Time Dilation: Self-Consistency Problem Explained

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Discussion Overview

The discussion revolves around the concept of time dilation in special relativity, specifically addressing the apparent contradictions that arise when comparing time measurements between two inertial frames moving relative to each other. Participants explore the implications of time dilation and the conditions under which it applies, as well as the need for Lorentz transformations for accurate comparisons.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant notes that a clock in frame A is time dilated with respect to a clock in frame B, and vice versa, leading to confusion about the relationship between the two time measurements.
  • Another participant clarifies that the simple time dilation formula does not apply universally and emphasizes the necessity of using the full Lorentz transformations to accurately translate time between frames.
  • A later reply acknowledges the clarification regarding events occurring at the same location in one frame and being separated in space in the other frame.
  • Further discussion questions the validity of the initial claim about the mutual time dilation of clocks in both frames and seeks to clarify the implications of the previous responses on this claim.

Areas of Agreement / Disagreement

Participants express differing views on the validity of the initial statements regarding time dilation, with some agreeing on the need for Lorentz transformations while others question the implications of those transformations on the original claims. The discussion remains unresolved regarding the interpretation of the time dilation statements.

Contextual Notes

The discussion highlights limitations in understanding the conditions under which time dilation applies, particularly the dependence on the spatial relationship of events in different frames and the need for precise definitions when discussing time measurements.

mathman44
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Hi all.

I'm having trouble getting an intuitive understanding for the following situation. Let frame A and frame B be moving with relative velocity v.

It's true that a clock in frame A will be time dilated with respect to a clock in frame B, but also that a clock in frame B will be time dilated with respect to a clock in frame A.

i.e. any time between two events measured in frame A must be multiplied by gamma to get the corresponding time measured between those two events in frame B, and correspondingly, that time as measured in frame B must be multiplied by gamma to get the corresponding time as measured in frame A. Obviously this would mean that

t_a = \gamma^2{t_a}

Can anyone explain this apparent contradiction?
 
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mathman44 said:
i.e. any time between two events measured in frame A must be multiplied by gamma to get the corresponding time measured between those two events in frame B,
In general, that's not true. You need the full Lorentz transformations to translate the time between two arbitrary events from one frame to another.

In the special case of events that take place at the same location in A, which could be measured with a single collocated clock in A, then the simple time dilation formula would apply. (Note that events that take place at the same location in A must of necessity take place at different locations in B; so it's true that ΔtB = γΔtA, but ΔtA ≠ γΔtB.)
 
Ah... yes, if the events occur at one location in space in one frame, they must be separated in space in the other frame.

Cheers!
 
Mathman, now that Doc Al has addressed the second part of your post, can you explain how that impacts the earlier part where you said:
"It's true that a clock in frame A will be time dilated with respect to a clock in frame B, but also that a clock in frame B will be time dilated with respect to a clock in frame A."

Specifically, does his answer mean that one or both of your "true" statements are not true?

It appears to me that he was focusing on just your first statement and it appears that what you call "a clock in frame A" is what he is calling "a single collocated clock in A" but I'm wondering that if you still consider this to be a true statement, where is the clock in frame B or what clock in frame B were you talking about?
 

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