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