A physical dipole consists of point charges and at and respectively

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Electric fields in matter · Electric fields in matter

The Boundary-Value Problem, Ch Polarisation and bound charge, completed

Problem

A physical dipole consists of point charges +q+q and −q-q at z=+d/2z=+d/2 and z=−d/2z=-d/2 respectively, with q=4.0×10−9 Cq = 4.0\times10^{-9}\,\mathrm{C} and d=1.0 mmd = 1.0\,\mathrm{mm}. Let a=4.0 cma = 4.0\,\mathrm{cm} (so a≫d/2a \gg d/2) and consider an imaginary sphere of radius aa centred at the origin, enclosing both charges. ((a)) Using the result that the field of a single point charge q′q' at position r′\mathbf{r}' inside a ball of radius aa, integrated over the ball's volume, equals −q′r′/3ε0-q'\mathbf{r}'/3\varepsilon_0 regardless of aa, find ∫ballE dτ\int_{\rm ball}\mathbf{E}\,d\tau for this dipole in terms of p=qdp=qd, and give its numerical value. ((b)) Divide by the ball's volume to get the average field ⟨E⟩\langle\mathbf{E}\rangle inside the sphere, and evaluate it numerically. ((c)) A uniformly polarised sphere of the same radius aa, carrying total dipole moment pp spread uniformly through its volume as P=p/VP = p/V, has interior field −P/3ε0-P/3\varepsilon_0 (a result derived from matching VV and its normal derivative at r=ar=a). Show algebraically that this equals ⟨E⟩\langle\mathbf{E}\rangle found in part (b).

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