The Magnetic Dipole Moment — Question 9

Section 28-9 · Physics pages 4648–4649

Question 9 The orbital moment of a single circulating charge is linked to its angular momentum A nonrelativistic charge q of mass m moves in a circular orbit of radius r and speed v. Define the orbit normal by the direction of angular momentum L. The signed equivalent current is q/T, where T is the orbital period. r⃗ B out of the page one orbiting charge q Schematic; labels, not drawing lengths, specify the data. (a) Derive the relation between the orbital magnetic moment and angular momentum. (b) If the orbit is maintained solely by a uniform magnetic field perpendicular to the motion, show that the orbital moment points opposite to the applied field and has magnitude K/B.
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Question 9 - Solution The orbital moment of a single circulating charge is linked to its angular momentum r⃗ B out of the page one orbiting charge q (a) Method and calculation I = q/T = qv/(2πr),⃗ µ = Iπr2 ˆL = 1 2qvrˆL.⃗ L = mvrˆL ⇒⃗µ = q 2m⃗L. (b) Interpretation and further calculation r = mv |q|B ⇒|µ| = |q|vr 2 = mv2 2B = K/B. q > 0 :⃗L opposes⃗B; q < 0 :⃗L follows⃗B. In both cases, the factor q in the moment makes⃗µ oppose⃗B. Physical check This is an orbital classical relation; intrinsic spin moments require their own gyromagnetic ratios.

Question 9

The orbital moment of a single circulating charge is linked to its angular momentum

A nonrelativistic charge q of mass m moves in a circular orbit of radius r and speed v. Define the orbit normal by the direction of angular momentum L. The signed equivalent current is q/T, where T is the orbital period.

Diagram shown in the original SVG worksheet.

  1. Derive the relation between the orbital magnetic moment and angular momentum.

  2. If the orbit is maintained solely by a uniform magnetic field perpendicular to the motion, show that the orbital moment points opposite to the applied field and has magnitude K/B.

Question 9 - Solution

The orbital moment of a single circulating charge is linked to its angular momentum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I=q/T=qv/(2πr),μ→=Iπr2L̂=12qvrL̂.I=q/T=qv/(2\pi r),\quad\vec\mu=I\pi r^2\hat L=\tfrac12qvr\hat L.L→=mvrL̂⇒μ→=q2mL→.\vec L=mvr\hat L\Rightarrow\vec\mu=\frac q{2m}\vec L.

(b) Interpretation and further calculation

r=mv|q|B⇒|μ|=|q|vr2=mv22B=K/B.r=\frac{mv}{|q|B}\Rightarrow|\mu|=\frac{|q|vr}{2}=\frac{mv^2}{2B}=K/B.q>0:L→ opposes B→;q<0:L→ follows B→.q>0:\ \vec L\text{ opposes }\vec B;\quad q<0:\ \vec L\text{ follows }\vec B.In both cases, the factor q in the moment makes μ→\vec\mu oppose B→\vec B.

Physical check

This is an orbital classical relation; intrinsic spin moments require their own gyromagnetic ratios.