Crazymechanic said:
nothing can travel faster than light in a straight line to the reference frame of light.
The way you state this is somewhat misleading. First of all, there is no such thing as "the reference frame of light"; see the
forum FAQ on this. I suspect what you mean is "in the reference frame of the light source", but I'm not sure.
Second, I'm not sure what you mean by "in a straight line". I suspect you mean "with zero acceleration", but your treatment of that doesn't seem right either; see further comments below.
Third, in curved spacetime there is no unique way to define the relative speed of spatially separated objects, so the statement "nothing can travel faster than light" won't work as it stands; there are interpretations according to which distant galaxies can be moving away from us "faster than light" due to the universe's expansion. Ned Wright's cosmology FAQ has
a good discussion of this. The correct way to generalize the statement "nothing can travel faster than light" to curved spacetime is to say that "nothing can move outside the local light cones".
Crazymechanic said:
Yes that's true but here we have a different situation were we have two massive objects traveling more than 0,5c away from each other in opposite directions now in each one of theirs reference frame they are not traveling faster than light but from a third reference frame which in our case would be an observer they are both traveling the opposite direction so if light from one would want to reach the other it would have to not only catch the other star but also get back where it was when it was emitted but because the objects from which it was emitted is itself traveling away from the other one it is trying to catch, now those distances double.
In flat spacetime (i.e., if the effects of gravity are negligible), which is what I think you intend here, this is not correct if the two objects are moving at constant velocity. (Acceleration does add a complication; see further comments below.) Velocities don't add in relativity the way they do in Newtonian mechanics. cwilkins gave the correct velocity addition formula, and that all by itself is enough to answer the OP's question. No matter how fast two objects are traveling in opposite directions, if they are both traveling at less than the speed of light (which they must be), then light emitted by either one will eventually catch up to the other.
Crazymechanic said:
if we would be perfectly stationary and the massive object "B" would be traveling with 0,90 c away from us then yes ofcourse we would still see the light from it , but we are in a position where the object "B" is traveling away from us at let's say 0,9c and we ourselves are also traveling at 0,9c only the opposite direction so the distance between us grows not with 0,9c but with 1,8c.
The rate of change of this "distance between us" is irrelevant to whether light from one object can catch the other. The speed of light is independent of the speed of the source; so as soon as one object emits a light beam towards the other, that light beam is moving at c in our reference frame. Since the other object is moving at less than c in our reference frame, the light will eventually catch up to it if it is moving at a constant velocity. It doesn't matter that the object that emitted the light is moving in the opposite direction.
Crazymechanic said:
The separate observer would ofcourse see the light from each of the oppositely accelerating objects as moving with c but the thing here is not about the redshift that we see from a distant star just because the light coming in a straight path to us experiences a planet or a object in that path and the objects gravity bends it around it slowing it down.
it's about the fact that if two bodies are very far away from each other and accelerating then their light sources can't reach the other side anymore after a certain speed of acceleration and distance traveled.
Now you're confusing me because you haven't mentioned acceleration or redshift at all up to now. What exactly is the scenario you are trying to describe? Are the two objects moving in opposite directions at a constant velocity of 0.9c (relative to "us")? Or are they accelerating? Also, is this scenario set in flat spacetime or in an expanding universe?
If either object is accelerating (meaning, firing a rocket to change its velocity relative to a given inertial frame), then there *will* be a region of spacetime that can't send light signals to that object. The boundary of this region of spacetime is called the Rindler horizon, and I recommend
Greg Egan's discussion of it. Note that only one object has to accelerate for a Rindler horizon to appear; it isn't necessary that both objects accelerate (as you imply in your analogy with the cars and shooters).
But I'm not sure if that's actually what you mean by "acceleration"; you might mean the accelerating expansion of the universe, which is a different phenomenon. I can't tell for sure because your description isn't precise enough; but later on you do say this:
Crazymechanic said:
the expansion and receding or large stars or objects in universe can happen at FTL because it's not the massive objects itself that is moving faster than light (which it couldn't ) but rather spacetime, the matrix of space itself expanding and hence separating those objects which it holds further away
This is true, and *if* the expansion is accelerating (which in our universe, according to our best current knowledge, it is), it creates a "cosmological horizon", behind which objects are receding from us in such a way that we can't send light signals that will catch them. The Ned Wright cosmology FAQ that I linked to above explains this. Note that the expansion has to be accelerating for this to be true; it is *not* sufficient just for there to be galaxies that appear to be receding from us "faster than light".