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W. See also: Bessel introduced in 1834 near See also:Konigsberg a See also:compound bar which constituted a metallic thermometer.' A See also:zinc bar is laid on an See also:iron bar two toises See also:long, both bars being perfectly planed and in free contact, the zinc bar being slightly shorter and the two bars rigidly See also:united at one end. As the temperature varies, the difference of the lengths of the bars, as perceived by the other end, also varies, and affords a quantitative correction for temperature See also:variations, which is applied to reduce the length to standard temperature. During the measurement of the base line the bars were not allowed to come into contact, the See also:interval being measured by the insertion of See also:glass wedges. The results of the comparisons of four measuring rods with one another and with the See also:standards were elaborately computed by the method of least-squares. The probable error of the measured length of 935 toises (about 6000 ft.) has been estimated as 1/863500 or 1.2 µ (r+ denoting a millionth). With this apparatus fourteen base lines were measured in See also:Prussia and some neighbouring states; in these cases a somewhat higher degree of accuracy was obtained. The See also:principal triangulation of See also:Great See also:Britain and See also:Ireland has seven base lines: five have been measured by See also:steel chains, and two, more exactly, by the See also:compensation bars of See also:General T. F. See also:Colby, an apparatus introduced in 1827—1828 at Lough Foyle in Ireland. Ten base lines were measured in See also:India in 1831—1869 by the same apparatus. This is a system of six compound-bars self-correcting for temperature.The bars may be thus described: Two bars, one of See also: brass and the other of iron, are laid in See also:parallelism side by side, firmly united at their centres, from which they may freely expand or See also:contract; at the standard temperature they are of the same length. Let AB be one bar, A'B' the other; draw lines through the corresponding extremities AA' (to P) and BB' (to Q), and make A'P=B'Q AA' being equal to BB'. If the ratio A'P/AP equals the ratio of the coefficients of expansion of the bars A'B' and AB, then, obviously, the distance PQ is See also:constant (or nearly so). In the actual See also:instrument i An arrangement acting similarly had been previously introduced by See also:Borda. P and Q are finely engraved dots so ft. apart. In practice the bars, when aligned, are not in contact, an interval of 6 in. being allowed between each bar and its See also:neighbour. This distance is accurately measured by an ingenious micrometrical arrangement constructed on exactly the same principle as the bars themselves. The last base line measured in India had a length of 8913 ft. In consequence of some suspicion as to the accuracy of the compensation apparatus, the measurement was repeated four times, the operations being conducted so as to determine the actual values of the probable errors of the apparatus. The direction of the line (which is at Cape See also:Comorin) is See also:north and See also:south. In two of the measurements the brass component was to the See also:west, in the others to the See also:east; the See also:differences between the individual measurements and the mean of the four were +0.0017, -0.0049, -0.0015, +0.0045 ft. These differences are very small; an elaborate investigation of allsources of error shows that the probable error of a base line in India is on the See also:average =2.8 A.These compensation bars were also used by See also: Sir See also:
He found that to•8 g was the mean of the probable errors of the seven bases measured by him. The Austro-Hungarian apparatus is similar; the distance of the rods is measured by a slider, which rests on one of the ends of each See also: rod. Twenty-two base lines were measured in 1840—1899. General See also:Carlos Ibanez employed in 1858—1879, for the measurement of nine base lines in See also:Spain, two apparatus similar to the apparatus previously employed by Porro in See also:Italy; one is complicated, the other simplified. The first, an apparatus of the See also:brothers See also:Brunner of See also:Paris, was a thermometric See also:combination of two bars, one of See also:platinum and one of brass, in length 4 metres, furnished with three levels and four thermometers. Suppose A, B, C three See also:micrometer microscopes very firmly supported at intervals of 4 metres with their axes vertical, and aligned in the plane of the base line by means of a transit instrument, their micrometer screws being in the line of measurement. The measuring bar is brought under say A and B, and those micro-meters read ; the bar is then shifted and brought under B and C. By repetition of this See also:process, the See also:reading of a micrometer indicating the end of each position of the bar, the measurement is made. Quite similar apparatus (among others) has been employed by the See also:French and Germans. Since, however, it only permitted a distance of about 300 M. to be measured daily, Ibanez introduced a simplification; the measuring rod being made simply of steel, and provided with inlaid mercury thermometers. This apparatus was used in See also:Switzerland for the measurement of three base lines. The accuracy is shown by the estimated probable errors: to•2 s to to•8 i.The distance measured daily amounts at least to 800 m. A greater daily distance can be measured with the same accuracy by means of Bessel's apparatus; this permits the ready measurement of 2000 M. daily. For this, however, it is important to See also: notice that a large See also:staff and favourable ground are necessary. An important improvement was introduced by See also:Edward Jaderin of Stock-holm, who See also:measures with stretched wires of about 24 metres long; these wires are about 1.65 mm. in See also:diameter, and when in use are stretched by an accurate spring See also:balance with a tension of to kg., The nature of the ground has a very trifling effect on this method. The difficulty of temperature determinations is removed by employing wires made of See also:invar, an alloy of steel (64 °A) and See also:nickel (36%) which has practically no linear expansion for small thermal changes 2 Geodetic Survey of South Africa, vol. iii. (1905), p. viii ; See also:Les Nouveaux Appareils pour la mesure rapide See also:des bases geod., See also:par J. Rene See also:Benoit et Ch. Ed. See also:Guillaume (1906). at See also:ordinary temperatures; this alloy was discovered in 1896 by BenSit and Guillaume of the See also:International See also:Bureau of Weights and Measures at See also:Breteuil. Apparently the future of base-line measurements rests with the invar wires of the Jaderin apparatus; next comes Porro's apparatus with invar bars 4 to 5 metres long. Results have been obtained in the United States, of great importance in view of their accuracy, rapidity of determination and See also:economy.For the measurement of the arc of meridian in longitude 98° E., in 1900, nine base lines of a See also: total length of 69.2 km. were measured in six months. The total cost of one base was $1231. At the beginning and at the end of the See also:
