JesseM
Science Advisor
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Not exactly, I mean what if you consider things from the perspective of an inertial frame where B is at rest after B accelerates. In this frame, A and B will initially both be traveling at velocity v, then B will accelerate and come to rest, while I'm not sure if you would say this would be true "from B's perspective" (perhaps you would say that both A and B were initially at rest from B's perspective)--as always, it's tricky to talk about the "perspective" of an observer who accelerates at any point during the time period you're considering, it's better to analyze the whole problem from the point of view of a single inertial frame.yogi said:All right Jesse - I will try to say it in a way that conveys what Einstien said as I see it unambiguously - let's keep it real simple. A and B at rest in the same frame separated by a distance d. Clocks brought to sync. B starts moving toward A at relative velocity v (a short acceleration to get up to speed - then cruises at constant relative v). Einstein says when B arrives the clocks will no longer read the same - B's clock lags (has logged less time - is younger - whatever you want to call it).
I am saying that this is a real difference - it is not an observational apparency - it is a real objective difference in the two clocks.
I think your question is - what if you consider things from B's perspective
Alternately, if you don't want to talk about "frames", you could talk about the perspective of a third observer C who has been traveling at velocity v relative to A since the beginning of the time period we're looking at, who at first sees B traveling at v and then sees B accelerate and come to rest.
I think the problem is that when you say "B's frame" you are considering a perspective where A is initially at rest and synchronized with B, but then after B accelerates A is moving with velocity v and running slow. But again, this isn't a valid frame, since acceleration was involved. If you consider things from the perspective of that third observer C who was always traveling at v relative to A, this observer C will initially see A and B traveling together at velocity v, and will see A's clock ahead of B's by vd/c^2. Then B will accelerate and come to rest, while A continues to move at velocity v in the direction of B. A's clock will be ticking slower than B's, but because A's was already ahead, A's clock will still be ahead when A and B meet. C's prediction about how much A's clock will be ahead of B's when they meet will exactly match the prediction made in A's frame, even though in this frame the explanation for why A's clock was ahead will be different.yogi said:once B is in motion, according to the transforms and the fact that B is now in an inertial frame - why can't he say that A's clock is running slow. He will measure it to be running slower if he considers himself at rest and A moving toward him in his own frame.
But if B draws this conclusion, it cannot be a reality. There is only apparent symmetry. When the two clocks arrive, we cannot have a result where B's clock reads less than A's while at the same time A's clock reads less than B's. So if you try to do the problem in the frame of B you would get a different answer if you fail to include the initial conditions
So, do you agree that the description from C's perspective is just as valid as the description from A's perspective? If not, do you at least agree that all mainstream physicists, including Einstein, would say that the perspective of one inertial frame is just as good as any other?
What if we only start looking at the problem at some time t after B has accelerated? Aren't the initial conditions at t enough to make complete predictions about what will happen in the future, without knowing what happened before t (ie without knowing if it was A or B who accelerated?)yogi said:But if you take into account the inital conditions (namely - how did the relative motion come about) you will get the correct answer in any frame in which the motions are transformed.
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