When a charged particle moves through a uniform magnetic field, it experiences a force perpendicular to both its velocity and the field direction. This force causes the particle to follow a circular or helical path. The rate at which it orbits is known as the cyclotron frequency. Scientists rely on this principle to build particle accelerators, analyze mass spectra, and study plasmas in space and in laboratory devices. The frequency depends only on the charge-to-mass ratio of the particle and the magnetic field strength, making it a powerful diagnostic tool.
The basic expression for the angular cyclotron frequency is
.
In terms of ordinary frequency, measured in hertz, this becomes
.
Here is the particle's charge in coulombs, is its mass in kilograms, and is the magnetic field strength in teslas. The direction of rotation depends on the sign of the charge, but the magnitude of the frequency follows this simple ratio.
Cyclotrons are circular particle accelerators that exploit this relationship. By applying an oscillating electric field at the cyclotron frequency, the device can accelerate particles to high energies as they spiral outward in the magnetic field. The concept, developed in the 1930s, remains foundational to modern accelerators used in medicine, industry, and fundamental research.
In plasma physics, the cyclotron frequency sets the characteristic scale for many phenomena. It influences wave propagation, resonance heating, and particle confinement. For example, ion cyclotron resonance heating (ICRH) injects energy into fusion plasmas by matching the frequency of radio waves to the ion cyclotron frequency. By measuring this frequency, scientists infer plasma composition and magnetic field strength.
Mass spectrometers often make use of the cyclotron motion of ions. Because the frequency depends on mass, different ions orbit at slightly different rates in the same field. Devices like Fourier Transform Ion Cyclotron Resonance (FT-ICR) spectrometers detect these frequencies with remarkable precision, allowing chemists to determine molecular masses and study complex mixtures.
To calculate the cyclotron frequency, input the particle's charge, mass, and the magnetic field. After clicking Compute, the calculator returns the result in hertz and kilohertz. The formula assumes the particle's velocity is not so high that relativistic effects become significant, which is a good approximation for many laboratory and space plasma conditions.
Consider a singly charged ion with charge , mass 40 atomic mass units (approximately kg), in a magnetic field of 1 tesla. Plugging these values into the formula yields a cyclotron frequency around 3.8 MHz. Doubling the field strength would double the frequency, illustrating how sensitive the motion is to the magnetic environment.
Different particles respond uniquely to the same magnetic field because their charge-to-mass ratios vary widely. The table below lists cyclotron frequencies in a 1 tesla field to highlight these contrasts.
Particle | Charge (C) | Mass (kg) | fc at 1 T (MHz) |
---|---|---|---|
Electron | 1.60×10-19 | 9.11×10-31 | 28.0 |
Proton | 1.60×10-19 | 1.67×10-27 | 15.2 |
Alpha particle | 3.20×10-19 | 6.64×10-27 | 7.3 |
Calcium ion (Ca+) | 1.60×10-19 | 6.66×10-26 | 0.38 |
These values demonstrate why light particles like electrons resonate at radio frequencies, while heavier ions fall into the kilohertz or low‑megahertz range. Experimentalists tune equipment to these natural frequencies to heat plasmas, trap ions, or separate isotopes.
The cyclotron was invented in the early 1930s by Ernest O. Lawrence and M. Stanley Livingston at the University of California, Berkeley. Their compact device accelerated ions in spiral paths using a magnetic field and an alternating voltage. The success of the cyclotron ushered in an era of high‑energy physics, enabling discoveries of new particles and paving the way for modern synchrotrons and colliders. The basic frequency relation presented here originates from the classical motion equations used in those pioneering machines. Today’s advanced accelerators still rely on the same fundamental physics, albeit with sophisticated control systems and enormous magnets.
At velocities approaching the speed of light, the particle’s effective mass increases by the Lorentz factor , reducing the cyclotron frequency. The relativistic expression becomes . Quantum mechanics introduces another twist: charged particles in magnetic fields occupy discrete Landau levels, leading to quantized energy spacings proportional to the cyclotron frequency. Although these effects lie beyond the scope of the simple calculator, understanding their existence helps researchers judge when classical formulas remain valid.
To deepen your exploration of electromagnetic dynamics, try the Lorentz Force Calculator for computing magnetic forces on moving charges and the Lorentz Factor Calculator to account for relativistic speeds. Together with the cyclotron frequency tool, these calculators build a coherent picture of particle motion.
The classical cyclotron formula assumes the magnetic field is uniform and that the particle's speed is small compared to the speed of light. In modern accelerators where particles approach relativistic speeds, modifications involving the Lorentz factor are necessary. Additionally, in non-uniform fields, particles can drift or mirror, leading to more complex trajectories.
By experimenting with different parameters in this calculator, you can gain intuition about how charged particles respond to magnetic fields. Whether designing an ion source, analyzing cosmic rays, or planning a plasma experiment, understanding the cyclotron frequency is an essential step.
Scientists often log frequency calculations when tuning equipment. Use the copy button to paste the output into lab notes or simulation files so you can revisit parameters without recalculating from scratch.