The Electrical-Mechanical Analogy — Question 3

Section 31-2 · Physics pages 4996–4997

Question 3 A scaled circuit analogue can run faster than the mechanical motion Let a mechanical solution x(s) satisfy mxss + bxs + kx = F(s). Build an electrical analogue with q(t) = ax(γt), where a has units C/m and gamma is dimensionless. Choose positive L. m k x Schematic; labels, not drawing lengths, specify the data. (a) Derive R and C so the circuit equation is a constant multiple of the mechanical equation. (b) Find the required driving voltage in terms of F.
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Question 3 - Solution A scaled circuit analogue can run faster than the mechanical motion m k x (a) Method and calculation ˙q = aγxs, ¨q = aγ2xss. R = Lγb/m, C = m/(Lγ2k) . (b) Interpretation and further calculation L¨q + R ˙q + q/C = Laγ2 m (mxss + bxs + kx). v(t) = Laγ2 m F(γt) . Physical check The time scale changes both damping and stiffness ratios; matching just the natural frequency is insufficient for a damped analogue.

Question 3

A scaled circuit analogue can run faster than the mechanical motion

Let a mechanical solution x(s) satisfy mxss+bxs+kx=F(s)m x_{ss}+b x_s+kx=F(s). Build an electrical analogue with q(t)=ax(γt)q(t)=a x(\gamma t), where a has units C/m and gamma is dimensionless. Choose positive L.

Diagram shown in the original SVG worksheet.

  1. Derive R and C so the circuit equation is a constant multiple of the mechanical equation.

  2. Find the required driving voltage in terms of F.

Question 3 - Solution

A scaled circuit analogue can run faster than the mechanical motion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

q̇=aγxs,q̈=aγ2xss.\dot q=a\gamma x_s,\quad\ddot q=a\gamma^2x_{ss}.R=Lγb/m,C=m/(Lγ2k).\boxed{R=L\gamma b/m,\quad C=m/(L\gamma^2k)}.

(b) Interpretation and further calculation

Lq̈+Rq̇+q/C=Laγ2m(mxss+bxs+kx).L\ddot q+R\dot q+q/C=\frac{La\gamma^2}{m}(mx_{ss}+bx_s+kx).v(t)=Laγ2mF(γt).\boxed{v(t)=\frac{La\gamma^2}{m}F(\gamma t)}.

Physical check

The time scale changes both damping and stiffness ratios; matching just the natural frequency is insufficient for a damped analogue.