The Magnetic Dipole Moment — Question 4

Section 28-9 · Physics pages 4638–4639

Question 4 The dipole energy barrier separates oscillation from full rotation A fixed-magnitude dipole starts aligned with uniform B and has initial rotational kinetic energy K0 about a frictionless planar pivot of inertia J. Its potential is U = −µB cos θ. θ U π 2π −µB +µB Schematic; labels, not drawing lengths, specify the data. (a) Find the critical initial speed separating bounded oscillations from continuous full rotations. (b) For K0=mu B/2, find the turning angle. Explain the special behavior exactly at the critical energy.
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Question 4 - Solution The dipole energy barrier separates oscillation from full rotation θ U π 2π −µB +µB (a) Method and calculation ∆U0→π = 2µB, 1 2Jω2 c = 2µB. ωc = 2 √ µB/J; |ω0| > ωc permits continuous rotation. (b) Interpretation and further calculation K0 = µB(1 −cos θmax) = µB/2 ⇒θmax = 60.0◦. K0 = 2µB : | ˙θ| = 2 √ µB/J| cos(θ/2)| →0 as θ →π. At this separatrix, the ideal dipole approaches the unstable top only asymptotically. Physical check Exactly reaching the barrier energy is not enough for finite-speed passage over the unstable orientation.

Question 4

The dipole energy barrier separates oscillation from full rotation

A fixed-magnitude dipole starts aligned with uniform B and has initial rotational kinetic energy K0 about a frictionless planar pivot of inertia J. Its potential is U=−μBcos⁡θU=-\mu B\cos\theta.

Diagram shown in the original SVG worksheet.

  1. Find the critical initial speed separating bounded oscillations from continuous full rotations.

  2. For K0=mu B/2, find the turning angle. Explain the special behavior exactly at the critical energy.

Question 4 - Solution

The dipole energy barrier separates oscillation from full rotation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔU0→π=2μB,12Jωc2=2μB.\Delta U_{0\to\pi}=2\mu B,\quad\tfrac12J\omega_c^2=2\mu B.ωc=2μB/J;|ω0|>ωc permits continuous rotation.\omega_c=2\sqrt{\mu B/J};\quad |\omega_0|>\omega_c\text{ permits continuous rotation}.

(b) Interpretation and further calculation

K0=μB(1−cos⁡θmax)=μB/2⇒θmax=60.0∘.K_0=\mu B(1-\cos\theta_{\max})=\mu B/2\Rightarrow\theta_{\max}=60.0^\circ.K0=2μB:|θ̇|=2μB/J|cos⁡(θ/2)|→0 as θ→π.K_0=2\mu B:\quad |\dot\theta|=2\sqrt{\mu B/J}|\cos(\theta/2)|\to0\text{ as }\theta\to\pi.At this separatrix, the ideal dipole approaches the unstable top only asymptotically.

Physical check

Exactly reaching the barrier energy is not enough for finite-speed passage over the unstable orientation.