Induced Magnetic Fields — Question 9

Section 32-2 · Physics pages 5208–5209

Question 9 A steady electric field contributes no magnetic circulation through its time derivative Inside a circular contour, the uniform axial field is Ez(t) = Eb + αt2 over area A. There is no conduction current through the disk. Take its boundary radius r, so A = πr2. a r ⊙Ez(t) Schematic; labels, not drawing lengths, specify the data. (a) Find the magnetic circulation and Bphi. (b) Compare the result when an arbitrary constant is added to Eb, and when time changes sign.
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Question 9 - Solution A steady electric field contributes no magnetic circulation through its time derivative a r ⊙Ez(t) (a) Method and calculation ∂tΦE = 2αtA ⇒ I B · dl = 2αtA/c2. Bϕ = αtr/c2 . (b) Interpretation and further calculation Eb →Eb + Eoffset : ∂tEz unchanged. Bϕ(−t) = −Bϕ(t), Bϕ(0) = 0 . Physical check Circulation responds to the rate of electric flux, even when the electric-field magnitude is large at t=0.

Question 9

A steady electric field contributes no magnetic circulation through its time derivative

Inside a circular contour, the uniform axial field is Ez(t)=Eb+αt2E_z(t)=E_b+\alpha t^2 over area A. There is no conduction current through the disk. Take its boundary radius r, so A=πr2A=\pi r^2.

Diagram shown in the original SVG worksheet.

  1. Find the magnetic circulation and Bphi.

  2. Compare the result when an arbitrary constant is added to Eb, and when time changes sign.

Question 9 - Solution

A steady electric field contributes no magnetic circulation through its time derivative

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂tΦE=2αtA⇒∮𝑩⋅d𝒍=2αtA/c2.\partial_t\Phi_E=2\alpha t A\Rightarrow\oint\mathbf B\cdot d\mathbf l=2\alpha tA/c^2.Bϕ=αtr/c2.\boxed{B_\phi=\alpha tr/c^2}.

(b) Interpretation and further calculation

Eb→Eb+Eoffset:∂tEzunchanged.E_b\to E_b+E_{\mathrm{offset}}:\quad\partial_tE_z\ \text{unchanged}.Bϕ(−t)=−Bϕ(t),Bϕ(0)=0.\boxed{B_\phi(-t)=-B_\phi(t),\quad B_\phi(0)=0}.

Physical check

Circulation responds to the rate of electric flux, even when the electric-field magnitude is large at t=0.