RL Circuits — Question 7

Section 30-8 · Physics pages 4904–4905

Question 7 The resistance seen by an inductor sets its time constant in a branched circuit A source V feeds series resistance Rs into a node connected to ground through resistor R and ideal inductor L in parallel. The source steps on at t=0 with zero inductor current. V Rs L i R Schematic; labels, not drawing lengths, specify the data. (a) Find the Thevenin voltage and resistance seen by L, then its current response. (b) Find initial current slope and final inductor current.
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Question 7 - Solution The resistance seen by an inductor sets its time constant in a branched circuit V Rs L i R (a) Method and calculation Vth = V R Rs + R, Rth = Rs ∥R = RsR Rs + R. iL(t) = V Rs (1 −e−t/τ), τ = L(Rs + R) RsR . (b) Interpretation and further calculation ˙iL(0+) = Vth/L = V R L(Rs + R) . iL(∞) = V/Rs ; vnode(∞) = 0. Physical check At steady state the ideal inductor shorts the parallel resistor; the transient resistance is nevertheless Rs in parallel with R.

Question 7

The resistance seen by an inductor sets its time constant in a branched circuit

A source V feeds series resistance Rs into a node connected to ground through resistor R and ideal inductor L in parallel. The source steps on at t=0 with zero inductor current.

Diagram shown in the original SVG worksheet.

  1. Find the Thevenin voltage and resistance seen by L, then its current response.

  2. Find initial current slope and final inductor current.

Question 7 - Solution

The resistance seen by an inductor sets its time constant in a branched circuit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vth=VRRs+R,Rth=Rs∥R=RsRRs+R.V_{\mathrm{th}}=\frac{VR}{R_s+R},\quad R_{\mathrm{th}}=R_s\parallel R=\frac{R_sR}{R_s+R}.iL(t)=VRs(1−e−t/τ),τ=L(Rs+R)RsR.\boxed{i_L(t)=\frac{V}{R_s}(1-e^{-t/\tau}),\quad\tau=\frac{L(R_s+R)}{R_sR}}.

(b) Interpretation and further calculation

i̇L(0+)=Vth/L=VRL(Rs+R).\boxed{\dot i_L(0^+)=V_{\mathrm{th}}/L=\frac{VR}{L(R_s+R)}}.iL(∞)=V/Rs;vnode(∞)=0.\boxed{i_L(\infty)=V/R_s};\quad v_{\mathrm{node}}(\infty)=0.

Physical check

At steady state the ideal inductor shorts the parallel resistor; the transient resistance is nevertheless Rs in parallel with R.