Capacitor with a Dielectric — Question 7

Section 25-5 · Physics pages 4104–4105

Question 7 A partially inserted dielectric experiences an inward force under either constraint A dielectric of relative permittivity κ > 1 slides distance x into a rectangular plate gap d. Plate width is w and length L; 0 < x < L. Use C(x) = ϵ0w[L + (κ −1)x]/d and neglect edge corrections. κ insertion Schematic; labels, not drawing lengths, specify the data. (a) Find the inward electric force at fixed voltage V. (b) Find it at fixed charge Q and compare how each depends on insertion depth.
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Question 7 - Solution A partially inserted dielectric experiences an inward force under either constraint κ insertion (a) Method and calculation C′(x) = ϵ0w(κ −1)/d. Fx,V = 1 2V 2C′(x) = ϵ0w(κ −1)V 2 2d > 0. (b) Interpretation and further calculation Fx,Q = −d dx Q2 2C(x) = Q2C′(x) 2C(x)2 > 0. Fx,V is constant; Fx,Q ∝[L + (κ −1)x]−2. Physical check The force remains inward at fixed charge, but weakens as the increasing capacitance lowers the voltage.

Question 7

A partially inserted dielectric experiences an inward force under either constraint

A dielectric of relative permittivity κ>1\kappa>1 slides distance x into a rectangular plate gap d. Plate width is w and length L; 0<x<L0<x<L. Use C(x)=ϵ0w[L+(κ−1)x]/dC(x)=\epsilon_0w[L+(\kappa-1)x]/d and neglect edge corrections.

Diagram shown in the original SVG worksheet.

  1. Find the inward electric force at fixed voltage V.

  2. Find it at fixed charge Q and compare how each depends on insertion depth.

Question 7 - Solution

A partially inserted dielectric experiences an inward force under either constraint

Diagram shown in the original SVG worksheet.

(a) Method and calculation

C′(x)=ϵ0w(κ−1)/d.C\prime(x)=\epsilon_0w(\kappa-1)/d.Fx,V=12V2C′(x)=ϵ0w(κ−1)V22d>0.F_{x,V}=\tfrac12V^2C\prime(x)=\frac{\epsilon_0w(\kappa-1)V^2}{2d}>0.

(b) Interpretation and further calculation

Fx,Q=−ddxQ22C(x)=Q2C′(x)2C(x)2>0.F_{x,Q}=-\frac d{dx}\frac{Q^2}{2C(x)}=\frac{Q^2C\prime(x)}{2C(x)^2}>0.Fx,V is constant;Fx,Q∝[L+(κ−1)x]−2.F_{x,V}\text{ is constant};\quad F_{x,Q}\propto[L+(\kappa-1)x]^{-2}.

Physical check

The force remains inward at fixed charge, but weakens as the increasing capacitance lowers the voltage.