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FOR THE See also:YERKES See also:OBSERVATORY use of an overhanging polar See also:axis the difficulty can be overcome ; it has been successfully adopted by Repsolds for their astrographic equatorials of 13-in. See also:aperture and 11.25-ft. See also:focus, and on a much smaller See also:scale by See also:Warner & Swasey for the See also:Bruce See also:telescope of Io-in. aperture and 50-in. focus, made for the Yerkes Observatory. The From See also:Professor See also:Hale's The Study of Stellar See also:Evolution, by permission of the University of See also:Chicago See also:Press. latter is shown in fig. 19. Stability in this method of mounting can only be secured by excessive See also:weight and rigidity in the support of the overhanging axis. In the See also:case of the See also:Victoria telescope (24-in. aperture and 222-ft. focus) mounted at the Cape of See also:Good dope on this See also:plan, it has been found necessary to add supporting stays where See also:great rigidity is required, and thus to See also:sacrifice continuous circuni-See also:meridian See also:motion for stars between the See also:zenith and the elevated See also:pole. Type D.—The first important See also:equatorial of type D was the 4-ft. 'effecting telescope of Lassell (Mem. R.A.S., See also:xxxvi. I-4), and later See also:Lord See also:Rosse's 36-in. reflecting telescope at See also:Birr See also:Castle (Phil. Trans., clxxi. 153), and A. See also:Common's 36-in. reflecting telescope mounted by him at See also:Ealing (Mem. R.A.S., xlvi. 173-182). In Lassell's See also:instrument (a reflector of the Newtonian type) the observer is mounted in the open See also:air on a supplementary See also:tower capable of motion in any See also:azimuth about the centre of motion of the telescope, whilst an observing See also:platform can be raised and lowered on the See also:side of the tower. In Lord Rosse's instrument (also of the Newtonian type) the observer is suspended in a cage near the See also:eye-piece, and the instrument is used in the open air. Common's telescope presents many ingenious features, especially the See also:relief-See also:friction by flotation of the polar axis in See also:mercury, and in the arrangements of the observatory for giving ready See also:access to the eye-piece of the telescope.
Type C seems indeed to be the type of mounting most suitable for reflecting telescopes, and this See also:form has been adopted for the 6o-in. reflector completed by G. W. Ritchey, under the direction of Professor G. E. Hale, for the See also:Mount See also: 20, and its See also:design is unquestion-ably the most perfect yet proposed for See also:modern astrophysical re-See also:search. The See also:declination axis is here represented by what are practically the trunnions or pivots of the See also:tube, resting in See also:bearings which are supported by the arms of a very massive See also:cast-See also:iron See also:fork bolted to the upper end of the polar axis. This axis is a hollow See also:forging of See also:nickel See also:steel, of which the accurately turned pivots See also:rest on bearings attached to cast-iron uprights bolted upon a massive cast-iron See also:base See also:plate. The base plate rests upon levelling screws which permit the See also:adjustment of the polar axis to be made with great precision. The combined overhanging weight of the cast-iron fork, the See also:mirror and tube is so great, that without a very perfect relief-friction See also:system the instrument could not be moved in right See also:ascension with any approach to See also:practical ease. But a hollow steel See also:float, Io ft. in See also:diameter, is bolted to the upper end of the polar axis just below the fork. This float dips into a tank filled with mercury so that practically the entire instrument is floated by the mercury, leaving only sufficient pressure on the bearings to ensure that the pivots will remain in contact with them. The 6o-in. See also:silver-on-See also:glass mirror (weighing about one ton) rests at the See also:lower end of the tube on a support-system consisting of a large number of weighted levers which press against the back of the glass and distribute the load. Similar weighted levers around the circumference of the mirror provide the edge support. The telescope is moved in right ascension and declination by electric See also:motors controlled from positions convenient for the observer. The See also:driving See also:clock moves the telescope in right ascension by means of a See also:worm-See also:gear See also:wheel, io ft. in diameter, mounted on the polar axis. The 60-in. mirror is of 25-ft. focus, but for certain classes of See also:work it is desirable to have the See also:advantage of greater See also:focal length. For this purpose the telescope can be used in the four different ways shown in fig. 21. (i) As a Newtonian reflector, fig. 21 (a), the converging rays from the 6o-in. mirror