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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 409

An illustration from Mécanique céleste, 1829, leaf 409
iprocal action of the satellites. We can then take,[6881] foj, H.sm.(Mti-E—I), the half of the first term of the equation of the centre of Jupiter ; and this term is equal to the follovi^ing expression ; *[6882] 61208,23.sin.(M + i: —/). This being supposed, we shall have, by noticing only the… … 4a.m 4a.m5 [6886] èv = — 353,69,. sin.(M+£—/). * (3496) The equation of the centre is 2e.s\n.{nt-\-i—ra) [669] ; and by changingthe notation so as to correspond to [6274—6277], it becomes 2U.sm.{Mt-\-E—i). The [6882i ] symbol H is the same as e = 0,04807670 [4080] ; hence 2H, in seconds, is2 X…

Celestial mechanics · Tides · Capillarity

Internet Archive · Wellesley College Library · Public Domain Mark 1.0. Free to use for anything.

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