The Magnetic Dipole Moment — Question 3

Section 28-9 · Physics pages 4636–4637

Question 3 A released dipole converts magnetic potential energy into rotational kinetic energy A rigid dipole of moment .0200 ampere square metre pivots in a plane containing a uniform .500 T field. Its rotational inertia is 1.00 × 10−5 kilogram square metre. It is released from rest at theta0=60.0 degrees. Ignore damping and keep the moment magnitude fixed.⃗ µ θ⃗ B Schematic; labels, not drawing lengths, specify the data. (a) Derive angular speed as a function of theta while it moves toward alignment. (b) Find the maximum angular speed and identify where it occurs.
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Question 3 - Solution A released dipole converts magnetic potential energy into rotational kinetic energy⃗ µ θ⃗ B (a) Method and calculation 1 2J ˙θ2 −µB cos θ = −µB cos θ0. | ˙θ| = √ 2µB J (cos θ −cos θ0). (b) Interpretation and further calculation cos θ ≤1 ⇒ωmax = √ 2µB J (1 −cos θ0). θ = 0 : ωmax = √ 1000 = 31.6228 rad/s. Physical check The dipole is fastest at minimum potential energy; without damping it overshoots rather than remaining aligned.

Question 3

A released dipole converts magnetic potential energy into rotational kinetic energy

A rigid dipole of moment .0200 ampere square metre pivots in a plane containing a uniform .500 T field. Its rotational inertia is 1.00×10−51.00\times10^{-5} kilogram square metre. It is released from rest at theta0=60.0 degrees. Ignore damping and keep the moment magnitude fixed.

Diagram shown in the original SVG worksheet.

  1. Derive angular speed as a function of theta while it moves toward alignment.

  2. Find the maximum angular speed and identify where it occurs.

Question 3 - Solution

A released dipole converts magnetic potential energy into rotational kinetic energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

12Jθ̇2−μBcos⁡θ=−μBcos⁡θ0.\tfrac12J\dot\theta^2-\mu B\cos\theta=-\mu B\cos\theta_0.|θ̇|=2μBJ(cos⁡θ−cos⁡θ0).|\dot\theta|=\sqrt{\frac{2\mu B}{J}(\cos\theta-\cos\theta_0)}.

(b) Interpretation and further calculation

cos⁡θ≤1⇒ωmax=2μBJ(1−cos⁡θ0).\cos\theta\le1\Rightarrow\omega_{\max}=\sqrt{\frac{2\mu B}{J}(1-\cos\theta_0)}.θ=0:ωmax=1000=31.6228rad/s.\theta=0:\quad\omega_{\max}=\sqrt{1000}=31.6228\,\mathrm{rad/s}.

Physical check

The dipole is fastest at minimum potential energy; without damping it overshoots rather than remaining aligned.