Displacement Current — Question 9

Section 32-3 · Physics pages 5228–5229

Question 9 A nonuniform displacement-current profile changes enclosed-current fractions Between circular capacitor plates, the axial displacement-current density is Jd(r) = J0(1 −r2/a2) for r<a. Assume axisymmetry and quasistatic fields. a r ⊙Ez(t) Schematic; labels, not drawing lengths, specify the data. (a) Find total current and the fraction enclosed at radius a/2. (b) Find the magnetic field at a/2 in terms of total current.
Show solutionHide solution
Question 9 - Solution A nonuniform displacement-current profile changes enclosed-current fractions a r ⊙Ez(t) (a) Method and calculation I = 2πJ0 ∫a 0 (1 −r2/a2)r dr = πJ0a2/2. I(r < a/2)/I = 2(1/2)2 −(1/2)4 = 7/16 . (b) Interpretation and further calculation B(a/2) 2π(a/2) = µ0(7I/16). B(a/2) = 7µ0I/(16πa) . Physical check A uniform-area estimate would give one-quarter; the center-weighted profile instead encloses seven-sixteenths.

Question 9

A nonuniform displacement-current profile changes enclosed-current fractions

Between circular capacitor plates, the axial displacement-current density is Jd(r)=J0(1−r2/a2)J_d(r)=J_0(1-r^2/a^2) for r<a. Assume axisymmetry and quasistatic fields.

Diagram shown in the original SVG worksheet.

  1. Find total current and the fraction enclosed at radius a/2.

  2. Find the magnetic field at a/2 in terms of total current.

Question 9 - Solution

A nonuniform displacement-current profile changes enclosed-current fractions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I=2πJ0∫0a(1−r2/a2)rdr=πJ0a2/2.I=2\pi J_0\int_0^a(1-r^2/a^2)r\,dr=\pi J_0a^2/2.I(r<a/2)/I=2(1/2)2−(1/2)4=7/16.\boxed{I(r<a/2)/I=2(1/2)^2-(1/2)^4=7/16}.

(b) Interpretation and further calculation

B(a/2)2π(a/2)=μ0(7I/16).B(a/2)\,2\pi(a/2)=\mu_0(7I/16).B(a/2)=7μ0I/(16πa).\boxed{B(a/2)=7\mu_0I/(16\pi a)}.

Physical check

A uniform-area estimate would give one-quarter; the center-weighted profile instead encloses seven-sixteenths.