Inductors and Inductance — Question 7

Section 30-6 · Physics pages 4864–4865

Question 7 Parallel inductors share changing current inversely in proportion to inductance Two uncoupled ideal inductors, L1=2.00 mH and L2=6.00 mH, are connected in parallel with zero initial branch currents. The total current is increased to 8.00 A. L2 L1 Schematic; labels, not drawing lengths, specify the data. (a) Derive the equivalent inductance and branch-current ratio. (b) Find the final branch currents.
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Question 7 - Solution Parallel inductors share changing current inversely in proportion to inductance L2 L1 (a) Method and calculation v = L1˙i1 = L2˙i2, ˙i = ˙i1 + ˙i2 = v(1/L1 + 1/L2). Leq = L1L2 L1 + L2 = 1.50 mH , i1/i2 = L2/L1 = 3. (b) Interpretation and further calculation i1 + i2 = 8.00, i1 = 3i2. i1 = 6.00 A, i2 = 2.00 A . Physical check The current ratio assumes zero initial currents. A pre-existing circulating current is not described by the ratio alone.

Question 7

Parallel inductors share changing current inversely in proportion to inductance

Two uncoupled ideal inductors, L1=2.00 mH and L2=6.00 mH, are connected in parallel with zero initial branch currents. The total current is increased to 8.00 A.

Diagram shown in the original SVG worksheet.

  1. Derive the equivalent inductance and branch-current ratio.

  2. Find the final branch currents.

Question 7 - Solution

Parallel inductors share changing current inversely in proportion to inductance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v=L1i̇1=L2i̇2,i̇=i̇1+i̇2=v(1/L1+1/L2).v=L_1\dot i_1=L_2\dot i_2,\quad\dot i=\dot i_1+\dot i_2=v(1/L_1+1/L_2).Leq=L1L2L1+L2=1.50mH,i1/i2=L2/L1=3.\boxed{L_{\mathrm{eq}}=\frac{L_1L_2}{L_1+L_2}=1.50\,\mathrm{mH}},\quad i_1/i_2=L_2/L_1=3.

(b) Interpretation and further calculation

i1+i2=8.00,i1=3i2.i_1+i_2=8.00,\quad i_1=3i_2.i1=6.00A,i2=2.00A.\boxed{i_1=6.00\,A,\quad i_2=2.00\,A}.

Physical check

The current ratio assumes zero initial currents. A pre-existing circulating current is not described by the ratio alone.