Copyright © 2000 David E. Rutherford
All Rights Reserved
We can derive an equation for the energy of a particle from the equation for the transformation of charge. The equation for transformation of charge, Eq. (64) is
Squaring Eq. (118), we get
or
Now, multiplying both sides of Eq. (120) by the square of the static electric
potential,
, we have
Remembering, from Eq. (87), that the potential four-vector for a single moving
point charge is
, we can
write Eq. (121) as
Taking the square root of both sides of Eq. (122), we get
or, in terms of the total energy,
, and proper
mass,
,
Noting that the spatial part of the four-momentum is
, where
, we can
write Eq. (124) as
We notice from Eq. (125) that the total energy,
, of a particle
can be either positive or negative. In addition, from Eq. (121) we see that,
when
, the
total energy due to translatory motion is zero. However, a particle may possess
energy due to its rotation in addition to the energy of its translational
motion, even though the magnitude of its spatial four-velocity,
, is the
speed of light,
. This
additional energy,
, due to
the frequency of rotation,
, is described
by the Planck relation,
, where
is Planck's
constant.
Copyright © 2000 David E. Rutherford
All Rights Reserved
E-mail: drutherford@softcom.net