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At the boundary of two perfect dielectric materials, ϵ1 and ϵ2, D1 is incident at an angle θ1, with respect to normal to the boundary surface.
written 7.1 years ago by | modified 3.3 years ago by |
It can be proved that
D2=D1√cos2θ1+(ϵ2ϵ1)2sin2θ1
E2=E1√sin2θ1+(ϵ1ϵ2)2cos2θ1
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