The Event Horizon Condition
At r = r_s = 2GM/c^2, the coefficient g_tt = -(1 - r_s/r) becomes zero, and g_rr = (1 - r_s/r)^-1 becomes infinite. This surface is defined as the event horizon.
Coordinate Singularity
The divergence of g_rr at r = r_s is a coordinate singularity, not a physical one. It arises because the standard Schwarzschild coordinates break down at the horizon, similar to how longitude is undefined at the Earth's poles. Physical quantities like tidal forces remain finite here.
Light Cone Behavior
As r approaches r_s from above, the light cones tilt inward. At the horizon, the outward-pointing light ray remains stationary at r = r_s. Inside the horizon, all future-directed light rays point toward decreasing r, meaning escape is impossible.