The same See also: device has been applied to the older bimetallic-compensating apparatus of See also:Bache-Wurdemann (six bases, 1847–1857) and of Schott. There was also employed a single rod bimetallic apparatus on F. Porro's principle, constructed by the brothers See also:Repsold for some base lines. Excellent results have been more recently obtained with invar tapes. The following results show the lengths of the same See also:German base lines as measured by different apparatus: metres. Base at See also:Berlin 1864 Apparatus of Bessel 2336.3920 T88o „ Brunner .3924 Base atStrehlen 1854 „ Bessel 2762.5824 1879 „ Brunner .5852 Old base at See also:Bonn 1847 Bessel 2133.9095 1892 New base at Bonn 1892 2512.9612 „ 1892 Brunner .9696 It is necessary that the altitude above the level of the sea of every See also:part of a base line be ascertained by spirit levelling, in order that the measured length may be reduced to what it would have been had the measurement been made on the surface of the sea, produced in See also:imagination. Thus if l be the length of a measuring bar, h its height at any given position in the measurement, r the radius of the earth, then the length radially projected on to the level of the sea is l(1-h/r). In the See also:Salisbury See also:Plain base line the reduction to the level of the sea is -0.6294 ft. The total number of base lines measured in See also:Europe up to the See also:present See also:time is about one See also:hundred and ten, nineteen of which do not exceed in length 2500 metres, or about If miles, and three—one in See also:France, the others in Bavaria—exceed 19,000 metres. The question has been frequently discussed whether or not the See also:advantage of a long base is sufficiently great to See also:warrant the See also:expenditure of time that it requires, or whether as much precision is not obtain.. able in the end by careful triangulation from a short base. But the See also:answer cannot be given generally; it must depend on the circumstances of each particular case. With Jaderin's apparatus, provided with invar wires, bases of 20 to 30 km. long are obtained with-out difficulty.In working away from a base line ab, stations c, d, e, f are carefully selected so as to obtain from well-shaped triangles gradually increasing sides Before, how- ever, finally leaving the base line, it is usual to verify it by triangulation. thus: during the measurement two or more points, as p; q (fig. I), are marked in the base in positions such that the lengths of the different segments of the line are known ; then, taking suitable See also: external stations, as h, k, the angles of the triangles bhp, phq, hqk, kqa are measured. From these angles can be computed the ratios of the segments, which must agree, if all operations are correctly performed, with the ratios resulting from XI. 20609 the measures. Leaving the base line, the sides increase up to to, 30 or 50 miles occasionally, but seldom reaching too miles. The triangulation points may either be natural See also:objects presenting them-selves in suitable positions, such as See also:
When the theodolite is required to be raised above the surface of the ground in order to command particular points, it is necessary to build two scaffolds,—the See also: outer one to carry the See also:observatory, the inner one to carry the instrument,—and these two edifices must have no point of contact. Many cases of high scaffolding have occurred on the See also:English See also:Ordnance Survey, as for instance at Thaxted church, where the See also:tower, 8o ft. high, is surmounted by a See also:spire of 90 ft. The See also:scaffold for the observatory was carried from the base to the See also:top of the spire; that for the instrument was raised from a point of the spire 140 ft. above the ground, having its bearing upon timbers passing through the spire at that height. Thus the instrument, at a height of 178 ft. above the ground, was insulated, and not affected by the See also:action of the See also:wind on the observatory. At every station it is necessary to examine and correct the adjustments of the theodolite, which are these: the line of collimation of the See also:telescope must be perpendicular to its axis of rotation; this axis perpendicular to the vertical axis of the instrument; and the latter perpendicular to the plane of the See also:horizon. The micrometer microscopes must also measure correct quantities on the divided circle or circles. The method of observing is this. Let A, B, C .. . be the stations to be observed taken in.order of azimuth; the telescope is first directed to A and the See also:cross-hairs of the telescope made to bisect the object presented by A, then the microscopes or verniers of the horizontal circle (also of the vertical circle if necessary) are read and recorded. The telescope is then turned to B, which is observed in the same manner; then C and the other stations. Coming round by continuous motion to A, it is again observed, and the agreement of this second reading with the first is some test of the stability of the instrument. In taking this round of angles—or " arc,” as it is called on the Ordnance Survey—it is desirable that the interval of time between the first and second observations of A should be as small as may be consistent with due care.Before taking the next arc the horizontal circle is moved through 2o° or 30°; thus a different set of divisions of the circle is used in each arc, which tends to eliminate the errors of division. It is very desirable that all arcs at a station should contain one point in See also: common, to which all angular measurements are thus referred,—the observations on each arc commencing and ending with this point, which is on the Ordnance Survey called the " referring object.” It is usual for this purpose to select, from among the points which have to be observed, that one which affords the best object for precise observation. For mountain tops a " referring object " is constructed of two rectangular plates of metal in the same vertical plane, their edges parallel and placed at such a distance apart that the See also:light of the See also:sky seen through appears as a vertical line about to” in width. The best distance for this object is from I to 2 miles. This method seems at first sight very advantageous.? but if, however, it.be desired to attain the highest accuracy, it is better, as shown by General See also:Schreiber of Berlin in 1878, to measure only single angles, and as many of these as possible between the directions to be determined. Division-errors are thus more perfectly eliminated, and errors due to the variation in the stability, &c., of the See also:instruments are diminished. This method is rapidly gaining See also:precedence. The theodolites used in geodesy vary in See also:pattern and in size—the horizontal circles ranging from to in. to 36 in. in diameter. In See also:Ramsden's 36-in. theodolite the telescope has a See also:focal length of 36 in. and an See also:aperture of 2.5 in., the ordinarily used magnifying See also:power being 54; this last, however, can of course be changed at the requirements of the observer or of the See also:weather. The probable error of a single observation of a fine object with this theodolite is about o"•2. Fig. 2 represents an altazimuth theodolite, of an improved pattern used on the Ordnance Survey.The horizontal circle of t4-in. diameter is read by three micrometer microscopes; the vertical circle has a diameter of 12 in., and is read by two micro-scopes. In the great trigonometrical survey of India the theodolites used in the more important parts of the work have been of 2 and 3 ft. diameter—the circle read by five equidistant microscopes. Every See also: angle is measured twice in each position of the zero of the horizontal circle, of which there are generally ten; the entire II number of measures of an angle is never less than 20. An examination of 1407 angles showed that the probable error of an observed angle is on the average = o"•28. For the observations of very distant stations it is usual to employ a See also:heliotrope (from the Gr. ijXcos, See also:sun; rpo,ror, a turn), invented by See also:Gauss at See