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7.9 Reflection and refraction with polarization perpendicular to k” the plane of
incidence. E and H are continuous. In terms of fields (7.49)–(7.51) these
boundary conditions at z = 0 are: [e(Eo + Eo") – e'Eo'] n = 0 [k × Eo + k" x Eo" – k'
x Eo'] n ...
parallel to and perpendicular to the velocity. But we have just seen that for
comparable parallel and perpendicular forces the radiation from the parallel
component is negligible (of order 1/y”) compared to that from the perpendicular
For simplicity we consider a small angle deflection so that AB is approximately
perpendicular to the incident direction. Figure 15.2 shows the vectorial
relationships. Without loss of generality n, the observation direction, is chosen in
the r-z ...
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Introduction to Electrostatics
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