Mutual Induction — Question 6

Section 30-11 · Physics pages 4962–4963

Question 6 An ideal shorted secondary reduces the effective primary inductance Two fixed lossless coils have positive M with M2 < L1L2. Coil 2 is shorted by a perfect conductor. Both currents start at zero. A prescribed current i1 is then established in coil 1. L1 L2 i1 i2 coil 2 shorted; M > 0 Schematic; labels, not drawing lengths, specify the data. (a) Find secondary current by conserving its total linkage. (b) Derive the primary terminal inductance and total stored energy.
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Question 6 - Solution An ideal shorted secondary reduces the effective primary inductance L1 L2 i1 i2 coil 2 shorted; M > 0 (a) Method and calculation v2 = d dt(L2i2 + Mi1) = 0 ⇒L2i2 + Mi1 = 0. i2 = −Mi1/L2 . (b) Interpretation and further calculation v1 = L1˙i1 + M˙i2 = ( L1 −M2/L2 ) ˙i1. Leff= L1 −M2/L2 = L1(1 −k2), U = 1 2Leffi2 1 . Physical check The opposing secondary current partly cancels primary linkage; the coupling bound keeps the effective inductance nonnegative.

Question 6

An ideal shorted secondary reduces the effective primary inductance

Two fixed lossless coils have positive M with M2<L1L2M^2<L_1L_2. Coil 2 is shorted by a perfect conductor. Both currents start at zero. A prescribed current i1 is then established in coil 1.

Diagram shown in the original SVG worksheet.

  1. Find secondary current by conserving its total linkage.

  2. Derive the primary terminal inductance and total stored energy.

Question 6 - Solution

An ideal shorted secondary reduces the effective primary inductance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v2=ddt(L2i2+Mi1)=0⇒L2i2+Mi1=0.v_2=\frac d{dt}(L_2i_2+Mi_1)=0\Rightarrow L_2i_2+Mi_1=0.i2=−Mi1/L2.\boxed{i_2=-Mi_1/L_2}.

(b) Interpretation and further calculation

v1=L1i̇1+Mi̇2=(L1−M2/L2)i̇1.v_1=L_1\dot i_1+M\dot i_2=\left(L_1-M^2/L_2\right)\dot i_1.Leff=L1−M2/L2=L1(1−k2),U=12Leffi12.\boxed{L_{\mathrm{eff}}=L_1-M^2/L_2=L_1(1-k^2),\quad U=\tfrac12L_{\mathrm{eff}}i_1^2}.

Physical check

The opposing secondary current partly cancels primary linkage; the coupling bound keeps the effective inductance nonnegative.