Mécanique Céleste Vol.2
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In our eReader you can find the full English version of the book. Read Mécanique Céleste Vol.2 Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Mécanique Céleste Vol.2
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sin. 2 è. [2120a] The integral in the first member must be a function of n, as in [137'", &z.c] ; and at the external surface, where n = 0, it becomes constant ; hence if we divide 131 522 FIGURE OF THE ATMOSPHERES [Méc. Cél, Putting R equal to the polar radius of the atmosphere, we shall have* [2121] c = - , therefore Equation /t of the sur- face of the t 2122 ] J = - + «»*. sin. 8 i.
pheie.
[2122] To obtain the ratio of the two axes of the atmosphere, we shall put R for the radius of its equa...tor, and the preceding equation will give,t [2123] « R' 3 = 2 .
It The maximum '° U ato f r!i'i° The greatest possible value of R! is that which extends to the point where the radius to the polar . m t radium centrifugal force becomes equal to gravity. JNow in this casef -=g = «it, [2124] or v.R' 3 = l; consequently, R [2125] ~R = %' [2120c] [21206] the whole equation by im, and put — = «, it will become as in [2120], c being a constant quantity. At the equator, where sin. Ô = 1, and r = 1 [2119'"], the centrifugal force ?i 2 r .
What to read after Mécanique Céleste Vol.2?
You can find similar books in the "Read Also" column, or choose other free books by Bowditch, N. I. (Nathaniel Ingersoll), 1805-1861 to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
sin. 2 è. [2120a] The integral in the first member must be a function of n, as in [137'", &z.c] ; and at the external surface, where n = 0, it becomes constant ; hence if we divide 131 522 FIGURE OF THE ATMOSPHERES [Méc. Cél, Putting R equal to the polar radius of the atmosphere, we shall have* [2121] c = - , therefore Equation /t of the sur- face of the t 2122 ] J = - + «»*. sin. 8 i.
pheie.
[2122] To obtain the ratio of the two axes of the atmosphere, we shall put R for the radius of its equa...tor, and the preceding equation will give,t [2123] « R' 3 = 2 .
It The maximum '° U ato f r!i'i° The greatest possible value of R! is that which extends to the point where the radius to the polar . m t radium centrifugal force becomes equal to gravity. JNow in this casef -=g = «it, [2124] or v.R' 3 = l; consequently, R [2125] ~R = %' [2120c] [21206] the whole equation by im, and put — = «, it will become as in [2120], c being a constant quantity. At the equator, where sin. Ô = 1, and r = 1 [2119'"], the centrifugal force ?i 2 r .
What to read after Mécanique Céleste Vol.2?
You can find similar books in the "Read Also" column, or choose other free books by Bowditch, N. I. (Nathaniel Ingersoll), 1805-1861 to read onlineMoreLess
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