Energy Stored in a Magnetic Field — Question 10

Section 30-9 · Physics pages 4930–4931

Question 10 A reversed source can recover part of the energy initially stored in an RL circuit A series RL circuit initially carries I0 = V/R in steady state. The source is reversed to -V at t=0. Until current reaches zero, i = I0(2e−t/τ −1) with τ = L/R. −V R L i Schematic; labels, not drawing lengths, specify the data. (a) Find the energy returned to the reversed source before current first reaches zero. (b) Find the heat dissipated in that interval and verify the energy balance.
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Question 10 - Solution A reversed source can recover part of the energy initially stored in an RL circuit −V R L i (a) Method and calculation i(t0) = 0 ⇒t0 = τ ln 2, Wreturned = ∫t0 0 V i(t)dt. Wreturned = LI2 0(1 −ln 2) . (b) Interpretation and further calculation U0 = 1 2LI2 0, U(t0) = 0. H = U0 −Wreturned = LI2 0(ln 2 −1/2) > 0 . Physical check The reversed source absorbs energy while the current retains its original direction; both recovered energy and heat come from the initial magnetic energy.

Question 10

A reversed source can recover part of the energy initially stored in an RL circuit

A series RL circuit initially carries I0=V/RI_0=V/R in steady state. The source is reversed to -V at t=0. Until current reaches zero, i=I0(2e−t/τ−1)i=I_0(2e^{-t/\tau}-1) with τ=L/R\tau=L/R.

Diagram shown in the original SVG worksheet.

  1. Find the energy returned to the reversed source before current first reaches zero.

  2. Find the heat dissipated in that interval and verify the energy balance.

Question 10 - Solution

A reversed source can recover part of the energy initially stored in an RL circuit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

i(t0)=0⇒t0=τln⁡2,Wreturned=∫0t0Vi(t)dt.i(t_0)=0\Rightarrow t_0=\tau\ln2,\quad W_{\mathrm{returned}}=\int_0^{t_0}Vi(t)dt.Wreturned=LI02(1−ln⁡2).\boxed{W_{\mathrm{returned}}=LI_0^2(1-\ln2)}.

(b) Interpretation and further calculation

U0=12LI02,U(t0)=0.U_0=\tfrac12LI_0^2,\quad U(t_0)=0.H=U0−Wreturned=LI02(ln⁡2−1/2)>0.\boxed{H=U_0-W_{\mathrm{returned}}=LI_0^2(\ln2-1/2)>0}.

Physical check

The reversed source absorbs energy while the current retains its original direction; both recovered energy and heat come from the initial magnetic energy.