monoman
26th July 2004, 02:41 AM
Hi All,
I’m familiar with the special relativity thought experiment involving a train carriage travelling to the right at a uniform velocity close to the speed of light. Two pulses of light are emitted, at the same time, from the centre of the carriage in opposite directions left and right. To an observer stood in the centre of the train (Einstein), the light pulses hit the carriage walls at the same time. To an observer on the platform (Me), the light pulse that is travelling left will hit the wall first because the wall is moving towards it.
Therefore, the simultaneity of the events depends on the frame of reference.
So, let’s say that the simultaneity of the events determines whether Einstein is going to shoot his cat or not. (There’s a cat and gun in the carriage too). If Einstein sees the two beams of light hit the carriage walls at the same time then the cat dies.
Now to me, I don’t mind the fact that the event’s simultaneity depends on the frame of reference but I can’t have the cat entering a quantum world of dead or alive depending on who observed the event. However, I think there’s no paradox here. As I observe the light beam going to the left, it reflects off the wall first but then has some chasing up to do to get to Einstein’s eyes which are now moving away from him. I think the reverse situation happens with the light beam going to the right so that both beams hit Einstein’s eyes at the same time. Is this right, or have I taken leave of my senses??
I’ll assume it’s right and enter another variable into the equation. As soon as the left beam hit’s the wall, Einstein pulls the emergency cord, which ignites a rocket on the right side of the train, and brings the train to a very quick halt relative to me. (If this causes problems with metal warping, spilt tea etc then just imagine an incredibly large carriage that we can bring to a halt at a nice reasonable pace over time).
I’ve now just realised typing this that my original question probably now doesn’t hold. I was assuming that both beams of light would still, according to Einstein, hit his eyes simultaneously but because the carriage is now accelerating this may not hold. Is this right?
Let me waste our time for moment and assume they do hit his eyes simultaneously, wrt him. So, the left beam, which has reflected from the wall, now has the advantage that Einstein is moving away from it slower & slower, wrt me, and vice versa for the right beam (after it has reflected off the wall). At the point where the carriage is at a stand still wrt me, both beams must be an equal distance from Einstein’s eyes to ensure that the cat dies wrt both of us.
How is this so? It obviously has something to do with general relativity due to the acceleration. Does the thrust on the right side of the carriage cause more length contraction on the right side, or time dilation or …spilt tea?…… Jesus, help!
Sorry for the long post
Oh, one more thing. What is it fundamentally about General Relativity that requires it to be described in terms of warping space. Could the equations also be described in terms of a classical force?
I’m familiar with the special relativity thought experiment involving a train carriage travelling to the right at a uniform velocity close to the speed of light. Two pulses of light are emitted, at the same time, from the centre of the carriage in opposite directions left and right. To an observer stood in the centre of the train (Einstein), the light pulses hit the carriage walls at the same time. To an observer on the platform (Me), the light pulse that is travelling left will hit the wall first because the wall is moving towards it.
Therefore, the simultaneity of the events depends on the frame of reference.
So, let’s say that the simultaneity of the events determines whether Einstein is going to shoot his cat or not. (There’s a cat and gun in the carriage too). If Einstein sees the two beams of light hit the carriage walls at the same time then the cat dies.
Now to me, I don’t mind the fact that the event’s simultaneity depends on the frame of reference but I can’t have the cat entering a quantum world of dead or alive depending on who observed the event. However, I think there’s no paradox here. As I observe the light beam going to the left, it reflects off the wall first but then has some chasing up to do to get to Einstein’s eyes which are now moving away from him. I think the reverse situation happens with the light beam going to the right so that both beams hit Einstein’s eyes at the same time. Is this right, or have I taken leave of my senses??
I’ll assume it’s right and enter another variable into the equation. As soon as the left beam hit’s the wall, Einstein pulls the emergency cord, which ignites a rocket on the right side of the train, and brings the train to a very quick halt relative to me. (If this causes problems with metal warping, spilt tea etc then just imagine an incredibly large carriage that we can bring to a halt at a nice reasonable pace over time).
I’ve now just realised typing this that my original question probably now doesn’t hold. I was assuming that both beams of light would still, according to Einstein, hit his eyes simultaneously but because the carriage is now accelerating this may not hold. Is this right?
Let me waste our time for moment and assume they do hit his eyes simultaneously, wrt him. So, the left beam, which has reflected from the wall, now has the advantage that Einstein is moving away from it slower & slower, wrt me, and vice versa for the right beam (after it has reflected off the wall). At the point where the carriage is at a stand still wrt me, both beams must be an equal distance from Einstein’s eyes to ensure that the cat dies wrt both of us.
How is this so? It obviously has something to do with general relativity due to the acceleration. Does the thrust on the right side of the carriage cause more length contraction on the right side, or time dilation or …spilt tea?…… Jesus, help!
Sorry for the long post
Oh, one more thing. What is it fundamentally about General Relativity that requires it to be described in terms of warping space. Could the equations also be described in terms of a classical force?