Magnets — Question 9

Section 32-5 · Physics pages 5268–5269

Question 9 A torsion fiber can stabilize an antiparallel magnet only below a threshold A torsion fiber has energy κθ2/2, where theta=0 places a permanent moment antiparallel to a uniform field B. The magnetic energy is mB cos θ and rotational inertia is J. B m at θ = 0 torsion fiber Schematic; labels, not drawing lengths, specify the data. (a) Find the small-angle equation and the threshold for stability at theta=0. (b) For mB just above kappa, expand through cubic order in the equilibrium torque equation to estimate the two nearby tilted equilibria.
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Question 9 - Solution A torsion fiber can stabilize an antiparallel magnet only below a threshold B m at θ = 0 torsion fiber (a) Method and calculation U = 1 2κθ2 + mB cos θ, J ¨θ = −κθ + mB sin θ. ω2 = (κ −mB)/J; θ = 0 stable for κ > mB . (b) Interpretation and further calculation 0 ≃(mB −κ)θ −mB 6 θ3. θ∗≃± √ 6(1 −κ/(mB)) (0 < mB −κ ≪mB). Physical check The two small tilted equilibria have positive local curvature to leading order; the expansion is invalid far above threshold.

Question 9

A torsion fiber can stabilize an antiparallel magnet only below a threshold

A torsion fiber has energy κθ2/2\kappa\theta^2/2, where theta=0 places a permanent moment antiparallel to a uniform field B. The magnetic energy is mBcos⁡θmB\cos\theta and rotational inertia is J.

Diagram shown in the original SVG worksheet.

  1. Find the small-angle equation and the threshold for stability at theta=0.

  2. For mB just above kappa, expand through cubic order in the equilibrium torque equation to estimate the two nearby tilted equilibria.

Question 9 - Solution

A torsion fiber can stabilize an antiparallel magnet only below a threshold

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=12κθ2+mBcos⁡θ,Jθ̈=−κθ+mBsin⁡θ.U=\tfrac12\kappa\theta^2+mB\cos\theta,\quad J\ddot\theta=-\kappa\theta+mB\sin\theta.ω2=(κ−mB)/J;θ=0 stable for κ>mB.\boxed{\omega^2=(\kappa-mB)/J;\quad\theta=0\text{ stable for }\kappa>mB}.

(b) Interpretation and further calculation

0≃(mB−κ)θ−mB6θ3.0\simeq(mB-\kappa)\theta-\frac{mB}{6}\theta^3.θ*≃±6(1−κ/(mB))(0<mB−κ≪mB).\boxed{\theta_*\simeq\pm\sqrt{6(1-\kappa/(mB))}}\quad(0<mB-\kappa\ll mB).

Physical check

The two small tilted equilibria have positive local curvature to leading order; the expansion is invalid far above threshold.