A particle of mass m is attracted to a force center with the force of magnitude k/ r2. Use plane polar coordinates and find Hamilton's equations of motion.
F=kr2,F=\frac k{r^2},F=r2k,
L=T−U=mr˙22−Fr,L=T-U=\frac{m\dot r^2}2-Fr,L=T−U=2mr˙2−Fr,
∂L∂r−ddt∂L∂r˙=0,\frac{\partial L}{\partial r}-\frac d{dt}\frac{\partial L}{\partial \dot r}=0,∂r∂L−dtd∂r˙∂L=0,
mrr˙−kr2r¨=0.mr\dot r-\frac k{r^2}\ddot r=0.mrr˙−r2kr¨=0.
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