Induced Magnetic Fields — Question 3

Section 32-2 · Physics pages 5196–5197

Question 3 A tapered electric-field profile moves the magnetic maximum inside the edge For r<a, a prescribed quasistatic vacuum field has ∂tEz = β(1 −r2/a2); outside, its time derivative vanishes. There is no conduction current. a r ⊙Ez(t) Schematic; labels, not drawing lengths, specify the data. (a) Integrate the electric-flux rate to find Bphi inside and outside. (b) Find the radius of maximum B for beta positive.
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Question 3 - Solution A tapered electric-field profile moves the magnetic maximum inside the edge a r ⊙Ez(t) (a) Method and calculation ˙ΦE(r) = 2πβ ∫r 0 (1 −s2/a2)s ds = πβ(r2 −r4/(2a2)). Bϕ = β c2 (r/2 −r3/(4a2)) (r < a); Bϕ = βa2 4c2r (r > a) . (b) Interpretation and further calculation ∂rBϕ = (β/c2)(1/2 −3r2/(4a2)) = 0. rmax = a √ 2/3, Bmax = βa 3c2 √ 2/3 . Physical check Using the center value of the electric-field rate everywhere would overcount flux.

Question 3

A tapered electric-field profile moves the magnetic maximum inside the edge

For r<a, a prescribed quasistatic vacuum field has ∂tEz=β(1−r2/a2)\partial_tE_z=\beta(1-r^2/a^2); outside, its time derivative vanishes. There is no conduction current.

Diagram shown in the original SVG worksheet.

  1. Integrate the electric-flux rate to find Bphi inside and outside.

  2. Find the radius of maximum B for beta positive.

Question 3 - Solution

A tapered electric-field profile moves the magnetic maximum inside the edge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φ̇E(r)=2πβ∫0r(1−s2/a2)sds=πβ(r2−r4/(2a2)).\dot\Phi_E(r)=2\pi\beta\int_0^r(1-s^2/a^2)s\,ds=\pi\beta(r^2-r^4/(2a^2)).Bϕ=βc2(r/2−r3/(4a2))(r<a);Bϕ=βa24c2r(r>a).\boxed{B_\phi=\frac\beta{c^2}(r/2-r^3/(4a^2))\ (r<a);\quad B_\phi=\frac{\beta a^2}{4c^2r}\ (r>a)}.

(b) Interpretation and further calculation

∂rBϕ=(β/c2)(1/2−3r2/(4a2))=0.\partial_rB_\phi=(\beta/c^2)(1/2-3r^2/(4a^2))=0.rmax=a2/3,Bmax=βa3c22/3.\boxed{r_{\max}=a\sqrt{2/3},\quad B_{\max}=\frac{\beta a}{3c^2}\sqrt{2/3}}.

Physical check

Using the center value of the electric-field rate everywhere would overcount flux.