The behavior of a charge in motion without restriction on its velocity
and acceleration is presented by using generalized expressions for th
e electromagnetic fields and an appropriate geometry in which to descr
ibe the fields. This combination makes it possible to obtain not only
the well-known specific cases (constant velocity and velocity parallel
or perpendicular to acceleration), but also the less well-known inter
mediate cases (for an arbitrary angle between velocity and acceleratio
n) and the extreme cases (Larmor or relativistic approximations) in a
continuous manner through computer simulation of the fields and the ra
diated energy.