A uniform solid sphere of mass and radius is situated at the origin. A massive particle is launched from the sphere's surface at with velocity .
When the particle lands again on the sphere, what is its -coordinate (in meters)?
Details and Assumptions:
- Universal gravitational constant
- The particle mass is much smaller than that of the sphere
- Ignore any effects of General Relativity
- The only gravity is due to the sphere
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Introduce vectors i = ⎝ ⎛ 1 0 0 ⎠ ⎞ j = 2 1 ⎝ ⎛ 0 1 1 ⎠ ⎞ k = 2 1 ⎝ ⎛ 0 − 1 1 ⎠ ⎞ Then i , j , k are a right-handed orthonormal triad such that the initial displacement and velocity of the particle are i and 2 3 i + 2 3 j . The equation of motion of the particle is r ¨ = − r 3 G M r so that d t d ( r ∧ r ˙ ) = r ∧ r ¨ = 0 , so that r ∧ r ˙ = 2 3 k is constant. The motion of the particle is in the i , j plane.
If we introduce θ so that r = r cos θ i + r sin θ j then the equation of motion tells us that r 2 θ ˙ = 2 3 r ¨ − r θ ˙ 2 = − G M r − 2 If we define u = r − 1 then d θ 2 d 2 u + u = 9 2 G M so that u = 9 2 G M + A cos θ + B sin θ for some A , B . Initially r = 1 and r ˙ = 2 3 , and hence we have that u = 1 and d θ d u = − 2 1 initially, and hence u = 9 2 G M + ( 1 − 9 2 G M ) cos θ − 2 1 sin θ The particle strikes the sphere when u = 1 , which means either sin 2 1 θ = 0 (the launch point) or tan 2 1 θ = 2 ( 2 G M − 9 ) 9 Since the position vector of the particle at the point of impact is cos θ i + sin θ j , we deduce that the x -coordinate ot the point of impact is cos θ , where θ = 2 tan − 1 ( 2 ( 2 G M − 9 ) 9 ) For the given values of G and M , this makes the answer − 0 . 3 6 5 1 1 6 . . .