Self-Induction — Question 2

Section 30-7 · Physics pages 4874–4875

Question 2 A constant current offset changes flux linkage but not the self-induced emf An ideal constant-L inductor carries i(t) = Ic + I0e−t/T with positive constants. Define passive voltage along the current reference direction. t i Schematic; labels, not drawing lengths, specify the data. (a) Find voltage and self-induced emf. (b) Find the voltage-time integral from zero to infinity and explain the role of Ic.
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Question 2 - Solution A constant current offset changes flux linkage but not the self-induced emf t i (a) Method and calculation ˙i = −I0e−t/T /T ⇒v = −LI0e−t/T /T . Eself = +LI0e−t/T /T . (b) Interpretation and further calculation ∫∞ 0 vdt = L[i(∞) −i(0)] = −LI0 . Λ = LIc + LI0e−t/T ; d dt(LIc) = 0. Physical check The coil maintains nonzero final linkage LIc while the induced emf tends to zero.

Question 2

A constant current offset changes flux linkage but not the self-induced emf

An ideal constant-L inductor carries i(t)=Ic+I0e−t/Ti(t)=I_c+I_0e^{-t/T} with positive constants. Define passive voltage along the current reference direction.

Diagram shown in the original SVG worksheet.

  1. Find voltage and self-induced emf.

  2. Find the voltage-time integral from zero to infinity and explain the role of Ic.

Question 2 - Solution

A constant current offset changes flux linkage but not the self-induced emf

Diagram shown in the original SVG worksheet.

(a) Method and calculation

i̇=−I0e−t/T/T⇒v=−LI0e−t/T/T.\dot i=-I_0e^{-t/T}/T\Rightarrow\boxed{v=-LI_0e^{-t/T}/T}.ℰself=+LI0e−t/T/T.\boxed{\mathcal E_{\mathrm{self}}=+LI_0e^{-t/T}/T}.

(b) Interpretation and further calculation

∫0∞vdt=L[i(∞)−i(0)]=−LI0.\int_0^\infty vdt=L[i(\infty)-i(0)]=\boxed{-LI_0}.Λ=LIc+LI0e−t/T;ddt(LIc)=0.\Lambda=LI_c+LI_0e^{-t/T};\quad\frac d{dt}(LI_c)=0.

Physical check

The coil maintains nonzero final linkage LIc while the induced emf tends to zero.