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由角动量守恒得出Kepler问题中$θ$和$t$的关系(Kepler第二定律):
这份讲义的45页的6.21式:
Time dependence The time dependence may be recovered by solving $\dot{\theta}=h u^{2}(\theta)$ as
$$
h t=\int \frac{\mathrm{d} \theta}{u^{2}(\theta)}=r_{0}^{2} \int \frac{\mathrm{d} \theta}{(1+e \cos \theta)^{2}}
$$
which gives $t$ as a function of $\theta$.
WolframAlpha:
Maple:
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