RL Circuits — Question 9

Section 30-8 · Physics pages 4908–4909

Question 9 A linearly increasing source produces an RL current that lags its resistive limit A series RL circuit starts with zero current and is driven by V (t) = αt for t nonnegative. Let τ = L/R. t i Schematic; labels, not drawing lengths, specify the data. (a) Solve for i(t). (b) Find the early-time leading behavior and the long-time difference from the purely resistive current alpha t/R.
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Question 9 - Solution A linearly increasing source produces an RL current that lags its resistive limit t i (a) Method and calculation L˙i + Ri = αt ⇒i(t) = α R[t −τ(1 −e−t/τ)] . t ≪τ : e−t/τ = 1 −t/τ + t2/(2τ 2) + · · · . (b) Interpretation and further calculation i(t) ≃αt2/(2L) (t ≪τ). t ≫τ : αt/R −i(t) →αL/R2 . Physical check The initial quadratic rise follows because both initial current and initial source voltage are zero.

Question 9

A linearly increasing source produces an RL current that lags its resistive limit

A series RL circuit starts with zero current and is driven by V(t)=αtV(t)=\alpha t for t nonnegative. Let τ=L/R\tau=L/R.

Diagram shown in the original SVG worksheet.

  1. Solve for i(t).

  2. Find the early-time leading behavior and the long-time difference from the purely resistive current alpha t/R.

Question 9 - Solution

A linearly increasing source produces an RL current that lags its resistive limit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Li̇+Ri=αt⇒i(t)=αR[t−τ(1−e−t/τ)].L\dot i+Ri=\alpha t\Rightarrow\boxed{i(t)=\frac\alpha R[t-\tau(1-e^{-t/\tau})]}.t≪τ:e−t/τ=1−t/τ+t2/(2τ2)+⋯.t\ll\tau:\quad e^{-t/\tau}=1-t/\tau+t^2/(2\tau^2)+\cdots.

(b) Interpretation and further calculation

i(t)≃αt2/(2L)(t≪τ).\boxed{i(t)\simeq\alpha t^2/(2L)}\quad(t\ll\tau).t≫τ:αt/R−i(t)→αL/R2.t\gg\tau:\quad\boxed{\alpha t/R-i(t)\to\alpha L/R^2}.

Physical check

The initial quadratic rise follows because both initial current and initial source voltage are zero.