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GIVE ME A HINT! Fourier series / Kepler's equation
By expanding e \sin\psi in a Fourier series in \omega t, show that Kepler's equation has the formal solution
\psi = \omega t + \sum_{n=1}^{\infty}{\frac{2}{n}J_{n}(ne)\sin{\omega t}}
where J_{n} is the Bessel function of order n. For small argument, the Bessel function can be approximated in a power series of the argument. Accordingly, from this result derive the first few terms in the expansion of \psi in powers of e.

By expanding e \sin\psi in a Fourier series in \omega t, show that Kepler's equation has the formal solution
\psi = \omega t + \sum_{n=1}^{\infty}{\frac{2}{n}J_{n}(ne)\sin{\omega t}}
where J_{n} is the Bessel function of order n. For small argument, the Bessel function can be approximated in a power series of the argument. Accordingly, from this result derive the first few terms in the expansion of \psi in powers of e.

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