Velocity
4-Vector
In Newtonian mechanics, the velocity in x direction for example, is defined as so it might be thought that is the analogous quantity, where xi is a coordinate of the space-time 4-Vector.
However, dt is not Lorentz invariant.
Instead, we should differentiate with respect to a Lorentz invariant quantity. We’ll use the proper time, dt, which is just time according to the frame of particle at its location.
(14)
Where ds is the space-time interval.
Hence, the 4-velocity of a particle can be written as:
(15)
where its components are:
or (16)
where ux, uy, uz, are the speed-components of a particle moving in the frame S.
If Lorentz matrix D acts on the 4-Vector , we get the particle speed components in the S’ frame.
(16)
The matrices product gives:
(17)
From the last expression, we obtain:
(18)
This one will be substitute in the first three relations, and we get:
(19)
One can compute the particle total speed u’ in the S’ frame:
and we get the following expression:
(20)
These relations express Einstein’s addition theorem for velocities. One can see that velocities do not add linearly in special relativity.