RL Circuits — Question 4

Section 30-8 · Physics pages 4898–4899

Question 4 Reversing the source does not reverse inductor current immediately A series RL circuit has reached steady current V/R under source +V. At t=0 the source is switched to -V with R and L unchanged. Define the old current direction as positive. V (t) R L i Schematic; labels, not drawing lengths, specify the data. (a) Find current for t>0. (b) Find when current first crosses zero and its slope immediately after reversal.
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Question 4 - Solution Reversing the source does not reverse inductor current immediately V (t) R L i (a) Method and calculation if = −V/R, i(0+) = V/R, τ = L/R. i(t) = −V/R + (2V/R)e−t/τ . (b) Interpretation and further calculation i = 0 ⇒e−t/τ = 1/2 ⇒t = τ ln 2 . ˙i(0+) = (−V −R(V/R))/L = −2V/L . Physical check During the initial interval after reversal, current still flows in the old direction while the source absorbs electrical power.

Question 4

Reversing the source does not reverse inductor current immediately

A series RL circuit has reached steady current V/R under source +V. At t=0 the source is switched to -V with R and L unchanged. Define the old current direction as positive.

Diagram shown in the original SVG worksheet.

  1. Find current for t>0.

  2. Find when current first crosses zero and its slope immediately after reversal.

Question 4 - Solution

Reversing the source does not reverse inductor current immediately

Diagram shown in the original SVG worksheet.

(a) Method and calculation

if=−V/R,i(0+)=V/R,τ=L/R.i_f=-V/R,\quad i(0^+)=V/R,\quad\tau=L/R.i(t)=−V/R+(2V/R)e−t/τ.\boxed{i(t)=-V/R+(2V/R)e^{-t/\tau}}.

(b) Interpretation and further calculation

i=0⇒e−t/τ=1/2⇒t=τln⁡2.i=0\Rightarrow e^{-t/\tau}=1/2\Rightarrow\boxed{t=\tau\ln2}.i̇(0+)=(−V−R(V/R))/L=−2V/L.\boxed{\dot i(0^+)=(-V-R(V/R))/L=-2V/L}.

Physical check

During the initial interval after reversal, current still flows in the old direction while the source absorbs electrical power.