Torque on a Current Loop — Question 8

Section 28-8 · Physics pages 4626–4627

Question 8 A freely pivoted current loop performs small angular oscillations about alignment A rigid N-turn loop has area A, maintained current I and rotational inertia J about a pivot through its center. In uniform field B, let theta be the angle of its normal from B. The pivot constrains rotation to one plane and adds no torque. loop, edge view ˆn θ⃗ B Schematic; labels, not drawing lengths, specify the data. (a) Write the exact angular equation and derive the small-angle period near theta=0. (b) Find the effect of doubling I on the small-angle period and test the equilibrium at theta=pi with a small perturbation.
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Question 8 - Solution A freely pivoted current loop performs small angular oscillations about alignment loop, edge view ˆn θ⃗ B (a) Method and calculation J ¨θ = −NIAB sin θ. |θ| ≪1 : ¨θ + Ω2θ = 0, Ω= √ NIAB/J, T = 2π √ J/(NIAB). (b) Interpretation and further calculation I′ = 2I ⇒T′ = T/ √ 2. θ = π + η : ¨η ≃+Ω2η ⇒η ∝e±Ωt; unstable. Physical check Aligned and antialigned orientations both have zero instantaneous torque, but their responses to small disturbances differ.

Question 8

A freely pivoted current loop performs small angular oscillations about alignment

A rigid N-turn loop has area A, maintained current I and rotational inertia J about a pivot through its center. In uniform field B, let theta be the angle of its normal from B. The pivot constrains rotation to one plane and adds no torque.

Diagram shown in the original SVG worksheet.

  1. Write the exact angular equation and derive the small-angle period near theta=0.

  2. Find the effect of doubling I on the small-angle period and test the equilibrium at theta=pi with a small perturbation.

Question 8 - Solution

A freely pivoted current loop performs small angular oscillations about alignment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Jθ̈=−NIABsin⁡θ.J\ddot\theta=-NIAB\sin\theta.|θ|≪1:θ̈+Ω2θ=0,Ω=NIAB/J,T=2πJ/(NIAB).|\theta|\ll1:\quad\ddot\theta+\Omega^2\theta=0,\quad\Omega=\sqrt{NIAB/J},\quad T=2\pi\sqrt{J/(NIAB)}.

(b) Interpretation and further calculation

I′=2I⇒T′=T/2.I\prime=2I\Rightarrow T\prime=T/\sqrt2.θ=π+η:η̈≃+Ω2η⇒η∝e±Ωt;unstable.\theta=\pi+\eta:\quad\ddot\eta\simeq+\Omega^2\eta\Rightarrow\eta\propto e^{\pm\Omega t};\quad\text{unstable}.

Physical check

Aligned and antialigned orientations both have zero instantaneous torque, but their responses to small disturbances differ.