How Does Time Dilation Affect Photon Transmission in Relative Motion?

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SUMMARY

The discussion focuses on the effects of time dilation on photon transmission between two observers, A and B, moving in opposite directions at speed v. In A's frame, the total time for A to receive the photon is calculated as YT(1 + v/c), while in B's frame, the time is T/(Y(1 - v/c)). The calculations reveal that both frames yield consistent results when accounting for time dilation, confirming that A's clock appears to run slower from B's perspective. The key takeaway is the importance of applying Lorentz transformations correctly to reconcile the differing observations of time.

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  • Understanding of special relativity concepts, particularly time dilation.
  • Familiarity with Lorentz transformations and gamma factor (Y).
  • Knowledge of the speed of light (c) and its implications in relativistic physics.
  • Ability to perform calculations involving relative motion and time intervals.
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  • Study the derivation and implications of Lorentz transformations in special relativity.
  • Explore the concept of simultaneity in different reference frames.
  • Learn about the twin paradox and its relation to time dilation.
  • Investigate practical applications of time dilation in modern technology, such as GPS systems.
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greendog77
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A and B leave from a common point and travel in opposite directions with
relative speed v. When B’s clock shows that a time T has elapsed, he (B)
sends out a light signal. When A receives the signal, what time does his (A’s)
clock show? Answer this question by doing the calculation entirely in (a) A’s
frame, and then (b) B’s frame.

(Y = gamma)

a)

In A's frame, when A's clock reads YT, B's clock reads T. This means B is at a distance YTv from A. When B emits the photon, the photon takes time YTv/c to reach A in A's frame. Thus, the total time for A is YT(1 + v/c).

b)

In B's frame, when his clock reads T, A is at a distance Tv away. Then, B emits a photon which travels at a speed of (c-v) relative to A in B's reference frame. Thus, the time taken for the photon to reach A is Tv/(c-v). Thus the total time this takes according to B is T + Tv/(c-v) = T(1 + v/(c-v)). By time dilation, in A the total time is YT(1 + v/(c-v)).

I get these two different answers. Does anyone know what I'm doing wrong?
 
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greendog77 said:
A and B leave from a common point and travel in opposite directions with
relative speed v. When B’s clock shows that a time T has elapsed, he (B)
sends out a light signal. When A receives the signal, what time does his (A’s)
clock show? Answer this question by doing the calculation entirely in (a) A’s
frame, and then (b) B’s frame.

(Y = gamma)

a)

In A's frame, when A's clock reads YT, B's clock reads T. This means B is at a distance YTv from A. When B emits the photon, the photon takes time YTv/c to reach A in A's frame. Thus, the total time for A is YT(1 + v/c).

b)

In B's frame, when his clock reads T, A is at a distance Tv away. Then, B emits a photon which travels at a speed of (c-v) relative to A in B's reference frame. Thus, the time taken for the photon to reach A is Tv/(c-v). Thus the total time this takes according to B is T + Tv/(c-v) = T(1 + v/(c-v)). By time dilation, in A the total time is YT(1 + v/(c-v)).

I get these two different answers. Does anyone know what I'm doing wrong?

Your calculation in B's frame is wrong. You got it correct, that the time, according to B's frame, for the photon to reach A is T_arrive = T(1+v/(c-v)) = T/(1 - v/c). But in B's frame, A's clock is running slower, so the elapsed time on A's clock is T'_arrive = T_arrive/Y = T/(Y (1-v/c)).

That's the same as your calculation in A's frame, since

T/(Y (1-v/c)) = YT (1+v/c)
 
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