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Then an explicit expression is * — no, 2 E3 = }(E1 + most + *Fo) +:[1-(*#")|- (*#")]"
coso (1249 where E' is given by (12.31). To obtain E, we merely interchange ms
and m, and change 0' into tr–0' (cos 0' → –cos 0'). The relation between angles ...
If fields (13.64) and (13.65) are inserted into (13.68) and (13.69), we find, after
some calculation, the expression due to Fermi, where A is given by (13.62). This
result can be obtained more elegantly by calculating the electromagnetic energy
where we have used the dipole moment expression (13.19). Assuming that the
second term is small, the imaginary part of 1/e(0) can be readily calculated and
substituted into (13.70). Then the integral over do can be performed in the same ...
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Introduction to Electrostatics
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