Ganges, The distance from Constantinople to Fao, at the mouth of the Shat-el- Arab on the Persian Gulf, through which the line will pass when the Montifie Arabs and the healthy season will permit its safe construction to Diwanyeh, is 1,570 miles, and passes through the following important towns, Scutari, Angora, Diarbekir, Mossul, Bagdad, and Diwanyeh. From Fao to Kurrachee, the submarine cable stretches along the bottom of the Persian Gulf for 1,300 miles, and 500 miles farther carries it across a por- tion of the British-Indian empire to Bombay. The eastern terminus of the Turkish line for the receipt of messages, is at present at Bagdad, and the only communication with Fao is by way of the Tigris, by one British and two Turkish steamers, which run regularly, occupying from five to six days in the passage up the river, and 24 down. Another route from England to India, in connection with the Persian gulf cable, passes through Russia by way of Tiflis to Teheran, thence to Ispahan and Shiraz, and joins the cable at Bushire. As the line running through the Montific country, when completed, can scarcely be depended upon, owing to the relations existing between the tribes, who are very powerful and warlike, and the pasha of Bagdad, against whom they have risen in rebellion, the British government have contracted for the con- struction of a line which, effecting a considerable detour, will avoid the dis- turbed district completely. This wire is to pass from Bushire, on the Persian Gulf, where the cable lands before starting 170 miles further, to its terminus at Shat-el-Arab, via Kazeroor, Shiraz, Ispahan, Teheran, and Khanakeen to Bagdad, the distance between Bushire and Khanakeen being about 1,100 miles. The Indiin telegraphs, which connect together Calcutta, Bombay, Madras, Delhi, and all the principal towns in India, are now advanced eastward as far as Rangoon; and the roates thence to China and to Austra- lia, by way of Singapore, Java, and Timor, are said to be almost entirely in comparatively shallow water, so far as the submarine part of the line is concerned, and do not otherwise offer any difficulty which should pre- vent instantaneous communication between London, Hong Kong, Mel- bourne, and Sidney. When the Atlantic cable and the Russian line are successfully in on- eration, we shall have two sep rate routes to China and India,—to -ue latter via London and Constantinople, via St. Petersburg and Teheran; and to the former via Russia line from Irkoutsk in Siberia to Pekin, and via the Persian gulf cable and India, 12* . 138 ANNUAL OF SCIENTIFIC DISCOVERY. ON THE MECHANICAL PROPERTIES OF THE ATLANTIC TELEGRAPH CABLE. At the British Association, 1864, Mr. Fairbairn, the celebrated English engineer and scientist, read the following paper on the above subject : —_— It appears that the Atlantic Telegraph Company, considering it essential to the public interest that the second attempt to submerge a telegraph cable across the Atlantic should not be left to chance, “and that a close and searching investigation should be entered upon, and that nothmeg should be ‘jeft undone that could be accomplished to insure success, sought the advice of a committee composed of men of eminence and experience in the various branches of science and en- gineering involved in such an undertaking to advise the Company 1 in the selection of a cable. For the satisfactory attainment of this biect it was considered necessary, in the first place, To determine a direct experiment the mechanical properties of cables submitted for submergence in deep water; 2d, To ascertain the chemical prop- erties of the insulator, and the best means to be adopted for the preservation and duration of the cable; and 3d, To determine the electrical properties and conditions of the cable when immersed, under pressure, at great: depths. On the author of the paper de- volved the duty of undertaking the first division of the inquiry, viz: to determine, by actual experiment, the streugths, combinations, forms, and conditions of every cable considered of suitable strength and proportion to cross the Atlantic. A laborious series of experi- ments was instituted, and, in order to attam accuracy as regards the resisting powers of each cable to a tensile strain, they were broken by dead weights, suspended from a crab or crane, by which they could be raised or lowered at pleasure. The weights were laid on one cwt. at a time, and the elongations were carefully taken and recorded in the table as each alternate 3} ewt. was placed on the scale until it was broken. By this process we were enabled to ascertain with reat exactitude the amount of elongation in seven ft. six in. The result of the investigation was, the selection of the cable of Messrs. Glass & Elhott, which stood highest in order of strength. In this inquiry, upwards of 40 specimens “of cables have been tested in their finished state, and this might have been suflicient for the Committee to determine the best description of cable; it was, how- ever, deemed advisable to investigate still further, not only the cable asa cable, but to test experimentally each separate part, in order that every security should be afforded as to the strength and quality of the material to be employed in the construction. With regard to the covering wires, constituting the principal strength of the cable, Mr. Fairbairn finds that with proper care in the selection of the ma- terial in the first instance, a judicious system of manipulation in the second, and a rigid system of inspection of the manufacture, a wire of homogeneous 1 iron oe inches diameter can be made of strength suffic ent te sustain from 900 to 1,600 Ibs., with an elongation of -OUG8, OY zy'oo parts of an inch per unit of length. This description of: iron appears to be the most suitable for the Atlantic cable, as it com- bines strength with ductility, and may be produced at a comparatively NATURAL PHILOSOPHY. 159 moderate cost. It was also found desirable to test the separate strands of each cable as well as the wires themselves. Tor this pur- pose a number of strands similar to those employed in the manufiae- ture of the different cables were produced, and the tensile breaking strain and elongations carefully observed and eae led. In order to ascertain whether the lei igth of the lay of the hemp and Manilla round the strand was of that spiral form which produced a maxinuin of strength, the yarn separated from the strand was also tested, and comparing the sum of the breaking strains of the wire and yara sep- arately, with that of the two in combination in the strand, the object by these means was approximately obtained. Another very impor- tant question arises in the construction of this cable, and th at is, the strength of the core and its conducting wire, and how it is to be pro- tected under a pressure of 7,000 lb. to 8,000 per square inch, when lodged at the bottom of the ocean. This appeared a question well entitled to consideration, and provided a properly insulated wire, of one or more strands, can, without any exterior covering, be deposited with safety at these great depths, it is obvious that the simpler the cable the better. Assuming, therefore, that gutta-percha is the most desirable material that can be empley; ed as an insulator, it then re- solves itself into the question, what additional covering and what additional strength is neeeReeNy to enable the engineer so to pay out of the ship a length of 2,600 miles, into the deepest water, as to deposit it, without strain, at the bottom of the ocean? This is the question the Committee had to solve, and for this very important object experiments were instituted. Regarding the circumstances bearing directly upon the ultimate strength of the cable, the Com- mittee have arrived at the conclusion that the cable No. 46, composed of homogeneous wire, calculated to pom not less than from 840 Ib. to 1,000 lb. per wire, with a stretch of 3%; of an inch in 50 inches, is the most suitable for the Atlantic cable. , Bhe following is the specifica- tion of No. 46 cable: The conductor consists of a copper strand of seven wires (six laid round one), each wire gauging ‘048 (or No. 18 of the Birmingham wire-gauze), the entire strand gauging *144 inch, (or No. 10 Birmingham ; gauge), and weighing ¢ 300 Ib. per nautical mile, imbedded for solidity i in the composition known as “ Chatterton’s Compound. ” ‘The insulator consists of gutta-percha, four layers of which are laid on alternately, with four thin layers of Chatterton’s compound, making a diameter of the core of -464inch, and a circum- ference of 1°392 inches. The weight of the entire insulator is 400 Ib. per nautical mile. ‘The external protection is in two parts. First, the core is surrounded with-a padding of soft jute yarn, saturated with a preservative mixture. Next to this padding is the protective coy- ering, which consists of ten solid wires of the gauge ‘095 inch, drawn from homogeneous iron, each wire surrounded. separately with five strands of Manilla yarn, saturated with a preservative compound ; the whole of the ten strands thus formed of the hemp and iron bemg laid spfrally round the padded core. The weight of this cable in air is 34 ewt. per nautical mile,—the weight j in water is 14 ewt. per nau- tical mile. ‘The breaking strain is 7 tons 15 ewt., or equal to 11 times its weight per nautical mile in caine —that is to say, if suspended perpendicularly, it would bear its own weight in 11 miles depth of 140 ANNUAL OF SCIENTIFIC DISCOVERY. water. The deepest ye to be encountered between Ireland and Newfoundland is about 2,490 fathoms, and one mile being equal to 1,014 fathoms, therefore 1,014%11—11,154, and 2: -400—=4'64: the cable having thus.a strength equal to 4-04 times of its own vertical weight in the deepest water. ON CELESTIAL DYNAMICS, BY DR. J. R. MAYER. The movements of celestial