Forced Oscillations — Question 4

Section 31-6 · Physics pages 5078–5079

Question 4 An ideal undamped resonant drive produces secular growth An ideal LC loop with zero resistance is driven from rest by Vp cos ω0t, where ω0 = 1/ √ LC. Initially q=i=0. t q Schematic; labels, not drawing lengths, specify the data. (a) Find q(t) using a trial solution proportional to t sin ω0t. (b) Find current and the leading large-time stored energy.
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Question 4 - Solution An ideal undamped resonant drive produces secular growth t q (a) Method and calculation (d2/dt2 + ω2 0)(t sin ω0t) = 2ω0 cos ω0t. q = Vp 2Lω0 t sin ω0t . (b) Interpretation and further calculation i = Vp 2Lω0 [sin ω0t + ω0t cos ω0t] . U(t) = V 2 p 8Lt2 + O(t) (t →∞) . Physical check No finite steady resonant amplitude exists when the model has no loss.

Question 4

An ideal undamped resonant drive produces secular growth

An ideal LC loop with zero resistance is driven from rest by Vpcos⁡ω0tV_p\cos\omega_0t, where ω0=1/LC\omega_0=1/\sqrt{LC}. Initially q=i=0.

Diagram shown in the original SVG worksheet.

  1. Find q(t) using a trial solution proportional to tsin⁡ω0tt\sin\omega_0t.

  2. Find current and the leading large-time stored energy.

Question 4 - Solution

An ideal undamped resonant drive produces secular growth

Diagram shown in the original SVG worksheet.

(a) Method and calculation

(d2/dt2+ω02)(tsin⁡ω0t)=2ω0cos⁡ω0t.(d^2/dt^2+\omega_0^2)(t\sin\omega_0t)=2\omega_0\cos\omega_0t.q=Vp2Lω0tsin⁡ω0t.\boxed{q=\frac{V_p}{2L\omega_0}t\sin\omega_0t}.

(b) Interpretation and further calculation

i=Vp2Lω0[sin⁡ω0t+ω0tcos⁡ω0t].\boxed{i=\frac{V_p}{2L\omega_0}[\sin\omega_0t+\omega_0t\cos\omega_0t]}.U(t)=Vp28Lt2+O(t)(t→∞).\boxed{U(t)=\frac{V_p^2}{8L}t^2+O(t)\quad(t\to\infty)}.

Physical check

No finite steady resonant amplitude exists when the model has no loss.