aditya23456 said:
suppose we have a moving frame and a rest frame..we know time dilution and length contraction had occurred in moving frame wrt rest frame,this is to make sure that speed of light is same in any frame..but this is not the case..consider measurement of speed of light in moving frame wrt rest frame we get...speed=distance/time
=x/t(gamma)(gamma)
Hence it is c/(gamma)^2
But we need it to be c right.?
So having a additional (gamma)^2 should be rectified and how's it done.?
If you look at the Lorentz transforms, there are actually 3 effects, and they are all three involved in the invariance of the speed of light:
- Length contraction
- Time dilation
- Relativity of simultaneity
The meaning of the latter is that clocks that are synchronized according to one coordinate system are NOT synchronized according to another. You have to take this into account when computing how things look in different frames--if you only use length contraction and time dilation, you'll get inconsistent results.
Here's the derivation using Lorentz transformations:
x' = γ (x - vt)
t' = γ (t - vx/c
2)
So dividing them gives:
x'/t' = (x-vt)/(t - vx/c
2)
If we let u = x/t and u' = x'/t', we find:
u' = (ut - vt)/(t - uvt/c
2)
= (u-v)/(1-uv/c
2)
So what that means is that if an object has speed u in the unprimed frame, then it has speed u' = (u-v)/(1-uv/c
2) in the primed frame. In the special case in which u=c (the object is a light signal), we find:
u' = (c-v)/(1-cv/c
2) = c
Now, the derivation in terms of length contraction, time dilation and relativity is a little complicated. But suppose that we measure the speed of light in the primed frame this way:
- Take two clocks at rest in the primed frame.
- Bring them together at x'=0 and set them to the same time, say t1'.
- Now, slowly move one of the clocks to the point x' = L. Let t2' be the time on that clock when it reaches its destination.
- At time t3' according to the first clock at x'=0, send a light signal from the first clock to the second.
- Let t4' be the time on the second clock when the light signal is received.
- Then the measured speed of light will be c = L/(t4' - t3')
To convince yourself of the last point from the point of view of the unprimed observer requires considering a bunch of different factors:
- The moving clocks are running slow, by a factor of γ.
- The second clock must travel even faster than the first clock in order to get to the point x' = L. So while it is traveling, its time dilation is even greater than the other clock. So afterward, it is no longer in synch with the first clock. Working it out, you'll find that it is running slow, compared with the first clock by an amount vL/c2.
- The distance between the clocks isn't L, but is L/γ, according to the unprimed observer.
- Light takes longer than time L/(c γ) to go from the first clock to the second, because the second clock is moving.
If you take all these into account, you'll find that the measured speed of light in the two frames is the same.