bodies in an absolute vacuum would be as uniform as those of a mathematical pendulum, whereas a resisting medium pervading all space would cause the planets to move in shorter and shorter orbits, and at last to fall into the sun. Assuming such a resisting medium, these wandering celestial bodies must have on the periphery of the solar system their cradle, and in its center their grave; and however long the duration, and however great the num- ber of their revolutions may be, as many masses will on the average in a certain time arrive at the sun as formerly ina like period of time came within his sphere of attraction. All these bodies plunge with a violent impetus into their common grave. Since no cause exists without an effect, each of these cosmical masses will, like a weight falling to the earth, produce by its percussion an amount of heat pro- portional to its vis viva. From the idea of a sun whese attraction acts throughout space, of ponderable bodies scattered throughout the universe, “and of a resist- ing ether, another idea necessarily follows,—that, namely, of a con- tinual and inexhaustible generation of heat on the central body of this cosmical system. Whether such a conception be realized in our solar system,—whether in other words the wonderful and permanent evolution of light and heat be caused by the uninterrupted fall of cos- mical matter into the sun s—will now be more closely examined. The existence of matter in a primordial condition moving about in the universe, and, assumed to follow the attraction of the nearest stel- lar system, will scarcely be denied by astronomers and physicists ; for the richness of surrounding nature, as well as the aspect of the starry heavens prevents: the belief that the wide space which separates our solar system from the regions governed by the other fixed stars is a vacant solitude destitute of matter. We shall leave, however, all suppositions concerning subjects so distant from us both in time and space, and confine our attention exclusiv ely to what may be lear ned from the observation of the existing state of things. Besides the 14 known planets with their 18 satellites, a great many other oo eet masses move within the space of the planetary sys- tem of which the comets deserve to be mentioned first. Kepler's celebrated statement that ‘‘there are more comets in the heavens than fish in the open, as founded on the fact that, of all the comets belonging to our solar system, comparatively few can be seen by the ini habitants of the earth, and ihenefone the not inconsiderable number of actually observed comets obliges us, according to the rules of the calculus of probabilities, to assume the existence of “a great many more beyond the sphere of our vision. Besides planets, satellites: and comets, another class of celestial bodies exists within cur solar system. These are masses which, on account of their smallness, may be considered as cosmical atoms, and NATURAL PHILOSOPHY. 141 which Arago has appropriately called asteroids. They, like the planets and the comets, are governed by gravity, and move in elliptical orbits round the sun. When accident brings them into the immediate neighborhood of the earth, they produce the phenomena of shooting stars and fireballs. It has been shown, by repeated observation, that on a bright night twenty minutes seldom elapse without a shooting- star being visible to an observer in any situation. At certain times these meteors are observed in astonishingly great numbers; during the great American meteoric shower, which lasted nine hours, when -they were said to fall, ‘‘crowded together like snowflakes,” they were estimated as at least 240,000. On the whole, the number of asteroids which come near the earth in the space of a year must be computed to be many thousands of millions.* This, without doubt, is only a smail fraction of the number of asteroids that move round the sun, which number, according to the rules of the calculus of probabilities, ap- proaches infinity. As has been already stated, on the existence of a resisting ether it depends whether the celestial bodies, the planets, the comets, and the asteroids move at constant mean distances around the sun, or whether they are constantly approaching that central body. Scientific men do not doubt the existence of such an ether. Littrow, amongst others, expresses himself on this point as follows: ‘The assumption that the planets and comets move in an absolute vacuum can in no way be admitted. Even if the space between celestial bodies contained no other matter than that necessary for the existence of light (whether light be considered as emission of matter or the undulations of a universal ether), this alone is sufficient to alter the motion of the planets in the course of time and the arrangement of the whole sys- tem itself; the fall of all the planets and the comets into the sun and the destruction of the present state of the solar system must be the final result of this action.” A direct proof of the existence of such a resisting medium has been furnished by the academician Encke. He found that the comet named after him, which revolves round the sun in the short space of 1,207 days, shows a regular acceleration of its motion, in consequence of which the time of each revolution is shortened by about six hours. From the great density and magnitude of the planets, the shorten- ing of the diameters of their orbits proceeds, as might be expected, very slowly, and is up to the present time inappreciable. The smaller the cosmical masses are, on the contrary, other circumstances remain- ing the same, the faster they move towards the sun: it may therefore happen that in a space of time wherein the mean distance of the earth from the sun would diminish one meter, a small asteroid would travel more than 1,000 miles towards the central body. As cosmical masses stream from all sides in immense numbers towards the sun, it follows that they must become more and more crowded together as they approach thereto. The conjecture at once suggests itself that the zodiacal light, the nebulous light of vast dimensions which sur- rounds the sun, owes its origin to such closely packed asteroids. * Compare Prof. Newton’s computation of the approximate number of meteors in the August ring alone, which makes it more than 300,000,000,000,000: Sidiman’s Journal, Xxxii. 451. 142 ANNUAL OF SCIENTIFIC DISCOVERY However it may be, this much is certain, this phenomenon is caused by matter which moves according to the same laws as the planets round the sun, and it consequently follows that the whole mass which origi= nates the zodiacal light is: continually approaching the sun and falling into it. This light does not surround the sun uniformly on all sides; that is to say, “it has not the form of a sphere, but that of a thin convex lens, the greater diameter of which is in the plane of the solar equator, and ‘accordingly it has to an observer on our globe a pyramidal form. Such lenticular distribution of the masses in the universe is repeated ina remarkable manner in the disposition of the plancts and the fixed stars. From the great number of cometary masses and asteroids and the zodiacal light on the one hand, and the existence of a resisting ether on the other, it necessarily follows that ponderable matter must con- tinually be arriving on the solar surface. ‘The effect produced by these masses evidently depends on their final velocity ; and, in order to determine the latter, we shall discuss some of the elements of the theory of gravitation. The final velocity of a weight attracted by, and moving toward, a celestial body will become creater as the hight through which are weight falls increases. This velocity , however, if it be only produced by the fall, cannot exceed a certain magnitude ; it has a maximum, the value of which depends on the volume and mass of the attracting celestial body. The author then by a series of ealeula: ions, shows, that an asteroid fallg into the sun, would on arriving have a mo- tion at least as great as that of a weight falling freely to the sun from a distance great as that. of the solar. radius, or 96,000 geographical miles; and that the calorific effect of the percussion would equal to from 273 to 55,000,000 of degrees of heat. An asteroid, ther efore, by its fail into the sun, develops from 4,600 to 9,200 times as much heat as would be generat fed by the eerinise of an equal mass of coal. [ Throughout this memoir the degrees of heat are expressed 1 in the Centigrade scale. Unless stated to the contrary, the ei of length are given in geographical miles. A geographical mile=— 08 degree of latitude—1, 878 meters, andan Hnelish mile=1,;609 meters.] The Heat of the Sun.—The question why the planets move in curved orbits, one of the grandest of problems, was solved by Newton in consequence, it is believed, of his reflecting on the fall of an apple. This story is not improbable, for we are on the right track for the dis- covery of truth when once we clearly recognize “that, between great and small, vo qualitative but only a ‘quantitative difference exists,— when we resist the suggestions of an ever active imagination, and look for the same laws in the greatest as well as in the ‘smallest pro- cesses of nature. This universal range is the essence of a law of nature, and the touchstone of the correctness of human theories. We observe the fall of an apple and investigate the law which gov- erns this plienomenon; for the earth we substitute the sun, and for the apple a planet, and thus possess ourselves of the key to the me- chanics of the heavens. As the same laws prevail in the greater as well as in the smaller processes cf nature, Newton’s method may be used in solving the NATURAL PHILOSOPHY. 