also:Gottingen in 1821. In its simplest See also:form this is a plane See also:mirror, 4, 6, or 8 in. in diameter, capable of rotation round a horizontal and a vertical axis. This mirror is placed at the station to be observed, and in fine weather it is kept so directed that the rays of the sun reflected by it strike the distant observing telescope. To the observer the heliotrope presents the See also:appearance of a See also:star of the first or second magnitude, and is generally a pleasant object for observing. Observations at See also:night, with the aid of light-signals, have been repeatedly made, and with good results, particularly in France by General See also:Francois Perrier, and more recently in the United States by the See also:Coast and Geodetic Survey; the See also:signal employed being an See also:acetylene See also:bicycle-See also:lamp, with a See also:lens 5 in. in diameter. Particularly noteworthy are the trigonometrical connexions of Spain and See also:Algeria, which were carried out in 1879 by Generals Ibanez and Perrier (over a distance of 270 km.), of See also:Sicily and See also:Malta in 1900, and of the islands of See also:Elba and See also:Sardinia in 1902 by Dr Guarducci (over distances up to 230 km.); in these cases artificial Astronomical Observations. The direction of the meridian is determined either by a theodolite or a portable transit instrument. In the former case the operation consists in observing the angle between a terrestrial object—generally a mark specially erected and capable of See also:illumination at night—and a See also:close circumpolar star at its greatest eastern or western azimuth, or, at any See also:rate, when very near that position.If the observation be made t minutes of time before or after the time of greatest azimuth, the azimuth then will differ from its maximum value by (4501)2 See also: sin 1" sin 25/ sin z, in seconds of angle, omitting ,smaller terms, S being the star's See also:declination and z its See also:zenith distance. The collimation and level errors are very carefully determined before and after these observations, and it is usual to arrange the observations by the reversal of the telescope so that collimation error shall disappear. If b, c be the level and collimation errors, the correction to the circle reading is b cot ztc cosec z, b being See also:positive when the west end of the axis is high. It is clear that any uncertainty as to the real See also:state of the level will produce a corresponding uncertainty in the resulting value of the azimuth an uncertainty which increases with the latitude and is very large in high latitudes. This may be partly remedied by observing in connexion with the star its reflection in mercury. In determining the value of " one division " of a level See also:tube, it is necessary to See also:bear in mind that in some the value varies considerably with the temperature. By experiments on the level of Ramsden's 3-See also:foot theodolite, it was found that though at the ordinary temperature of 66° the value of a division was about one second, yet at 32° it was about five seconds. In a very excellent portable transit used on the Ordnance Survey, the uprights carrying the telescope are constructed of See also:mahogany, each upright being built of several pieces glued and screwed together; the base, which is a solid and heavy See also:plate of iron, carries a See also:reversing apparatus for lifting the telescope out of its See also:bearings, reversing it and letting it down again. Thus is avoided the See also:change of temperature which the telescope would incur by being lifted by the hands of the observer. Another form of transit is the German See also:diagonal form, in which the rays of light after passing through the object-glass are turned by a total reflection See also:prism through one of the trans-See also:verse arms of the telescope, at the extremity of which arm is the See also:eye-piece. The unused See also:half of the ordinary telescope being cut away is replaced by a counterpoise. In this instrument there is the advantage that the observer without moving the position of his eye commands the whole meridian, and that the level may remain on the pivots whatever be the See also:elevation of the telescope.But there is the disadvantage that the flexure of the transverse axis causes a variable collimation error depending on the zenith distance of the star to which it is directed; and moreover it has been found that in some cases the personal error of an observer is not the same in the two positions of the telescope. To determine the direction of the meridian, it is well to erect two marks at nearly equal angular distances on either side of the north meridian line, so that the See also: pole star crosses the vertical of each mark a short time before and after attaining its greatest eastern and western azimuths. If now the instrument, perfectly levelled, is adjusted to have its centre See also:wire on one of the marks, then when elevated to the star, the star will See also:traverse the wire, and its exact positipn in the field a,t any moment can be measured by the micrometer wire. Alternate observations of the star and the terrestrial mark, combined with careful level readings and reversals of the instrument, will enable one, even with only one mark, to determine the direction of the meridian in the course of an See also:hour with a probable error of less than a second. The second mark enables one to See also:complete the station more rapidly and gives a check upon the work. As an instance, at See also:Findlay Seat, in latitude 57° 35', the resulting azimuths of the two marks were 177° 45' 37"•2940"•2o and 182° 17' 15"•61 to"•13, while the angle between the two marks directly measured by a theodolite was found to be 4° 31' 37"•43E0"•23• We now come to the consideration of the determination of time with the transit instrument. Let fig. 3 represent the sphere stereo-graphically projected on the plane of the horizon,—ns being the meridian, we the See also:prime vertical, Z,P the zenith and the pole. Let p be the point in which the See also:production of the axis of the instrument meets the See also:celestial sphere, S the position of a star when observed on a wire whose distance from the collimation centre is c. Let a be the azimuthal deviation, namely, the angle wZp, b the level error so that Zp=9o°—b. Let also the hour angle corresponding to p be 90°—n, and the declination of the same =m, the star's declination being S, and the Flo. latitude ..Then to find the hour 3. angle ZPS=r of the star when observed, in the triangles pPS, pPZ we have, since pPS=9o+r—n, —Sin c=sin m sin S+See also: cos m cos S sin (n—r), Sin m= sin b sin 0—cos b cos d sin a, Cos m sin n = sin b cos +cos b sin cis sin a. And these equations solve the problem, however large be the errors of the instrument. Supposing, as usual, a, b, m, rt to be small, we have at once r=n+c sec S+m tan S, which is the correction to the observed time of transit. Or, eliminating m and n by means of the second and third equations, and putting z for the zenith distance of the star, t for the observed time of transit, the corrected time is t+ (a sin z+b cos z+c)/ cos S. Another very convenient form for stars near the zenith is r=b sec ¢+c sec S+m (tan S—tan ch). Suppose that in commencing to observe at a station the' error of the chronometer is not known; then having secured for the instrument a very solid foundation, removed as far as possible level and collimation errors, and placed it by estimation nearly in the meridian, let two stars differing considerably in declination be observed—the instrument not being reversed between them. From these two stars, neither of which should be a close circumpolar star, a good