A Dipole in an Electric Field — Question 8

Section 22-8 · Physics pages 3626–3627

Question 8 Induced dipole energy includes the cost of creating the dipole A small polarizable object has scalar induced moment p along a positive prescribed field E(x). Its model energy is U(p, x) = p2/(2α) −pE(x) with α > 0. The dipole adjusts quasistatically to minimize U at each x; neglect other forces and higher multipoles. − + E(x) p = αE Schematic; labels, not drawing lengths, specify the data. (a) Minimize over p and find the effective position-dependent energy. (b) Derive the force for E(x) = E0 + Gx > 0, and show why inserting p = αE into −pE alone gives an incorrect factor.
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Question 8 - Solution Induced dipole energy includes the cost of creating the dipole − + E(x) p = αE (a) Method and calculation ∂U ∂p = p/α −E = 0 ⇒p = αE, ∂2U ∂p2 = 1/α > 0. Ueff= αE2 2 −αE2 = −1 2αE2. (b) Interpretation and further calculation Fx = −dUeff dx = αE dE dx = αG(E0 + Gx). −d(−αE2) dx = 2αE dE dx = 2Fx. The internal polarization cost supplies the missing positive term in the energy; omitting it doubles the inferred force. Physical check For positive polarizability the force points toward increasing E2, within the stated quasistatic model.

Question 8

Induced dipole energy includes the cost of creating the dipole

A small polarizable object has scalar induced moment p along a positive prescribed field E(x)E(x). Its model energy is U(p,x)=p2/(2α)−pE(x)U(p,x)=p^2/(2\alpha)-pE(x) with α>0\alpha>0. The dipole adjusts quasistatically to minimize U at each x; neglect other forces and higher multipoles.

Diagram shown in the original SVG worksheet.

  1. Minimize over p and find the effective position-dependent energy.

  2. Derive the force for E(x)=E0+Gx>0E(x)=E_0+Gx>0, and show why inserting p=αEp=\alpha E into −pE-pE alone gives an incorrect factor.

Question 8 - Solution

Induced dipole energy includes the cost of creating the dipole

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂U∂p=p/α−E=0⇒p=αE,∂2U∂p2=1/α>0.\frac{\partial U}{\partial p}=p/\alpha-E=0\Rightarrow p=\alpha E,\quad\frac{\partial^2U}{\partial p^2}=1/\alpha>0.Ueff=αE22−αE2=−12αE2.U_{\mathrm{eff}}=\frac{\alpha E^2}{2}-\alpha E^2=-\tfrac12\alpha E^2.

(b) Interpretation and further calculation

Fx=−dUeffdx=αEdEdx=αG(E0+Gx).F_x=-\frac{dU_{\mathrm{eff}}}{dx}=\alpha E\frac{dE}{dx}=\alpha G(E_0+Gx).−d(−αE2)dx=2αEdEdx=2Fx.-\frac{d(-\alpha E^2)}{dx}=2\alpha E\frac{dE}{dx}=2F_x.The internal polarization cost supplies the missing positive term in the energy; omitting it doubles the inferred force.

Physical check

For positive polarizability the force points toward increasing E2E^2, within the stated quasistatic model.