143 problem of the origin of the sun’s heat. We know the connection between the space “through which a body falls, the velocity, the vis viva, and the generation “of heat on the surface of this globe; if we avain substitute for the earth the sun; with a mass 350,000 greater, and for a height of a few meters celestial distances, we ob- tain a generation of heat exceeding all terrestrial measures. And since we have sufficient reason to assume the actual existence of such mechanical processes in the heavens, we find therein the only tenable explanation of the origin of the heat of the sun. The fact that the development of heat by mechanical means on the surface of our globe is, as a rule, not so great, and cannot be so ereat as the generation of the same agent by chemical means, as by combustion, follows from the laws alre sady discussed; and this fact cannot be used as an argument against the assumption of a greater development of heat by a greater expenditure of mechanical work. it has been shown that the heat generated by a weight falling from a hizht of 367 meters is only gs; part of the heat produced by the combustion of the same weight of coal ; just as small asis the amount of heat developed by a weight moving ‘with the not inconsiderable velocity of 85 meters in one second. But, according to the laws of mechanics, the effect is proportional to the square of the velocity ; if, therefore, the weight move 100 times faster, or with a velocity of 8,500 meters in one second, it will produce a greater effect than the combustion of an equal quantity of coal. It is true that so great a velocity cannot be obtained by human means; everyday experience, however, shows the development of high degrees of temperature by mechanical processes. In the com- mon flint and steel, the particles of steel which are struck off are sufficiently heated to burn in air. A few blows directed by a skill- ful blacksmith with a sledge-hammer against a piece of cold metal may raise the temperature ‘of the metal at the points of collision to redness. The new crank of a steamer, whilst being polished by friction, becomes red-hot, several backen of water being required to cool it down to its ordinary temperature. When a railroad train passes with even less than its ordinary velocity along a very sharp curve of the line, sparks are observed in consequence “of the friction against the rails. One of the grandest constructions for the produc- tion of motion by human art is the channel in which the wood was allowed to glide down from the steep and lofty sides of Mount Pila- tus into the plain below. ‘This wooden channel which was built avout thirty years ago by the engineer Rupp, was nine English miles in length; the largest trees were shot down it from the top to the bottom of the mountain in about two minutes and a half. ‘The mo- mentuin possessed by the trees on their escaping at their journey’s end from the channel was sufficiently great to bury their thicker ends in the ground to the depth of from six to eight meters. To prevent the wood getting too hot and taking fire, “water was conducted in many places into the channel. This stupendous mechanical process, when compared with cosmi- cal processes on the sun appears infinitely small. In the latter case it is the mass of the sun which attracts, and in place of the hight of Mount Pilatus we have distances of 100,000 and more miles ; the 144 ANNUAL OF SCIENTIFIC DISCOVERY. amount of heat generated by cosmical falls is therefore at least 9,000,000 times greater than in our terrestrial example. Rays of heat on passing through glass and other transparent bodies undergo partial absorption, which differs in degree, however, accord- ing to the temperature of the source from which the heat is derived. Heat radiated from sources less warm than boiling water is almost completely stopped by thin plates of glass. As the temperature of a source of heat increases, its rays pass more copiously through diather- mic bodies. A plate of glass, for example, weakens the rays of a red-hot substance, even when the latter is placed very close to it, - much more than it does those emanating at a much greater distance from a white-hot body. If the quality of the sun’s rays be examined in this respect, their diathermic energy is found to be far superior to that of all artificial sources of heat. The temperature of the focus of a concave metallic reflector in which the sun’s ight has been col- lected is only diminished from 4 to 4 by the interposition of a screen of glass. If the same experiment be made with an artificial and luminous source of heat, it is found that, though the focus be very hot when the screen is away; the interposition of the latter cuts off nearly all the heat; moreover, the focus will not recover its former temperature when reflector and screen are placed sufficiently near to the source of heat to make the focus appear brighter than it did in the former position without the glass screen. The empirical law, that the diathermic energy of heat increases with the temperature of the source from which the heat is radiated, teaches us that the sun’s surface must be much hotter than the most powerful process of combustion could render it. Other methods furnish the same conclusion. If we imagine the sun to be surrounded by a hollow sphere, it is clear that the mner surface of this sphere must receive all the heat radiated from the sun. At the distance of our globe from the sun, such a sphere would have a radius of 215 times as great, and an area 46,000 times as large, as the sun himself; those luminous and calorific rays, therefore, which meet this spherical surface at right angles retain only zg4y55 part of their original intensity. If it be further considered that our atmosphere absorbs a part of the solar rays, it is clear that the rays which reach the tropics of our earth at noonday can only possess from 34395 to gpigq of the power with which they started. These rays wien gathered from a surface of from five to six square meters, and concentrated in an area of one square centimetre, would produce about the temperature which exists on the sun, a temperature more than suflicient to vaporize platinum, rhodium, and similar metals. A correct theory of the origin of the sun’s heat must explain the cause of such enormous temperatures. This explanation can be deduced from the foregoing statement. According to Pouillet, the temperature at which bodies appear intensely white-hot is about 1,50U0° C. The heat generated by the eombustion of one kilogram of hydrogen is, as determined by Dulong, 34,500, and according: to the more recent experiments of Grassi, 34,666, units of heat. One part of hydrogen combines with eight parts of oxygen to form water ; hence one kilogram of these two gases mixed in this ratio would produce 3,850°. NATURAL PHILOSOPHY. 145 Let us now compare this heat with the amount of the same agent generated by the fall of an asteroid into the sun. Without taking into account the low specific heat of such masses when compared with that of water, we find the heat developed by the asteroid to be from 7,000 to 14,000 times greater than that of the oxyhydrogen mixture. From data like these the extraordinary diathermic energy ol the sun’s rays, the immense radiation from his surface, and the high tempera- ture in the focus of the re(lector are easily accounted for. The facts above mentioned show that unless we assume on the sun the existence of matter with unheard-of chemical properties as a deus ex machind, no chemical process could maintain the present high radi- ation of the sun; it also follows from the above results that the chem- ical nature of bodies which fall into the sun does not in the least affect our conclusions; the effect produced by the most inflammable sub- stance would not differ by jj); part from that resulting from the fall of matter possessing but feeble chemical affinities. As the brightest artificial light appears dark in comparison with the sun’s light, so the mechanical processes of the heavens throw into the shade the most powerful chemical actions. The quality of the sun’s rays, as dependent on his temperature, is of the greatest importance to mankind. If the solar heat were orig- inated by a chemical process, and amounted near its source to a tem- perature of a few thousand degrees, it would be possible for the light to reach us, whilst the greater part of the more important calorific rays would be absorbed by the higher strata of our atmosphere and then returned to the universe. In consequence of the high temperature of the sun, however, our atmosphere is highly diathermic to his rays, so that the latter reach the surface of our earth and warm it. The comparatively low tem- perature of the terrestrial surface is the cause why the heat cannot easily radiate back through the atmosphere into the universe. The atmosphere acts, therefore, like an envelop, which is easily pierced by the solar rays, but which offers considerable resistance to the radi- ant heat escaping from our earth; its action resembles that of a valve which allows a liquid to pass freely in one direction, but stops the flow in the opposite. The action of the atmosphere is of the greatest importance as regards climate and meteorological processes. It must raise the mean temperature of the earth’s suriace. After the setting of the sun,—in fact, in all places where his rays do not reach the surface, the tem- perature of the earth would soon be as low as that of the universe if the atmosphere were removed, or if it did not exist. Even the powerful solar rays in the tropics would be unable to preserve water in its liquid state. Between the great cold which would reign at all times and in ail places, and the moderate warmth which in reality exists on our globe, intermediate temperatures may be imagined; and it is easily seen that the mean temperature would decrease if the atmosphere were to become more and more rare. Such a rarefaction of a valve-like act- ing atmosphere actually takes place as we ascend higher and higher above the level of the sea, and it is accordingly and necessarily accompanied by a corresponding diminution of temperature. 