A Dipole in an Electric Field — Question 2

Section 22-8 · Physics pages 3614–3615

Question 2 Quasistatic rotation distinguishes external work from field work A permanent rigid dipole of magnitude p rotates in a uniform field of magnitude E. Let θ be the angle between the moment and field, and choose U(90◦) = 0. An external actuator slowly rotates it from 30◦to 120◦without changing its kinetic energy. E p θ Schematic; labels, not drawing lengths, specify the data. (a) Derive U from the field torque and calculate the external work. (b) Find the work done by the field and the largest opposing torque magnitude encountered during this rotation.
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Question 2 - Solution Quasistatic rotation distinguishes external work from field work E p θ (a) Method and calculation τθ = −pE sin θ, dU dθ = −τθ ⇒U = −pE cos θ. Wext = ∆U = pE(cos 30◦−cos 120◦) = √ 3 + 1 2 pE. (b) Interpretation and further calculation Wfield = −∆U = − √ 3 + 1 2 pE. max 30◦≤θ≤120◦|τθ| = pE at θ = 90◦. Quasistatic balance requires the actuator torque to oppose the field torque at each angle, not merely on average. Physical check The potential energy rises during the entire prescribed rotation since sin θ > 0 along the path.

Question 2

Quasistatic rotation distinguishes external work from field work

A permanent rigid dipole of magnitude p rotates in a uniform field of magnitude E. Let θ\theta be the angle between the moment and field, and choose U(90∘)=0U(90^\circ)=0. An external actuator slowly rotates it from 30∘30^\circ to 120∘120^\circ without changing its kinetic energy.

Diagram shown in the original SVG worksheet.

  1. Derive U from the field torque and calculate the external work.

  2. Find the work done by the field and the largest opposing torque magnitude encountered during this rotation.

Question 2 - Solution

Quasistatic rotation distinguishes external work from field work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

τθ=−pEsin⁡θ,dUdθ=−τθ⇒U=−pEcos⁡θ.\tau_\theta=-pE\sin\theta,\quad\frac{dU}{d\theta}=-\tau_\theta\Rightarrow U=-pE\cos\theta.Wext=ΔU=pE(cos⁡30∘−cos⁡120∘)=3+12pE.W_{\mathrm{ext}}=\Delta U=pE(\cos30^\circ-\cos120^\circ)=\frac{\sqrt3+1}{2}pE.

(b) Interpretation and further calculation

Wfield=−ΔU=−3+12pE.W_{\mathrm{field}}=-\Delta U=-\frac{\sqrt3+1}{2}pE.max30∘≤θ≤120∘|τθ|=pEat θ=90∘.\max_{30^\circ\le\theta\le120^\circ}|\tau_\theta|=pE\quad\text{at }\theta=90^\circ.Quasistatic balance requires the actuator torque to oppose the field torque at each angle, not merely on average.

Physical check

The potential energy rises during the entire prescribed rotation since sin⁡θ>0\sin\theta>0 along the path.