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DEFINITIVE ELEMENTS 
 
 OF 
 
 COMET 1898X, (BROOK'S) 
 
 A THESIS 
 
 PRESENTED TO THE FACULTY OF THE GRADUATE SCHOOL OF THE 
 UNIVERSITY OF PENNSYLVANIA 
 
 BY 
 JOHNATHAN T. RORER 
 
 IN PARTIAL FULFILMENT OF THE REQUIREMENTS FOR THE DEGREE 
 OF DOCTOR OF PHILOSOPHY 
 
 PHILADELPHIA 
 
 1910 
 
DEFINITIVE ELEMENTS 
 
 OF 
 
 COMET 1898 X, (BKOOK'S) 
 
 A THESIS 
 
 PRESENTED TO THE FACULTY OF THE GRADUATE SCHOOL OF THE 
 UNIVERSITY OF PENNSYLVANIA 
 
 BY 
 JOHNATHAN T. RORER 
 
 IN PARTIAL FULFILMENT OF THE KEQUIREMENTS FOR THE DEGREE 
 OF DOCTOR OF PHILOSOPHY 
 
 PHILADELPHIA 
 
 1910 
 
PRESS OF 
 THE NEW ERA PRINTING COMPANY 
 
 LANCASTER. PA. 
 
DEFINITIVE ELEMENTS OF COMET 1898 X, 
 (BKOOK'S). 
 
 Comet 1898 X was discovered October 20th, 1898, by Dr. W. 
 K. Brooks of Geneva, N. Y. Observers generally recorded the 
 brightness of its central condensation from 10 m to ll m . Mr. 
 Perrine early called attention to the similarity of the elements of 
 1881 IV (Schaeberle) to those of this comet (A. J., XIX, 145). 
 
 The provisional elements assumed' in this computation were 
 those published by Hussey (A. J., XIX, 120), based on obser- 
 vations of Oct. 21st, 23d and 25th. One hundred and eighty- 
 four observations were collected from all available sources and 
 compared with an ephemeris computed from the above elements. 
 To perfect these and lessen the residuals, a least square solution 
 regarding the orbit as elliptic was then made. The six normal 
 equations thus formed lead to indeterminate results. It was at 
 first suspected that this might be due to the perturbations of the 
 Earth pad Venus ; the computation of these perturbations for 
 the time covered by the observations showed them to be but small 
 fractions of a second of arc and they were therefore disregarded. 
 
 It was next determined to use the data at hand to obtain the 
 most probable parabolic elements. Three new normal dates were 
 selected, each being intermediate between successive pairs of 
 former normal dates and the normal equations then used to obtain 
 corrected positions for these dates. 
 
 For a parabolic orbit from these, the following elements result : 
 
 r= 1898 Nov. 23. 16356 B. M. T. 
 
 = 123 31' 34".89 ,-,,... , , , ^ . 
 
 fl = 9620'41".26 Ecliptic and MeanEqumox 
 
 = 140 21' 5".05 
 log. g =9.8786106 
 
 The usual checks were applied to verify the work. 
 
 3 
 
 240959 
 
From the above elements the positions of the comet were 
 computed for ten selected dates of observation. The resulting 
 residuals, while showing a marked improvement over those from 
 Hussey's elements, were deemed capable of further improvement, 
 and accordingly the residuals for the date of each observation 
 were found by interpolation and correction of the previous resi- 
 duals. Ten normal places were then formed from which correc- 
 tions to the above elements were derived by a second least square 
 solution. These corrections were : 
 
 ATT = - 242". 80 
 
 Ai = + 51.36 
 AI 7 = - 0.00206 
 Ag = - 0.0000284, 
 
 leading to the elements : 
 
 T= 1898, Nov. 23. 16150 
 w = 123 29' 40".30 
 ft = 96 18' 33".05 
 i = 140 21' 56".41 
 log q = 9.8785943 
 
 After the completion of the above computation forty-five ad- 
 ditional observations became available ; an effort was therefore 
 made to still further reduce the residuals by the employment of 
 these observations. Using the above elements a new ephemeris 
 was computed at four-day intervals for the time covered by the 
 observations and from this by interpolation the computed place 
 was found for each of the two hundred and twenty-nine observa- 
 tions. The residuals thus formed were plotted, and a smooth 
 curve was traced representing the points as closely as possible. 
 It was not deemed necessary to recompute the coefficients of the 
 corrections to the elements used in the normal equations, and con- 
 sequently the same normal dates were used. A least square 
 
solution reduced the twenty resulting equations to five normal 
 equations of the usual form : 
 
 [1] +38.083A7T 68.580Ai2 16.373A* 21.725A2\+8.323Ag 1 +2175.976=0 
 
 [2] 68.580 +124.173 +27.701 +38.568 15.216 3809.574=0 
 
 [3] 16.373 + 27.701 +47.936 +19.797 + 4.170 1983.742=0 
 
 [4] 21.725 + 38.568 +19.797 +15.131 - 2.766 1548.340=0 
 
 [5] + 8.323 - 15.216 + 4.170 2.766 + 3.548 + 255.329=0 
 
 From these there was obtained : AH = 31". 373 
 
 10 6 A^ = Aft = + 94 .901 
 
 ATT = +126.000 
 
 ( Ai = - 136.805 
 
 10 4 AT= A2; = + 559.540 
 
 A substitution of these values in the five normal equations leads 
 to the residuals : 
 
 -0.14 
 + 0.21 
 -0.85 
 -0.19 
 -0.05 
 
 Considering the size of the constants, the above residuals are 
 thought to be satisfactory and the following elements resulting 
 from the above corrections are adopted as the final values. 
 
 FINAL ELEMENTS. 
 Nov. 23. 21745 
 
 n AO or it fL Ecliptic and Mean Equinox 
 
 o , V* of 1898.0 
 
 i = 140 19' 39". 60 
 
 log q = 9.8786488 
 
 The short time this comet was observed, 36 days, the flatness 
 of the arc traversed, the slowness of the motion, and the difficul- 
 ties arising from its physical appearance, all combine to produce 
 indeterminate results. Much effort was expended to obtain a 
 
6 
 
 greater refinement from the data, and the present publication has 
 been long delayed in the hope that better elements might be ob- 
 tained. Further investigation, however, warrants the conclusion 
 that the above elements may be considered as final. 
 
 Since the above calculations were completed S. Sharbe has pub- 
 lished definitive elements of this comet (A. N., 164, p. 378). Both 
 parabolic and elliptic elements are given, the latter being deemed 
 definitive. These are here reproduced. A comparison with th e 
 elements given above shows substantial agreement, the greatest 
 differences being in the inclination of the orbit and the time of 
 perihelion passage. 
 
 Elements of the Author Sharbe's Parabolic Sharbe' s Elliptic 
 
 T 1898 Nov. 23. 21745 Nov. 23. 189594 Nov. 23. 195124 
 
 w 123 32' 17". 67 123 31' 53". 96 123 32' 23".70 
 
 G 96 18' 1".68 96 18' 14".47 96 18 12".46 
 
 i 140 19' 39 // .60 140 2(X 57". 50 140 20' 51". 52 
 
 log q 9.8786488 9.8785281 9.8785038 
 
 e 1. 1. 0.9997421 
 
 The value of de given by Scharbe is 0.0002579 0.000- 
 2600. The limits of error are evidently so large that there is no 
 sufficient reaaon for giving preference to elliptic elements. The 
 probable errors of all the elements indicate the indeterminate 
 character of the orbit, to which reference has already been made. 
 
MAKERS 
 
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