Train Experiment Problem: Solve Derailment Mystery!

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    Experiment Train
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Discussion Overview

The discussion revolves around a train experiment problem involving relativistic effects during acceleration, specifically addressing the synchronization of clocks on a moving train and the implications of acceleration on the train's structure and behavior. Participants explore concepts related to length contraction, the Bell's spaceship paradox, and the effects of acceleration on time perception within the train's frame.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes a scenario where the rear and front of the train are programmed to accelerate simultaneously, raising concerns about potential derailment due to the timing of their movements.
  • Another participant references the Bell's spaceship paradox to illustrate the complications of synchronized acceleration in a relativistic context.
  • A different viewpoint suggests that assuming instantaneous acceleration can lead to confusion, advocating for a consideration of normal acceleration instead.
  • One participant explains that as the train accelerates, it undergoes length contraction, which affects the perceived acceleration of the rear compared to the front, while maintaining a constant distance in the train's frame.
  • There is a discussion about how light signals emitted from the front and rear of the train behave differently due to relativistic effects, leading to discrepancies in perceived clock rates between the two ends of the train.
  • Another participant emphasizes the importance of understanding that there is no instantaneous acceleration in reality, noting the extreme forces that would be involved in such a scenario.

Areas of Agreement / Disagreement

Participants express differing views on the implications of acceleration and synchronization of clocks, with no consensus reached on the best approach to understanding the problem. Some agree on the need to consider normal acceleration, while others highlight the complexities introduced by relativistic effects.

Contextual Notes

Participants note that assumptions about instantaneous acceleration can lead to misunderstandings, and that the discussion is limited by the need for a clearer understanding of accelerating world lines and their implications in special relativity.

Stephanus
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Dear PF forum,
I have a problem with Train experiment.
Perhaps someone can take a look at it and tell me where did I go wrong?
Janus said:
trainsimul1.gif
V = 0.6c;
Gamma = 1.25
Train length = 1500
Platform length = 1200, so the light can reach the observer at the same time.
I draw the space diagram for that problem:
ST-01.jpg

Where the train (Green) is at rest first. The cars in train synchronize their clock. And preprogrammed at S1 (for the train Stern) and B1 (for the train Bow), it moves to the station.
But in platform frame, S and B can't reach the platform at the same time wrt platform.
See, the zoomed section.
And if I draw this as Pic 2
ST-02.jpg

Then, S1 and B1 don't start at the same time wrt train rest. This means that S1 (stern) starts first then the bow follows. Shouldn't it derail or destroy the train if the back car moves first?
Where did I go wrong?
Can anyone help?

Thanks.
 
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Stephanus said:
Where the train (Green) is at rest first. The cars in train synchronize their clock. And preprogrammed at S1 (for the train Stern) and B1 (for the train Bow), it moves to the station.
The train will break if both ends try to accelerate at the same time (as synchronized before). This is Bell's spaceship paradox.
 
The problem is that you are trying to assume instantaneous acceleration and that can be confusing.

Instead consider normal acceleration:

As the train gains speed it contracts as seen in the frame of the tracks, so in effect, the rear of the train does accelerate faster than the front, but since the train is undergoing length contraction at the same time, there is no "squeezing" of the train in the train's frame.

The world lines of the two train ends will look something like this in the embankment frame with the rear of the train's world line line curving slightly differently than the front of the train. Notice how they get closer together. ( the yellow "light" lines, I'll touch on later.)

accdopp1.gif


At any point, the distance between the two ends will equal to the length contracted length of the train while moving at that speed.

In the train's frame, the length of the train stays fixed. If we want to look the space time diagram for the train we are stuck with picking a particular "moment" during the acceleration. If we want to see the whole acceleration period we would need to look at a series of images. In each image, the distance between the ends of the train at that instant will always be the same.
Here's the moment close to when the lights emitted when the train started accelerating reach the opposite ends.

accdopp2.gif


I picked this moment as it demonstrates what happens to clocks in the train frame when the train is under acceleration. The two sets of light pulses were sent with the same time separation. ( shown in the first image), but on arrival, the pulses hitting the rear of the train are closer together,and the pulses hitting the front are spaced further apart. In effect, the rear of the train will see light coming from the front of the train as blue-shifted and the front of the train will see light coming from the rear as red-shifted. Further someone in the rear will see a clock in the front running fast, and someone in the front sees a clock in the rear run slow.

Now typically when we deal with a Doppler shift, even Relativistically, there is a component of that shift that is due to the changing distance between the sender and receiver. It is after you factor this component out that you are left with the time dilation component. But in this situation, this isn't the case, as far as occupants of the train are concerned, the distance from front to back remains constant at all times, so there is no changing distance component to account for, and all that is left is the time dilation component. Ergo, as far as anyone in the train is concerned, the clock in the front of the train really runs faster than the one at the rear. If the clocks started in sync before acceleration, they will be out of sync afterwards. (this means that if you want the clocks to be in sync for the up coming experiment, you will have to re-sync them after the acceleration. )
 
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Janus said:
The problem is that you are trying to assume instantaneous acceleration and that can be confusing.

Instead consider normal acceleration:[..]
Thanks a lot! That makes things clear for me. No I know what I don't know.
I think it's about time to study accelerating world line?
 
Janus said:
The problem is that you are trying to assume instantaneous acceleration and that can be confusing.

Instead consider normal acceleration:
Yes, there's no such thing as instanteous acceleration in real world. We "talk" instant acceleration to understand the concept of SR. Instant acceleration even as small as 0.0%c per second -> 30km/sec2 will kill any passenger in the rocket. 3000g?
 

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