0 146 ANNUAL OF SCIENTIFIC DISCOVERY. This well-known fact of the lower mean temperature of places of greater altitude has led to the strangest hypotheses. The sun’s rays were not supposed to contain all the conditions for warming a body, but to set in motion the ‘‘substance” of heat contained in the earth. This ‘‘substance” of heat, cold when at rest, was attracted by the earth, and was therefore found in greater abundance near the center of the globe. This view, it was thought, explained why the warming power of the sun was so much weaker at the top of a mountain than at the bottom, and why, in spite of his immense radiation, he retained his full powers. This belief, which especially prevails amongst imperfectly informed people, and which will scarcely succumb to correct views, is directly contradicted by the excellent experiments made by Pouillet at differ- ent altitudes with the pyrheliometer. These experiments show that, everything else being equal, the generation of heat by the solar rays is more powerful in higher altitudes than near the surface of our globe, and that consequently a portion of these rays is absorbed on their passage through the atmosphere. Why, in spite of this partial absorption, the mean temperature of low altitudes is nevertheless higher than it is in more elevated positions, is explained by the fact that the atmosphere stops to a far greater degree the caloriiic rays emanating from the earth than it does those from the sun. REMARKABLE PLUMB-LINE DEFLECTION AT COWHYTHE, SCOTLAND. The Banffshire Journal, Scotland, publishes the following statement re- specting a curious local disturbance of the plumb-line, in the vicinity of Cowhythe, now under the process of investigation by Sir Henry James, Superintendent of the British Ordnance Survey. It says :— Early during the present century the headland eastward of Portsoy on Cowhythe was visited by an officer of the Royal Engineers with the zenith sector, constructed for the Ordnance survey of this country by the celebrated Ramsden, and from the observations made with that instru- ment to determine the latitude of the trigonometrical station there, it was found that the plumb-line, instead of being vertical, was deflected north- ward of the zenith and southward of the earth’s center fully 9” of angu- lar measure. This extraordinary and unexpected result was viewed with great interest by the scientific world, especially by such as were employed by their respective governments in connection with the determination of the figure of the earth; and, by way of verification, a party of the same corps, some 16 years back, furnished with a new zenith sector, designed by the present Astronomer Royal, and constructed by Troughton and Sims, visited the same spot. More observations, and to a greater number of stars, resulted in confirming the first or earlier determination, and here the matter rested, merely as a subject of occasional wonder to those con- cerned, till recently the Russian Engineers, in prosecution of their national survey, came upon a similar anomaly in the neighborhood of their ancient capital, Moscow. On tracing it to its limit, which they have done ina public-spirited and most creditable manner, they concluded that there is a vacuum, or a comparative vacuum, of a great many square miles in extent, under the earth’s surface in that country. To give some idea of the reasoning which leads to so startling a conclusion, the reader may conceive NATURAL PHILOSOPHY. 147 a wide, deep pit with a plummet suspended from its mouth at the earth’s surface. The plumb-line will be vertical only when in the center of the pit (er shaft, it is called in connection with mines), because it will there be equally attracted in every direction, If carried round the side of the pit, the line will be so deflected from the vertical as to cause all the lines, if produced upwards, to meet in a point above the earth’s surface ; and such are the phenomena discovered by the geodetical engineers of Russia. The pit, it is true, is closed at its mouth, and no plumb-line can be let down into it, but the spirit-level, being always at right angles to the piumb-line, discloses the fact as clearly to the mind as the open pit would to the eye. Now, whether the Cowhythe deflection is to be accounted for by a compar- ative vacuum on the north under the Moray Firth, or by some unknown mass of extraordinary density on the south, or partly by both, is the prob- lem to be solved, and, doubtless, it will ultimately be solved by the staff of astronomical observers and computers under Sir Henry James. ‘The gen- eral result of the investigations thus far, may be briefly stated to be a diminution of the deflection as the observers proceed southwards, but how far it may extend is of course at preseut unknown. THE BAROMETER AS AN INDICATOR OF THE EARTH’S ROTATION. Mr. Pliny Earle Chase, in a paper recently read before the Ameri- ean Philosophical Society—On the Barometer as an Indicator of the Earth’s Rotation and the Sun’s Distance; sets forth the following views: The existence of daily barometric tides has been known for more than 150 years, but their cause is still a matter of dispute. It is evident that they cannot be accounted for by variations of tempera- ture, for Ist, their regularity is not perceived until all the known effects of temperature have been eliminated; 2d, they occur in all climates, and at all seasons; 3d, opposite effects are produced at dif- ferent times, under the same average temperature. ‘Thus at St. Hel- ena, the mean of three years’ hourly observation gives the following average barometric heights :— From 0° to 12" 28:2801 in. From 18° to 6° 28:2838 in. © 19> to 0° 28-2761 “6 to18" 28-2784 « The upper lines evidently embrace the coolest parts of the day, and the lower ines the warmest. Dividing the day in the first method, the barometer is highest when the thermometer is highest; but in the second division the high barometer prevails during the coolest half of the day. On account of the combined effects of the earth’s rotation and revo- lution, each particle of air has a velocity in the direction of its orbit, yarying at the equator from about 65,000 miles per hour, at noon, to 67,000 miles per hour, at midnight. The force of rotation may be readily compared with that of gravity by observing the effects pro- duced by each in 24 hours, the interval that elapses between two suc- cessive returns of any point to the same relative position with the sun. The force of rotation producing a daily motion of 24,895 miles, and the force of terrestrial gravity a motion of 22,738,900 miles, the ratio of the former to the latter is 3248%5,,, or 00109. This ratio repre- sents the proportionate elevation or depression of the barometer above or below its mean height that should be caused by the earth’s rotation, and it corresponds very nearly with the actual disturbance at stations near the equator. 148 ANNUAL OF SCIENTIFIC DISCOVERY. From Oh. to 6h. the air has a forward motion greater than that of the earth, so that it tends to fly away; its pressure is therefore dimin- ished, and the mercury falls. From 6h..to 12h. the earth’s motion is greatest ; it therefore. presses against the lagging air, and the barom- eter rises. From 12h. to 18h. the earth moves away from the air, and the barometer falls; while from 18h. to 24h. the increasing velocity of the air urges it against the earth, and the barometer rises. From a relation of these forces to the power of gravitation, &e. Mr. Chase calculates what should be the daily changes in the hight of the barometer, and the results are found to correspond very closely with the changes in the barometer at St. Helena, the point nearest the equator where a long series of barometric observations have been made. J*rom these changes in the barometric pressure he also com- putes the distance of the sun from the earth, and obtains results agree- ing pretty nearly with those obtained by the most approved of other methods. His conclusions also suggest that the revolution of the sun around the great Central Sun must also cause barometric fluctuations that may possibly be measured by delicate instruments and long and patient observation. The Toricellian column may thus become a valuable auxiliary in verifying or rectifying our estimates of the dis- tances and masses of the principal heavenly bodies. POPULAR EXPLANATION OF THE THEORY OF THE TIDES. Mr. Williim Dennis, of Philadelphia, contributes to Silliman’s Journal, March, 1864, an interesting article on the best method of presenting in a popular form the “ Theory of the Tides ;” from which we make the following extracts :— After alluding to the difficulty which many persons experience, in understanding how the tides are produced, the author says: Ifa learner be told that the waters of the ocean are ruised by the moon’s attraction, his first idea, in many cases, will be that they are lifted up by main strength, as it were, the force of gravity being overcome, and haying nowhere observed any similar effcvct of the moon’s attraction, he cannot conceive how this can be. Nor will it tend in any degree to lessen his perplexity if he shall see it stated (as he may) that, according to Newton’s calculations, the disturbing power of the moon’s attraction on the surface of the earth is less than a ten millionth part of the force of gravity, and that of the sun’s attraction not even half as great as it. It is therefore important to show, by a preliminary explanation, that the waters of the ocean, in their general figure and outline, are in a stite of perfect equilibrium or perfectly balanced, s» that, in view of tiis. and of their vast extent and perfect freedom of motion, they m ry be compared to a scale-beam in perfect equipoise, suspended in tiie most delice te manner, and several thousand miles in length. To omit this would be much the same as if one should state, in proof and illv.tration of the attraction of gravitation, that a weight or ball at the side of a mountain had been observed (referring to the Schehallien experiment) to be drawn towards the mountain by its attraction, leaving the learner to suppose that the weight wis pliced on a table or other level surfuce instead of being suspended by a long thre:d or wire. In explaining this condition of equilibrium the most obvious course NATURAL PHILOSOPHY. 