Magnetism and Electrons — Question 8

Section 32-6 · Physics pages 5286–5287

Question 8 The electron gyromagnetic sign determines precession direction A magnetic moment obeys µ = −γL with positive gamma in a uniform field Bˆz. Treat the expectation vector semiclassically with dL/dt = µ × B. B, Ω L Schematic; labels, not drawing lengths, specify the data. (a) Find the angular-velocity vector of precession and determine whether Lz changes. (b) Compare orbital and spin precession angular frequencies for an electron, using orbital gamma=e/(2me) and spin gamma=e/me.
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Question 8 - Solution The electron gyromagnetic sign determines precession direction B, Ω L (a) Method and calculation ˙L = −γL × B = (γB) × L. Ω= +γBˆz, ˙Lz = 0 . (b) Interpretation and further calculation ΩL = eB/(2me), Ωs = eB/me. Ωs/ΩL = 2 . Physical check The torque changes the transverse direction while conserving both the magnitude and the field-axis projection in this ideal model.

Question 8

The electron gyromagnetic sign determines precession direction

A magnetic moment obeys 𝝁=−γ𝑳\boldsymbol\mu=-\gamma\mathbf L with positive gamma in a uniform field BẑB\hat z. Treat the expectation vector semiclassically with d𝑳/dt=𝝁×𝑩d\mathbf L/dt=\boldsymbol\mu\times\mathbf B.

Diagram shown in the original SVG worksheet.

  1. Find the angular-velocity vector of precession and determine whether Lz changes.

  2. Compare orbital and spin precession angular frequencies for an electron, using orbital gamma=e/(2me) and spin gamma=e/me.

Question 8 - Solution

The electron gyromagnetic sign determines precession direction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑳̇=−γ𝑳×𝑩=(γ𝑩)×𝑳.\dot{\mathbf L}=-\gamma\mathbf L\times\mathbf B=(\gamma\mathbf B)\times\mathbf L.𝛀=+γBẑ,L̇z=0.\boxed{\boldsymbol\Omega=+\gamma B\hat z,\quad\dot L_z=0}.

(b) Interpretation and further calculation

ΩL=eB/(2me),Ωs=eB/me.\Omega_L=eB/(2m_e),\qquad\Omega_s=eB/m_e.Ωs/ΩL=2.\boxed{\Omega_s/\Omega_L=2}.

Physical check

The torque changes the transverse direction while conserving both the magnitude and the field-axis projection in this ideal model.