Time Dilation: Clock A & B Confusion

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Discussion Overview

The discussion revolves around the concept of time dilation as it relates to two clocks, A and B, moving relative to each other. Participants explore the implications of time intervals measured by each clock and the conditions under which time dilation formulas apply. The scope includes theoretical considerations and clarifications regarding the Lorentz transformations and simultaneity in different inertial frames.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant states that if clock B is moving with speed ##v## relative to clock A, then the time interval for two events measured by clock A is ##t_0## and by clock B is ##t=\gamma t_0##, suggesting time runs slower for clock B.
  • Another participant challenges the validity of the equation ##t=\gamma t_0##, indicating it only holds true when the two events occur at the same location in frame A.
  • A later reply emphasizes that the condition for the two events being the same is trivial unless ##v=0##.
  • Further clarification is provided that the general expression for time transformation is given by the Lorentz transforms, which require specifying the time and position of each event separately.
  • One participant expresses understanding after realizing the importance of the relative positions of the clocks and events.
  • Another participant points out that stating a clock is at rest relative to two events is nonsensical, suggesting that the events must occur at the same location in the rest frame of clock A.
  • One participant notes that simultaneity of events differs between inertial frames, recommending a previous post for further explanation.

Areas of Agreement / Disagreement

Participants generally agree on the limitations of the time dilation formula and the necessity of using Lorentz transformations for accurate calculations. However, there remains some disagreement regarding the interpretation of events and the conditions under which the time dilation formula applies.

Contextual Notes

Limitations include the dependence on the spatial location of events and the need for careful application of the Lorentz transformations. The discussion does not resolve the nuances of simultaneity across different frames.

Haorong Wu
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TL;DR
time dilation
Suppose there are two clocks. Clock B is moving with a speed of ##v## relative to clock A. Then clock A is moving with a speed of ##-v## relative to clock B.

Let ##t_0## be the time interval for two events in the framework of clock A, while ##t## be the time interval for the same two events in the framwork of clock B.

Then ##t=\gamma t_0##. Since ##\gamma## is greater than one, so for clock B time runs slower than for clock A.

But, also, ##t_0=\gamma t##, then time in clock A runs slower than in clock B.

This seems wrong. But where?

Thanks!
 
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Haorong Wu said:
Then ##t=\gamma t_0##.
This is not true in general. It is only true in the special case that the two events occur at the same location in frame A.
 
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Haorong Wu said:
This seems wrong. But where?

They can't possibly be the same two events except in the trivial case where ##v=0##.
 
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As others have pointed out, ##t=\gamma t_0## is a special case that only applies when the events happen at the same spatial location. That will only apply to at most one frame (unless ##v=0##, as @Mister T notes).

The general expression is the Lorentz transforms:$$\begin{eqnarray*}
t'&=&\gamma\left(t-\frac v{c^2}x\right)\\
x'&=&\gamma\left(x-vt\right)
\end{eqnarray*}$$and their inverse:$$\begin{eqnarray*} t&=&\gamma\left(t'+\frac v{c^2}x'\right)\\ x&=&\gamma\left(x'+vt'\right) \end{eqnarray*}$$Note that you need to specify the time and position of each event and transform each one separately to get its transformed time and position. Then you can work out the time difference in either frame. (A useful trick is to declare that the origin is where and when one of the events is - ##(x,t)=(0,0)## transforms to ##(0,0)##.)

We generally recommend that you forget you ever heard of the time dilation formula and always use the Lorentz transforms until you are comfortable enough with them that you can see instantly whether you are allowed to use the time dilation formula in a given situation or not.
 
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Thanks, guys. I got it now. I forgot that the clock A remain still relative to the two events. Thanks again!
 
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Haorong Wu said:
I forgot that the clock A remain still relative to the two events.

Events are points in spacetime. To say that a clock is at rest relative to two events does not make sense. Instead, what you might mean is what @Dale said: that the two events occur at the same place in the rest frame of clock A.
 

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