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MTW section 25, from eq. 25.16 onwards, derives an orbital equation (with G=c=1, u = M/r, E and L Schwarzschild constants for energy and angular momentum respectively):
\left(\frac{du}{d\phi}\right)^2 = \frac{M^2}{L^2}(E^2-1) + \frac{2M^2}{L^2}u - u^2 + 2u^3
This equation is readily differentiable to give
\frac{d^2u}{d\phi^2}= \frac{M^2}{L^2} - u + 3u^2
which is often used for numerical integration to obtain orbital plots of r against \phi.
My question: since both equations seem to be well behaved for any u < \infty, can they be used to plot the 'infalling' orbit inside the horizon? Or are either E or L or both not valid there?
\left(\frac{du}{d\phi}\right)^2 = \frac{M^2}{L^2}(E^2-1) + \frac{2M^2}{L^2}u - u^2 + 2u^3
This equation is readily differentiable to give
\frac{d^2u}{d\phi^2}= \frac{M^2}{L^2} - u + 3u^2
which is often used for numerical integration to obtain orbital plots of r against \phi.
My question: since both equations seem to be well behaved for any u < \infty, can they be used to plot the 'infalling' orbit inside the horizon? Or are either E or L or both not valid there?