being reflected to the side of the tube where a h _. From Professor Hale's The Study of Stellar Evolution, by permission of the University of Chicago Press. the See also:image is formed, and where it may be photographed or viewed with an eye-piece. In this case the image is formed without secondary magnification and the focal length is 25 ft. (2) See also:Asa Cassegrain reflector, fig. 21 (b), in which case the upper See also:section of the tube bearing the See also:plane mirror is removed and a shorter section substituted for it. This latter carries a hyperboloidal 6o irich Reflecting Telescope See also:Dome and See also:Building, Solar Observatory Mount Wilson,Calif. Designed G.W.Ritchey Atr.tightligofd See also:Joint betustw Dome and Building From Professor Hale's The Study of Stellar Evolution, by permission of the University of Chicago Press. mirror, which returns the rays towards the centre of the large mirror and causes them to converge less rapidly. They then meet a small plane mirror supported at the point of intersection of the polar and declination axes, whence they are reflected down through the hollow polar axis as shown in fig. 2, and come to focus on the slit of the powerful spectroscope that is mounted on a See also:pier in the chamber of See also:constant temperature as shown in fig. 20. In this case the See also:equivalent focal length is 15o ft. (3) As a Cassegrain reflector, for photographing the See also:moon, See also:planets or very See also:bright nebulae on a large scale, as shown in fig. 21 (c), with an equivalent focal length of too ft. (4) As a Cassegrain reflector, for use with a spectroscope mounted in See also:place of the photographic plate, fig. 21 (d); in this case a See also:convex mirror of different curvature is employed, the equivalent focus of the See also:combination being 8o ft. Type E.—In the Comp/es Rendus for the See also:year 1883, vol. 96, pp. 735-741, Loewy gives an See also:account of an instrument which he calls an " equatorial coude," designed (1) to attain Loewy's greater stability and so to measure larger angles than is See also:equator- generally possible with the See also:ordinary equatorial; (2) to ietttoude enable a single astronomer to point the telescope and make observations in any See also:part of the See also:sky without changing his position; (3) to abolish the usual expensive dome, and to substi- tute a covered See also:shed on wheels (which can be run back at See also:pleasure), leaving the telescope in the open air, the observer alone being sheltered. These conditions are fulfilled in the manner shown in fig. 22. E P is the polar axis, rotating on bearings at F. and P. The See also:object-glass is at 0, the eye-piece at E. There is a plane mirror at M, which reflects rays converging from the object-glass to the eye-piece at E. A second mirror N, placed at 45° to the See also:optical axis of the object-glass, reflects rays from a See also:star at the pole; but by rotating the See also:box which contains this mirror on the axis of its supporting tube T a star of any declination can be observed, and by combining this motion with rotation of the polar axis the astronomer seated at E is able to view any object whatever in the visible heavens, except' circumpolar stars near lower transit. An See also:hour circle attached to E P and a declination circle attached to the box containing the mirror N, both of which can be read or set from E, See also:complete the essentials of the instrument. There must be a certain loss of See also:light from two additional reflections; but that could be tolerated for the See also:sake of other advantages, provided that the the mirrors could be made sufficiently perfect optical planes. By making the mirrors of '\ silvered glass, one-See also:fourth of their diameter in thickness, the Henrys have not only ~`. \ succeeded in mounting them with all \\ necessary rigidity See also:free from flexure `. but have given them optically '. s true plane surfaces, notwith-N See also:standing their large diameters, viz., t t and 15.7 in. See also:Sir See also:David Gill tested the equatorial coude on See also:double stars at the See also:Paris Observatory in 1884, and his last doubts as to the practical value of the instrument were dispelled. He has Equatorial. optical See also:definition in any of the many telescopes he has employed, and certainly never measured a See also:celestial object in such favourable conditions of See also:physical comfort. The easy position of the observer, the convenient position of the handles for See also:quick and slow motion, and the See also:absolute rigidity of the mounting leave little to be desired. In a much larger
instrument of the same type subsequently mounted at Paris, and in like See also:instruments of intermediate See also:size mounted at other See also:French observatories, the object-glass is placed outside the mirror N, so that both the silvered mirrors are protected from exposure to the See also:outer air.
