Energy Density of a Magnetic Field — Question 2

Section 30-10 · Physics pages 4934–4935

Question 2 Integrating toroidal field energy reproduces its inductance A vacuum toroid of rectangular cross section has inner radius a, outer radius b, height h, and N turns carrying I. Inside, B(r) = µ0NI/(2πr); neglect leakage. a b azimuthal magnetic field Schematic; labels, not drawing lengths, specify the data. (a) Integrate magnetic energy over the toroidal volume. (b) Infer L and the fraction of energy inside radius c = √ ab.
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Question 2 - Solution Integrating toroidal field energy reproduces its inductance a b azimuthal magnetic field (a) Method and calculation dV = 2πrh dr, U = ∫b a B(r)2 2µ0 2πrh dr. U = µ0N2I2h 4π ln(b/a) . (b) Interpretation and further calculation L = 2U/I2 = µ0N2h 2π ln(b/a) . U(a < r < c) U = ln(c/a) ln(b/a) = 1 2 . Physical check Equal logarithmic radial intervals contain equal energy, despite unequal geometric volumes.

Question 2

Integrating toroidal field energy reproduces its inductance

A vacuum toroid of rectangular cross section has inner radius a, outer radius b, height h, and N turns carrying I. Inside, B(r)=μ0NI/(2πr)B(r)=\mu_0NI/(2\pi r); neglect leakage.

Diagram shown in the original SVG worksheet.

  1. Integrate magnetic energy over the toroidal volume.

  2. Infer L and the fraction of energy inside radius c=abc=\sqrt{ab}.

Question 2 - Solution

Integrating toroidal field energy reproduces its inductance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

d𝒱=2πrhdr,U=∫abB(r)22μ02πrhdr.d\mathcal V=2\pi rh\,dr,\quad U=\int_a^b\frac{B(r)^2}{2\mu_0}2\pi rh\,dr.U=μ0N2I2h4πln⁡(b/a).\boxed{U=\frac{\mu_0N^2I^2h}{4\pi}\ln(b/a)}.

(b) Interpretation and further calculation

L=2U/I2=μ0N2h2πln⁡(b/a).\boxed{L=2U/I^2=\frac{\mu_0N^2h}{2\pi}\ln(b/a)}.U(a<r<c)U=ln⁡(c/a)ln⁡(b/a)=12.\boxed{\frac{U(a<r<c)}{U}=\frac{\ln(c/a)}{\ln(b/a)}=\tfrac12}.

Physical check

Equal logarithmic radial intervals contain equal energy, despite unequal geometric volumes.