Forced Oscillations — Question 10

Section 31-6 · Physics pages 5090–5091

Question 10 An undamped off-resonant switch-on retains beats instead of settling A lossless LC loop starts from q=i=0 under Vp cos ωt, with ω̸ = ω0. t q Schematic; labels, not drawing lengths, specify the data. (a) Find the exact charge including the natural-frequency term. (b) Factor the result to expose the slow modulation when the frequencies are close.
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Question 10 - Solution An undamped off-resonant switch-on retains beats instead of settling t q (a) Method and calculation qp = Vp cos ωt L(ω2 0 −ω2), qh = −Vp cos ω0t L(ω2 0 −ω2). q = Vp(cos ωt −cos ω0t) L(ω2 0 −ω2) . (b) Interpretation and further calculation cos a −cos b = −2 sin[(a + b)/2] sin[(a −b)/2]. q = 2Vp sin[(ω0 + ω)t/2] sin[(ω0 −ω)t/2] L(ω2 0 −ω2) . Physical check Without resistance the natural component does not disappear, so a unique attracting steady state is absent.

Question 10

An undamped off-resonant switch-on retains beats instead of settling

A lossless LC loop starts from q=i=0 under Vpcos⁡ωtV_p\cos\omega t, with ω≠ω0\omega\ne\omega_0.

Diagram shown in the original SVG worksheet.

  1. Find the exact charge including the natural-frequency term.

  2. Factor the result to expose the slow modulation when the frequencies are close.

Question 10 - Solution

An undamped off-resonant switch-on retains beats instead of settling

Diagram shown in the original SVG worksheet.

(a) Method and calculation

qp=Vpcos⁡ωtL(ω02−ω2),qh=−Vpcos⁡ω0tL(ω02−ω2).q_p=\frac{V_p\cos\omega t}{L(\omega_0^2-\omega^2)},\quad q_h=-\frac{V_p\cos\omega_0t}{L(\omega_0^2-\omega^2)}.q=Vp(cos⁡ωt−cos⁡ω0t)L(ω02−ω2).\boxed{q=\frac{V_p(\cos\omega t-\cos\omega_0t)}{L(\omega_0^2-\omega^2)}}.

(b) Interpretation and further calculation

cos⁡a−cos⁡b=−2sin⁡[(a+b)/2]sin⁡[(a−b)/2].\cos a-\cos b=-2\sin[(a+b)/2]\sin[(a-b)/2].q=2Vpsin⁡[(ω0+ω)t/2]sin⁡[(ω0−ω)t/2]L(ω02−ω2).\boxed{q=\frac{2V_p\sin[(\omega_0+\omega)t/2]\sin[(\omega_0-\omega)t/2]}{L(\omega_0^2-\omega^2)}}.

Physical check

Without resistance the natural component does not disappear, so a unique attracting steady state is absent.