A modification of Loewy's equatorial coude has been suggested by Lindemann (See also:Asir. Nachr., No. 3935); it consists in placing both the mirrors of Loewy's " equatorial coude " at the See also:top of the. polar axis instead of the. lower end of it. By this arrangement the See also:long See also:cross tube becomes unnecessary, and neither the pier nor the observatory obstruct the view of See also:objects above the See also:horizon near lower transit as is the case in Loewy's form. The reflected rays pass down the tube from the direction of the elevated pole instead of upward towards that pole. The observer is, therefore, at the bottom of the tube instead of the top and looks upward instead of downward. The drawbacks to this plan are (I) the necessarily large size of the upper See also:pivot (viz. the diameter of the tube) and of the lower pivot (which must be perforated by a hole at least equal in diameter to the photographic See also: R. Dub. See also:Soc., vol. iii. See also:series 2, p. 61) proposed a form of equatorial telescope of which an The excellent example was erected at See also:Cambridge (Eng). in The 1898. The instrument in some respects resembles the tirubbNal equatorial coude of Loewy, but instead of two mirrors equato at See also:cam- there is only one. A flanged cast-iron box, strongly See also:bridge. ribbed and open on one side, forms the centre of the polar axis. One pivot of the polar axis is attached to the lower end of this box, and a strong hollow See also:metal See also:cone, terminating in the other pivot, forms the upper part of the polar axis. The declination axis passes through the two opposite sides of the central box. Upon an axis concentric with the declination axis is carried a plane mirror, which is geared so as always to bisect the See also:angle between the polar axis and the optical axis of the telescope. If then the See also:objective tube is directed to any star, the convergent See also:beam from the object-glass is received by the plane mirror from which it is reflected upwards along the polar axis and viewed through the hollow upper pivot. Thus, as in the equatorial coude, the observer remains in a fixed position looking down the polar tube from above. He is provided with quick and slow motions in right ascension and declination, which can be operated from the eye-end, and he can work in a closed and comfortably heated room. A large slot has to be cut in the cone which forms the upper part of the polar axis, in See also:order to allow the telescope to be pointed nearer to the pole than would otherwise be possible; even so stars within 15° of the pole cannot be observed. An illustrated preliminary description of the instrument is given by Sir See also:Robert See also:Ball (Mon. Not. R.A.S., lix. 152). The instrument has a triple photo-visual See also: See also:Foucault appears to have been the first to appreciate these advantages and to See also:face the difficulty of designing a siderostat which, theoretically at least, fulfils the above-mentioned conditions. A large siderostat, constructed by Eichens after Foucault's design, was completed in 1868—the year of Foucault's See also:death. It remained at the Paris Observatory, where it was subsequently employed by Deslandres for solar See also:photography. The largest refracting telescope yet made, viz., that constructed by See also:Gautier for the Paris The Parrs See also:exhibition of 1900, was arranged on this plan (type F), h refeactor the stars' rays being reflected along the horizontal axis • x900). of a telescope provided with visual and with photo- graphic object-glasses of 49-in. diameter and nearly Zoo-ft. focal length. Up to 1908 neither the optical qualities of the images given by the object-glasses and reflecting plane nor the practical working of the instrument, have, so far as we know, been submitted to any severe test. It is, however, certain that the Foucault siderostat is not capable, in practice, of maintaining the reflected image in a constant direction with perfect uniformity on account of the sliding See also:action on the See also:arm that regulates the motion of the mirror; such an action must, more or less, take place by jerks. There are farther inconveniences in the use of such a telescope, viz., that the image undergoes a diurnal rotation about the axis of the horizontal telescope, so that, unless the sensitive plate is also rotated by clockwork, it is impossible to obtain See also:sharp photographs with any but instantaneous exposures. In the spectroscopic observation of a single star with a slit-spectroscope, this rotation of the image presents no inconvenience, and the irregular action of a siderostat on Foucault's plan might be overcome by the following arrangement : A B (fig. 23) is a polar axis, like that of an equatorial telescope, rotating in twenty-four See also:hours by clockwork. Its lower extremity terminates in a fork on which is S mounted a mirror C D, capable of turning about A on an axis at right angles to A B, the plane of the f4 mirror being parallel to this latter axis. The mirror C D is set at such an angle as to reflect rays from the star S in the direction of the polar axis to the mirror R and thence to the horizontal telescope T. The mirrors of Lindemann's ~- equatorial coude reflecting light R ` Q- - T- -- downwards upon the mirror R FIG.2 would furnish an ideal siderostat for stellar See also:spectroscopy in See also:conjunction with a fixed horizontal telescope. Coelostat.