Solution
= Solution
The inward radial kick also leaves <angular momentum> unchanged and increases <orbital energy> by $m\delta^2/2$. Its <eccentricity> and <semi-major axis> equal those in case $b$, but the orientation of its <eccentricity vector> is reflected about the initial radius. The satellite initially moves inward on its <ellipse>, toward <pericentre>. \b[Neither radial kick decreases the orbital energy.]