A point charge sits at height above the flat face of a semi-infinite linear…

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Conductors, capacitance and boundary-value electrostatics · Electric fields in matter

The Boundary-Value Problem, Ch Linear dielectrics and the boundary-value problem with matter in it

Problem

A point charge qq sits at height dd above the flat face of a semi-infinite linear dielectric of permittivity ε=εrε0\varepsilon = \varepsilon_r\varepsilon_0 filling the region z<0z < 0; the region z>0z > 0 is vacuum. There is no free surface charge on the interface. ((a)) Guess the image system: for z>0z>0, the real charge qq at (0,0,d)(0,0,d) plus a single image charge q′q' at (0,0,−d)(0,0,-d), both radiating into vacuum permittivity ε0\varepsilon_0; for z<0z<0, a single charge q′′q'' at (0,0,d)(0,0,d) radiating into a uniform medium of permittivity ε\varepsilon filling all space. Impose continuity of VV and of the normal component of D\mathbf{D} at z=0z=0 and solve for q′q' and q′′q'' in terms of qq and εr\varepsilon_r. ((b)) Show that as εr→∞\varepsilon_r \to \infty, q′→−qq' \to -q and identify the limit. ((c)) The sphere response factor has εr+2\varepsilon_r+2 in its denominator. Identify, from the matching algebra of part (a), the single number that plays the analogous role for this flat-interface problem, and explain in one sentence why it is smaller than the sphere's.

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