SPECIAL  THEORY  OF 

RELATIVITY

 

 

 

 

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Experiment 5

    A light clock lies on its side on a railroad car as the car moves to the left with velocity v.


Question: How is the length of the clock affected?

Answer:

We know that the time between ticks on the moving clock, as we see it, will be tī = . Let,

t1 = time that takes the light to go from the first mirror to the second , as we perceive it.
t2 = time that it takes the light to go from the second mirror back to the first, as we perceive it.
Lī= length of the light clock, as we perceive it.

We can analyze the situation as follows:


From the above picture we see that the distance the light traveled in time t1 was Lī+ vt1. However, this distance is also equal to ct1 (rate x time). Also, the distance the light traveled on the return trip was Lī- vt2 = ct2. Solving for t1, we have

Lī+ vt1 = ct1

which implies that Lī= ct1 - vt1,

which implies Lī= (c - v)t1,

which implies t1 = .

Similarly,

Lī- vt2 = ct2

which implies that Lī= ct2 + vt2,

which implies Lī= (c + v)t2,

which implies t2 = .

Thus,

tī = t1 + t2


=


=


=


which implies that = .

Since t = (2L)/c,

=


which implies that = ,


which implies = ,


which implies = ,


which implies Lī = L .


Conclusion

    Since is less than 1, this shows that we will measure the length of his light clock as being less than ours. Thus, when an object is moving in a straight line with a fixed velocity v, we will see its length, as measured in the direction in which it is moving, shorten.