Magnetic Materials — Question 8

Section 32-7 · Physics pages 5306–5307

Question 8 An anisotropic induced moment has a one-half factor in its energy A small weakly magnetic crystal of volume V has principal susceptibilities chi1 and chi2 in a plane. A uniform external B makes angle theta with axis 1. Neglect demagnetization. Use U = −V B · χB/(2µ0). axis 1 axis 2 B θ Schematic; labels, not drawing lengths, specify the data. (a) Find energy as a function of theta and the generalized magnetic torque about the normal to the plane. (b) For chi1 greater than chi2, identify the stable orientation and the work needed to rotate from 0 to 90 degrees.
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Question 8 - Solution An anisotropic induced moment has a one-half factor in its energy axis 1 axis 2 B θ (a) Method and calculation U(θ) = −V B2 2µ0 (χ1 cos2 θ + χ2 sin2 θ). τθ = −V B2 2µ0 (χ1 −χ2) sin 2θ . (b) Interpretation and further calculation χ1 > χ2 ⇒θ = 0 (mod π) is stable . W0→π/2 = V B2 2µ0 (χ1 −χ2) > 0 . Physical check The induced moment varies with field, so inserting it into the fixed-dipole expression without the one-half factor would double the energy.

Question 8

An anisotropic induced moment has a one-half factor in its energy

A small weakly magnetic crystal of volume V has principal susceptibilities chi1 and chi2 in a plane. A uniform external B makes angle theta with axis 1. Neglect demagnetization. Use U=−V𝑩⋅𝝌𝑩/(2μ0)U=-V\mathbf B\cdot\boldsymbol\chi\mathbf B/(2\mu_0).

Diagram shown in the original SVG worksheet.

  1. Find energy as a function of theta and the generalized magnetic torque about the normal to the plane.

  2. For chi1 greater than chi2, identify the stable orientation and the work needed to rotate from 0 to 90 degrees.

Question 8 - Solution

An anisotropic induced moment has a one-half factor in its energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(θ)=−VB22μ0(χ1cos⁡2θ+χ2sin⁡2θ).U(\theta)=-\frac{VB^2}{2\mu_0}(\chi_1\cos^2\theta+\chi_2\sin^2\theta).τθ=−VB22μ0(χ1−χ2)sin⁡2θ.\boxed{\tau_\theta=-\frac{VB^2}{2\mu_0}(\chi_1-\chi_2)\sin2\theta}.

(b) Interpretation and further calculation

χ1>χ2⇒θ=0(mod⁡π) is stable.\chi_1>\chi_2\Rightarrow\boxed{\theta=0\pmod\pi\text{ is stable}}.W0→π/2=VB22μ0(χ1−χ2)>0.\boxed{W_{0\to\pi/2}=\frac{VB^2}{2\mu_0}(\chi_1-\chi_2)>0}.

Physical check

The induced moment varies with field, so inserting it into the fixed-dipole expression without the one-half factor would double the energy.