Potential Due to an Electric Dipole — Question 6

Section 24-7 · Physics pages 3922–3923

Question 6 Rotating a dipole in an external voltage gradient changes its interaction energy A small rigid dipole has charges ±q separated by vector d from minus to plus. An external uniform field is Eˆz with potential Vext = −Ez + C. Its moment magnitude is p=qd. E p Schematic; labels, not drawing lengths, specify the data. (a) Sum the two source-potential energies and obtain the orientation-dependent interaction energy. (b) Find the quasistatic external work rotating it from 30◦to 120◦relative to the field.
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Question 6 - Solution Rotating a dipole in an external voltage gradient changes its interaction energy E p (a) Method and calculation U = qVext(z+) −qVext(z−) = −qE(z+ −z−). U = −pE cos θ; qC −qC = 0. (b) Interpretation and further calculation Wext = Uf −Ui = pE(cos 30◦−cos 120◦). Wext = √ 3 + 1 2 pE ≈1.36603pE. Physical check The internal energy of the rigid dipole is unchanged; only its interaction with the external field contributes to the rotation work.

Question 6

Rotating a dipole in an external voltage gradient changes its interaction energy

A small rigid dipole has charges ±q\pm q separated by vector d from minus to plus. An external uniform field is E𝒛̂E\hat{\mathbf z} with potential Vext=−Ez+CV_{\mathrm{ext}}=-Ez+C. Its moment magnitude is p=qd.

Diagram shown in the original SVG worksheet.

  1. Sum the two source-potential energies and obtain the orientation-dependent interaction energy.

  2. Find the quasistatic external work rotating it from 30∘30^\circ to 120∘120^\circ relative to the field.

Question 6 - Solution

Rotating a dipole in an external voltage gradient changes its interaction energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=qVext(z+)−qVext(z−)=−qE(z+−z−).U=qV_{\mathrm{ext}}(z_+)-qV_{\mathrm{ext}}(z_-)=-qE(z_+-z_-).U=−pEcos⁡θ;qC−qC=0.U=-pE\cos\theta;\quad qC-qC=0.

(b) Interpretation and further calculation

Wext=Uf−Ui=pE(cos⁡30∘−cos⁡120∘).W_{\mathrm{ext}}=U_f-U_i=pE(\cos30^\circ-\cos120^\circ).Wext=3+12pE≈1.36603pE.W_{\mathrm{ext}}=\frac{\sqrt3+1}{2}pE\approx1.36603pE.

Physical check

The internal energy of the rigid dipole is unchanged; only its interaction with the external field contributes to the rotation work.