approximation to the , chronometer error can be obtained; thus light was employed: in the first case electric light and in the two others acetylene lamps. let e1, e2, be the apparent See also:clock errors given by these stars if 81, 82 be their declinations the real error is e=ei+(e1-e2) (tan 0-tan 81)/(tan Si-tan 82). Of course this is still only approximate, but it will enable the observer (who by the help of a table of natural tangents can compute s in a few minutes) to find the meridian by placing at the proper time, which he now knows approximately, the centre wire of his instrument on the first star that passes—not near the zenith. The transit instrument is always reversed at least once in the course of an evening's observing, the level being frequently read and recorded. It is necessary in most instruments to add a correction for the difference in See also:size of the pivots.The transit instrument is also used in the prime vertical for the determination of latitudes. In the preceding figure let q be the point in which the See also: northern extremity of the axis of the instrument produced meets the celestial sphere. Let nZq be the azimuthal deviation=a, and b being the level error, Zq=9o°-b; let also nPq=r and Pq=Ile Let S' be the position of a star when observed on a wire whose distance from the collimation centre is c, positive when to the south, and let h be the observed hour angle of the star, viz. ZPS'. Then the triangles qPS', qPZ give -Sin c=sin 8 cos 4-cos 8 sin ,, cos (h+r), Cos 4, = sin b sin 0-}-cos b cos 4' cos a, Sin ,y sin r=cos b sin a. Now when a and b are very small, we see from the last two equations that 4,=4-b, a =r sin 4,, and if we calculate ¢' by the See also:formula cot ¢' =cot 8 cos h, the first See also:equation leads us to this result =4'+(a sin z+b cos z+c)/cos z, the correction for instrumental error being very' similar to that applied to the observed time of transit in the case of meridian observations. When a is not very small and z is small, the formulae required are more complicated. The method of determining latitude by transits in the prime vertical has the disadvantage of being a somewhat slow process, and of requiring a very precise knowledge of the time, a disadvantage from which the zenith telescope is free. In principle this instrument is based on the proposition that when the meridian zenith distances of two stars at their upper culminations—one being to the north and the other to the south of the zenith —are equal, the latitude is the mean of their declinations; or, if the zenith distance of a star culminating to the south of the zenith be Z, its declination being 8, and that of another culminating to the north with zenith distance Z' and declination 8', then clearly the latitude is s(6+6')+ 1(Z-Z'). Now the zenith telescope does away with the divided circle, and substitutes the measurement micrometrically of the quantity Z'-Z. In fig. 4 is shown a zenith telescope by H.Wanschaff of Berlin, which is the type used (according to the Central Bureau at See also: Potsdam) since about 1890 for the determination of the variations of latitude due to different, but as yet imperfectly understood, influences. The instrument is sup-ported on a strong See also:tripod, fitted with levelling screws; to this tripod is fixed the azimuth circle and a long vertical steel axis. Fitting on this axis is a hollow axis which carries on its upper end a short transverse horizontal axis with a level. This latter carries the telescope, which, supported at the centre of its length, is free to rotate in a vertical plane. The telescope is thus mounted eccentrically with respect to the vertical axis around which it revolves. Two extremely sensitive levels are attached to the telescope, which latter carries a micrometer in its eye-piece, with a See also:screw of long range for measuring differences of zenith distance. Two levels are employed for controlling and increasing the accuracy. For this instrument stars are selected in pairs, passing north and south of the zenith, culminating within a few minutes of time and within about twenty minutes (angular) of zenith distance of each other. When a pair of stars is to be observed, the telescope is set to the mean of the zenith distances and in the plane of the meridian. The first star on passing the central meridional wire is bisected by the micrometer; then the telescope is rotated very carefully through 180° round the vertical axis, and the second star on passing through the field is bisected by the micrometer on the centre wire. The micrometer has thus measured the difference of the zenith distances, and the calculation to get the latitude is most simple. Of course it is necessary to read the level, and the observations are not necessarily confined to the centre wire.In fact if n, s be the north and south readings of the level for the south star, n', s' the same for the north star, l the value of one division of the level, m the value of one division of the micrometer, r, r' the See also: refraction corrections, µ, the micrometer readings of the south and north star, the micrometer being supposed to read from the zenith, then, supposing the observation made on the centre wire, 4, = 1(s+8')+a (l4-A')m+4 (n+n'-s-s')l+1(r-r'). It is of course of the highest importance that the value m of the screw be well determined. This is done most effectually by observing the vertical movement of a close circumpolar star when at its greatest azimuth. In a single night with this instrument a very accurate result, say with a probable error of about 0"•2, could be obtained for latitude from, say, twenty pair of stars; but when the latitude is required to be obtained with the highest possible precision, two nights at least are necessary. The weak point of the zenith telescope lies in the circumstance that its requirements prevent the selection of stars whose positions are well fixed ; very frequently it is necessary to have the declinations of the stars selected for this instrument specially observed at fixed observatories. The zenith telescope is made in various sizes from 30 to 54 in. in focal length; a 3o-in. telescope is sufficient for the highest purposes and is very portable. The See also:net observation probable-error for one pair of stars is only t 0"• I . The zenith telescope is a particularly pleasant instrument to work with, and an observer has been known (a sergeant of Royal See also:Engineers, on one occasion) to take every star in his See also:list during eleven See also:hours on a stretch, namely, from 6 o'clock P.M. until 5 A.M., and this on a very See also:cold See also:November night on one of the highest points of the See also:Grampians. Observers accustomed to geodetic operations attain considerable See also:powers of endurance. Shortly after the commencement of the observations on one of the hills in the Isle of See also:Skye a See also:storm carried away the wooden houses of the men and See also:left the observatory roofless. Three observatory See also:roofs were subsequently demolished, and for some time the observatory was used without a roof, being filled with See also:snow every night and emptied every See also:morning. Quite different, however, was the experience of the same party when on the top of See also:Ben See also:Nevis, 4406 ft. high.For about a fortnight the state of the See also: atmosphere was unusually See also:calm, so much so, that a lighted See also:candle could often be carried between the tents of the men and the observatory, whilst at the foot of the See also:
