Mutual Induction — Question 7

Section 30-11 · Physics pages 4964–4965

Question 7 A finite primary ramp produces a delayed secondary current and a fixed total charge A primary current is zero before t=0, rises as i1 = αt for 0 < t < T, and remains constant afterward. A fixed secondary has inductance L2, resistance R2, positive M, and initial current zero. Positive currents enter dotted ends. t i1 T Schematic; labels, not drawing lengths, specify the data. (a) Solve L2˙i2 + R2i2 = −M˙i1 during and after the ramp. (b) Find total signed secondary charge from zero to infinite time, including the decay tail.
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Question 7 - Solution A finite primary ramp produces a delayed secondary current and a fixed total charge t i1 T (a) Method and calculation τ2 = L2/R2, i2(t) = −Mα R2 (1 −e−t/τ2) (0 < t < T) . i2(t) = i2(T)e−(t−T)/τ2 (t > T) . (b) Interpretation and further calculation ∫∞ 0 (L2˙i2 + R2i2)dt = −M∆i1, i2(0) = i2(∞) = 0. Q2 = −MαT/R2 = −M∆i1/R2 . Physical check Secondary inductance reshapes the current pulse but does not change its integrated charge when the endpoint currents vanish.

Question 7

A finite primary ramp produces a delayed secondary current and a fixed total charge

A primary current is zero before t=0, rises as i1=αti_1=\alpha t for 0<t<T0<t<T, and remains constant afterward. A fixed secondary has inductance L2, resistance R2, positive M, and initial current zero. Positive currents enter dotted ends.

Diagram shown in the original SVG worksheet.

  1. Solve L2i̇2+R2i2=−Mi̇1L_2\dot i_2+R_2i_2=-M\dot i_1 during and after the ramp.

  2. Find total signed secondary charge from zero to infinite time, including the decay tail.

Question 7 - Solution

A finite primary ramp produces a delayed secondary current and a fixed total charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

τ2=L2/R2,i2(t)=−MαR2(1−e−t/τ2)(0<t<T).\tau_2=L_2/R_2,\quad\boxed{i_2(t)=-\frac{M\alpha}{R_2}(1-e^{-t/\tau_2})\quad(0<t<T)}.i2(t)=i2(T)e−(t−T)/τ2(t>T).\boxed{i_2(t)=i_2(T)e^{-(t-T)/\tau_2}\quad(t>T)}.

(b) Interpretation and further calculation

∫0∞(L2i̇2+R2i2)dt=−MΔi1,i2(0)=i2(∞)=0.\int_0^\infty(L_2\dot i_2+R_2i_2)dt=-M\Delta i_1,\quad i_2(0)=i_2(\infty)=0.Q2=−MαT/R2=−MΔi1/R2.\boxed{Q_2=-M\alpha T/R_2=-M\Delta i_1/R_2}.

Physical check

Secondary inductance reshapes the current pulse but does not change its integrated charge when the endpoint currents vanish.