LC Oscillations, Qualitatively — Question 10

Section 31-1 · Physics pages 4990–4991

Question 10 Reversing current reconstructs the earlier charge history At some instant an ideal LC oscillator has state (q∗, i∗). An idealized external operation reverses current without changing its magnitude or the capacitor charge. Ignore the switching implementation. q/Q i/Imax Schematic; labels, not drawing lengths, specify the data. (a) Compare the energy immediately before and after reversal. (b) Using the time-reversal symmetry of ¨q = −q/(LC), write the subsequent charge in terms of the original trajectory.
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Question 10 - Solution Reversing current reconstructs the earlier charge history q/Q i/Imax (a) Method and calculation U−= q2 ∗/(2C) + Li2 ∗/2, U+ = q2 ∗/(2C) + L(−i∗)2/2. U+ = U−. (b) Interpretation and further calculation qnew(t) = qold(−t) ⇒qnew(0) = q∗, ˙qnew(0) = −i∗. ¨qnew = −qnew/(LC) . Physical check Current reversal mirrors the initial state across the charge axis; subsequent charge values retrace the earlier charge history.

Question 10

Reversing current reconstructs the earlier charge history

At some instant an ideal LC oscillator has state (q*,i*)(q_*,i_*). An idealized external operation reverses current without changing its magnitude or the capacitor charge. Ignore the switching implementation.

Diagram shown in the original SVG worksheet.

  1. Compare the energy immediately before and after reversal.

  2. Using the time-reversal symmetry of q̈=−q/(LC)\ddot q=-q/(LC), write the subsequent charge in terms of the original trajectory.

Question 10 - Solution

Reversing current reconstructs the earlier charge history

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U−=q*2/(2C)+Li*2/2,U+=q*2/(2C)+L(−i*)2/2.U_- =q_*^2/(2C)+Li_*^2/2,\quad U_+=q_*^2/(2C)+L(-i_*)^2/2.U+=U−.\boxed{U_+=U_-}.

(b) Interpretation and further calculation

qnew(t)=qold(−t)⇒qnew(0)=q*,q̇new(0)=−i*.q_{\mathrm{new}}(t)=q_{\mathrm{old}}(-t)\Rightarrow q_{\mathrm{new}}(0)=q_*,\quad\dot q_{\mathrm{new}}(0)=-i_*.q̈new=−qnew/(LC).\boxed{\ddot q_{\mathrm{new}}=-q_{\mathrm{new}}/(LC)}.

Physical check

Current reversal mirrors the initial state across the charge axis; subsequent charge values retrace the earlier charge history.