—If a mirror is mounted on a truly adjusted polar axis, the plane of the mirror being parallel to that axis, the normal to that mirror will always be directed to some point on the celestial equator through whatever angle the axis is turned. Also, if the axis is made to revolve at See also:half the apparent diurnal motion of the stars, the image of the celestial See also:sphere, viewed by reflection from such a moving tnieror, will appear at rest at every point—hence the name coelostat applied to the apparatus. Thus, any fixed telescope directed towards the mirror of a properly adjusted coelostat in motion will show all the stars in the field of view at rest; or, by rotating the polar axis independently of the clockwork, the observer can pass in See also:review all the stars visible above the horizon whose declinations come within the limits of his See also:original field of view. Therefore, to observe stars of a different declination it will be necessary either to shift the direction of the fixed telescope, keeping its axis still pointed to the coelostat mirror, or to employ a second mirror to reflect the rays from the coelostat mirror along the axis of a fixed telescope. In the latter case it will be necessary to provide means to mount the coelostat on a See also:carriage by which it can be moved See also:east and See also:west without changing the See also:altitude or azimuth of its polar axis, and also to shift the second mirror so that it may receive all the light from the reflected beam. Besides these complications there is another See also:drawback to the use of the coelostat for See also:general astronomical work, viz., the obliquity- of the angle of reflection, which can never be less than that of the declination of the star, and may be greater to any extent. For these reasons the coelostat is never likely to be largely employed in general astronomical work, but it is admirably adapted for spectroscopic and bolometric observations of the See also:sun, and for use in See also:eclipse expeditions. For details of the coelostat applied to the See also:Snow telescope—the most perfect installation for See also:spectroheliograph and bolometer work yet erected—see The Study of Stellar Evolution by Prof. G. E. Hale, p. 131. The Zenith Telescope The zenith telescope is an instrument generally employed to measure the difference between two nearly equal and opposite zenith distances. Its original use was the determination of See also:geographical latitudes in the field' work of See also:geodetic operations; more recently it has been extensively employed for the determination of variation of See also:latitude, at fixed stations, under the auspices of the See also:International Geodetic See also:Bureau, and for the astronomical determination of the constant of See also:aberration. The instrument is shown in its most See also:recent form in fig. 24. A is a See also:sleeve that revolves very freely and without shake on a See also:vertical steel cone. This cone is mounted on a circular base b which rests on three levelling screws, two of which are visible in the figure. The sleeve carries a cross-piece on its upper extremity to which the bearings of the horizontal axis c are attached. A reversible level d rests on the accurately turned pivots of this axis. The telescope is attached to one end of this axis and a counterpoise e to the other. The long arm f serves to clamp the telescope in zenith distance and to communicate slow motion in zenith distance when so clamped. On the side of the telescope opposite to the horizontal axis is attached a graduated circle g, and, turning concentrically with this circle, is a framework h, to which the readers and verniers of the circle are fixed. This See also:frame carries two very sensitive levels, k and 1, and the whole frame can be clamped to the circle g by means of the clamping See also:screw in. The object-glass of the telescope is, of course, attached by its See also:cell to the upper end of the telescope tube. Within the focus of the object-glass is a right-angled See also:prism of See also:total reflection, which diverts the converging rays from the object-glass at right angles to the axis of the telescope, and permits the observing See also:micrometer n to he mounted in the very convenient position shown in the figure. A small graduated circle p concentric with A is attached to the circular base b and read by the microscopes q r, attached to a. The instrument is thus a See also:theodolite, although, compared with its other dimensions, feeble as an apparatus for the measurement of absolute altitudes and azimuths, although capable of determining these co-ordinates with considerable precision. In practice the vertical circle is adjusted once for all, so that when the levels k and I are in the centre of their run, the verniers read true zenith distances. When the instrument has been set up and levelled (either with aid of the cross level d, or the levels k and I), the See also:reading of the circle p for the meridional position of the telescope is determined either by the method of transits in the meridian (see TRANSIT CIRCLE), or by the observation of the azimuth of a known star at a known hour angle. This done, the stops s and t are clamped and adjusted so that when arm r comes in contact with the screw of stop t the telescope will point due See also:north, and when in contact with s, it will point due See also:south, or See also:vice versa. A pair of stars of known declination are selected such that their zenith distances, when on the meridian, are nearly equal and opposite, and whose right ascensions differ by five or ten minutesof See also:time. Assuming, for example, that the See also:northern star has the smaller right ascension, the instrument is first, with the aid of the stop, placed in the meridian towards the north; the verniers of the graduated circle g are set to read to the reading 4–10s+o ) where is the approximate latitude of the place and b., O. the declinations of the northern and See also:southern star respectively; then the level frame h is turned