The force is central force, so its torque about the star vanishes. The specific angular momentum is therefore constant:
Taking the scalar product of with gives
Thus conservation of energy gives the second constant
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Put . Since , the radial equation becomes the Binet equation
where primes denote derivatives with respect to the polar angle. Choosing the angular origin at periapsis gives
Writing the semi-latus rectum as yields the Kepler orbit
Hence the specific angular momentum and specific orbital energy are
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In axes directed toward periapsis and along the motion there, the position is . Differentiating it and using gives
Differentiating the orbit equation gives , and substitution simplifies the components to
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Let be the speed of the circular Kepler orbit at radius . The release velocity relative to the planetesimal is
The particle starts at the same position as its parent, so the change in specific orbital energy is
Using the velocity components from part (c),
Since and , rearrangement gives
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The kick changes the tangential velocity by . With and , the new specific angular momentum is
Every Kepler orbit satisfies . Combining this identity with the value of found in part (d) gives
where is the explicit function of in part (d).
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An orbit is unbound precisely when its specific orbital energy is nonnegative, equivalently . At periapsis, , and for the condition from part (d) is
The directions are sampled from the uniform distribution on a circle. The fraction satisfying is ; setting it equal to gives . Therefore
The positive root is
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