Energy Stored in an Electric Field — Question 9

Section 25-4 · Physics pages 4088–4089

Question 9 A voltage-driven spring plate loses stability before the gap closes A movable capacitor plate of area A is attached to a spring of stiffness K. Its zero-voltage gap is d0 and its displacement toward the fixed plate is x. At fixed V, take the attractive force as Fe = ϵ0AV 2/[2(d0 −x)2], for 0 < x < d0. x Schematic; labels, not drawing lengths, specify the data. (a) Find the equilibrium relation between V and x. (b) Use force-slope stability to find the critical displacement and pull-in voltage.
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Question 9 - Solution A voltage-driven spring plate loses stability before the gap closes x (a) Method and calculation Kx = ϵ0AV 2 2(d0 −x)2 . V 2 = 2K ϵ0Ax(d0 −x)2. (b) Interpretation and further calculation stable: K > dFe dx = ϵ0AV 2 (d0 −x)3 = 2Kx d0 −x ⇒x < d0/3. xcrit = d0/3, Vpull = √ 8Kd3 0 27ϵ0A. Physical check The unstable branch is not a second stable operating state; the ideal fixed-voltage force grows faster than the restoring force beyond the threshold.

Question 9

A voltage-driven spring plate loses stability before the gap closes

A movable capacitor plate of area A is attached to a spring of stiffness K. Its zero-voltage gap is d0 and its displacement toward the fixed plate is x. At fixed V, take the attractive force as Fe=ϵ0AV2/[2(d0−x)2]F_e=\epsilon_0AV^2/[2(d_0-x)^2], for 0<x<d00<x<d_0.

Diagram shown in the original SVG worksheet.

  1. Find the equilibrium relation between V and x.

  2. Use force-slope stability to find the critical displacement and pull-in voltage.

Question 9 - Solution

A voltage-driven spring plate loses stability before the gap closes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Kx=ϵ0AV22(d0−x)2.Kx=\frac{\epsilon_0AV^2}{2(d_0-x)^2}.V2=2Kϵ0Ax(d0−x)2.V^2=\frac{2K}{\epsilon_0A}x(d_0-x)^2.

(b) Interpretation and further calculation

stable: K>dFedx=ϵ0AV2(d0−x)3=2Kxd0−x⇒x<d0/3.\text{stable: }K>\frac{dF_e}{dx}=\frac{\epsilon_0AV^2}{(d_0-x)^3}=\frac{2Kx}{d_0-x}\Rightarrow x<d_0/3.xcrit=d0/3,Vpull=8Kd0327ϵ0A.x_{\mathrm{crit}}=d_0/3,\quad V_{\mathrm{pull}}=\sqrt{\frac{8Kd_0^3}{27\epsilon_0A}}.

Physical check

The unstable branch is not a second stable operating state; the ideal fixed-voltage force grows faster than the restoring force beyond the threshold.