Question on special relativity from "Basic Relativity"

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SUMMARY

The forum discussion revolves around a question from "Basic Relativity" by Richard A. Mould regarding special relativity concepts. The user seeks confirmation on their understanding of length contraction and time dilation as applied to a train and platform scenario. Key points include the correct application of the Lorentz transformation, which is essential for solving the problem accurately. The discussion emphasizes that the train observer perceives the length of the platform differently than the platform observer, and the need to clarify the synchronization of clocks in different reference frames.

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  • #61
[Sorry for the late reply]
PeroK said:
In any case for part b) there was no given event to transform.
Sure there is - the event is the one on the worldline of clock 2 that is simultaneous in the train frame with clock 1 reading 4:00. Taking 4:00 on clock 1 to be the shared origin, we know that this event has the same ##t'##, so ##t'=0## and we know that the length ##L## platform is length contracted to ##L/\gamma## in this frame so ##x'=-L/\gamma##. We just need to calculate ##t## for this event and relate that to 4:00.
 
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  • #62
Ibix said:
[Sorry for the late reply]

Sure there is - the event is the one on the worldline of clock 2 that is simultaneous in the train frame with clock 1 reading 4:00. Taking 4:00 on clock 1 to be the shared origin, we know that this event has the same ##t'##, so ##t'=0## and we know that the length ##L## platform is length contracted to ##L/\gamma## in this frame so ##x'=-L/\gamma##. We just need to calculate ##t## for this event and relate that to 4:00.
Isn't that equivalent to deriving the "leading clocks lag" rule in the first place? I don't see that every time you have the scenario of synchronised moving clocks, then you go back to the derivation from first principles.
 
  • #63
PeroK said:
Isn't that equivalent to deriving the "leading clocks lag" rule in the first place? I don't see that every time you have the scenario of synchronised moving clocks, then you go back to the derivation from first principles.
I find the Lorentz-every-time approach easier than remembering rules derived from it. I appreciate that not everyone agrees. 😁
 
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  • #64
Ibix said:
I find the Lorentz-every-time approach easier than remembering rules derived from it. I appreciate that not everyone agrees. 😁
I agree with you. BTW, doesn't the problem statement say that, in the platform frame of reference (and the clocks are at rest in this frame), the front of the train passes clock 1 at 4:00 and the rear of the train passes clock 2 at 4:00. Don't these same readings have to be on the ground clocks, as observed by train observers at the front and rear of the train, when the front of the train passes clock 1 and the rear of the train passes clock 2?
 
  • #65
Chestermiller said:
Don't these same readings have to be on the ground clocks, as observed by train observers at the front and rear of the train, when the front of the train passes clock 1 and the rear of the train passes clock 2?
These are spacetime events. They need no specific observer.

The physics is the same whether there is anyone on the train or not.
 
  • #66
Chestermiller said:
Don't these same readings have to be on the ground clocks, as observed by train observers at the front and rear of the train, when the front of the train passes clock 1 and the rear of the train passes clock 2?
Yes. But the question is what time does clock 2 show when the front of the train passes clock 1 according to the train observer, and "front passes 1" and "rear passes 2" are only simultaneous in the platform frame.
 
  • #67
Ibix said:
Yes. But the question is what time does clock 2 show when the front of the train passes clock 1 according to the train observer, and "front passes 1" and "rear passes 2" are only simultaneous in the platform frame.
Sorry. I guess I mis-read or mis-interpreted the question.
 
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  • #68
I wonder if this drawing of the moving platform seen fom the top would help solve the problem in this thread.
leng_con1a.jpg
 

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