LC Oscillations, Quantitatively — Question 1

Section 31-3 · Physics pages 5012–5013

Question 1 Two nonzero initial conditions determine the LC phase An ideal LC loop has L = .500 H, C = 2.00 µF, q(0) = 6.00 µC, and i(0) = 8.00 mA, with i = ˙q. C L q i = ˙q Schematic; labels, not drawing lengths, specify the data. (a) Find q(t), its amplitude, and its phase in the form Q cos(ωt −δ). (b) Find peak current and total energy.
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Question 1 - Solution Two nonzero initial conditions determine the LC phase C L q i = ˙q (a) Method and calculation ω = 1/ √ LC = 1000 s−1, q = q0 cos ωt + (i0/ω) sin ωt. q = (10.0 µC) cos(1000t −.927295), δ = tan−1(8/6) . (b) Interpretation and further calculation Imax = ωQ = .0100 A, U = Q2/(2C). U = 25.0 µJ . Physical check A positive initial current requires a negative phase in the cosine argument.

Question 1

Two nonzero initial conditions determine the LC phase

An ideal LC loop has L=.500L=.500 H, C=2.00μFC=2.00\,\mu F, q(0)=6.00μCq(0)=6.00\,\mu C, and i(0)=8.00i(0)=8.00 mA, with i=q̇i=\dot q.

Diagram shown in the original SVG worksheet.

  1. Find q(t), its amplitude, and its phase in the form Qcos⁡(ωt−δ)Q\cos(\omega t-\delta).

  2. Find peak current and total energy.

Question 1 - Solution

Two nonzero initial conditions determine the LC phase

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ω=1/LC=1000s−1,q=q0cos⁡ωt+(i0/ω)sin⁡ωt.\omega=1/\sqrt{LC}=1000\,s^{-1},\quad q=q_0\cos\omega t+(i_0/\omega)\sin\omega t.q=(10.0μC)cos⁡(1000t−.927295),δ=tan⁡−1(8/6).\boxed{q=(10.0\,\mu C)\cos(1000t-.927295),\quad\delta=\tan^{-1}(8/6)}.

(b) Interpretation and further calculation

Imax=ωQ=.0100A,U=Q2/(2C).I_{\max}=\omega Q=.0100\,A,\quad U=Q^2/(2C).U=25.0μJ.\boxed{U=25.0\,\mu J}.

Physical check

A positive initial current requires a negative phase in the cosine argument.