The determination of the personal errors of the observers in this delicate operation is a See also: matter of the greatest importance. as therein lies probably the See also:chief source of residual error. illl(~II See also:Ili III. i These errors can nevertheless be almost entirely avoided by using the impersonal micrometer of Dr Repsold (See also:Hamburg, 1889). In this device there is a movable micrometer wire which is brought by hand into coincidence with the star and moved along with it; at fixed points there are See also:electrical contacts, which replace the fixed wires. Experiments at the Geodetic See also:Institute and Central Bureau at Potsdam in 1891 gave the following personal equations in the case of four observers: A–B Older See also:Procedure. New Procedure. –os•io8 –os•oo4 A–G -0'314 –os•o35 A–S –o'.184 -09.027 B–G –o9.225 +os•oi3 B–S –os•o86 -09.023 G–S . . . +o'-Io9 –o9•oo6 These results show that in the later method the personal equation is small and not so variable; and consequently the repetition of longitude determinations with exchanged observers and apparatus entirely eliminates the constant errors, the probable error of such determinations on ten nights being scarcely to9•oI. Calculation of Triangulation. The surface of Great Britain and Ireland is uniformly covered by triangulation, of which the sides are of various lengths from to to III miles. The largest triangle has one angle at See also:Snowdon in See also:Wales, another on Slieve Donard in Ireland, and a third at Scaw See also:Fell in See also:Cumberland; each side is over a hundred miles and the spherical excess is 64". The more ordinary method of triangulation is, however, that of chains of triangles, in the direction of the meridian and perpendicular thereto.The principal triangulations of France, Spain, See also:
Now the angle A of the triangle as measured by a theodolite is the inclination of the planes BAa and CAa, and the angle at B is that contained by the planes AB/3and CB O. But the planes See also: ABa and AB/3 containing the line AB in common cut the surface in two distinct plane curves. In order, therefore, that a spheroidal triangle may be exactly defined, it is necessary that the nature of the lines joining the three vertices be stated. In a mathematical point of view the most natural See also:definition is that the sides be geodetic or shortest lines. C. C. G. Andrae, of See also:Copenhagen, has also shown that other lines give a less convenient computation. K. F. Gauss, in his See also:treatise, Disquisitiones generales circa superricies curvas, entered fully into the subject of geodetic (or geodesic) triangles, and investigated expressions for the angles of a geodetic triangle whose sides are given, not certainly finite expressions, but approximations inclusive of small quantities of the See also:fourth order, the side of the triangle or its ratio to the radius of the nearly spherical surface being a small quantity of the first order. The terms of the fourth order, as given by Gauss for any surface in general, are very complicated even when the surface is a spheroid.If we retain small quantities of the second order only, and put A, B, @1 for the angles of the geodetic triangle, while A, B, C are those of a plane triangle having sides equal respectively to those of the geodetic triangle, then, a being the See also: area of the plane triangle and a, Li, r the measures of curvature at the angular points, A =A+a(2a+h+r) /12, = B+a(a+2h+r)/12, (Q = C+a(a+h +2t) /12.For the sphere a=h=r, and making this simplification, we obtain the theorem previously given by A. M. See also:Legendre. With the terms of the fourth order, we have (after Andrae): A–A=3+3k IT-~ 1- 4k a—k) 36–B=3+3k (m 202 20bzk+h4kk)' (II–C3+3 (M2 20 c'1z+r4kk) in which s=ak{1+(m2k/8)}, 3m2=a'+b2+c2, 3k=a+h+r. For the ellipsoid of rotation the measure of curvature is equal to I/pn, p and n being the radii of curvature of the meridian and perpendicular. It is rarely that the terms of the fourth order are required. As a See also:rule spheroidal triangles are calculated as spherical (after Legendre), i.e. like plane triangles with a decrease of each angle of about s/3; € must, however, be calculated for each triangle separately with its mean measure of curvature k. The geodetic line being the shortest that can be See also:drawn on any surface between two given points, we may be conducted to its most important characteristics by the following considerations: let p, q be adjacent points on a curved surface; through s the See also:middle point of the chord pq imagine a plane drawn perpendicular to pq, and let S be any point in the intersection of this plane with the surface; then pS+Sq is evidently least when sS is a minimum, which is when sS is a normal to the surface; hence it follows that of all plane curves on the surface joining p, q, when those points are in-definitely near to one another, that is the shortest which is made by the normal plane. That is to say, the osculating plane at any point of a geodetic line contains the normal to the surface at that point. Imagine now three points in space, A, B, C, such that AB = BC =c; let the direction cosines of AB be 1, m, n, those of BC l', m', n', then x, y, z being the co-ordinates of B, those of A and C will be respectively- x–cl : y–cm : z–cn x+cl': y+cm': z+cn'. Hence the co-ordinates of the middle point M of AC are x+ZC(1'-l), y+zc(m'–m), z+zc(n'–n), and the direction cosines of BM are therefore proportional to l'–l: m'–m: n'–n. If the angle made by BC with AB be indefinitely small, the direction cosines of BM are as Sl : Sm : 6n.Now if AB, BC be two contiguous elements of a geodetic, then BM must be a normal to the surface, and since Sl, 3m, Sn are in this case represented by S(dx/ds), 3(dy/ds), S(dz/ds), and if the equation of the surface be u=o, we have d'x /du d'y du–dzz /du ds2/dx=ds'/dy ds'/Tz' which, however, are See also: equivalent to only one equation. In the case of the spheroid this equation becomes d2x d2y yds2 –xds' =0, which integrated gives ydx–xdy=Cds. This again may be put in the form r sin a=C, where a is the azimuth of the geodetic at any point—the angle between its direction and that of the meridian—and r the distance of the point from the axis of revolution. From this it may be shown that the azimuth at A of the geodetic joining AB is not the same as the astronomical azimuth at A of B or that determined by the vertical plane AaB. Generally speaking, the geodetic lies between the two plane See also:section curves joining A and B which are formed by the two vertical planes, supposing these points not far apart. If, however, A and B are nearly in the same latitude, the geodetic may cross (between A and B) that plane curve which lies nearest the adjacent pole of the spheroid. The See also:condition of See also:crossing is this. Suppose that for a moment we drop the consideration of the earth's non-sphericity, and draw a perpendicular from the pole C on AB, See also:meeting it in S between A and B. Then A being that point which is nearest the pole, the geodetic will cross the plane curv& if AS be between ;AB and BAB. If AS lie between this last value and .AB, the geodetic will lie wholly to the north of both plane curves, that is, supposing both points to be in the northern hemisphere. The difference of the azimuths of the vertical section AB and of the geodetic AB, i.e. the astronomical and geodetic azimuths, is very small for all observable distances, being approximately: ' Geod. azimuth = Astr. azimuth – I e2 s cost cp sin 2a+ 12 t –e'pn lsin 2¢ sin a) , in which: e and a are the numerical eccentricity and semi-See also:major axis respectively of the meridian See also:ellipse, ¢ and a are the latitude and azimuth at A, s=AB, and p and n are the radii of curvature of the meridian and perpendicular at A. For s = too kilometres, only the first See also:term is of moment; its value is o"•028 cos' di sin 2a, and it lies well within the errors of