- #1
Domenicaccio
- 86
- 0
I don't know why this question puzzles me...
I believe I can understand the general idea that a lightwave moving in the vicinity of a source of gravity would be deflected by it, as in the "rubber sheet" model, and would curve slightly towards the mass.
But is this also valid when the light is traveling along a direction that directly passes through the mass?
It would seem impossible for a lightwave going straight into a large mass to be accelerated from it, since it cannot accelerate further beyond c (e.g. a ray of light from sun to earth).
And at the same time it would seem impossible that the lightwave would be "slowed down" when moving straight away from the mass (e.g. an EM wave generated on Earth and sent to space).
So does the curvature have an effect only to the lightwave's trasversal movement?
But OTOH gravity/curvature does indeed have an effect on anything non-relativistic (a "slow" mass) in a radial direction.
How do you link all these things together?
I believe I can understand the general idea that a lightwave moving in the vicinity of a source of gravity would be deflected by it, as in the "rubber sheet" model, and would curve slightly towards the mass.
But is this also valid when the light is traveling along a direction that directly passes through the mass?
It would seem impossible for a lightwave going straight into a large mass to be accelerated from it, since it cannot accelerate further beyond c (e.g. a ray of light from sun to earth).
And at the same time it would seem impossible that the lightwave would be "slowed down" when moving straight away from the mass (e.g. an EM wave generated on Earth and sent to space).
So does the curvature have an effect only to the lightwave's trasversal movement?
But OTOH gravity/curvature does indeed have an effect on anything non-relativistic (a "slow" mass) in a radial direction.
How do you link all these things together?