A train with proper length L has clocks at the front and back. A photon is fired from the front to the back. Working in the train frame, we can easily say that if the photon leaves the front of the train when a clock there reads zero, then it arrives at the back when a clock there reads L/c. Now consider this setup in the ground frame, where the train travels by at speed v. Rederive the above frame-independent result (namely, if the photon leaves the front of the train when a clock there reads zero, then it arrives at the back when a clock there reads L/c) by working only in the ground frame.

Explanation:

In train's rest frame, the speed of photon is and the proper length of the train is . The time taken by the photon to cross the train is

In ground frame, the speed of the photon is given as follows:

The speed of light or photon remains same in every frame of reference.

Now, the speed of train is very less as compared to the speed of photon so that So that,

The length contraction in the ground frame is given as follows:

Time taken by the photon to travel the length of the train in ground frame is .

1 - wave length

2 - amplitude

3 - crest

4 - trough

explanation:

duh.

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explanation: