The Electrical-Mechanical Analogy — Question 10

Section 31-2 · Physics pages 5010–5011

Question 10 A nonlinear capacitor corresponds to a hardening spring A supplied lossless capacitor model has voltage vC(q) = q/C + βq3 with positive beta. In series with L it is analogous to a cubic restoring spring. q vC Schematic; labels, not drawing lengths, specify the data. (a) Find the capacitor energy by integrating voltage against charge. (b) For a small oscillation about a maintained bias charge qb, find the local natural frequency; assume the bias source supplies constant voltage.
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Question 10 - Solution A nonlinear capacitor corresponds to a hardening spring q vC (a) Method and calculation UC(q) = ∫q 0 vC(u)du = q2/(2C) + βq4/4. L¨q + q/C + βq3 = 0 without bias . (b) Interpretation and further calculation q = qb + δq, vC(q) −vC(qb) ≃(1/C + 3βq2 b)δq. ω2 small = (1/C + 3βq2 b)/L . Physical check The cubic term changes local stiffness; the constant-C amplitude independence no longer applies.

Question 10

A nonlinear capacitor corresponds to a hardening spring

A supplied lossless capacitor model has voltage vC(q)=q/C+βq3v_C(q)=q/C+\beta q^3 with positive beta. In series with L it is analogous to a cubic restoring spring.

Diagram shown in the original SVG worksheet.

  1. Find the capacitor energy by integrating voltage against charge.

  2. For a small oscillation about a maintained bias charge qb, find the local natural frequency; assume the bias source supplies constant voltage.

Question 10 - Solution

A nonlinear capacitor corresponds to a hardening spring

Diagram shown in the original SVG worksheet.

(a) Method and calculation

UC(q)=∫0qvC(u)du=q2/(2C)+βq4/4.U_C(q)=\int_0^qv_C(u)du=q^2/(2C)+\beta q^4/4.Lq̈+q/C+βq3=0without bias.\boxed{L\ddot q+q/C+\beta q^3=0\quad\text{without bias}}.

(b) Interpretation and further calculation

q=qb+δq,vC(q)−vC(qb)≃(1/C+3βqb2)δq.q=q_b+\delta q,\quad v_C(q)-v_C(q_b)\simeq(1/C+3\beta q_b^2)\delta q.ωsmall2=(1/C+3βqb2)/L.\boxed{\omega_{\mathrm{small}}^2=(1/C+3\beta q_b^2)/L}.

Physical check

The cubic term changes local stiffness; the constant-C amplitude independence no longer applies.