The mathematical computation leading from Eq.(65) and ending with Eq.(69) can be
extended without any effort to T.M. radiation. The extension consists of
replacing a T.E. source with a corresponding T.M. source,

or equivalently

Consequently, the formula for the flow of T.M. radiant energy due to an electric dipole subject to uniform linear acceleration is

The justification for this extension is Eqs.(58) and (34). They are the same for T.E. and T.M. radiation. The radiation intensity expressed by Eq.(70) extends the familiar Larmor formula for radiation from an

Ulrich Gerlach 2001-10-09