Induced Electric Fields — Question 10

Section 30-5 · Physics pages 4850–4851

Question 10 A reversible flux pulse can return a track-bound particle to its initial speed A charged particle on a frictionless circular track initially has angular momentum L0. An axisymmetric source changes the enclosed flux by DeltaPhi and later returns it exactly to the initial value. There is no radiation or dissipative force. Use ∆Lz = −q∆Φ/(2π). t Φ −Φ0 Schematic; labels, not drawing lengths, specify the data. (a) Find the intermediate and final angular momenta. (b) Find the net electric work over the complete pulse and explain how nonzero work can occur during each stage.
Show solutionHide solution
Question 10 - Solution A reversible flux pulse can return a track-bound particle to its initial speed t Φ −Φ0 (a) Method and calculation Lmid = L0 −q∆Φ/(2π). Lf = Lmid + q∆Φ/(2π) = L0 . (b) Interpretation and further calculation W1 = L2 mid −L2 0 2mr2 , W2 = L2 0 −L2 mid 2mr2 . Wtotal = 0 . Physical check Zero final energy change here follows from the lossless constrained-particle model; it differs from the positive heat of a resistive pickup.

Question 10

A reversible flux pulse can return a track-bound particle to its initial speed

A charged particle on a frictionless circular track initially has angular momentum L0. An axisymmetric source changes the enclosed flux by DeltaPhi and later returns it exactly to the initial value. There is no radiation or dissipative force. Use ΔLz=−qΔΦ/(2π)\Delta L_z=-q\Delta\Phi/(2\pi).

Diagram shown in the original SVG worksheet.

  1. Find the intermediate and final angular momenta.

  2. Find the net electric work over the complete pulse and explain how nonzero work can occur during each stage.

Question 10 - Solution

A reversible flux pulse can return a track-bound particle to its initial speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Lmid=L0−qΔΦ/(2π).L_{\mathrm{mid}}=L_0-q\Delta\Phi/(2\pi).Lf=Lmid+qΔΦ/(2π)=L0.\boxed{L_f=L_{\mathrm{mid}}+q\Delta\Phi/(2\pi)=L_0}.

(b) Interpretation and further calculation

W1=Lmid2−L022mr2,W2=L02−Lmid22mr2.W_1=\frac{L_{\mathrm{mid}}^2-L_0^2}{2mr^2},\quad W_2=\frac{L_0^2-L_{\mathrm{mid}}^2}{2mr^2}.Wtotal=0.\boxed{W_{\mathrm{total}}=0}.

Physical check

Zero final energy change here follows from the lossless constrained-particle model; it differs from the positive heat of a resistive pickup.