Lesson 3 of 15

Cyclotron Motion

Cyclotron Motion

When a charged particle moves in a magnetic field, the Lorentz force F=qv×B\mathbf{F} = q\mathbf{v} \times \mathbf{B} acts perpendicular to the velocity, causing the particle to gyrate in a circle. This circular motion is called cyclotron motion (or gyromotion).

Gyrofrequency (Cyclotron Frequency)

The angular frequency of the circular orbit:

ωc=∣q∣Bm\omega_c = \frac{|q| B}{m}

This is independent of the particle's speed — all particles of the same charge-to-mass ratio gyrate at the same frequency in a given field.

Gyroperiod

The time for one complete orbit:

Tc=2πωc=2πm∣q∣BT_c = \frac{2\pi}{\omega_c} = \frac{2\pi m}{|q| B}

Larmor Radius (Gyroradius)

The radius of the circular orbit depends on the perpendicular velocity v⊥v_\perp:

rL=mv⊥∣q∣Br_L = \frac{m v_\perp}{|q| B}

Key parameters:

  • e=1.602×10−19e = 1.602 \times 10^{-19} C
  • me=9.109×10−31m_e = 9.109 \times 10^{-31} kg (electron)
  • mp=1.673×10−27m_p = 1.673 \times 10^{-27} kg (proton)

Physical Intuition

  • Electrons gyrate at much higher frequencies than ions (smaller mass → higher ωc\omega_c)
  • Higher energy particles have larger Larmor radii
  • In fusion devices, small Larmor radii confine particles to magnetic field lines
  • Cyclotron resonance heating (ICRH, ECRH) drives plasma heating by injecting waves at ωc\omega_c

Implement the three gyration functions below.

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