observation.If we imagine the geodetic AB, it will generally trisect the angles between the vertical sections at A and B, so that the geodetic at A is near the vertical section AB, and at B near the section BA.' The greatest distance of the vertical sections one from another is e2sa cos' ¢o sin 2ao/16a', in which 00 and ao are the mean latitude and azimuth respectively of the middle point of AB. For the value s =64 kilometres, the maximum distance is 3 mm. An See also: idea of the course of a longer geodetic line may be gathered from the following example. Let the line be that joining See also:Cadiz and St See also:Petersburg, whose approximate positions are Cadiz. St Petersburg. See also:Lat. 36° 22' N. 59° 56' N. Long. 6° i8' w. 300 17' E. If G be the point on the geodetic corresponding to F on that one of the plane curves which contains the normal at Cadiz (by " corresponding " we mean that F and G are on a meridian) then G is to the north of F; at a See also:quarter of the whole distance from Cadiz GF is 458 ft., at half the distance it is 637 ft.,'and at three-quarters it is 473 ft.The azimuth of the geodetic at Cadiz differs 20" from that of the vertical plane, which is the astronomical azimuth. The azimuth of a geodetic line cannot be observed, so that the line does not enter of See also: necessity into See also:practical geodesy, although many formulae connected with its use are of great simplicity and elegance. The geodetic line has always held a more important See also:place in the See also:science of geodesy among the mathematicians of France, Germany and Russia than has been assigned to it in the operations of the English and See also:Indian triangulations. Although the observed angles of a triangulation are not geodetic angles, yet in the calculation of the distance and reciprocal bearings of two points which are far apart, and are connected by a long See also:chain of triangles, we may fall upon the geodetic line in this manner: If A, Z be the points, then to start the calculation from A, we obtain by some preliminary calculation the approximate azimuth of Z, or the angle made by the direction of Z with the side AB or AC of the first triangle. Let P1 be the point where this line inter-sects BC; then, to find P2, where the line cuts the next triangle side CD, we make the angle BP1P2 such that BP1P2+BPIA=18o°. This fixes P2, and Pa is. fixed by a repetition of the same process; so for P4, P4.... Now it is clear that the points PI, P2, Pa so computed are those which would be actually fixed by an observer with a theodolite, proceeding in the following manner. Having set the instrument up at A, and turned the telescope in the direction of the computed bearing,. an assistant places a mark P1 on the line BC, adjusting it till bisected by the cross-hairs of the telescope at A. The theodolite is then placed over P1, and the telescope turned to A; the horizontal circle is then moved through 18o°. The assistant then places a mark P2 on the line CD, so as to be bisected by the telescope, which is then moved to P2, and in the same manner Pa is fixed. Now it is clear that the See also:series of points P1, P2, Pa approaches to the geodetic line, for the plane of any two consecutive elements Ps, P„ P„+I contains the normal at P,,. If the objection be raised that not the geodetic azimuths but the astronomical azimuths are observed, it is necessary to consider that the observed vertical sections do not correspond to points on the sea-level but to elevated points.Since the normals of the ellipsoid of rotation do not in general intersect, there consequently arises an See also: influence of the height on the azimuth. In the case of the measurement of the azimuth from A to B, the instrument is set to a point A' over the surface of the ellipsoid (the sea-level), and it is then adjusted to a point B', also over the surface, say at a height h'. The vertical plane containing A' and B' also contains A but not B: it must therefore be rotated through a small azimuth in order to contain B. The correction amounts approximately to—e2h' cos' sin 2a/2a; in the case of h'=See also:i000 m., its value is o"•io8 cos'¢ sin 2a. This correction is therefore of greater importance in the case of observed azimuths and horizontal angles than in the previously considered case of the astronomical and the geodetic azimuths. The observed azimuths and horizontal angles must therefore also be corrected in the case, where it is required to dispense with geodetic lines. When the angles of a triangulation have been adjusted by the method of least squares, and the sides are calculated, the next process is to calculate the latitudes and longitudes of all the stations starting from one given point. The calculated latitudes, longitudes and azimuths, which are designated geodetic latitudes, longitudes and azimuths, are not to be confounded with the observed latitudes, longitudes and azimuths, for these last are subject to somewhat large errors. Supposing the latitudes of a number of.stations in the triangulation to be observed, practically the mean of these determines the position in latitude of the network, taken as a whole. So the See also:orientation or general azimuth of the whole is inferred from all the azimuth observations. The triangulation is then supposed to be projected on a spheroid of given elements, representing as nearly as one knows the real figure of the earth. Then, taking the latitude of one point and the direction of the meridian there as given ' See a paper " On the Course of Geodetic Lines on the Earth's Surface " in the Phil.Mag. 1870; Helmert, Theorien der hoheren Geodasie, I. 32I.obtained, namely, from the astronomical observations there—one can compute the latitudes of all the other points with any degree of precision that may be considered desirable. It is necessary to employ for this purpose formulae which will give results true even for the longest distances to the second place of decimals of seconds, otherwise there will arise an See also: accumulation of errors from imperfect calculation which should always be avoided. For very long distances, eight places of decimals should be employed in logarithmic calculations; If seven places only are available very great care will be required to keep the last place true. Now let di, co' be the latitudes of two stations A and B; a, a* their mutual azimuths counted from north by east continuously from o° to 36o°; is their difference of longitude measured from west to east; and s the distance AB. First compute a latitude 4'I by means of the formula 01=4, + (s cos a)/p, where p is the radius of curvature of the meridian at the latitude ~; this will require but four places of logarithms. Then, in the first two of the following, five places are sufficient s2 s2 e2nsin a cos a, r7=2 See also:resin 2a tan chi , P 4'—0=— cos(a-se)—77, s sin(a— 3e) co n cos(4'+ln)' a*—a= sin(4'+327) —e+18o°. Here n is the normal or radius of curvature perpendicular to the meridian; both n and p correspond to latitude and po to latitude 1(0+0'). For calculations of latitude and longitude, tables of the logarithmic values of p sin 1", n sin 1", and 2np sin i" are necessary. The following table contains these logarithms for every ten minutes of latitude from 52° to 53° computed with the elements a=20926060 and a : b=295 : 294 : Lat. See also:Log.p sin 1 "• Log.n Log'2pn sin 1" in 1 ".52 0 7.9939434 7.9928231 0.37131 to 9309 8190 29 20 9185 8148 28 30 9060 8107 26 40 8936 8065 24 5o 8812 8024 23 53 0 8688 7982 22 The See also: logarithm in the last See also:column is that required also for the calculation of spherical excesses, the spherical excess of a triangle being expressed by ab sin C/2pn sin 11'. It is frequently necessary to obtain the co-ordinates of one point