The derivation of Laplace’s and Poisson’s equations assumed constant permittivity, but there are cases of spatially varying permittivity in which the equations will still apply. Consider the vector identity, ∇ · (ψG) = G · ∇ ψ + ψ ∇ · G, where ψ and Gare scalar and vector functions, respectively.
Figure 6.14 See Problem 6.39.
Determine a general rule on the allowed directions in which ϵ may vary with respect to the local electric field.
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