149 will be to refer to mere hydrostatic equilibrium, in which any portion of these waters may be regarded as exactly balanced by any other con- tiguous portion, each being maintained at its level by the pressure of the other which supports it; consequently, if this pressure, be in the case of either portion, lessened or increased, in the least degree, that is to say, if the force of gravity, to which this pressure is dus, be in any degree counteracted or added to by any other force in one of these portions and not in the other, the lighter portion will immediately give way and be buoyed up by the heavier, which will of course simultaneously sink: and this would be an explanation sufficient for the purpose. But as this stitement, though true, is not the whole truth, it may be weil to go a step further. ‘lhe waters of the ocean do not maintain their general figure and outline under the influence of gravity alone. On the contrary, it is well known that, by the centrifugal force generated by the earth’s rotation on its axis, they are kept at a higher level or greater distance from the center on other parts of the globe than at the poles, this eleva- tion amounting at the equator where it is greatest to about 13 miles. They are therefore exactly suspended or poised between these two forces, namely, the force of gravity and the centrifugal force just mentioned, and any other force that should in the least degree add to or counteract the influence of either of these forces would at once cause a change in the figure of these waters. While therefore it is properly the hydrostatic equilibrium existing between the different portions of the waters them- selves that is disturbed by the action of the forces that produce the tides, the statement just made may serve to show more clearly how far these waters are, in their normal condition, from lying as a dead weight in the depressions of the e:rth’s surface that contain them. Again, it is stated in a familiar way, that the tide on the side of the earth towards the moon is owing to the waters there being attracted by it more than the mass of the earth because they are nearer, while the tide raised at the same time on the opposite side of the earth results from the earth being drawn away from the waters there because they are more remote than the mass of the earth and are thus “ left behind,” or “left heaped up;” and then we are told that, at full moon, when the attractions of the sun and moon are opposite in direction, they conspire to produce spring tides in the same manner as at new moon when their attractions coincide in direction. Now, as it is not easy to see howa body can be drawn away so as to leave any thing behind in two opposite directions at the same time, these stitements appear quite inconsistent and are well calculated to confuse and perplex. It is therefore important and indeed indispensable to the communication of an intelligible view of this phenomenon to explain, as be ore remarked, the conditions and circumstances, or, to express it more definitely, the relations and de- pendences existing among the bodies concerned in it: a course at once so natural and so needful that it seems remarkable that it should not have been more generally and more fully adopted. As the earth is held to its curved path around the sun by the attrac- tion of that body acting in opposition to the centrifugal force generated by its rapid motion, in the same manner that a heavy ball or weight attached to the end of a cord and whirled around the head is held or restrained by the cord, we may regard it as suspended between these two forces, and if a ball be merely suspended by a cord it will be a fair 13* 150 ANNUAL OF SCIENTIFIC DISCOVERY. illustration of its condition; the force of gravity or weight of the ball standing in place of the centrifugal force in the case of the earth, and the tension of the cord representing the restraining force of the sun’s attraction which at each instant holds the earth to the place in its orbit which it occupies. ut as this attraction of the sun diminishes rapidly with an increase of distance it is plain that it cannot hold ald paris of the earth alike or equally, the nearest part being about 8,000 mules less distant than the most remote, while of course it holds tie whole as a mass as it would hold it were it at the mean distance of ail the parts, that is, at the distance of the center. Consequently on the nearest part or side towards the sun the attractive force being greater than the mean, there will be a small excess over what is sufficient to hold this part to its place in the orbit, and this excess acting upon the surface waters there in opposition to the force of gravity renders them specifically lighter and the exact equilibrium before described is mmediately dis- turbed: these waters will therefore rise somewhat while those that are so situated as to be unafiected by this disturbing influence will sink simply from the giving way of those which having become lighter yield to their superior pressure. Again on the opposite side of the earth or that most remote from the sun, the attractive or restraining force will be less than the mean and therefore not quite equal to the centrifugal force, and here accordingly there will be an excess of this latter force: but on this side it is this centrifugal force that acts in a direction oppo- site to that of gravity, and this excess of it will consequently disturb the equilibrium of the surface waters here in precisely the same manner as in the other case. Such is a statement of the general principle upon which the attraction of the sun (or of the moon) tends to produce a tidal elevation on two opposite sides of the earth, with intermediate depressions. ON A NEW FORMULA FOR CALCULATING THE INITIAL PRESSURE OF STEAM. In a communication on the above subject, made to the British Association, 1864, by Mr. R. A. Peacock, the author stated that some years ago he had occasion to attempt to calculate the probable pres- sure of steam at the highest known temperatures, and found, amongst other things, that between the pressures of 20 lb. per square inch and 800 lb. to the square inch, the latter being the highest pressure to which trustwortl:y experiments had been carried, the law of increase was, approximately: ‘that the temperature of high-pressure steam of say 25 lb. to the square inch and upwards, increases as the 4$ root of the pressure; and that, conversely, the pressure of the steam of say 25 ib. to the square inch and upwards, increases as the 44 power ot the temperature. At lower pressures than about Zo Ib. per square inch, a difierent law prevails. As it is necessary to verily the new formula by comparison with some well-known formule and experi- ments, the author has attempted to do so m a very voluminous table, and graphically in a very carejuily-executed diagram. What is to be gathered from these is, that the new formula agrees with Dr. Fair- bairn’s experiments, from about 40 lb. to 60 lb., and very nearly with Regnault’s, between 220 lb. and 486 lb. NATURAL PHILOSOPHY. 151 CURIOUS APPLICATION OF AIR EXPANSION THROUGH HEAT. It is well known that the air confined under glass, if it receive the direct rays of the sun, will become much heated, far beyond the tem- perature of the rays, owing to the action of the glass in absorbing these rays and conveying tue absorbed heat to the air within. Prof. Mouchot, of Alencon, has made the following application of the heat thus acquired. He takes a bell of silver, very thin and covered with lampblack, and places over it two bells of glass, and exposes the whole to the rays of the sun. Two curved tubes, furnished with stopeocks, pass under the black bell, one of them to supply water when it is required, the other to give exit to the water ; the latter ter- minating outside in an ordinary jet d’eau orifice. Being now exposed to the solar rays,—whose heat is transformed into non-luininous heat in its passage through the walls of the bells, an effect that goes on accumulating without cessation,—the air situated above the water dilates, and by its pressure causes a jet to rise, attaming sometimes in Mouchot’s trials a hight of nearly 33 feet. When the water is ex- hausted, a screen placed before the sun will cool the interior and cause the water to return, or a new supply may be introduced through the supply-pipe. Many times the shade thrown over the apparatus by spec- tators caused it to stop, much to their surprise. —Les dondes, Sept. 22. EFFECT OF THE SUN ON SOIL AND AT, The relative heating of the soil aad air by the solar rays on a high mountain and in a plam has been examined by the distinguished trav- eler, M. Ch. Marteus, who has reported on the subject to the Acad- emy of Sciences at Paris. We give a few notes: A solar ray, it is said, falling on an elevated summit, should be hotter than one which, after traversing the lower and denser strata of the atmosphere, de- scends into a plain, since these strata necessarily absorb a notable quantity of the heat of the ray. All travelers who have ascended high mountains have been surprised at the extraordinary heat of the sun and the soil compared with the temperature of the air in the shade, or