with reference to another point; that is, let a perpendicular arc be drawn from B to the meridian of A meeting it in P, then, a being the azimuth of B at A, the co-ordinates of B with reference to A are AP=s cos (a—ic), BP=s sin (a—ae), where a is the spherical excess of APB, viz. s2 sin a cos a multiplied by the quantity whose logarithm is in the fourth column of the above table. If it be necessary to determine the See also:geographical latitude and longitude as well as the azimuths to a greater degree of accuracy than is given by the above formulae, we make use of the following formula: given the latitude 4' of A, and the azimuth a and the distance s of B, to determine the latitude 0' and longitude co of B, and the back azimuth a'. Here it is understood that a' is symmetrical to a, so that a*+a =36o°. Let _ B =sA/a, where A = (1—e2 sin 24,)f and 4(I2~2C2)cos 4' sin 2a, r'= 6(i 3 e2)c0524 cos' a; r, l'' are always very minute quantities even for the longest distances; then, putting K =90 -4', a'+Nis sin Z(K—B--a tan 2 sin Z(K+3'')cota See also:tana'++w=cos'(K-0—,') a 2 cos Z(K+@ r')o s sin (a'+ —a) 1 62 zat2' —~—eo sin 2(a'+3' +a) (i+12cosc 2 ) ; here po is the radius of curvature of the meridian for the mean latitude 1(0+¢'). These formulae are approximate only, but they are sufficiently precise even for very long distances. For lines of any length the formulae of F. W. Bessel (See also:Asir. Nach., 1823, iv. 241) are suitable. If the two points A and B be defined by their geographical distances and azimuths, of any two points on a spheroid whose latitudes and difference of longitude are given.By a series of reductions from the equations containing ;'' it may be shown that a+a'=3+I'+ae4w(4,'-0)2 cos 4¢o sin 4,o+... , where ¢o is the mean of 4, and 4', and the higher powers of e are neglected. A short computation will show that the small quantity on the right-hand side of this equation cannot amount even to the thousandth part of a second for k<o•1a, which is, practically speaking, zero; consequently the sum of the azimuths a+a' on the spheroid is equal to the sum of the spherical azimuths, whence follows this very important theorem (known as Dalby's theorem). If rk, See also: gyp' be the latitudes of two points on the surface of a spheroid, w their difference of longitude, a, a' their reciprocal azimuths, tan 2w =cot 2(ad-a') (cos Z(¢'—¢)/sin The computation of the geodetic from the astronomical azimuths has been given above From k we can now compute the length s of the vertical section, and from this the shortest length. The difference of length of the geodetic line and either of the plane curves is co-ordinates, we can accurately calculate the corresponding astronomical azimuths, i.e. those of the vertical section, and then proceed, in the case of not too great distances, to determine the length and the azimuth of the shortest lines. For any distances recourse must again be made to Bessel's formula.' Let a, a' be the mutual azimuths of two points A, B on a spheroid, k the chord line joining them, µ, the angles made by the chord with the normals at A and B, 4, ¢', w their latitudes and difference of longitude, and (x2+y2)/See also:a2+z2b2=i the equation of the surface; then if the plane xz passes through A the co-ordinates of A and B will be x = (a/A) cos ¢, x' _ (a/A') cos 4,' cos w, y =o y' = (a/A') cos 4,' sin w, z = (a/0) (i—e2) sin 4,, z' = (a/o') (i —e2) sin ¢', where i = (1 —e2 sin2 4,)l, A' = f i —e2 sine ¢')', and e is the eccentricity. Let f, g, h be the direction cosines of the normal to that plane which contains the normal at A and the point B, and whose inclinations to the meridian plane of A is =a; let also 1, m, n and 1', m', n' be the direction cosines of the normal at A, and of the tangent to the surface at A which lies in the plane passing through B, then since the first line is perpendicular to each of the other two and to the chord k, whose direction cosines are proportional to x'—x, y'—y, z'—z, we have these three equations f(x'—x)+gy'+h(z'—z) =o f l +gm +hn =o f l'+gm'+hn'=o. Eliminate f, g, h from these equations, and substitute l=cos ¢ l'= —sin 4' cos a m=o m' =sin a n = sin 4, n' = cos 4, cos a, and we get (x'—x) sin 4'+y' cot a—(z'—z) cos 0=0. The substitution of the values of x, z, x', y', z' in this equation will give immediately the value of cot a; and if we put for the corresponding azimuths on a sphere, or on the supposition e =o, the following relations exist cot a—cot = e2 ccc's os ¢'Q cot a'— cot.' — e2 cos 't''Q cos OA' A'sin 0—0 sin 49' = Q sin w. If from B we let fall a perpendicular on the meridian plane of A, and from A let fall a perpendicular on the meridian plane of B, then the following equations become geometrically evident: k sin sin a= (a/p') cos 4,' sin w k sin µ' sin a' = (a/J) cos 4, sin w. Now in any surface a=o we have k2 = (x'— x)2 + (y' — y)2 + (z' — z)2 — du dii (dudueduel cosµ= [(x' x)dxdu+(y"—y)ay+ (z —z)az] l k (d x2+dY2+dz2) du du du I (due due See also:duel i/ cos µ' = [(x'—x)dx,+(y—Y)ay"+(z z)dz'j'k (dx2+dye+dz'2/ a In the present case, if we put xx' zz' b b2=U, th zen a2=2U—e2(zz bz)2 cos µ = (a/k)AU ; cos µ' _ (a/k) 0'U. Let u be such an angle that (1—e2)'sin ¢=0 sin u cos rp = A cos u, then on expressing x, x', z, z' in terms of u and u', U=1—cos u cos u' cos w—sin u sin u'; also, if v be the third side of a spherical triangle, of which two sides are zir—u and zr—u' and the included angle w, using a subsidiary angle 4, such that sin 4, sin 2v=e sin 1 (u'—u) cos a(u'+u), we obtain finally the following equations: k = 2a cos ¢ sin Iv cos µ=i sec ¢ sin 2v cos µ' _A' sec 4' sin 2v sinµ sin a = (a/k) cos u' sin w sin µ' sin a' _ (a/k) cos u sin w.These determine rigorously the distance, and the mutual zenith Helmert, Theorien der hokeren Geodasie, 1. 232, 247.2 then i = a° 1 +i e2e2 cos 24,o cos See also: gaol , and approximately sin (s/2r) k/2r. These formulae give, in the case of k=o•ia, values certain to eight logarithmic decimal places. An excellent series of formulae for the See also:solution of the problem, to determine the azimuths, chord and distance along the surface from the geographical co-ordinates, was given in 1882 by Ch. M. Schols (Archives Neerlandaises, vol. xvii.). Irregularities of the Earth's Surface. In considering the effect of unequal See also:distribution of matter in the earth's crust on the form of the surface, we may simplify the matter by disregarding the considerations of rotation and eccentricity. In the first place, supposing the earth a sphere covered with a film of See also:water, let the See also:density p be a See also:function of the distance from the centre so that surfaces of equal density are concentric See also:spheres. Let now a disturbance of the arrangement of matter take place, so that the density is no longer to be expressed by p, a function of r only, but is expressed by p+p', where p' is a function of three co-ordinates 0, ¢, r. Then p' is the density of what may be designated disturbing matter; it is positive in some places and negative in others, and the whole quantity of matter whose density is p' is zero. The previously spherical surface of the sea of radius a now takes a new form.Let P be a point on the disturbed surface, P' the corresponding point vertically below it on the undisturbed surface, PP'=N. The knowledge of N over the whole surface gives us the form of the disturbed or actual surface of the sea; it is an equipotential surface, and if V be the potential at P of the disturbing matter p', M the See also: mass of the earth (the attraction-constant is assumed equal to unity) a-MN+V=C=a—¢N+V. As far as we know, N is always a very small quantity, and we have with sufficient approximation N=3V/476a, where S is the mean density of the earth. Thus