Mutual Induction — Question 8

Section 30-11 · Physics pages 4966–4967

Question 8 Fixed-current mutual energy requires accounting for both sources to predict force Two coaxial coils have M(x) = C/x3 > 0 and constant self-inductances. Sources hold positive currents I1 and I2 fixed while separation x changes quasistatically. Ignore resistance. Positive force points toward increasing x. source I1(t) pickup Φ x Schematic; labels, not drawing lengths, specify the data. (a) Find electrical work and field-energy change for a small dM. (b) Use energy balance to obtain mechanical force and its direction.
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Question 8 - Solution Fixed-current mutual energy requires accounting for both sources to predict force source I1(t) pickup Φ x (a) Method and calculation dWe = I1d(MI2) + I2d(MI1) = 2I1I2dM. dU = d(MI1I2) = I1I2dM ⇒dWmech = dWe −dU = I1I2dM. (b) Interpretation and further calculation Fxdx = dWmech ⇒Fx = I1I2 dM dx . Fx = −3CI1I2/x4 < 0 (attraction) . Physical check Using minus the fixed-current field-energy gradient alone would reverse the force because it omits work from the current sources.

Question 8

Fixed-current mutual energy requires accounting for both sources to predict force

Two coaxial coils have M(x)=C/x3>0M(x)=C/x^3>0 and constant self-inductances. Sources hold positive currents I1 and I2 fixed while separation x changes quasistatically. Ignore resistance. Positive force points toward increasing x.

Diagram shown in the original SVG worksheet.

  1. Find electrical work and field-energy change for a small dM.

  2. Use energy balance to obtain mechanical force and its direction.

Question 8 - Solution

Fixed-current mutual energy requires accounting for both sources to predict force

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dWe=I1d(MI2)+I2d(MI1)=2I1I2dM.dW_e=I_1d(MI_2)+I_2d(MI_1)=2I_1I_2dM.dU=d(MI1I2)=I1I2dM⇒dWmech=dWe−dU=I1I2dM.dU=d(MI_1I_2)=I_1I_2dM\Rightarrow dW_{\mathrm{mech}}=dW_e-dU=I_1I_2dM.

(b) Interpretation and further calculation

Fxdx=dWmech⇒Fx=I1I2dMdx.F_xdx=dW_{\mathrm{mech}}\Rightarrow F_x=I_1I_2\frac{dM}{dx}.Fx=−3CI1I2/x4<0(attraction).\boxed{F_x=-3CI_1I_2/x^4<0\quad\text{(attraction)}}.

Physical check

Using minus the fixed-current field-energy gradient alone would reverse the force because it omits work from the current sources.