RL Circuits — Question 3

Section 30-8 · Physics pages 4896–4897

Question 3 Winding resistance changes both the final current and the rise time A coil with inductance L=.240 H and winding resistance r=2.00 ohms is placed in series with external resistance R=4.00 ohms and a 9.00-V step source. Initial current is zero. V R + r L i Schematic; labels, not drawing lengths, specify the data. (a) Find current as a function of time. (b) Find the steady terminal voltage across the complete coil and the error in the time constant if r is ignored.
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Question 3 - Solution Winding resistance changes both the final current and the rise time V R + r L i (a) Method and calculation L˙i + (R + r)i = V ⇒i = 1.50(1 −e−t/.0400) A . τ = L/(R + r) = .0400 s, i∞= 1.50 A. (b) Interpretation and further calculation vcoil,∞= ri∞= 3.00 V . τnaive = L/R = .0600 s ⇒(τnaive −τ)/τ = 50.0% . Physical check An ideal inductor has zero steady voltage, but a real coil retains the voltage drop across its winding resistance.

Question 3

Winding resistance changes both the final current and the rise time

A coil with inductance L=.240 H and winding resistance r=2.00 ohms is placed in series with external resistance R=4.00 ohms and a 9.00-V step source. Initial current is zero.

Diagram shown in the original SVG worksheet.

  1. Find current as a function of time.

  2. Find the steady terminal voltage across the complete coil and the error in the time constant if r is ignored.

Question 3 - Solution

Winding resistance changes both the final current and the rise time

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Li̇+(R+r)i=V⇒i=1.50(1−e−t/.0400)A.L\dot i+(R+r)i=V\Rightarrow\boxed{i=1.50(1-e^{-t/.0400})\,A}.τ=L/(R+r)=.0400s,i∞=1.50A.\tau=L/(R+r)=.0400\,s,\quad i_\infty=1.50\,A.

(b) Interpretation and further calculation

vcoil,∞=ri∞=3.00V.v_{\mathrm{coil,\infty}}=ri_\infty=\boxed{3.00\,V}.τnaive=L/R=.0600s⇒(τnaive−τ)/τ=50.0%.\tau_{\mathrm{naive}}=L/R=.0600\,s\Rightarrow\boxed{(\tau_{\mathrm{naive}}-\tau)/\tau=50.0\%}.

Physical check

An ideal inductor has zero steady voltage, but a real coil retains the voltage drop across its winding resistance.