A Current-Carrying Coil as a Magnetic Dipole — Question 8

Section 29-5 · Physics pages 4746–4747

Question 8 Two small coaxial coils attract with an inverse-fourth-power force Two small coils have fixed moments µ1 = .0200 and µ2 = .0300 ampere square metre, both along +z. Coil 1 is fixed at z=0; coil 2 is on axis at d=.100 m. Both coil radii are much smaller than d. Use B1(z) = µ0µ1/(2πz3) and the mechanical interaction potential U = −µ2B1. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. z d left coil right coil⃗ µL⃗ µR Schematic; labels, not drawing lengths, specify the data. (a) Find the axial force on coil 2 and its direction. (b) Find the quasistatic external mechanical work to move coil 2 from d to 2d while both moments remain fixed.
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Question 8 - Solution Two small coaxial coils attract with an inverse-fourth-power force z d left coil right coil⃗ µL⃗ µR (a) Method and calculation U(z) = −µ0µ1µ2 2πz3 , Fz = −dU dz = −3µ0µ1µ2 2πz4 . Fz(d) = −3.60 µN toward coil 1. (b) Interpretation and further calculation Wext = U(2d) −U(d) = µ0µ1µ2 2πd3 ( 1 −1 8 ) . Wext = 1.05 × 10−7 J . Physical check This is mechanical work at fixed moments; maintaining real coil currents during motion also involves their supplies. The force law assumes the dipole regime throughout.

Question 8

Two small coaxial coils attract with an inverse-fourth-power force

Two small coils have fixed moments μ1=.0200\mu_1=.0200 and μ2=.0300\mu_2=.0300 ampere square metre, both along +z. Coil 1 is fixed at z=0; coil 2 is on axis at d=.100 m. Both coil radii are much smaller than d. Use B1(z)=μ0μ1/(2πz3)B_1(z)=\mu_0\mu_1/(2\pi z^3) and the mechanical interaction potential U=−μ2B1U=-\mu_2B_1. Use vacuum permeability μ0≃4π×10−7Tm/A\mu_0\simeq4\pi\times10^{-7}\,\mathrm{T\,m/A} where numerical values are needed.

Diagram shown in the original SVG worksheet.

  1. Find the axial force on coil 2 and its direction.

  2. Find the quasistatic external mechanical work to move coil 2 from d to 2d while both moments remain fixed.

Question 8 - Solution

Two small coaxial coils attract with an inverse-fourth-power force

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(z)=−μ0μ1μ22πz3,Fz=−dUdz=−3μ0μ1μ22πz4.U(z)=-\frac{\mu_0\mu_1\mu_2}{2\pi z^3},\quad F_z=-\frac{dU}{dz}=-\frac{3\mu_0\mu_1\mu_2}{2\pi z^4}.Fz(d)=−3.60μNtoward coil 1.\boxed{F_z(d)=-3.60\,\mu\mathrm N}\quad\text{toward coil 1}.

(b) Interpretation and further calculation

Wext=U(2d)−U(d)=μ0μ1μ22πd3(1−18).W_{\mathrm{ext}}=U(2d)-U(d)=\frac{\mu_0\mu_1\mu_2}{2\pi d^3}\left(1-\frac18\right).Wext=1.05×10−7J.\boxed{W_{\mathrm{ext}}=1.05\times10^{-7}\,\mathrm J}.

Physical check

This is mechanical work at fixed moments; maintaining real coil currents during motion also involves their supplies. The force law assumes the dipole regime throughout.