Mutual Induction — Question 2

Section 30-11 · Physics pages 4954–4955

Question 2 Changing separation induces a voltage even at constant primary current Two coaxial coils have positive mutual inductance M(x) = C/x3, where x is separation and C is constant. Coil 2 is open. Define its induced emf as E2 = −d(MI1)/dt. source I1(t) pickup Φ x Schematic; labels, not drawing lengths, specify the data. (a) Find the emf when both primary current and separation can change. (b) For constant positive I1 and constant outward speed v, find the emf and the current law that would instead cancel it.
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Question 2 - Solution Changing separation induces a voltage even at constant primary current source I1(t) pickup Φ x (a) Method and calculation E2 = −M ˙I1 −I1 dM dx ˙x = −C x3 ˙I1 + 3CI1 ˙x x4 . E2 = 3CI1v/x4 ( ˙I1 = 0) . (b) Interpretation and further calculation E2 = 0 ⇒d(MI1)/dt = 0 ⇒I1/x3 = constant. I1(t) = I1(0)[x(t)/x(0)]3 . Physical check An open secondary has no load current but can still have induced emf. Both current and geometry change the linked flux.

Question 2

Changing separation induces a voltage even at constant primary current

Two coaxial coils have positive mutual inductance M(x)=C/x3M(x)=C/x^3, where x is separation and C is constant. Coil 2 is open. Define its induced emf as ℰ2=−d(MI1)/dt\mathcal E_2=-d(MI_1)/dt.

Diagram shown in the original SVG worksheet.

  1. Find the emf when both primary current and separation can change.

  2. For constant positive I1 and constant outward speed v, find the emf and the current law that would instead cancel it.

Question 2 - Solution

Changing separation induces a voltage even at constant primary current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℰ2=−Mİ1−I1dMdxẋ=−Cx3İ1+3CI1ẋx4.\mathcal E_2=-M\dot I_1-I_1\frac{dM}{dx}\dot x=-\frac{C}{x^3}\dot I_1+\frac{3CI_1\dot x}{x^4}.ℰ2=3CI1v/x4(İ1=0).\boxed{\mathcal E_2=3CI_1v/x^4\quad(\dot I_1=0)}.

(b) Interpretation and further calculation

ℰ2=0⇒d(MI1)/dt=0⇒I1/x3=constant.\mathcal E_2=0\Rightarrow d(MI_1)/dt=0\Rightarrow I_1/x^3=\text{constant}.I1(t)=I1(0)[x(t)/x(0)]3.\boxed{I_1(t)=I_1(0)[x(t)/x(0)]^3}.

Physical check

An open secondary has no load current but can still have induced emf. Both current and geometry change the linked flux.