The Schwarzschild radius from general relativity is given to be $r = \frac{2GM}{c^2}$.
One can obtain the same answer using classical calculations. That is, the escape velocity of a particle is given by $v = \sqrt\frac{2GM}{r}$, which can be arranged to give $r = \frac{2GM}{v^2}$, which can be interpreted as the maximum radius for which a particle travelling at velocity $v$ cannot escape. By treating light as simply a particle travelling at velocity $c$ and substituting in the above equation, one arrives at the Schwarzschild radius.
Is it just a coincidence that the classical approach gives the same result as the general relativity result, or is there some merit to the classical approach?