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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 663

An illustration from Mécanique céleste, 1829, leaf 663
the particle at D ; and it is evident that we may suppose DK to be infinite, because the action of the points situated beyond K are supposed to be insensible on the particle at D ; therefore the whole action of the body, upon the particle at D, will be represented by r?°p.(/s.n(s) in the direction… … P; lids r=^; ddx 1^~ ^ dts P, Q [34], being the forces acting upon the particle in the directions parallel to the rectangular co-ordinates x, s, respectively, and tending to increase the co-ordinates [34^]. In the present case, the only force acting upon the particle is that in [8158A], which is…

Celestial mechanics · Tides · Capillarity

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