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.

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