Astrophysics: Deriving Newton's Gravitational Formula from Kepler's

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knowlewj01
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Homework Statement



Dervie Newton's form of Kepler's third law.

decrribing the orbital motion of two stars in circular orbits with masses M1 and M2, separation a, and period P

ie.

Obtain

F=[tex]\frac{ G M1 M2 }{ a^2 }[/tex]

From

M1+M2=[tex]\frac{4 \pi^2 a^3 }{GP^2}[/tex]

Homework Equations



Centre of mass:

M1r1 = M2r2

a = r1 + r2

P = [tex]\frac{2\pi r}{v}[/tex]

The Attempt at a Solution



[not to good at this LaTeX thing so i'll wing it]

1: switch the (M1 + M2) For P^2

P^2 = (4π^2 a^3)/(G(M1 + M2))

switch the P for the term above:

(4π^2 r^2)/v^2 = (4π^2 a^3)/(G(M1 + M2))

π's cancel:

r^2/v^2 = a^3 / G(M1 + M2)

problem is here that i don't know what the r is, do i have to work out this for r1 and r2 seperatly?

anyone done this before that could point me in the right direction?
 
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Thanks, I think i got it, it looks a bit eggy but i got there, there may be something wrong.

M = [tex]\frac{4\pi^2r^3}{GP^2}[/tex]

P2 = [tex]\frac{4\pi^2r^3}{GM}[/tex]

[tex]\frac{4\pi^2r^2}{v^2}[/tex] = [tex]\frac{4\pi^2r^3}{GM}[/tex]

[tex]\frac{r^2}{v^2}[/tex] = [tex]\frac{r^3}{GM}[/tex]

[tex]\Rightarrow[/tex] acceleration = [tex]\frac{v^2}{r}[/tex]

a = centrepetal acceleration

[tex]\frac{r}{a}[/tex] = [tex]\frac{r^3}{GM}[/tex]

a = [tex]\frac{GM}{r^2}[/tex]

[tex]\Rightarrow[/tex] F= ma

F = [tex]\frac{GMm}{r^2}[/tex]