with that of the soil during the night. The observations of MM. Peltier, Gravais, and Marteus (two series, 125 in the whole), made on the Fauthorn, Switzerland, between 6 A. M. and 6 P. M., continued indifferently in fine and bad weather, give, nevertheless, for the mean temperature of the soil during the day, 11:75 per cent, that of the air being only 5°50. It became evident that heating of the soil during the day was twice that of the air; but the observers were not aware what had been the relative heating of the earth and air in the plain below during the same period. ‘To obtain this knowledge, M. Mar- teus selected the summit of the Pic du Midi, in the Pyrenees, and a garden in the plain at Bagnéres. By his observations, which began on Sept. 4%, 1864, he obtained the following results: The mean of the temperature of the air in the shade, deduced from 20 observations at Bagnéres, was 22°3; from the same on the Pic du Midi, 10:1 only. The mean temperature of the surface of the soil at Bagnercs was 56:1; on the Pic, 33°8. ‘The mean excess of the temperature of the soil over that of the air at the two stations is then as 10 : 171,—nearly double that on the mountain. ‘These experiments put out of doubt the great- er calorific power of the sun upon the mountain than upon the plain, 152 ANNUAL OF SCIENTIFIC DISCOVERY. A NEW THERMOGRAPH. M. Marcy has addressed to the French Academy the following description of an instrument for marking small variations of tempera- ture: 1. The first part of this thermograph consists of a copper tube a meter in length, the interior diameter of which is capillary, not being more than } of a millimeter. It is open at one end, and soldered to a hollow copper ball at the other end. 2. The second part of the apparatus consists of a wheel resting upon knife-edges, like those of a pair of scales, whereby a very delicate oscillation may be imparted to it. The axle of the wheel carries a long vertical needle, marking the degrees on a circular scale. ‘To the circumference of the wheel is fixed a glass tube six millimeters in diameter, and bent in conformity to the curvature of the wheel, and so situated that the middle of the tube lies vertically underneath the needle when the wheel is at rest. One of its extremities is hermetically closed, while the other is open. Now, if a little mercury be poured into this tube it will settle at the lowest point, and the interior of the tube will thus be divided into two chambers, one closed and with air confined in it, the other open. 3. Now introduce the copper tube into the glass one, giving it of course the same curvature, and so that its extremity may pass through the mercury, thus establishing a communication between the hollow copper ball and the confined chambers, and the apparatus, with a few accessory appliances, will be complete. The end of the copper tube dipping into the mercury should be varnished to prevent its being attacked by the latter metal; or better still, the end might be made of platinum. 4. To use this apparatus, put your hand to the copper ball; the warmth thus imparted to it will dilate the air it contains, and drive part of it into the confined chamber; the mercury will therefore recede, and thereby make the wheel turn round its center of gravity ; the very small are thus described will be revealed by the needle, the difference of its present position with its previous one when at rest. If, on the contrary, the copper ball be cooled, by water, for instance, the air inside will be contracted, a portion of the air of the confined chamber will rush in, and the mercury will be driven forward, the needle turning in the inverse direction. By means of this experiment very delicate physiological experiments on animal heat may be con- ducted. HEAT AND FORCE. Whenever friction is overcome, heat is produced; and the amount of heat so produced is the exact measure of the force extended in overcoming the friction. Prof. Tyndall, speaking upon the subject of ‘* eat considered as a Mode of Motion,” says: ‘‘We usually put oil upon the surface of a hone; we grease the saw, and are careful to lubricate the axles of our railway carriages. What are we really doing in these cases? Let us get general notions first ; we shall come to particulars afterwards. It is the object of the railway engineer to urge his train boldly from one place to another. He wishes to apply the force of his steam or his furnace, which gives tension to the steam to this particular purpose. It is not his interest to allow any portion of that force to be converted into another form of force which would NATURAL PHILOSOPHY. 153 not further the attainment of his object. He does not want his axies heated, and thence he avoids as much as possible expending his power in heating them. In fact he has obtained his force from heat, and it is not his object to reconvert the force thus obtained into its primitive form. For by every degree of temperature generated by the friction of his axle, a deiinite amount would be withdrawn from the urging force of his engine. ‘There is no force lost absolutely. Could we gather up all the heat generated by the friction, and could we apply it mechanically, we should by it be able to impart to the train the precise amount of speed which it lost by the friction. ‘Thus every one of those railway porters whom you see moving about with his can of ycilow grease, and opening the little boxes which surround the car- jiage axles, is, without knowing it, illustrating a principle which forms the very solder of nature. In so doing he is unconsciously affirming both the convertibility and the indestructibility of force. He is prac- tically asserting that mechanical energy may be converted into heat, and that whem so converted it cannot still exist as mechanical energy, but that for every degree of heat developed, a strict and proportional equivalent of locomotive force of the engine disappears. A station is approached say at the rate of JO or 40 miles an hour; the brake is applied, and smoke and sparks issue trom the wheel on which it presses. The train is brought to rest; how? Simply by converting the entire moving force’ wuich it possessed at the moment the brake was applied, into heat.” THE COOLING OF THE EARTH AND ITS CONSEQUENCES, BY DR. J. KR. MAYER. If we assume that our globe was once in an incandescent state (as is now generally adinitted), it must have lost heat at first at a ver rapid rate; gradually this process became slower; and although it has nov yet entirely ceased, the rate of cooling must have diminished to a comparatively small magnitude. ‘Two phenomena are caused by the cooling of the earth, which on account of their common origm are intimately related. The de- crease of temperature, and consequent contraction of the earth’s crust, must have caused frequent disturbances and revolutions on its suriace, accompanied by the ejection of molten masses and the formation of protuberances: on the other hand, according to the laws of mechan- ics, the velocity of rotation must have increased with tie diminution of the volume of the sphere, or in otier words, the cooling of the earth must have shortcned ihe length of tlie day. As the intensity of such disturbance and the velocity of rotation are closely connected, it is ciecar that the youth of our planet must have been characterized by continual violent transformations of its crust anda perceptible accelera- tion of the velocity of its axial rotation; while in the present time the metamorphoses of its suriace are much slower, and the acceleration of its axial revolution diminished to a very small amount. if we imagine the times when the Alps, the chain of the Andes, and the Peak of Teneriffe were upheaved from the deep, and compare with such changes the earthquakes and volcanic eruptions of historic times, we perceive in these modern transformations but weak inages of t..e analogous processes of bygone ages. 154 ANNUAL OF SCIENTIFIC DISCOVERY. While we are surrounded on every side by the monuments of violent volcanic convulsions, we possess no record of the velocity of the axial rotation of our planet in antediluvian times. It is of the’ greatest im- portance that we should have an exact knowled ge of a change in this velocity, or in the length of the day during historic times. The inves- tigation of this su bject by the ereat Laplace forms a bright monument in the department of exact science. These calculations are essentially conducted in the following man- ner: In the first place, the time between two eclipses of the sun, wide- ly apart from each other, is as accurately as possible expressed in days, and from this the ratio of the time of the earth’s rotation to th mean time of the moon’s revolution determined. If, now, the shee vations of ancient astronomers be compared with those of our present time, the least alteration in the absolute length of a day may be detect- ed by achange in this ratio, or in a disturbance in the lunar revolution. The most perfect agreement of ancient records on the movemen’s of the moon and the planets, on the eclipses of the sun, &e. revealed to Laplace the remarkable fact that, i the course of 25 oe the time in which our earth revolves on its axis has not altered 315 part of a sex- agesimal second ; and the length of a day therefore may be considered to have been bodaiade during historic times. This result, as impor- tant as it was convenient for astronomy, was nev ertheless of a nature to create some difliculties for the physicist. With apparently good reason it was concluded that, if the velocity of rotation had remained constant, the volume of the earth could have undergone no change. The earth completes one revolution on its axis in 86, ,400 sidereal sec onds; it consequently oo if this time has not altered iene Bs 500 years to the extent of <1; of a second, or z35 TVTTOT part of a day, that