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questions, but we may state that they are all of more or less general interest, and that the large majority are practically useful. Some deal with local improvements; others, with the statistics of the country; and others. again, require investigations in the various branches of Physical and Mechanical Science, in Crystallography, Geology, Chemistry, Botany, Physiology, &c.

The replies of competitors, which are expected to take the form of short essays, may be indited in the Dutch, French, English, German, or Latin languages, and as far as we are enabled to judge from the precautions taken to ensure impartiality to all candidates, and secrecy to unsuccessful ones, we should say that students are justified in placing their labours in the hands of the Society in perfect confidence that they will receive fair treatment.

As we have already observed, we hope that some move will be made in this practical direction amongst our English Institutions; the Society of Arts already awards such prizes, but there is no reason why every important "Philosophical" Society should not do the same, and we shall be glad to receive more of these programmes from other countries, in order to extract from them any new features in their management, for the benefit of our English readers.

SPECTRUM ANALYSIS.

THOSE of our readers who may be able to read the Dutch language, will find in it one of the best works yet published on Spectrum Analysis.* The book is so good that it deserves translation into a language that would ensure it a wider circulation; and as we are in want of such a work in England, we commend it to the notice of any good Dutch scholar and chemist. Tracing the art from its first origin, the author brings down his account of the successive discoveries to the latest published observations of Bunsen, Kirchoff, and Miller, describing most of the observed spectra, and giving what will be found extremely useful to many-a very complete bibliography of the subject. The work is accompanied by some beautifully-executed coloured drawings of various spectra.

One of the earliest applications of the prism to chemical analysis was that of Plucker, who observed the lines produced by the passage of electricity through a rarefied gas, and noticed that in every gas, when pure, a particular system of lines was obtained. The minute portion of a gas, whether simple or compound, that could be analysed in this way induced the author to style the method microchemistry. It was really spectrum-analysis. M. Morren followed up the researches of Plucker, and now publishes at Marseilles a tract,† the object of which, he says, is to point out how this mode of analysis may help to solve

* De Spectraal-Analyse &c.'-On Spectrum Analysis, &c. By H. C. Dibbits. Rotterdam E. H. Tassemeijer. 1863.

+ Des Phénomènes Lumineux que présentent quelques Flammes, et en particulier celle du Cyanogène, et de l'Acetylène, &c.'^ Par M. Morren. Marseilles: Arnaud & Co., 1863.

questions which ordinary chemical processes are unable to unriddle. What, for example, constitutes the blue part of the flame of a candle? The spectroscope answers, vapour of carbon. The author once thought that the blue was caused by light carburetted-hydrogen, since he observed the same spectrum from the flame of this gas, and also from that of the base of a candle flame. A perusal of Dr. Attfield's paper on the "Spectrum of Carbon," however, induced him to reconsider the subject, and to examine the spectra of numerous other carbon compounds. In all these he observed the same spectrum, which, being common to everyone, must have been derived from the common constituent, carbon. The means which the author employed, and the appearances he observed, are well described in this tract; and any experimenters working in the same direction would do well to consult it.

CHEMICAL FORMULE.

DR. ODLING has published* a set of tables of chemical formula, which we venture to say will prove as useful to teachers as to students of chemistry. He adopts an original mode of classifying the elements which is, perhaps, as reasonable as any other yet proposed, or possible, in the present state of our knowledge of these bodies.

The formulæ are all constructed on the unitary system of notation, and in the absence of a complete work of chemistry based on that system, these tables will prove of great assistance to students, who are obliged to read a book written upon the old system, and listen to a lecturer who teaches upon the new.

Lecturers who are beginning to teach the unitary system, will find in the tables the materials of a very useful set of diagrams.

*Tables of Chemical Formulæ,' arranged by W. Odling, M.B., F.R.S, &c., &c. London: Taylor and Francis, 1864.

NOTES AND CORRESPONDENCE.

SILVERED GLASS TELESCOPES AND CELESTIAL PHOTOGRAPHY IN AMERICA. By Professor HENRY DRAPER, M.D., New York University.

NEW YORK, Feb. 2, 1864.

THE first photographs of the moon were taken in 1840 by my father, Professor John W. Draper, M.D., who published notices of them in his quarto work, On the Forces that Organize Plants,' and in the 'Philosophical Magazine.' The specimens were about an inch in diameter, and were presented to the Lyceum of Natural History of New York. They were made by means of a lens of five inches aperture, furnished with an eye-piece to increase the magnifying power, and mounted on a polar axis driven by a clock. At that time it was generally supposed that the moon's light contained no actinic rays, and was entirely without effect on the sensitive silver compounds used in daguerreotyping.

In 1850, Mr. Bond made use of the Cambridge (Massachusetts) refractor of 15 inches' aperture, to produce daguerreotype impressions of our satellite, the sensitive plate being placed at the focus of the objectglass, without the intervention of an eyepiece. Pictures two inches in diameter were thus produced, and, subsequently, some of the same size were made on glass, and mounted stereoscopically. Mr. Bond also made a series of experiments to determine whether photography could be advantageously applied to the measurement of double stars, and concluded that the results were as reliable as those derived from the micrometer.'

Soon after, Mr. Warren De La Rue, of Cranford, near London, undertook by the aid of a 13-inch speculum, ground and polished by himself, to procure a series of photographs of the moon and other celestial objects. The excellent re

*Astron. Nach,' No. 1129.

sults that he has obtained, together with those of Professor Phillips, Mr. Hartnup, Mr. Crookes, Father Secchi, and other physicists, are doubtless familiar to all scientific men, having been published in the form of a report to the British Association in 1859. No detailed description of them is necessary, therefore, in this place.

