Classical Electrodynamics · Problem 3.15

Multipoles, Electrostatics of Macroscopic Media, Dielectrics — John David Jackson

Physics — E&M · boundary-value-problems-spherical-coordinates

Problem

Consider the following ``spherical cow'' model of a battery connected to an external circuit. A sphere of radius aa and conductivity σ\sigma is embedded in a uniform medium of conductivity σ′\sigma'. Inside the sphere there is a uniform (chemical) force in the zz direction acting on the charge carriers; its strength as an effective electric field entering Ohm's law is FF. In the steady state, electric fields exist inside and outside the sphere and surface charge resides on its surface. (a) Find the electric field (in addition to FF) and current density everywhere in space. Determine the surface-charge density and show that the electric dipole moment of the sphere is p=4πϵ0σa3F/(σ+2σ′)p = 4\pi\epsilon_0 \sigma a^3 F/(\sigma + 2\sigma'). (b) Show that the total current flowing out through the upper hemisphere of the sphere is I=2σσ′σ+2σ′⋅πa2FI = \frac{2\sigma\sigma'}{\sigma + 2\sigma'} \cdot \pi a^2 F Calculate the total power dissipation outside the sphere. Using the lumped circuit relations, P=I2Re=IVeP = I^2 R_e = IV_e, find the effective external resistance ReR_e and voltage VeV_e. (c) Find the power dissipated within the sphere and deduce the effective internal resistance RiR_i and voltage ViV_i. (d) Define the total voltage through the relation, Vt=(Re+Ri)IV_t = (R_e + R_i)I and show that Vt=4aF/3V_t = 4aF/3, as well as Ve+Vi=VtV_e + V_i = V_t. Show that IVtIV_t is the power supplied by the ``chemical'' force. Reference: W. M. Saslow, Am. J. Phys. 62, 495--501 (1994).

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