Schwarzschild metric in Eddington-Finklestein coordinates reads
$$ds^2=-\left(1-\frac{2M}{r}\right)dv^2+2dvdr+r^2d\Omega^2$$
My professor claimed that at $r=2M$, this metric becomes Minkowski metric. I was suspicious about his claim, so I asked him about it after class and he hastily told me the below coordinate transform
$$t=v-r\qquad x=v+r$$
Using his coordinate transform, I obtained this metric
$$ds^2=-\left(1-\frac{2M}{r}\right)(dx+dt)^2+2(dx^2-dt^2)+r^2d\Omega^2$$
By setting $r=2M$, the first term vanishes and the metric becomes $ds^2=-2dt^2+2dx^2+r^2d\Omega^2$. I am not sure if this is the metric for the flat spacetime. Is the spacetime really flat to an observer hovering around Schwarzschild radius? If so, this observer is in an inertial reference frame?