Inductors and Inductance — Question 4

Section 30-6 · Physics pages 4858–4859

Question 4 Internal inductance accounts for only the fraction of current linked by each flux strip A solid round wire of radius a carries uniform axial current I. Inside, B(r) = µ0Ir/(2πa2). For length ell, use the supplied internal-linkage rule dΛ = [I(r)/I]B(r)ℓdr, where I(r) = Ir2/a2. r a uniform axial current density Schematic; labels, not drawing lengths, specify the data. (a) Derive the internal inductance per unit length. (b) Compare it with a model in which all current is on the wire surface and the internal magnetic field is zero.
Show solutionHide solution
Question 4 - Solution Internal inductance accounts for only the fraction of current linked by each flux strip r a uniform axial current density (a) Method and calculation Λint = ∫a 0 r2 a2 µ0Ir 2πa2 ℓdr = µ0Iℓ 2πa4 a4 4 . Lint/ℓ= µ0/(8π) . (b) Interpretation and further calculation Binterior = 0 ⇒Λint = 0. (Lint/ℓ)surface = 0 . Physical check This comparison concerns internal inductance only; the external return-path geometry still contributes inductance.

Question 4

Internal inductance accounts for only the fraction of current linked by each flux strip

A solid round wire of radius a carries uniform axial current I. Inside, B(r)=μ0Ir/(2πa2)B(r)=\mu_0Ir/(2\pi a^2). For length ell, use the supplied internal-linkage rule dΛ=[I(r)/I]B(r)ℓdrd\Lambda=[I(r)/I]B(r)\ell\,dr, where I(r)=Ir2/a2I(r)=Ir^2/a^2.

Diagram shown in the original SVG worksheet.

  1. Derive the internal inductance per unit length.

  2. Compare it with a model in which all current is on the wire surface and the internal magnetic field is zero.

Question 4 - Solution

Internal inductance accounts for only the fraction of current linked by each flux strip

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Λint=∫0ar2a2μ0Ir2πa2ℓdr=μ0Iℓ2πa4a44.\Lambda_{\mathrm{int}}=\int_0^a\frac{r^2}{a^2}\frac{\mu_0Ir}{2\pi a^2}\ell\,dr=\frac{\mu_0I\ell}{2\pi a^4}\frac{a^4}{4}.Lint/ℓ=μ0/(8π).\boxed{L_{\mathrm{int}}/\ell=\mu_0/(8\pi)}.

(b) Interpretation and further calculation

Binterior=0⇒Λint=0.B_{\mathrm{interior}}=0\Rightarrow\Lambda_{\mathrm{int}}=0.(Lint/ℓ)surface=0.\boxed{(L_{\mathrm{int}}/\ell)_{\mathrm{surface}}=0}.

Physical check

This comparison concerns internal inductance only; the external return-path geometry still contributes inductance.