Magnets — Question 7

Section 32-5 · Physics pages 5264–5265

Question 7 Parallel side-by-side dipoles repel despite having parallel moments Two small magnets have parallel fixed moments along +y and are separated by r along +x. At the second magnet the equatorial field of the first is B1 = −µ0m1ˆy/(4πr3). m1 m2 r B1 Schematic; labels, not drawing lengths, specify the data. (a) Find their interaction energy and radial force. (b) Compare the force magnitude with that of the same magnets in the coaxial parallel arrangement; then reverse only m2 and determine the new force sign.
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Question 7 - Solution Parallel side-by-side dipoles repel despite having parallel moments m1 m2 r B1 (a) Method and calculation U = −m2 · B1 = µ0m1m2 4πr3 . Fr = +3µ0m1m2 4πr4 (repulsion). (b) Interpretation and further calculation |Fside|/|Faxial| = 1/2 . m2 →−m2 ⇒U →−U, Fr →−Fr (attraction). Physical check Parallel moments alone do not determine attraction; the separation direction also enters the dipole field.

Question 7

Parallel side-by-side dipoles repel despite having parallel moments

Two small magnets have parallel fixed moments along +y and are separated by r along +x. At the second magnet the equatorial field of the first is 𝑩1=−μ0m1ŷ/(4πr3)\mathbf B_1=-\mu_0m_1\hat y/(4\pi r^3).

Diagram shown in the original SVG worksheet.

  1. Find their interaction energy and radial force.

  2. Compare the force magnitude with that of the same magnets in the coaxial parallel arrangement; then reverse only m2 and determine the new force sign.

Question 7 - Solution

Parallel side-by-side dipoles repel despite having parallel moments

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=−𝒎2⋅𝑩1=μ0m1m24πr3.U=-\mathbf m_2\cdot\mathbf B_1=\frac{\mu_0m_1m_2}{4\pi r^3}.Fr=+3μ0m1m24πr4(repulsion).\boxed{F_r=+\frac{3\mu_0m_1m_2}{4\pi r^4}}\quad\text{(repulsion)}.

(b) Interpretation and further calculation

|Fside|/|Faxial|=1/2.\boxed{|F_{\mathrm{side}}|/|F_{\mathrm{axial}}|=1/2}.𝒎2→−𝒎2⇒U→−U,Fr→−Fr(attraction).\mathbf m_2\to-\mathbf m_2\Rightarrow U\to-U,\quad\boxed{F_r\to-F_r}\quad\text{(attraction)}.

Physical check

Parallel moments alone do not determine attraction; the separation direction also enters the dipole field.