Induction and Energy Transfers — Question 10

Section 30-4 · Physics pages 4830–4831

Question 10 A constant induced emf minimizes heat for a prescribed linkage change and duration A resistive circuit of resistance R undergoes a prescribed total external linkage change DeltaLambda over duration T. Self-inductance is negligible, but the time profile can be chosen. Use the inequality ( ∫T 0 fdt)2 ≤T ∫T 0 f2dt. t |E| Schematic; labels, not drawing lengths, specify the data. (a) Derive a lower bound on heat. (b) Identify the linkage history that attains it and compare a triangular emf pulse with the same voltage-time integral.
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Question 10 - Solution A constant induced emf minimizes heat for a prescribed linkage change and duration t |E| (a) Method and calculation H = 1 R ∫T 0 E2dt, ∫T 0 Edt = −∆Λ. H ≥(∆Λ)2/(RT) . (b) Interpretation and further calculation E = −∆Λ/T constant ⇒Λ(t) = Λ(0) + ∆Λ t/T. triangular pulse: Epeak = 2|∆Λ|/T, H = E2 peakT/(3R) = 4 3Hmin . Physical check The bound is on the prescribed resistive model; allowing self-inductance introduces stored magnetic energy and changes the current response.

Question 10

A constant induced emf minimizes heat for a prescribed linkage change and duration

A resistive circuit of resistance R undergoes a prescribed total external linkage change DeltaLambda over duration T. Self-inductance is negligible, but the time profile can be chosen. Use the inequality (∫0Tfdt)2≤T∫0Tf2dt(\int_0^T fdt)^2\le T\int_0^T f^2dt.

Diagram shown in the original SVG worksheet.

  1. Derive a lower bound on heat.

  2. Identify the linkage history that attains it and compare a triangular emf pulse with the same voltage-time integral.

Question 10 - Solution

A constant induced emf minimizes heat for a prescribed linkage change and duration

Diagram shown in the original SVG worksheet.

(a) Method and calculation

H=1R∫0Tℰ2dt,∫0Tℰdt=−ΔΛ.H=\frac1R\int_0^T\mathcal E^2dt,\quad\int_0^T\mathcal E dt=-\Delta\Lambda.H≥(ΔΛ)2/(RT).\boxed{H\ge(\Delta\Lambda)^2/(RT)}.

(b) Interpretation and further calculation

ℰ=−ΔΛ/T constant⇒Λ(t)=Λ(0)+ΔΛt/T.\mathcal E=-\Delta\Lambda/T\text{ constant}\Rightarrow\Lambda(t)=\Lambda(0)+\Delta\Lambda\,t/T.triangular pulse: Epeak=2|ΔΛ|/T,H=Epeak2T/(3R)=43Hmin.\text{triangular pulse: }E_{\mathrm{peak}}=2|\Delta\Lambda|/T,\quad H=E_{\mathrm{peak}}^2T/(3R)=\boxed{\tfrac43H_{\min}}.

Physical check

The bound is on the prescribed resistive model; allowing self-inductance introduces stored magnetic energy and changes the current response.