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If the captured object do not have tangential velocity, it's just the free-fall time. But when it has, it may take longer time to fall in, right ? The function should be $\ddot{r} = -GM/r^2 + (v_0r_0/r)^2 / r = -GM/r^2 + v_0^2r_0^2 / r^3$ , where v_0 is the initial tangential velocity . After one integration, it becomes $\dot{r}^2/2=GM(1/r-1/r_0)-v_0^2r_0^2(1/r^2-1/r_0^2)/2 $ . I don't know how to deal with it. But I guess there is a analytic solution. Anyone knows something about it ? |
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We are talking just Newtonian gravity here. You should probably know that the orbit in this case is just a conic section. Depending on the initial angular momentum and energy you can compute the closest point to the star on the orbit. The object will fall into star if and only if this point is inside the star. Now, supposing you already determined that the object will fall into the star, you can solve for the point of crossing star's surface (this is just geometry, intersection of the conic section and the circle) and then solving for the time of arrival into that point. All of this is simplified by noting that you only need to know the $r$-coordinate which is simply the radius of the star. So this all boils down to finding a solution to your equation. You can do that just by taking a square root, separating variables and computing the integral. That will give you dependence of $t = t(r)$. So then just plug in the radius of the star and you're done. This means that the problem is reduced to finding integrals. Try some software for that (because the integral doesn't look easy) like Wolfram Mathematica Integrator. If you have any problems with this I suggest you ask what to do next at math.SE to get better answers. |
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