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Mécanique céleste (1829) Laplace, Pierre Simon, marquis de, 1749-1827, Bowditch, Nathaniel, 1773-1838, Bowditch, N. I. (Nathaniel Ingersoll), 1805-1861 · Boston, Hillard, Gray, Little, and Wilkins · leaf 832
angle saa, we have, sa = r,sa ■== R, aa = p.seed, and, by using [62] Int.we obtain the expression (9T), which is easilyreduced to the form (98), being the same as thefirst equation of La Places method [806] ; r^^.^^-2R.(p.secJ).\eos.{Çî)-a.).cosJl+{p.sec.êf=iJ2_2iJ.p.cos.(©—a)4-,A sec^.^. This last… … 797 [5994] (90)(9)) (93)(93) (93) (94) (95) (9C)(9C-) (97)(98) (90) 798 APPENDIX, BY THE TRANSLATOR; -^ which, by substituting p = iVi.p (29), becomes as in (32) ; corresponding to the thirdobservation. We shall now suppose, fora moment, that the place of the comet at the first observation,is… Celestial mechanics · Tides · Capillarity
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