Relativistic Energy
Equation (3.169) can be
written
 |
(3.173) |
Let us define the relativistic energy,
, of our particle as
 |
(3.174) |
The previous two equations suggest that the particle possesses two types of energy. First,
the particle possesses kinetic energy,
, by virtue of its motion. Second, the particle
possesses rest mass energy,
 |
(3.175) |
by virtue of its rest mass. The conjecture that mass is a form of energy was first made by Einstein in 1905.
Incidentally, Equation (3.174) implies that conservation of energy in relativistic dynamics is
equivalent to conservation of relativistic mass.