Energy Stored in a Magnetic Field — Question 3

Section 30-9 · Physics pages 4916–4917

Question 3 Stored energy decays twice as fast in its exponent as the RL current An inductor L with initial current I0 discharges through resistance R. There is no source and the geometry is fixed. R L i Schematic; labels, not drawing lengths, specify the data. (a) Find stored energy as a function of time. (b) Compare the energy half-life with the current half-life and find heat released at the energy half-life.
Show solutionHide solution
Question 3 - Solution Stored energy decays twice as fast in its exponent as the RL current R L i (a) Method and calculation i = I0e−t/τ, τ = L/R ⇒U = 1 2LI2 0e−2t/τ. U(t) = U0e−2t/τ . (b) Interpretation and further calculation t1/2,U = 1 2τ ln 2 = 1 2t1/2,i . H(t1/2,U) = U0/2 = LI2 0/4 . Physical check Energy depends on current squared; applying the current decay fraction directly to energy gives the wrong time scale.

Question 3

Stored energy decays twice as fast in its exponent as the RL current

An inductor L with initial current I0 discharges through resistance R. There is no source and the geometry is fixed.

Diagram shown in the original SVG worksheet.

  1. Find stored energy as a function of time.

  2. Compare the energy half-life with the current half-life and find heat released at the energy half-life.

Question 3 - Solution

Stored energy decays twice as fast in its exponent as the RL current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

i=I0e−t/τ,τ=L/R⇒U=12LI02e−2t/τ.i=I_0e^{-t/\tau},\quad\tau=L/R\Rightarrow U=\tfrac12LI_0^2e^{-2t/\tau}.U(t)=U0e−2t/τ.\boxed{U(t)=U_0e^{-2t/\tau}}.

(b) Interpretation and further calculation

t1/2,U=12τln⁡2=12t1/2,i.\boxed{t_{1/2,U}=\tfrac12\tau\ln2=\tfrac12t_{1/2,i}}.H(t1/2,U)=U0/2=LI02/4.\boxed{H(t_{1/2,U})=U_0/2=LI_0^2/4}.

Physical check

Energy depends on current squared; applying the current decay fraction directly to energy gives the wrong time scale.