during this long space of time the radius of the earth also cannot have altered more than this fraction of its length. The earth’s radius measures 6,569,800 meters, and ther efore its ‘length ought not to have diminished more than 15 centimeters in 25 centuries. The diminution in volume, as a result of the cooling-process, is however, closely connected with the changes on the earth’s surface. When we consider that gipeeb a day passes without the occurrence of an earthquake or shock in one place or another, and that of the 300 active volcanos some are always in action, it would appear that such a lively reaction of the interior of the earth against the crust is incompatible with the constancy of its volume. This apparent discrepancy between Cordier’s theory of’ the connection between the cooling of the earth and Be reaction of the interior or the exterior parts, ‘and Laplace’s calculation showing the constancy of the leneth of the day, a calculation which is undoubtedly corre ct, has induced most scientific men to abandon Cordier’s theory, and thus to deprive themselves of any tenable explanati on of volcanic activity. The continued cooling of the earth cannot be denied, for it takes place according to the laws of nature ; in this respect the earth cannot comport itself “differently from any other mass, however small it be. In spite of the heat which it receives from the sun, the earth will have a tendency to cool so long as the temperature of its interior is higher than the mean temperature of its surface. Between the tropics. the mean temperature produced by the sun is about 28°, and the sun NATURAL PHILOSOPHY. 155 therefore is as little able to stop the cooling tendency of the earth as the moderate warmth of the air can prevent the cooling of a red-hot ball suspended in aroom, Many phenomena—for instanc e, the melting of the glaciers near the bed on which they rest—show the wninter- rupted emission of heat from the interior toward the exterior of the earth; and the question is, Has the earth in 25 centuries actually lost no more heat than that which is requisite to shorten a radius of more than 6,000,000 of meters only 15 centimeters ? In answering this question, three points enter into our calculation: 1, the absolute amount of heat lost by the earth in a certain time, say one day; 2, the earth’s capacity for heat; and 3, the coeflicient of expansion of the mass of the earth. As none of these quantities can be determined by direct measurements, we are obliged to content ourselves with probable estimates ; these estimates will car ry the more weight the less they are formed in favor of some preconceived opinion. Considering what is known about the expansion and contraction of solids and liquids by heat and cold, we arrive at the conclusion that for a diminution of 1° in Lonaperatanes the linear contraction of the earth cannot well be less than yg 9's¢¢. part, a number which we all the more readily adopt because it has been used by Laplace, Arago, and others. If we compare the capacity for heat of all solid and liquid bedies which have been examined, we find that, both as regards volume and weight, the capacity of water is the greatest. Even the gases come under this rule; hydrogen, however, forms an exception, it having the greatest capacity for heat of all bodies when compared with an equal weight of water. In order not to take the capacity for heat of the mass of the earth too small, we shall consider it to be equal to that of its volume of water, which, when calculated for equal weights, amounts to 0° 184. If we accept Laplace’s result, that the length of a day has remained constant during the last 2,500 years, and conclude that the earth’s radius has not diminished 1$ decimeter m consequence of cooling, we are obliged to assume, according to the premises stated, that the mean temper rature of our planet cannot have decreased ah ° in the same period of time. ‘The volume ofthe earth amounts to 2 24650, 000,- O09 of cubie miles. uelismosswwohiolinsa7O Gas, absorption of, by porcelain and “ET hey Atcha 1 ia 5 cf > COMPLESSION Oli cids heise! 0) ehslienteco Gelatin, NEwalse fOr. s. « 10:60) evewttd Geographical explorations, recent . 342 INDEX. Geology, curious factsinm. . . « . « 10 negative evidencein .. . 308 ee recent progress of. . ... 268 Geologic evidence, minute. . .. . 308 Geological discovery, interesting. . 310 Geological opinions, changes in. . 282 ae summary . cree ege © « GUS Geysers Cf leeland => 5.) semiomeamer Ghost, real, how to detect ... . . 327 Ghosts , photographie RA pooh ap Se Glacial epoch, antiquity of. . . 281, 292 * CHUSE Of 6 =, meine C10; 501 Gold in GHG SUE cs) oleusr es «) teneue toto “ of California, geological age of, 299 Gold, extraction of from auriferous jute ee aes eee Granite, formation: Off.) <: stisreus neriole Graphite, Origin Of0 eu erotaslolie een ie, Great Britain, recent geological Changes Il. sone aetieme We eae sare AO: Gum, mew, adhesives 5 = ous teneae se, 45 Gunnery, curious phenomena in . . 190 se new principle in ..... 99 Gun cotton, electrical properties of. 121 st English views respect- INg «+ e220 ° 2.910 French views respecting, 102 Gun-metal mew. :.) 10) sysiite. ee, o2 sy OD Guns, large Grials OLS ce eniowinise el Ob gel OY ‘¢ “new method of rifling . . .. 102 EO U8: (ALINOL, au onts suse dedenianio wll O “cc “ce Gunpowder, illustrations of the force OL «, © ©, 0. .53.0)..2) Os ae) alae ene Biepie Health, effects of alcohol and tobacco QS 6 SiiGesnoest oes - Hearing, inequality in the organs of 192 Heat, atiecting density of minerals. 161 ee and force oo. sun es eae des Se" “CONGUCHION AOL, Sie te de cee eet OO “¢ mechanical development of . 143 ME CO) EA HIST Seg nnat a a aes ele “ vibrations, nature of. ... . 164 Herschel, on standards of measure- MEM «16.5; 6 @.lstcmioggen Menon MEL Huggins, discoveries in spectrum analysis .. . Human fossils from Gibraltar. . - 287 Hurricane, greatest on record . .. 198 Hydrophobia, treatment of by elec- ETICILY c, @ 1s eNeEemRer oo ae et co Tce, artificial manufacture of. . .. 65 ‘¢ prismatic formation ofin glaciers 163 Ice-caves BY APS, pr « Wethewiedin ne” (seine Katine iiaaalik Rdeorraphye c _«, .=:eseeiet eure deena ens Ol Tilumination, artificial. ...... 175 Indium, M@w metal <\. cus ue.ke; sus cpcole Infusorial deposits, new use of. . . 72 Iron, absorption of carbon by... 46 “¢ and gteel, microscopic structure OE eos Nia lose ree aap ms lab eel cc", LDOLLETS; \COLLOSION FOL soreaet eek ao Tron- bars, immense, rolling of. . . 103 cast, tensile strength is ly “ reduction of by super-heated SLOAN GS: ceeie! ladies ealenielaads sine: (t| MOXADLUILY, (Ol cise, ce seu bin a suemenence ‘* Jengthened by magnetism . . ‘¢ magnetized, crackle of .... ‘* targets, percussion of shot on. 100 Metamorphism of rocks . . INDEX. 3538 Iron, permeability of. . . - . + - « 220! Metals, coating of . ...... 51 ‘© plate, enormous ...:. +... 44 or HG Wiis, liste uatlan pila. 215 “¢ plates, resistance of to shot. . &§ : optical properties of . . * prokediae of from oxydation. 49 “f preservationof. .... 48 Iron-clad, latest British 04 “cc oh vessels, different contrast- Gea te ior eee Re vessels in action. . ... &8 “ce PLO TORS cei erie) on aac te. is, 6 Ls Te) .e) OS Iron-girders, strength of. ..... 44 “ Jronsides” frigate, American .. 94 ICOny., RECMICIAI yess sas isi wie oer tO Japan, agricultureof.... - 61 Jupiter, supposed 5th satellite of. . 322 Lake habitations, QNCIENE os 2.0) «200 Language, universal. .......- 8l Languages, mastery of. ...... 194 of BUUGVAOU is deiccl tom ete choi Ang Larynx of the white man and the FEST e < isiietic) ois, «1s 01 6 s10 OOO Laurentian rocks, fossilsin .. . . 304 Lead, protection of water pipes from, 245 Lea’s cleaning solution. . ..... 145 Lithium, use and distribution of. . 216 Light, artificial, conditions of. . . 175 2” effects ot’ the atmosphere on, 208 s¢ measurement of the chemical CULO MOM Menletts 3.6. Us: Ueuislse) ie polarized, new use of . . . - 209 Lights, colored, applied to sculpture, intensity OLEVEIOUSi. wet le ex endl “c Liquids, cohesion, figures of. . . . 240 Liquids, size of adropof ..... 121 iithorraph, lareeve, fc <6 9 3.6 + 48 Locomotion, ourfuture. ...... 38 Longevity and open-air exercise. . 328 Loom, improved. . .- + «+«.«.«« 46 Machinery, vs. man-power .... 23 Magnesium, observations on the STEVET ETE Ase Sake een chia tach irae) Wd Magnet, electro, great .....-.-. 131 "new formof....... + 202 Magnetic action, illustrations of . . 124 disturbances, curious. . . 129 LC needle, new form Ove! ete oO f storms, analysis of. . . . 129 Magnetism, new researches into the laws of 128 of iron and steel turnings, 201 TESIGUS! 6 os erie) sie 6) bl: Magnitudes, minute .......-s. 18 Man, early migrations of. .... . 342 “« fixity of the typesof .... 3483 «“ new facts concerning the anti- GHITY Ofielepics, avn sliel wr 'et © = 203 Manna inthe desert ......«--. 313 Manures, industry of. .....e+-+- 59 Marriages, effects of consanguineous, 328 Masts, iron Matter, construction of. . ..... 112 fe transitions of 113 Measure, French and English stand- HAE scale e eee 17 Meats, preservation of . . . . 52, 54, 55 Mechanics, animal. ....<«e.2.- 12 Men, hairy, of Yesso. « « + « « © ¢ act of «es OO. Bite Rise 28) aie elas ‘@ Metamorphosis, the universal MICTCOLIC NAIM 0.6 2 2m) « Meteorites, meteorological structure, 3 Micrographical machine... .+. Microscopes, improvementsin ... Microscopie structure of iron and SECC] ar aleioh ai sauisyasiaoes sine. fey, catelae Minerals, coloring matterin. .. . 247 . ° * . . > \) _ ; = ao os variation in density by DEGtiee ce cette ol wast cemenelol MIST; TOPMALLON-OL 1 came sleienies eae ee Moa of New Zealand. ....... 307 Monitors, iron-cladsin service ... 92 Moon and the earth, effects of colli- SION OL. wu lb ia sincm cane aie nama *¢ does it revolve?. ..... . 190 ‘¢ ew views respecting. .... 