In 1857 Mr. Lewis M. Rutherfurd, of New York, erected an equatorial refractor of 11 inches' aperture, the object-glass of which he had himself corrected, and has taken a large number of lunar photographs with it. They have generally borne to be magnified to five inches, and he is now engaged in perfecting a correcting lens that will allow still greater enlargement to be used.

The moon, as seen by the naked eye, is about one-tenth of an inch in diameter,although persons generally estimate it at 10 inches. That the first statement is true is easily proved either by taking a photograph with a lens of 10 inches' focal length, or more convincingly by holding up between the moon and the eye a little disc one-tenth of an inch across, at the nearest distance of distinct vision (10 inches). A picture of the moon of the size commonly attributed to her requires to be made under a power of 100 times.

In 1857 I visited Lord Rosse's great reflecting telescopes at Parsonstown, and had an oppertunity of not only seeing the grinding and polishing operation by which they were produced, but also of observing some stars through the six-foot instrument. On returning home in 1858 it was determined to construct a large instrument by similar means, and devote it especially to celestial photography. The speculum was of

15 inches' aperture, and 12 feet focal length. Subsequently, however, this metal mirror was abandoned, and silvered glass, as suggested by M. Foucault, substituted. This latter, according to Steinheil's experiments, reflects more than 90 per cent. of the light falling upon it, while speculum metal only returns 63 per cent. A detailed account of this instrument, amply illustrated, is now being published by the Smithsonian Institution at Washington, and therefore only a general idea of its peculiarities will be given.

As the telescope was intended especially for photography, the following general principles were adopted. 1st. A reflector was, of course, preferred to an achromatic object-glass, because all the rays falling upon it are reflected to the same focal plane, and there is not, as in the latter, one focus for distinct vision, and another for the photographically actinic rays, an inch distant perhaps. In the reflector a sensitive plate put where the image is seen to be most sharply defined, will be sure to give a good result. In the achromatic, on the contrary, the sensitive plate must be placed in a position which can only be found by tedious trials. 2nd. Silvered glass was used instead of speculum metal, because it is lighter and more highly reflecting. Besides, if a reddish or yellowish film should accumulate on it-an accident liable to occur to either kind of reflector and seriously diminishing the photographic powerit can either be repolished with a piece of buckskin-an operation obviously impossible in the case of a speculum metal-or the silver can be dissolved off with nitric acid, and a new film deposited on the glass concave. The glass which has been made accurately parabolic before the first silvering, is not changed in figure, the silver being only deposited in a layer 2000 of an inch thick, and consequently, if carefully prepared, copying the glass below so closely that no error larger than a small fraction of that amount is possible. As the glass only serves as a basis or mould for the thin

sheet of silver, and is not penetrated by the light, its quality is a matter of but little moment, that which is used for skylights or light-openings in floors answering perfectly. 3rd. A mounting, presenting the greatest degree of steadiness possible was necessary. For this purpose the telescope was supported at both ends, the lower one resting in a loop of wire rope. 4th. Instead of driving the whole mass of the instrument by clockwork acting upon a polar axis, and thus being forced to move a weight of at least half-a-ton-the usual system in equatorials only the sensitive plate and its frame, weighing an ounce, were caused to follow the moon or other object, the mass of the apparatus remaining perfectly at rest. This idea is due to Lord Rosse. 5th. Instead of using a clock with wheelwork for a prime mover, a clepsydra was substituted. This consists of a heavy weight supported by the rod of a piston, which fits into a cylinder filled with water. At the bottom of the cylinder a stopcock permits the water to flow out at a variable speed, depending on the amount of opening. The sensitive plate can thus easily be caused to coincide in rate with the moving object, and yet by a motion free from irregularity and tremor.

The value of a silver reflector turns, of course, entirely upon the perfection of the glass concave on which the metallic film is to be de

posited. This must be of a parabolic figure, so that spherical aberration may be completely corrected. A person is, however, content to take the utmost pains to produce it, because, once attained, the figure cannot be lost except by fracture, and the value does not diminish with time as in the case of a speculum. It never requires re-polishing. The best method of grinding and polishing the glass is by means of an apparatus that I have called a "Local-correcting Machine," by which all the parts of the surface can be attacked in succession and reduced to the desired curvature,

and yet at the same time a uniform curve and absence of local irregularities secured. I have spent five years in the investigation of this subject, and have polished more than 100 mirrors of from 19 inches to one-fourth of an inch in diameter, on seven different machines built at various times. The quality of those I have at present is indicated by the fact that they will show Debillisima to be quintuple, and will render the close companion of Sirius, discovered by Alvan Clark's magnificent 18-inch refractor, visible.

The Observatory at Hastingsupon-Hudson, near New York, lat. 40° 59' 25" N., long. 73° 52′ 25" W. of Greenwich, is upon the summit

of a hill 225 feet above low-water mark. It is 20 feet square, with a wing 9 x 10 for a photographic laboratory. As the telescope is a Newtonian, with the mounting so contrived as to have the eyepiece stationary at all altitudes, a plan originally suggested by Miss Herschel, there are peculiar facilities offered for easy access to the eyepiece, or place of the sensitive plate. The interior height of the Observatory, 22 feet, is divided into two stories, around the upper of which an observer's chair runs to follow the telescope. The dome turns upon a pivot at its centre, instead of on rollers or cannon-balls around the edge, and is moved consequently with but slight exertion.

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