Electromagnetism · Experiment

Charge in a Magnetic Field

A magnetic field pushes a moving charge sideways, always at right angles to its motion. The result is a perfect circle — the basis of cyclotrons, mass spectrometers and the aurora.

velocity v force F = qv×B field B (• out / ✕ in) + charge / − charge

Controls

Speed |v|150
Gyroradius r = mv/qB100
Period T = 2πm/qB4.2 s
Cyclotron freq f0.24 Hz
Force |F| = qvB225
A positive charge moving right in a field out of the page curves downward.
About this experiment

What you are looking at

A charged particle moves through a uniform magnetic field that points straight out of (•) or into (✕) the screen. The green arrow is its velocity, the gold arrow is the magnetic force on it, and the curve is the path it traces. Notice the force is always perpendicular to the velocity — it never speeds the particle up or slows it down, it only turns it.

The Lorentz force

A magnetic field exerts a force on a moving charge given by the cross product:
F = q v × B
Its size is F = qvB sin θ (maximum when v is perpendicular to B), and its direction is given by the right-hand rule, flipped for negative charges. Because the force is always sideways, it acts as a centripetal force and bends the path into a circle. Setting qvB = mv²/r and solving gives the radius and period:
r = m v / (q B)    T = 2π m / (q B)    f = q B / (2π m)
A striking fact: the period and frequency do not depend on the speed — a faster particle simply travels a bigger circle in the same time. That constant "cyclotron frequency" is what makes the cyclotron particle accelerator work.

What changes the orbit

A stronger field or larger charge tightens the circle (smaller r); a heavier or faster particle widens it. Flip the sign of the charge or reverse the field and the particle curves the opposite way — this is exactly how a mass spectrometer separates ions, since heavier ones swing wider.

Crossed fields: the velocity selector

Switch on a perpendicular electric field and the two forces compete. When the electric force qE exactly balances the magnetic force qvB, the particle sails straight through — this happens only at one special speed, v = E/B, so crossed fields act as a velocity selector. Off that speed the path becomes a drifting cycloid, with an overall E×B drift at velocity E/B regardless of charge.

Things to try

Launch a positive charge and then a negative one in the same field to see them curl in opposite directions. Crank up B to shrink the circle; raise the speed to grow it while the period stays put. Turn on the electric field and hunt for the speed v = E/B where the path goes perfectly straight.