221 proof of no atmosphere in. . 267 Speen analysis of the light (0) . . ° e . . ° temperature and climate of. . 338 Mortality and ignorance, relation between .......-..-+. ~ 320 Mountains, highest in the United SLATES) < lonses clover iceiciia Len emremenrlO Mural decorations, % ost 5, cus. el aul eo Music, as a physical and moral agent, 195 Musk-ox, fossil . Cr ee ee 2 | 311 Naval ordnance, report of Bureau of, Nebular hypothesis <<: 2. « «1+ ox Nebul, discoveries in respect to. . 257 ty DOW) on os ie\lceCieinesta Sotto hal colts ef PIANC LANs eeu. el eskelisiseuian= Nebulous matter, invisibility of .. Nerve structure, researches on. . . Nitrogen-protoxyd, liquefaction of. Novelties, industrial ........ 7 Oi SeottoOneseeai an eiece. settler Oils, essential, preparations of. . Opacity and transparency... . Ordinance, Ames’s wrought iron . ce heavy, endurance of. . 104 a: monster . . . « « « 106, 107 Orion, a. constitution of ..... . 254 cL nebule in o's, 16 donors ToUL Organic bodies, discrimination of by . e ° e ° i SI ie a) optical properties . ..... . 165. Osteological collections ..... . 328 Oxygen, cheap production of. . . . 222 IMNMAWOM TOL 0. oi ,est~ ue Lee Oysters, artificial cultivation of. .. 7: Ozone and the atmosphere. . . . . 223 ‘¢ influence of, on vegetation. . 223 s¢ mew source Of . 0» = « « « 220 a CEUs LOM cule eo. aie Ramune on ee oleae Pearl oysters, mortality among. . . 326 Petrifaction, artificial . . ...-.. 236 Petroleum, gE QUOC nce es pebkeeee S s impervious barrels for . 77 4s rocks in which found. . 296 ae volatile constituents of. 244 Phantom images. . ..+«-e-e-eee 116 354 PhenicMcid wUSeiOtie|. wees Mele t eee oS Phosphorus, migrations of. . . . . 235 Photographie g BHOSUS ei E Mellel =e 160 printing, improvement dette aed ae chs Se OS? Photographing natural colors. . . 182 Photos sraphs, ‘diamond cameo” . 189 elecericalin. sie hs, 120 ee of the electric spark. 201 186 Photography and Physiology. ... EC applied to topography, 211 185 “e ce improvementsin... W othly’s improvements in Photometry, discovery in. .... 176 PHOLO=-SCUlpIUITE: 7). Soke hee leet .c Ae?) 1Ge Physiological errors in astronomi- cal. observations) 5 «242. 2... 2°. 169 Pianos, self-instructing scale for. . 76 Pictures, Pettenkofer’s process of restoring Pipes, water, action of on flow. .. Planetary law, new... ...«e . . . . . . . . . 8 pe es is \2. 2 (9 in 9 @ite Planets mew, 106 1862 7 =) 6) 2 ensi Soe Plants, green coloring matter of. . 313 Plumb-line deviation, remarkable. 146 Pneumatic despatch,improved... 42 ne Pal WV is teal hen te 40 Poisoning, vegetable, use of char- Coal Inceset = - 246 Poisons, detection of. by dialy sis . » 247 Pole, North, new expedition to. . . 340 Potash, the available sources of .. 7: Probe, Nelaton’s . sue Koeiamenle cols Projectiles, measurement of the ve- NOCHE Ofire meisaie ce bol ecsSave ne SOTIy Pump, common, simplification of . 209 Pyroxiline paper, electrical proper- fete ce cot ety, , 199 Quicklime, new use for ...... 69 Race, aboriginal, extinction of an . 326 Radiations, luminous and obscure . 178 Railway car-trucks, improved ... 43 ee pneumatic Speke fowe 6. qoute) JO MampOws ATUMNCAl sj. 26 ease ofc ae lz 2 Rocks, breaking DYpHECy ete. 6) oe 100 tubber, vulcanized, waste of ... 70 Rust, prevention ofoniron .... 50 Salmon, propagation of ...... 317 Smee shifting, settlementof ... 66 Dap, Maples flowsOh, cnc co be ic 0.16 10 (04 Sculpture, by colored light. .... 172 es through photography . - 183 Sea, absorption of terrestrial heat DV Aah elrouis aa w_ sienas sontemiontel oui zs Sea water, action of on iron and COPPEr. mins «cae, eae occultation of the spectrum OVER Oa) OhOn de co IS On oy. er shooting, what we know of . 334 Statistics; curious vital ~ (02. 2021327 Statues, chemical preservation of . 246 Steam, condensation of in cylinders, 27 expansive working of 26 new formula for calculating “ “ec “ “ “ce Ste, Ve tells Weil oe OOO “c cs cc Pressure’ol.) cy ce eLseeeO ‘© new mechanical action of . 38 ‘¢ superheated, production of ateelipy.o. "remo wes Rae Steam boilers, improvementsin .. 31 ‘¢ engine, economy Ole te \aikengo Lat Steel, Cazanave’ Sprocess ..... 45 «« improvements in the manufac- TREO 5 Gioia gia 6 Oo) Geae Gs €se SIRIUPS) |. 45 Zapeeracteme rest es culate Moka Stereoscope without lenses’. . 0.473 Stereotrope, ‘The se. wie ts. us pe tomemales irae CASes cae vse stole = ae Sugar, m maple, manufactured in the United States ...... 63 ‘¢ produced in animals by cold, 323 Sun, central, of the universe. ... 148 chemical action of rays of .. 181 *° effects of on soiland air ... 151 eu be Ges So Eos. sil “. Heat of>. 4d) Bile ee sc physical aspect of: ... . « « . 179 ‘“* theory of the constitution of . 337 Sun’s heat upon the earth, numeri- cal value of Surfaces, flat... .eeeeceee ofette wie tele sl Geter et DO 22 INDEX, . Targets of wool, effects of shot on. Telegraph, a metcorological indica- 101 Appt? ter Sv TOMMraeE Yo “e ATIONCIC. «se soe creke waloe Telegraphic construction, progress Se erie e sta eee Low 0) Telegraphing by electro-m: ignetism, 135 Tellurium, new source of 216 ‘ Temuessee, ” jron-clad, action with, 88 Thalium, distribution of... . 216, -Thermoeraph, NGWie: Wee, is © sis o's Tides, popular explanation of ... Tin, ancient sources of... . ... . ce “scrap, wutilization Of <2 2. - +71 Tobacco and alcohol, effects of on RCW es. ec G2 BA Be best method of smoking . 4 es influence of in producing GISCHSE). a6 2 6 8 oie © aoe - physiological effects of . . 229 x products of the combustion of : duoono oe! Topography, application of photog- APU VAL ON ate) c) jes 4s) is) elle) fee Ld Torpedo warfare. ....-+-++-«-s 9 Transparency CPG SOG BVO PONCE, Grannicolor of. =. ss. 3". 172 Tunnel, MGS CORIS, sero cxencns sc, 0 1 16 Twilight, GQuUEAHOMIOL es. 6 3 ae 209 United States, highest mountains in, 300 Vapors, condensation on the surface GiESOlIGS. aicuct ciel el.e teh oo ee Vegetation, curious conditions of . 313 Ventilation and warmth. .... . 227 163. Vibrations, heat, nature of . Vision, motions of the eye in se some peculiarities of . Vital force and contractility . Volcanoes and hot springs. . 28 we & or > eS *_* © @© @ Doon => = ~ Warfare by torpedoes ... .%...« 95 ne MNOVEIGISM IN se os 0) e! sal Ue Waste products, utilization of ... 70 Water and lead pipes .....e.. 245 boiled in paper vessels ... 163 “ boiling, researches on. . . . 162 U consumption OLGA te, ois) atte, cs OZ “flow of through irregular TUDES: 51 'n0 selartotis, vet bemaltein Oz ‘¢ temperature of under at SUC). Sy oNetis 275 Weather indicated by ‘the state of the teléoraphi) 2/275) fe! 3) sn a teledlak yen and measures, uniformity . . . e . . . . . . . . . * 4 Welding by hydraulic pressure .. 44 Wells, Artesian, of the Sahara. . . 305 Wood, action of sulphate of copper OL OM Narre Gucatir Hiss fai! ‘© conversion into coal under PIESSUNCJsiksirs Nath pableiteana <¢ ) new-ornamentaly iis o%. 2. 20 Se PLreSeLrvatlOn Ofis et «1 ements Wool, compressed, for targets Work and waste, bodil Writing, recovery of defaced . or 6) 6.8 — o = LANC COMAZE airs Yona iol semana aera ae ‘“ native ‘* waste of in galvanizing ... 70 eee (of ehte” © @" el & Jee ad 4 hie BG Be cari ri i. ti Mag eure iv eh ESE) ee POM aes LAN on es a etpepesk 5 at eh as eS ol 7 Uy wy gs A sly ie 1 hi ais : "hee ee cas 4 ie ' a, " e ’ Oy RT i ties Mey ey rim j re ' | oe aa 5, ANE aS are nonce Xo oh pal ator 5 a 7 = +e os wid Shes . Fil i ‘ y ka ne is vane tM, 6° ° Seutue Asatte + dh Oe St ie > = Porc Nisa Songs ig GARSs ; ; “Hy = raed Bho Livy’ pen ey ~~ 7%, e} aS yy. Mis. a es y . + deo ay NS » k ee eeee! het Meas rae hr a ee Ass 1 y , * (timate x ie ( rere ; oe ™ ‘ | P ik ee Hae hed ‘h “tare ail anemone enereedy eivexta ~ 2 Seatsyehe ak, Bee ; . ary is aie he ese Yee Tae ae Oe hides Ceca eh ee eES, ira a baad senres saadapen, wee Vind he Ve msantole edt | See hash Tota he ~ ie naira dete, hes ior ce Uh. dda ae aes; eee 5 oe ith * it? Poe i A ae f es 4 Rit Phas (2 ei? son! baths MWe, enn. quaonae Pp ‘ Wrisphi ¥° ‘29 ail ; a, ries ed <4 : a pe SS - ead if a ty oa tht wee | ‘ ax ; 7 J ’ Rete f a ? oe e + hay y W3ee B (et eee Si hae. + de eM soc sie EU ee ¥ poten ete ae ot icin OQ vate sib? Sal (ey Fs PRE os | Lae Pn a : ‘ r ; ik tea take sires amy Titan (Get yrs os ere pom ree ~ GAGE, ah RE AIA TS, ica, Se ee ee ie . MD 007 5% ‘aban ‘Y ha Fa 1s a Py peepee? re We tis weed ti ‘ . Spi iihae Wsatteed Werte pi: A he RENO pee Ae ia my ae ne ' a ae < ' hs 1d acy oe *_ £ CH eT TY ee! OA. re ‘4 +) fe = : a ae ge fs ck” a hed & eT Tes 5 sane tp Pate esi iw ee Lpatene adel ‘ono rth ‘2 Mond een a ae uA © rm be 4 iv CANT wit Lee atte Moe it oe ee . “i ae Ppeu 4 ae a ae vt ER Sige sie Testone OVER XO, AEE 24. 3%. Se LARK ow . ES ia Ww eo eA eae , ae # xt ait

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WINGATE THORNTON. 8yo, cloth, 2.50. ug “ Arare contribution to the early history of New England.” — Journal. 5 4 P Uae Pie shut 7 oat an par vi ‘ er Pei reeset eH aah , : ; aa tes ' »! rhe ox. ; \ 4 ‘ i 3), De wes 2 i : te ’ agi F < ; eid < WP heder’* f;. ae, AE are h “i, raalen bd 3 : ss - a f° a a pe s j * > s if 5 Pay" rice wu y ik es Pa i TALS ie ee 3 a ’ ) AV rd & if ‘ 7 r bY sa WA i 4 du { mo, . ae ' ee wo’ BONN l oe #2 i» ’ pricks fon fees nade aay — ot ae rsdn roar Liye we ce tah Bae we 10 Mitad 2 ela ees Berenit 34t Pf ates) «+ : r So oey € iduvveag \) bon = * ‘ = : * ~~ ; , = : : a a Pe er A ee ae 4:0 @\ept bay ; “ PS RRK SETS OO NT DOM ek eae “ebiyibot & 7 ee Ve aNd were) wf Fei il ug Ut aly ver aeretc es a ft Se liedy Au. oh ee, “wv ot lari 7 te ns 4 q f i a ’ = Uresrgrs vores POP OC urine Bika e mull oie Dione > Pie wr bp ueal mn ¢ apt ” LW 2 a wh : : “ i = b= etd weakd ‘ay ee heat ' ; Me ~~ y 5 ~ 6 Te ANH x. wre Ae) ee ie" 5 A ek beens y kt css: iID ca a e Wy) 27 sin we air, rich! 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