Introduction to Electrodynamics · Problem 7.61

Conservation Laws — David J. Griffiths

Physics · displacement-current-wire

Problem

The magnetic field of an infinite straight wire carrying a steady current II can be obtained from the displacement current term in the Amp\`ere/Maxwell law, as follows: Picture the current as consisting of a uniform line charge λ\lambda moving along the zz axis at speed vv (so that I=λvI = \lambda v), with a tiny gap of length ϵ\epsilon, which reaches the origin at time t=0t = 0. In the next instant (up to t=ϵ/vt = \epsilon/v) there is no real current passing through a circular Amperian loop in the xyxy plane, but there is a displacement current, due to the "missing" charge in the gap. (a) Use Coulomb's law to calculate the zz component of the electric field, for points in the xyxy plane a distance ss from the origin, due to a segment of wire with uniform density −λ-\lambda extending from z1=vt−ϵz_1 = vt - \epsilon to z2=vtz_2 = vt. (b) Determine the flux of this electric field through a circle of radius aa in the xyxy plane. (c) Find the displacement current through this circle. Show that IdI_d is equal to II, in the limit as the gap width (ϵ\epsilon) goes to zero.

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