October 2015
Intermediate to advanced
363 pages
7h 54m
English
In this section we will again consider the geometry of Section 7.2, but now with a static field “incident” upon the scatterer (i.e., the incident field is what would be produced by the impressed sources in the absence of the conductor S)8 In the static limit, the electric and magnetic problems decouple, and we consider them separately (see Section E.2).
Let a static incident electric field Ei(r) = −∇Φi(r) be characterized by means of a potential Φi(r), which is the result of some static charge distribution ρext(r) located external to S. When a perfect conductor9 whose surface is S is introduced into this incident field, a redistribution of ...
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