RL Circuits — Question 5

Section 30-8 · Physics pages 4900–4901

Question 5 A finite charging pulse followed by a different discharge resistance has two time constants An initially unenergized inductor L is charged from source V through Rc for time T. It is then disconnected from the source and closed through Rd. Switching keeps a continuous current path and introduces no impulse voltage. t i Schematic; labels, not drawing lengths, specify the data. (a) Find current at the end of charging and during the subsequent discharge. (b) Find the total charge through Rd after switching.
Show solutionHide solution
Question 5 - Solution A finite charging pulse followed by a different discharge resistance has two time constants t i (a) Method and calculation τc = L/Rc, iT = V Rc (1 −e−T/τc) . i(T + s) = iT e−s/τd, τd = L/Rd, s ≥0 . (b) Interpretation and further calculation Qd = ∫∞ 0 iT e−s/τdds = iT τd. Qd = LV RcRd (1 −e−TRc/L) . Physical check Current is continuous at the switching time, but its derivative generally changes because the driving circuit changes.

Question 5

A finite charging pulse followed by a different discharge resistance has two time constants

An initially unenergized inductor L is charged from source V through Rc for time T. It is then disconnected from the source and closed through Rd. Switching keeps a continuous current path and introduces no impulse voltage.

Diagram shown in the original SVG worksheet.

  1. Find current at the end of charging and during the subsequent discharge.

  2. Find the total charge through Rd after switching.

Question 5 - Solution

A finite charging pulse followed by a different discharge resistance has two time constants

Diagram shown in the original SVG worksheet.

(a) Method and calculation

τc=L/Rc,iT=VRc(1−e−T/τc).\tau_c=L/R_c,\quad\boxed{i_T=\frac V{R_c}(1-e^{-T/\tau_c})}.i(T+s)=iTe−s/τd,τd=L/Rd,s≥0.\boxed{i(T+s)=i_Te^{-s/\tau_d},\quad\tau_d=L/R_d,\quad s\ge0}.

(b) Interpretation and further calculation

Qd=∫0∞iTe−s/τdds=iTτd.Q_d=\int_0^\infty i_Te^{-s/\tau_d}ds=i_T\tau_d.Qd=LVRcRd(1−e−TRc/L).\boxed{Q_d=\frac{LV}{R_cR_d}(1-e^{-TR_c/L})}.

Physical check

Current is continuous at the switching time, but its derivative generally changes because the driving circuit changes.