v_bachtiar said:
Why can't light escape black holes?
Isn't light as an electromagnetic radiation massless, thus not affected by gravitational pull?
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Even in classical physics, there is an expected divergence of light with gravity. I've never fully understood this myself, but as a start, note that the acceleration of a very light body in a gravitational field is independent of its mass.
If you drop a one kilogram weight, it falls at the same speed as a two kilogram weight.
This is because there is an equivalence of "inertial mass" (which says how much force is required to make something diverge a bit) and "gravitational mass" (which says how much force is applied in a gravitational field).
Light may be massless... but that's both inertial mass and gravitational mass, in classical physics. I think. You can apply a limit as both internal and gravitational mass tend to zero, and that (I think) is the classical expectation for light... assuming the equivalence of inertial and gravitational mass. (Someone correct me if I have this wrong).
Consider a particle of mass m being pushed around by a large mass M. The force involved is GmM/r^2. The amount of gravitational acceleration is F/m, or GM/r^2.
Note that the "m" term is now gone.
Although you actually need relativity to analyze a black hole properly, you can calculate the boundary beyond which light cannot escape using classical physics.
Potential energy of a lightweight particle is -GMm/r. Kinetic energy is 0.5mv^2.
A particle is gravitational bound when GMm/r > 0.5mv^2, so the escape velocity at distance r is v=sqrt(2GM/r). The quantity "m" does not appear. If you use "c" as the escape velocity and solve for r, you actually get the Schwartzchild radius of a black hole: 2GM/c^2
Classical physics is an approximation. For a full treatment, you need some quantum physics in which light does have inertia in the sense of having momentum; and some relativity to deal properly with gravity in terms of geometry rather than a force in Euclidean space. But it turns out you still get the same result for the limit at which light is trapped at a black hole.
Cheers -- sylas