till the levels k and l are in the See also:middle of their run, and there clamped by the screw m, aided in the final adjustment by the adjoining slow motion screw shown in the figure. The telescope is now turned on the horizontal axis till the levels read near the centres of these scales and the telescope is clamped to the arm f. When the star enters the field of view its image is approximately bisected by the spider See also:web of the micrometer n, the exact bisection being completed in the immediate See also:neighbour-See also:hood of the meridian. The readings of the levels k and l and the reading of the micrometer-See also:drum are then entered, and the observation of the northern star is complete. Now the instrument is slowly turned towards the south, till the azimuth arm is gently brought into contact with the corresponding stop s, care being taken not to See also:touch any part of the instrument except the azimuth arm itself. When the southern star enters the field the same See also:process is repeated. Suppose now, for the moment, that the readings of the levels k and I are identical in both observations, we have then, in the difference between the micrometer readings north and south, a measure of the difference of the two zenith distances expressed in terms of the micrometer screw; and, if the " value of one revolution of the micrometer screw " is known in seconds of arc we have for the resulting latitude =2t(i —i ) +(S,. T&,)1, where i',, is the difference of the micrometer readings converted into arc—it being assumed that increased micrometer readings correspond with increased zenith distance of the star. If between the north and south observation there is a See also:change in the level readings of the levels k and 1, this indicates a change in the zenith distance of the axis of the telescope. By directing the telescope to a distant object, or to the intersection of the webs of a fixed collimating telescope (see TRANSIT CIRCLE) ,it is easy to measure the effect of a small change of zenith distance of the axis of the telescope in terms both of the level and of the micrometer screw, and thus, if the levels are perfectly sensitive and uniform in curvature and See also:graduation, to determine the value of one See also:division of each level in terms of the micrometer screw. The value of " one revolution of the screw in seconds of arc " can be determined either by observing at transit the difference of zenith distance of two stars of known declination in terms of the micrometer screw, the instrument remaining at rest between their transits; or by measuring at known instants in terms of the screw, the change of zenith distance of a See also:standard star of small polar distance near the time of its greatest See also:elongation. The See also:reason why two levels are employed is that sometimes crystals are formed by the decomposition of the glass which cause the bubble to stick at different points and so give false readings. Two levels are hardly likely to have such causes of See also:error arise at exactly corresponding points in their run, and thus two levels furnish an See also:independent See also:control the one on the other. Also it is impossible to make levels that are in every respect perfect, nor even to deter-mine these errors for different lengths of bubble and at different readings with the highest precision. The mean of two levels there-fore adds to the accuracy of the result. Attempts have been made to overcome the difficulties connected with levels by adopting the principle of See also:Kater's floating collimator (Phil, Trans., 1825 and 1828). On this principle the use of the level is abolished, the telescope is mounted on a metallic float, and it is assumed that, in course of the rotation of this float, the zenith distance of the axis of the telescope will remain undisturbed, that is, of course, after the undulations, induced by the disturbance of the mercury, have ceased. S. C. See also:Chandler in 1884 constructed an equal altitude instrument on this principle, which he called the almucantar, and he found that after disturbance the telescope recovered its original zenith distance within of a second of arc. R. A. See also:Sampson at See also:Durham (Monthly Notices R.A.S. Ix. 572) and H. A. See also:Howe (See also:Ast. Jahrb. xxi. 57) have had instruments constructed on the same general principle. It is, however, obviously impossible to apply a micrometer with advantage to such instruments, because to touch such an instrument, in order to turn a micrometer screw, would obviously set it into motion. The almucantar was therefore used only to observe the vertical transits of stars in different azimuths over fixed horizontal webs, without touching the telescope. By the use of photography, however, it is possible to photograph the trail of a star as it transits the meridian when the telescope is directed towards the north, and another trail be similarly photo-graphed when the telescope is directed towards the south. The See also:interval between the true trails, measured at right angles to the direction of the trails, obviously corresponds to the difference of zenith distance of the two stars. This principle has been applied with great completeness and ingenuity of detail by See also:Bryan Cookson to the construction of a " photographic floating zenith telescope," 4s- which he has erected at Cambridge (Eng.) and applied to an investigation of the change of latitude and a determination of the constant of See also:refraction. A description of the instrument, and some preliminary results obtained by it, is given by him (Monthly Notices R.A.S., lxi. 314). [D. Additional information and CommentsThere are no comments yet for this article.
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