Energy Stored in a Magnetic Field — Question 6

Section 30-9 · Physics pages 4922–4923

Question 6 Increasing inductance has different energy consequences at fixed current and fixed linkage A lossless linear inductor is changed slowly from L0 to 2L0 by moving part of its geometry. Initially its current is I0 and energy U0. Compare a current-controlled case with an isolated zero-resistance case having conserved linkage. B ℓ N turns; cross section A geometry changes L0 →2L0 Schematic; labels, not drawing lengths, specify the data. (a) Find final current and energy in each case. (b) For the fixed-current case, find electrical work and mechanical work delivered by the magnetic system.
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Question 6 - Solution Increasing inductance has different energy consequences at fixed current and fixed linkage B ℓ N turns; cross section A geometry changes L0 →2L0 (a) Method and calculation I = I0 : Uf = 1 2(2L0)I2 0 = 2U0 . Λ = L0I0 : If = I0/2, Uf = Λ2/(4L0) = U0/2 . (b) Interpretation and further calculation Welec = ∫ I2 0dL = L0I2 0 = 2U0. Wmech,out = Welec −∆U = U0 . Physical check A moving geometry allows mechanical energy exchange. Using only the change in stored energy misses the source contribution at fixed current.

Question 6

Increasing inductance has different energy consequences at fixed current and fixed linkage

A lossless linear inductor is changed slowly from L0 to 2L0 by moving part of its geometry. Initially its current is I0 and energy U0. Compare a current-controlled case with an isolated zero-resistance case having conserved linkage.

Diagram shown in the original SVG worksheet.

  1. Find final current and energy in each case.

  2. For the fixed-current case, find electrical work and mechanical work delivered by the magnetic system.

Question 6 - Solution

Increasing inductance has different energy consequences at fixed current and fixed linkage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I=I0:Uf=12(2L0)I02=2U0.I=I_0:\quad U_f=\tfrac12(2L_0)I_0^2=\boxed{2U_0}.Λ=L0I0:If=I0/2,Uf=Λ2/(4L0)=U0/2.\Lambda=L_0I_0:\quad I_f=I_0/2,\quad U_f=\Lambda^2/(4L_0)=\boxed{U_0/2}.

(b) Interpretation and further calculation

Welec=∫I02dL=L0I02=2U0.W_{\mathrm{elec}}=\int I_0^2dL=L_0I_0^2=2U_0.Wmech,out=Welec−ΔU=U0.\boxed{W_{\mathrm{mech,out}}=W_{\mathrm{elec}}-\Delta U=U_0}.

Physical check

A moving geometry allows mechanical energy exchange. Using only the change in stored energy misses the source contribution at fixed current.