we have the disturbance in elevation of the sea-level expressed in terms of the potential of the disturbing matter. If at any point P the value of N remain constant when we pass to any adjacent point, then the actual surface is there parallel to the ideal spherical surface; as a rule, however, the normal at P is inclined to that at P', and astronomical observations have shown that this inclination, the deflection or deviation, amounting ordinarily to one or two seconds, may in some cases exceed io", or, as at the foot of the Himalayas, even 60". By the expression " mathematical figure of the earth " we mean the surface of the sea produced in imagination so as to percolate the continents. We see then that the effect of the uneven distribution of matter in the crust of the earth is to produce small elevations and depressions on the mathematical surface which would be otherwise spheroidal. No geodesist can proceed far in his work without encountering the irregularities of the mathematical surface, and it is necessary that he should know how they affect his astronomical observations. The whole of this subject is dealt with in his usual elegant manner by Bessel in the Astronomische Nachrichten, Nos. 329, 330, 331, in a paper entitled "See also:Lieber den Einfluss der Unregelmassigkeiten der falser der Erde auf geodatische Arbeiten, &c." But without entering into further details it is not difficult to see how local attraction at any station affects the determinations of latitude, longitude and azimuth there. Let there be at the station an attraction to the north-east throwing the zenith to the south-west, so that it takes in the celestial sphere a position Z', its undisturbed position being Z. Let the rectangular components of the displacement ZZ' be I measured southwards e4sicos 4¢o sin 22ao/36o See also:a4.At least this is an approximate expression. Supposing s=o•ia, this quantity would be less than one-hundredth of a millimetre. The line s is now to be calculated as a circular arc with a mean radius r along AB. If eo=a(4'+4'), ao=1(18o°+a—a'), Ao—(i—e2 sin 200)1, and n measured westwards. Now the great circle joining Z' with the pole of the heavens P makes there an angle with the meridian PZ =n cosec PZ' =n sec ¢, where 4) is the latitude of the station. Also this great circle meets the horizon in a point whose distance from the great circle PZ is n sec 4) sin 4) =n tan 0. That is, a meridian mark, fixed by observations of the pole star, will be placed that amount to the east of north. Hence the observed latitude requires the correction E; the observed longitude a correction n sec 4); and any observed azimuth a correction n tan ¢. Here it is supposed that azimuths are measured from north by east, and longitudes eastwards. The horizontal angles are also influenced by the deflections of the plumb-line, in fact, just as if the direction of the vertical axis of the theodolite varied by the samc amount. This influence, however, is slight, so long as the See also: sights point almost horizontally at the objects, which is always the case in the observation of distant points. The expression given for N enables one to form an approximate estimate of the effect of a compact mountain in raising the sea-level.Take, for instance, Ben Nevis, which contains about a couple of cubic miles; a simple calculation shows that the elevation produced would only amount to about 3 in. In the case of a mountain mass like the Himalayas, stretching over some 1500 miles of See also: country with a breadth of 300 and an average height of 3 miles, although it is difficult or impossible to find an expression for V. yet we may ascertain that an elevation amounting to several hundred feet may exist near their base. The geodetical operations, however, rather negative this idea, for it was shown by See also:Colonel See also:
Then in starting the calculation of geodetic latitudes, longitudes and azimuths from A, we must take, not the observed elements ¢, a, but for 0, 4)+f, and for a, a+n tan 0, and zero longitude must be replaced by n sec O. At the same time suppose the elements of the spheroid to be altered from a, e to a+da, e+de. Confining our See also: attention at first to the two points A, B, let (¢'), (a'), (w) be the numerical elements at B as obtained in the first calculation, viz. before the shifting and alteration of the spheroid; they will now take the form (0') +1E+gn+hda+kde, (a')+1'E+g'n+h'da+k'de, (w) -f1 " +g"n+h"da+k"de, where the coefficients f, g, . . . &c. can be numerically calculated. Now these elements, corresponding to the See also:projection of B on the spheroid of reference, must be equal severally to the astronomically determined elements at B, corrected for the inclination of the surfaces there. If i;', n' be the components of the inclination at that point, then we have = (0') -4,'+fs+gn+hda+kde, n' tan ¢' =. (a') —a'+1's+g'n+h'da+k'de, n' sec ¢'= (w) —w+1" +g"n+•h"da+k"de, where 4,', a', w are the observed elements at B. Here it appears that the observation of longitude gives no additional See also:information, but is available as a check upon the azimuthal observations. If now there be a number of astronomical stations in the tri-, angulation, and we form equations such as the above for each point, then we can from them determine those values of E, n, da, de, which 'make the quantity 2+n2+S'2+n'2+ . . . a minimum. Thus we obtain that spheroid which best represents the surface covered by the triangulation.In the Account of the Principal Triangulation of Great Britain and Ireland will be found the determination, from 75 equations, of the spheroid best representing the surface of the See also: British Isles. Its elements are a=20927005*295 ft., b : a—b=28o*8; and it is so placed that at See also:Greenwich Observatory E = I '•864, n = —o"•546.(MARTEL) 615 Taking See also:Durham Observatory as the origin, and the tangent plane to the surface (determined by f _ —o"•664, n = -4"• 117) as the plane of x and y, the former measured northwards, and z measured vertically downwards, the equation to the surface is •99524953x2+•99288005y2+•9976305212 — 0.00671003xz — 41655070z =0. Altitudes. The precise determination of the altitude of his station is a matter of secondary importance to the geodesist; nevertheless it is usual to observe the zenith distances of all trigonometrical points. Of great importance is a knowledge of the height of the base for its reduction to the sea-level. Again the height of a station does influence a little the observation of terrestrial angles, for a vertical line at B does not lie generally in the vertical plane of A (see above). The height above the sea-level also influences the geographical latitude, inasmuch as the centrifugal force is increased and the magnitude and direction of the attraction of the earth are altered, and the effect upon the latitude is a very small term expressed by the formula h(g'—g) sin 20/ag, where g, g' are the values of gravity at the See also:equator and at the pole. This is h sin 24)/5820 seconds, h being in metres, a quantity which may be neglected, since for ordinary mountain heights it amounts to only a few hundredths of a second. We can assume this amount as joined with the northern component of the plumb-line perturbations. 'I he uncertainties of terrestrial refraction render it impossible to determine accurately by vertical angles the heights of distant points. Generally speaking, refraction is greatest at about daybreak; from that time it diminishes, being at a minimum for a couple of hours before and after See also:mid-day; later in the afternoon it again increases. This at least is the general See also:
The vertical angles measured at the station on See also:
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