Damped Oscillations in an RLC Circuit — Question 5

Section 31-4 · Physics pages 5040–5041

Question 5 An energy envelope cannot replace the exact instantaneous loss equation Consider an underdamped source-free RLC circuit. A proposed exact energy law is U(t) = U(0)e−Rt/L for release from q=Q0, i=0. ωt q/Q0 Schematic; labels, not drawing lengths, specify the data. (a) Test the proposed law at t=0 using the exact energy derivative. (b) Show why this exponential law does hold for energies sampled one damped period apart.
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Question 5 - Solution An energy envelope cannot replace the exact instantaneous loss equation ωt q/Q0 (a) Method and calculation ˙U = −Ri2 ⇒˙U(0) = 0. ˙Uproposed 0 = −RU(0)/L̸ = 0 not an exact continuous-time law . (b) Interpretation and further calculation (q, i)(t + Td) = e−αTd(q, i)(t), 2α = R/L. U(t + Td) = e−RTd/LU(t) . Physical check The same-phase sampled energy has a simple exponential ratio even though instantaneous energy includes phase dependence.

Question 5

An energy envelope cannot replace the exact instantaneous loss equation

Consider an underdamped source-free RLC circuit. A proposed exact energy law is U(t)=U(0)e−Rt/LU(t)=U(0)e^{-Rt/L} for release from q=Q0, i=0.

Diagram shown in the original SVG worksheet.

  1. Test the proposed law at t=0 using the exact energy derivative.

  2. Show why this exponential law does hold for energies sampled one damped period apart.

Question 5 - Solution

An energy envelope cannot replace the exact instantaneous loss equation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U̇=−Ri2⇒U̇(0)=0.\dot U=-Ri^2\Rightarrow\dot U(0)=0.U̇proposed|0=−RU(0)/L≠0not an exact continuous-time law.\left.\dot U_{\mathrm{proposed}}\right|_0=-RU(0)/L\ne0\quad\boxed{\text{not an exact continuous-time law}}.

(b) Interpretation and further calculation

(q,i)(t+Td)=e−αTd(q,i)(t),2α=R/L.(q,i)(t+T_d)=e^{-\alpha T_d}(q,i)(t),\quad2\alpha=R/L.U(t+Td)=e−RTd/LU(t).\boxed{U(t+T_d)=e^{-RT_d/L}U(t)}.

Physical check

The same-phase sampled energy has a simple exponential ratio even though instantaneous energy includes phase dependence.