A Current-Carrying Coil as a Magnetic Dipole — Question 4

Section 29-5 · Physics pages 4738–4739

Question 4 Canceling the central field of concentric coils leaves a large far-field moment Two concentric coplanar coils each have N turns, with radii R and 2R. The inner coil has current I and moment along +z. The outer coil carries an adjustable positive current magnitude I2 with moment along -z. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. O I1 I2 R 2R Schematic; labels, not drawing lengths, specify the data. (a) Choose I2 to cancel the field at the common center. (b) Find the resulting total dipole moment and the leading field far away on the positive z axis.
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Question 4 - Solution Canceling the central field of concentric coils leaves a large far-field moment O I1 I2 R 2R (a) Method and calculation Bz(0) = µ0NI 2R −µ0NI2 4R = 0. I2 = 2I . (b) Interpretation and further calculation⃗ µtotal = NπR2Iˆz −Nπ(2R)2(2I)ˆz = −7NπR2Iˆz .⃗ B(z) ≃−7µ0NIR2 2z3 ˆz (z ≫2R) . Physical check Central field weights turns by inverse radius, whereas dipole moment weights them by radius squared; canceling one need not cancel the other.

Question 4

Canceling the central field of concentric coils leaves a large far-field moment

Two concentric coplanar coils each have N turns, with radii R and 2R. The inner coil has current I and moment along +z. The outer coil carries an adjustable positive current magnitude I2 with moment along -z. 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. Choose I2 to cancel the field at the common center.

  2. Find the resulting total dipole moment and the leading field far away on the positive z axis.

Question 4 - Solution

Canceling the central field of concentric coils leaves a large far-field moment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Bz(0)=μ0NI2R−μ0NI24R=0.B_z(0)=\frac{\mu_0NI}{2R}-\frac{\mu_0NI_2}{4R}=0.I2=2I.\boxed{I_2=2I}.

(b) Interpretation and further calculation

μ→total=NπR2Iẑ−Nπ(2R)2(2I)ẑ=−7NπR2Iẑ.\vec\mu_{\mathrm{total}}=N\pi R^2I\hat z-N\pi(2R)^2(2I)\hat z=\boxed{-7N\pi R^2I\hat z}.B→(z)≃−7μ0NIR22z3ẑ(z≫2R).\boxed{\vec B(z)\simeq-\frac{7\mu_0NIR^2}{2z^3}\hat z\quad(z\gg2R)}.

Physical check

Central field weights turns by inverse radius, whereas dipole moment weights them by radius squared; canceling one need not cancel the other.