G2

f

f * \

1 + g2

U - -

V

I g2 V

3 dv

* Note that the relativistic diagram is identical to that for the classical calculation.

(where the upper limit of the integral, g =

The final step:

Total energy, mc2 = kinetic energy + rest energy The expression for 'invariant mass' — a useful relationship:

Momentum p = gmQV

0 0

Post a comment