I was so bored on a flight, so I borrowed a pen from my neighbor passenger and wrote a quick derivation of a few results in special relativity:
Suppose an observer is doing a light speed measurement on a train by measuring the time it takes to go upwards and then reflect back and measure the time elapsed, he measures the time elapsed to be 2t and the distance traveled to be 2h.
But the train is moving, so to an observer outside of the train, he measures the light moved in diagonal manner, let the time spent to be t0, and the overall distance the light traveled is 2√(vt0)2+h2. We assumed the two observers measure the same h and the same v.
Both measurements are speed of light, so they equals:
2h2t=2√(vt0)2+h22t0=c
First, we cancel out all the 2.
ht=√(vt0)2+h2t0=c
Suppose an observer is doing a light speed measurement on a train by measuring the time it takes to go upwards and then reflect back and measure the time elapsed, he measures the time elapsed to be 2t and the distance traveled to be 2h.
But the train is moving, so to an observer outside of the train, he measures the light moved in diagonal manner, let the time spent to be t0, and the overall distance the light traveled is 2√(vt0)2+h2. We assumed the two observers measure the same h and the same v.
Both measurements are speed of light, so they equals:
2h2t=2√(vt0)2+h22t0=c
First, we cancel out all the 2.
ht=√(vt0)2+h2t0=c
Square the second equality to get
(vt0)2+h2=c2t20
Rearranging, get
h2=(c2−v2)t20
Dividing by c2 get
h2c2=(1−v2c2)t20
But h2c2 is simply t2 by the first equality, therefore
t2=(1−v2c2)t20
or
t=√1−v2c2t0.
The equation shows a few things:
First, v≤c, for it does not make sense to have imaginary time. That indicates nothing can run faster than the speed of light.
Second, 0≤√1−v2c2≤1, therefore, the time interval between the same events is shorter for the observers on the train. Suppose t0=1 second, then t is less than a second, so if there is a clock there, it doesn't tick yet. So for the observer outside the train, it appears that a moving clock go slower. This is called time dilation.
Third, since the both observers agrees on the relative velocity, the distance traveled, measured by the two observers are vt and vt0 respectively. We know t≤t0, therefore, to the observer on the train, distance appears shorter as well. This is called length contraction.