LC Oscillations, Qualitatively — Question 7

Section 31-1 · Physics pages 4984–4985

Question 7 A vanishing current marks maximum capacitor energy rather than no dynamics At an instant in an ideal LC loop, i = 0 and q = −Q. Use L˙i = −q/C. C L q i = ˙q Schematic; labels, not drawing lengths, specify the data. (a) Find the sign of the current derivative and the next direction of current. (b) Find the leading small-time changes in current and charge, measuring time from that instant.
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Question 7 - Solution A vanishing current marks maximum capacitor energy rather than no dynamics C L q i = ˙q (a) Method and calculation ˙i(0) = Q/(LC) > 0 ⇒i(dt) > 0 . i(dt) = Q LC dt + O(dt3). (b) Interpretation and further calculation q(dt) = q(0) + ∫dt 0 i(t)dt. q(dt) = −Q + Q 2LC dt2 + O(dt4) . Physical check The restoring capacitor voltage is largest when current is momentarily zero.

Question 7

A vanishing current marks maximum capacitor energy rather than no dynamics

At an instant in an ideal LC loop, i=0i=0 and q=−Qq=-Q. Use Li̇=−q/CL\dot i=-q/C.

Diagram shown in the original SVG worksheet.

  1. Find the sign of the current derivative and the next direction of current.

  2. Find the leading small-time changes in current and charge, measuring time from that instant.

Question 7 - Solution

A vanishing current marks maximum capacitor energy rather than no dynamics

Diagram shown in the original SVG worksheet.

(a) Method and calculation

i̇(0)=Q/(LC)>0⇒i(dt)>0.\dot i(0)=Q/(LC)>0\Rightarrow\boxed{i(dt)>0}.i(dt)=QLCdt+O(dt3).i(dt)=\frac{Q}{LC}dt+O(dt^3).

(b) Interpretation and further calculation

q(dt)=q(0)+∫0dti(t)dt.q(dt)=q(0)+\int_0^{dt}i(t)dt.q(dt)=−Q+Q2LCdt2+O(dt4).\boxed{q(dt)=-Q+\frac{Q}{2LC}dt^2+O(dt^4)}.

Physical check

The restoring capacitor voltage is largest when current is momentarily zero.