00:01
Is length contraction in two dimensions where the length contraction is only happening in one of the two directions.
00:08
So i have the gamma term, which is the lorentz modification scaling factor.
00:17
And i have the ordinary equation for length contractions, l prime equals the proper length divided by gamma.
00:26
We have a rod of length l in a frame that's moving at speed v.
00:31
So ordinarily, you have a stationary frame s and a moving frame s prime, and the left -hand side is as observed from the stationary frame, and you're relating what the length would be in the moving frame.
00:57
In this problem, they inverted the situation.
01:01
So they have the observer being in the stationary frame.
01:09
So they're observing the proper length lp, and then some frame moving speed v away in the same direction is what refers to the length l.
01:23
So it's a subtle thing.
01:25
It inverts the whole problem.
01:27
So just be clear, this is, the length would be more.
01:59
Moving frame.
02:06
Okay, so since this is an inverted situation, this means that what you actually have, the stationary frame is lp, the proper line, and then it's l divided by gamma.
02:21
So that's the real situation here.
02:25
So l is degrees theta from the x -axis, and l -p is theta p.
02:38
So since the speed is only in the x direction, nothing on the y direction.
02:48
There's no length contraction at all in the y direction.
02:52
And we have to find the x and y components of the length on the x and y axis...