Consider two-body central force problem in polar co-ordinates $r, \theta$. Corresponding 2nd order differential equation is obtained by using conservation of angular momentum. This equation is :
$$ \frac{d^2 r}{dt^2} = \frac{l^2}{m^2r^3} - \frac{GM}{r^2}$$
where $r(t)$ is radial position of particle (of mass $m$) as a function of time $t$, $l$ is angular momentum which is constant, $G$ is gravitational constant & $M$ is mass of the heavier body, assumed to be at rest at the origin of co-ordinate system i.e. at $(r,\theta)=(0,0)$.
I want to solve above non-linear differential equation; it is non-linear since dependent variable $r$ has powers -3 and -2 on RHS.
Can I use 4-order Runge-Kutta method to solve this equation ?