Damped Oscillations in an RLC Circuit — Question 6

Section 31-4 · Physics pages 5042–5043

Question 6 Damping delays the first zero of charge beyond a quarter damped period An underdamped circuit is released from q=Q0 and i=0, with q = Q0e−αt[cos ωdt+(α/ωd) sin ωdt]. ωt q/Q0 Schematic; labels, not drawing lengths, specify the data. (a) Find the first positive time at which q=0. (b) Compare it with the first current zero after release.
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Question 6 - Solution Damping delays the first zero of charge beyond a quarter damped period ωt q/Q0 (a) Method and calculation tan ωdt = −ωd/α, π/2 < ωdt < π. tq=0 = π/2 + tan−1(α/ωd) ωd . (b) Interpretation and further calculation i ∝−e−αt sin ωdt ⇒ti=0 = π/ωd . Td/4 < tq=0 < Td/2 . Physical check For zero damping the charge zero returns to T/4; finite damping changes the release phase.

Question 6

Damping delays the first zero of charge beyond a quarter damped period

An underdamped circuit is released from q=Q0 and i=0, with q=Q0e−αt[cos⁡ωdt+(α/ωd)sin⁡ωdt]q=Q_0e^{-\alpha t}[\cos\omega_dt+(\alpha/\omega_d)\sin\omega_dt].

Diagram shown in the original SVG worksheet.

  1. Find the first positive time at which q=0.

  2. Compare it with the first current zero after release.

Question 6 - Solution

Damping delays the first zero of charge beyond a quarter damped period

Diagram shown in the original SVG worksheet.

(a) Method and calculation

tan⁡ωdt=−ωd/α,π/2<ωdt<π.\tan\omega_dt=-\omega_d/\alpha,\quad\pi/2<\omega_dt<\pi.tq=0=π/2+tan⁡−1(α/ωd)ωd.\boxed{t_{q=0}=\frac{\pi/2+\tan^{-1}(\alpha/\omega_d)}{\omega_d}}.

(b) Interpretation and further calculation

i∝−e−αtsin⁡ωdt⇒ti=0=π/ωd.i\propto-e^{-\alpha t}\sin\omega_dt\Rightarrow\boxed{t_{i=0}=\pi/\omega_d}.Td/4<tq=0<Td/2.\boxed{T_d/4<t_{q=0}<T_d/2}.

Physical check

For zero damping the charge zero returns to T/4; finite damping changes the release phase.