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Larmor precession describes how a magnetic moment, such as a spinning charged particle or atomic nucleus, rotates around an external magnetic field. This reference helps students connect torque, angular momentum, and magnetic field strength in one clear model. It is useful for understanding magnetic resonance, spin behavior, and why particles do not simply line up instantly with a field.

The central idea is that a magnetic field creates a torque τ=μ×B\vec{\tau} = \vec{\mu} \times \vec{B} on a magnetic moment. When the magnetic moment is proportional to angular momentum, μ=γL\vec{\mu} = \gamma \vec{L}, the torque changes the direction of L\vec{L} instead of mainly changing its size. The precession angular frequency has magnitude ωL=γB\omega_L = |\gamma|B, and the ordinary frequency is fL=ωL2πf_L = \frac{\omega_L}{2\pi}.

In quantum settings, resonance occurs when photon energy matches the spin energy splitting, hf=ΔEhf = \Delta E.

Key Facts

  • The magnetic torque on a magnetic dipole is τ=μ×B\vec{\tau} = \vec{\mu} \times \vec{B}, so its magnitude is τ=μBsinθ\tau = \mu B\sin\theta.
  • The magnetic potential energy of a dipole in a uniform magnetic field is U=μB=μBcosθU = -\vec{\mu}\cdot\vec{B} = -\mu B\cos\theta.
  • If the magnetic moment is proportional to angular momentum, the relation is μ=γL\vec{\mu} = \gamma \vec{L}, where γ\gamma is the gyromagnetic ratio.
  • The Larmor angular frequency has magnitude ωL=γB\omega_L = |\gamma|B, where BB is the magnetic field strength.
  • The Larmor frequency in cycles per second is fL=ωL2π=γB2πf_L = \frac{\omega_L}{2\pi} = \frac{|\gamma|B}{2\pi}.
  • For a particle with charge qq, mass mm, and gg-factor gg, the gyromagnetic ratio is γ=gq2m\gamma = \frac{gq}{2m}.
  • The precession direction depends on the sign of γ\gamma, so positive and negative charges precess in opposite senses around B\vec{B}.
  • Magnetic resonance occurs when an applied wave satisfies hf=ΔEhf = \Delta E, often matching f=fLf = f_L for spin transitions.

Vocabulary

Larmor precession
Larmor precession is the steady rotation of a magnetic moment or angular momentum vector around an external magnetic field.
Magnetic moment
A magnetic moment μ\vec{\mu} measures how strongly an object behaves like a tiny magnet and how it interacts with B\vec{B}.
Gyromagnetic ratio
The gyromagnetic ratio γ\gamma is the constant relating magnetic moment to angular momentum through μ=γL\vec{\mu} = \gamma \vec{L}.
Angular frequency
Angular frequency ω\omega measures rotational rate in radians per second, with ω=2πf\omega = 2\pi f.
Torque
Torque τ\vec{\tau} is a twisting effect that changes angular momentum according to τ=dLdt\vec{\tau} = \frac{d\vec{L}}{dt}.
Resonance
Resonance occurs when an applied oscillating field has the correct frequency to transfer energy efficiently, such as hf=ΔEhf = \Delta E.

Common Mistakes to Avoid

  • Using fL=γBf_L = \gamma B instead of fL=γB2πf_L = \frac{|\gamma|B}{2\pi} is wrong because γB\gamma B gives angular frequency in radians per second, not cycles per second.
  • Ignoring the sign of γ\gamma is wrong because the sign determines whether the precession is clockwise or counterclockwise around B\vec{B}.
  • Treating the torque as parallel to B\vec{B} is wrong because τ=μ×B\vec{\tau} = \vec{\mu} \times \vec{B} is perpendicular to both μ\vec{\mu} and B\vec{B}.
  • Assuming precession always changes the size of L\vec{L} is wrong because ideal Larmor precession mainly changes the direction of L\vec{L} while keeping its magnitude constant.
  • Forgetting unit conversions for BB is wrong because formulas such as ωL=γB\omega_L = |\gamma|B require magnetic field strength in teslas when using SI units.

Practice Questions

  1. 1 A proton has γ2π=42.58MHz/T\frac{\gamma}{2\pi} = 42.58\,\text{MHz/T}. What is its Larmor frequency in a field of B=1.50TB = 1.50\,\text{T}?
  2. 2 An electron spin has γ=1.76×1011rads1T1|\gamma| = 1.76 \times 10^{11}\,\text{rad}\,\text{s}^{-1}\text{T}^{-1}. Find ωL\omega_L when B=0.020TB = 0.020\,\text{T}.
  3. 3 A magnetic moment has μ=3.0×1023J/T\mu = 3.0 \times 10^{-23}\,\text{J/T} in a field B=0.40TB = 0.40\,\text{T} at an angle of 3030^{\circ}. Calculate the torque magnitude using τ=μBsinθ\tau = \mu B\sin\theta.
  4. 4 Why does a magnetic moment precess around B\vec{B} instead of immediately pointing exactly along B\vec{B} when angular momentum is present?