(a) Two earthed conducting half-planes meet along the -axis, with the field-filled…

PHYSICS · Subjective · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Electrostatic fields and potential · Conductors, capacitance and boundary-value electrostatics

The Boundary-Value Problem, Ch Cylindrical geometry, edges, and what a field does to a dipole

Problem

(a) Two earthed conducting half-planes meet along the zz-axis, with the field-filled region between them opening through an angle β=5π/4\beta = 5\pi/4 (an exterior, re-entrant edge). Following the wedge derivation, write the leading angular and radial dependence of the potential near the edge, and give the exponent pp such that EE and σ\sigma vary as sps^p with distance ss from the edge. State whether surface charge crowds towards or drains away from this edge. (b) A small body of polarisability α\alpha sits in a static, curl-free field E(r)\mathbf{E}(\mathbf{r}) whose magnitude varies with position, so that it acquires an induced dipole moment p=αE\mathbf{p}=\alpha\mathbf{E}. Starting from the force law F=(p⋅∇)E\mathbf{F}=(\mathbf{p}\cdot\nabla)\mathbf{E}, show that F=∇(12αE2)\mathbf{F}=\nabla\left(\tfrac12\alpha E^2\right), and hence that the potential energy of the induced dipole is U=−12αE2U=-\tfrac12\alpha E^2. Apply this to a small conducting sphere of radius 2.0 mm2.0\,\mathrm{mm} (polarisability α=4πε0a3\alpha = 4\pi\varepsilon_0a^3) placed where the field magnitude is 1.0×105 V m−11.0\times10^5\,\mathrm{V\,m^{-1}}, and give its energy.

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