Energy Density of a Magnetic Field — Question 1

Section 30-10 · Physics pages 4932–4933

Question 1 A solenoid converts circuit energy into a local field density A long vacuum solenoid has N turns, length ell, area A, L = µ0N2A/ℓ, and B = µ0NI/ℓ. Neglect end fields. Take µ0 ≈4π × 10−7 H/m. B ℓ N turns; cross section A Schematic; labels, not drawing lengths, specify the data. (a) Derive magnetic energy per unit volume from the circuit energy. (b) Evaluate the density and total energy for B=.200 T and field volume .00300 cubic meters.
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Question 1 - Solution A solenoid converts circuit energy into a local field density B ℓ N turns; cross section A (a) Method and calculation U = 1 2LI2 = µ0N2A 2ℓ ( Bℓ µ0N )2 = B2 2µ0 Aℓ. uB = U/(Aℓ) = B2/(2µ0) . (b) Interpretation and further calculation uB = (.200)2 8π × 10−7 = 1.59155 × 104 J/m3. U = uBV = 47.7465 J . Physical check Energy density is nonnegative and quadratic in field magnitude.

Question 1

A solenoid converts circuit energy into a local field density

A long vacuum solenoid has N turns, length ell, area A, L=μ0N2A/ℓL=\mu_0N^2A/\ell, and B=μ0NI/ℓB=\mu_0NI/\ell. Neglect end fields. Take μ0≈4π×10−7\mu_0\approx4\pi\times10^{-7} H/m.

Diagram shown in the original SVG worksheet.

  1. Derive magnetic energy per unit volume from the circuit energy.

  2. Evaluate the density and total energy for B=.200 T and field volume .00300 cubic meters.

Question 1 - Solution

A solenoid converts circuit energy into a local field density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=12LI2=μ0N2A2ℓ(Bℓμ0N)2=B22μ0Aℓ.U=\tfrac12LI^2=\frac{\mu_0N^2A}{2\ell}\left(\frac{B\ell}{\mu_0N}\right)^2=\frac{B^2}{2\mu_0}A\ell.uB=U/(Aℓ)=B2/(2μ0).\boxed{u_B=U/(A\ell)=B^2/(2\mu_0)}.

(b) Interpretation and further calculation

uB=(.200)28π×10−7=1.59155×104J/m3.u_B=\frac{(.200)^2}{8\pi\times10^{-7}}=1.59155\times10^4\,J/m^3.U=uB𝒱=47.7465J.\boxed{U=u_B\mathcal V=47.7465\,J}.

Physical check

Energy density is nonnegative and quadratic in field magnitude.