Question about relativity of simultaneity

In summary: If we could be sure that the contraction was uniform then we could use the midpoint as a measure of distance between any two points in the universe. In summary, the author is trying to say that everyone agrees that the midpoint of the train is equidistant from the ends of the train in the train frame. However, this midpoint changes depending on the frame of reference.
  • #1
AlonsoMcLaren
90
2
In the train example that supposedly shows the relativity of simultaneity, why, in the frame of the observer on the ground, the "midpoint" of the train in the train's frame is still the midpoint?

Does it have anything to do with Lorentz contraction? If so, there might be some circular reasoning here as Lorentz contraction is usually later than relativity of simultaneity in a textbook.
 
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  • #2
AlonsoMcLaren said:
In the train example that supposedly shows the relativity of simultaneity, why, in the frame of the observer on the ground, the "midpoint" of the train in the train's frame is still the midpoint?
Not sure what you mean. The midpoint of the train is a point on the train. That fact is independent of reference frame. (Just like the end of the train is still the end of the train, no matter who is watching.)
 
  • #3
AlonsoMcLaren said:
why, in the frame of the observer on the ground, the "midpoint" of the train in the train's frame is still the midpoint?
I am not clear what you are asking. The embankment observer is at the midpoint between the flashes in the embankment frame. The train observer is at the midpoint between the flashes in the train frame. Neither stays at the midpoint for more than an instant in the others frame.
 
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  • #4
DaleSpam said:
I am not clear what you are asking. The embankment observer is at the midpoint between the flashes in the embankment frame. The train observer is at the midpoint between the flashes in the train frame. Neither stays at the midpoint for more than an instant in the others frame.

On "six ideas that shaped physics" p.43 the author says

"The observer in the Home Frame (ground) will agree that the right and left clocks in the Other Frame (train) are always equidistant from the center clock in the Other Frame,"

I don't understand why. Are we in a position to be sure about this before learning Lorentz contraction? Before we learned about Lorentz contraction, how can we have any clue about the distance between the right clock and the center clock (and the distance between the left clock and the center clock) as observed from the Home Frame(ground)?
 
  • #5
AlonsoMcLaren said:
In the train example that supposedly shows the relativity of simultaneity, why, in the frame of the observer on the ground, the "midpoint" of the train in the train's frame is still the midpoint?

Are you looking at the version where the flashes are emitted from the center, or received at the center?
 
  • #6
AlonsoMcLaren said:
"The observer in the Home Frame (ground) will agree that the right and left clocks in the Other Frame (train) are always equidistant from the center clock in the Other Frame,"
How about this equivalent restatement: Everyone agrees that the midpoint of the train is equidistant from the ends of the train in the train frame.
 
  • #7
AlonsoMcLaren said:
Before we learned about Lorentz contraction, how can we have any clue about the distance between the right clock and the center clock (and the distance between the left clock and the center clock) as observed from the Home Frame(ground)?
Aren't these clocks on the train?
 
  • #8
AlonsoMcLaren said:
I don't understand why. Are we in a position to be sure about this before learning Lorentz contraction?

Homogenity is underlying in the theory. If something changes, the change is homogeneous in the front half and back half of the train.
Such a case that only front half is contracted or only back clock is delayed does not take place. This assures that the middle point remains middle in transformation.
 
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  • #9
AlonsoMcLaren said:
"The observer in the Home Frame (ground) will agree that the right and left clocks in the Other Frame (train) are always equidistant from the center clock in the Other Frame,"
Hmm, that is indeed a very confusing quote. I am not sure what the author is trying to convey. If this quote is indicative of the writing in the rest of the book then I would recommend looking for some other learning material.

AlonsoMcLaren said:
Are we in a position to be sure about this before learning Lorentz contraction? Before we learned about Lorentz contraction, how can we have any clue about the distance between the right clock and the center clock (and the distance between the left clock and the center clock) as observed from the Home Frame(ground)?
Length contraction is a derived result in most formulations of SR. Typically you would start with the two postulates, derive the Lorentz transform, and then use that to derive time dilation, length contraction, and the relativity of simultaneity. Alternatively you can start with the spacetime metric or with some basic symmetry assumptions. Either way you would derive the Lorentz transform from those assumptions, and then derive the relativistic effects.
 
  • #10
Assume any length contraction, if it existed, would be uniform. Then all reference frames will agree on which point is the midpoint between the two end points. They will only disagree on the distance from that midpoint to the ends. With that assumption, the equations can be worked out and they agree with experimental results. The assumption is a very natural one to make. The logic is not "circular". In fact, the relativity of simultaneity explains the Lorentz contraction without assuming that it exists at all.
 
  • #11
The platform observer agrees with the train observer that the distance from the midpoint to the right-hand end is equal to the distance from the midpoint to the left-hand end but because she sees this midpoint moving towards the flash at the right end she observes that it has less far to travel to reach that end. The flash from the left end has further to travel to catch up with the midpoint. Both agree that the midpoint is the midpoint, but the train observer thinks it is stationary while the platform observer thinks it is moving.
 

FAQ: Question about relativity of simultaneity

1. What is the relativity of simultaneity?

The relativity of simultaneity is a concept in the theory of special relativity which states that the perception of the timing of events can differ between two observers, depending on their relative motion. This means that two events that appear to happen at the same time for one observer may not appear simultaneous for another observer.

2. How does the relativity of simultaneity affect time?

The relativity of simultaneity is closely related to the idea of time dilation in special relativity. According to this concept, time appears to pass differently for observers in different frames of reference. This means that the perception of simultaneity can also be affected by an observer's relative motion, as time can appear to pass at different rates for different observers.

3. Can the relativity of simultaneity be observed in everyday life?

Yes, the relativity of simultaneity can be observed in everyday life, but the effects are only noticeable at very high speeds or in extreme situations, such as near the speed of light or in the presence of strong gravitational fields. In most cases, the differences in the perception of simultaneity are too small to be detected by humans.

4. How is the relativity of simultaneity related to the concept of space-time?

The relativity of simultaneity is a fundamental aspect of the theory of special relativity, which describes the relationship between space and time. In this theory, space and time are not separate entities, but are instead combined into a four-dimensional structure known as space-time. The relativity of simultaneity is an important factor in understanding how space and time are perceived differently by observers in different frames of reference.

5. What is an example of the relativity of simultaneity in action?

An example of the relativity of simultaneity is the famous "twin paradox". In this thought experiment, one twin remains on Earth while the other travels in a spaceship at near the speed of light. When the traveling twin returns, they have aged much less than their twin on Earth, due to the effects of time dilation. This shows how the perception of simultaneity can differ for observers in different frames of reference.

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