This post builds on the post about the Michelson-Morley experiment *here*.

One “Derivation of time dilation” (e.g., *here*) uses a light clock, pictured below:

The illustration on the left shows a light clock at rest, with a light beam reflecting back and forth between two mirrors. The distance of travel is set at the beginning with the separation of the mirrors. It is like a race: one lap is a round-trip between the two mirrors. So distance is the variable in common. This is key to properly understanding the experiment.

In the stationary frame the round trip longitudinal distance between the two mirrors is 2*L*, the pace is 1/*c*, and the time of one cycle is *T* = 2*L*/*c*.

The illustration on the right shows an observer moving with lenticity *w*_{t} transversely to the light clock. In this case there are two components of motion: the longitudinal axis and the transverse axis. These components are independent of one another since they are in different dimensions. The transverse axis is the same as the stationary case above: the total distance is 2*L* and the total time is 2*L*/*c*. The mean pace is 2*T*/(2*cT*) = 1/*c*, which is equivalent to a mean speed of *c*.

The longitudinal axis is simply the Galilean transform: *t′* = *t* + *w*_{ℓ }*x* since motion in different dimensions is independent. If the light clocks coincide at *t* = 0, this is *t′* = *w*_{ℓ }*x*, which is what was given.

Thus the distance, time, and mean speed are the same for both observers and independent of their relative velocity, which is what the Michelson-Morley experiment found, though didn’t expect.