Given potential is V=−krV = -\frac{k}{r}V=−rk
Let L be angular momentum then total effective potential will be
V0=V+L22Mr2=−kr+L22Mr2V_0 = V + \frac{L^2}{2Mr^2} = -\frac{k}{r} + \frac{L^2}{2Mr^2}V0=V+2Mr2L2=−rk+2Mr2L2
Differentiate with respect to r and differentiation will be zero at r=r0r = r_0r=r0
Hence, dVdr=kr2−L2Mr3\frac{dV}{dr} = \frac{k}{r^2} - \frac{L^2}{Mr^3}drdV=r2k−Mr3L2
dVdr∣r=r0=kr02−L2Mr03=0\frac{dV}{dr}|_{r=r_0} = \frac{k}{r_0^2} - \frac{L^2}{Mr_0^3} = 0drdV∣r=r0=r02k−Mr03L2=0
Solving it we get,
L=kMr0L = \sqrt{kMr_0}L=kMr0
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