Menu Close

Cloud Chamber: Ionisation Trails in a Magnetic Field

Cloud Chamber: Ionisation Trails in a Magnetic Field

Watch the trails left by alpha and beta particles, then switch on a magnetic field and measure how they curve
v1
Seen from above. The chamber is 20 cm wide and the trails are to scale; the droplets are enlarged.

Measure a trail

Live values

Think first: before you switch on the magnetic field, predict which trails will curve more, the alpha trails or the beta trails, and why.
Source
Particle from the source
Magnetic field
Trails in view

Equations

How a cloud chamber works. The chamber holds air saturated with alcohol vapour above a very cold base, cooled by dry ice to about −78 °C. Just above the base the vapour is supersaturated: it is ready to condense but needs something to condense on. A charged particle passing through ionises air molecules along its path, and droplets of alcohol form on the ions, leaving a trail of mist.

Alpha trails. An alpha particle is strongly ionising, so its trail is thick and dense. It loses its energy quickly and stops after about 4 cm in air. Every alpha particle from americium-241 has the same energy, 5.5 MeV, so the trails are all the same length.

Beta trails. A beta particle is weakly ionising, so its trail is thin and faint, and collisions with air molecules knock it sideways. Beta particles are emitted with a range of energies. A beta particle can travel more than a metre in air, so most beta trails end when the particle leaves the thin layer of supersaturated vapour, not because it has stopped.

V-shaped trails. A thorium gas mantle gives off radon-220 gas. A radon-220 nucleus emits an alpha particle and becomes polonium-216, which has a half-life of 0.145 s and emits a second alpha particle. The two trails start from the same point, making a V.

Background radiation. Even with no source, trails appear: long, thin, straight trails from cosmic-ray muons, short wandering electron trails, and the occasional alpha trail from radon in the air.

The magnetic field. The force on a moving charge is at right angles to its velocity, so the particle moves along the arc of a circle. Positive and negative particles curve in opposite directions. Fleming’s left-hand rule gives the direction of the force; remember that the current is in the opposite direction to the motion of a negative particle.

The model. The ranges and momenta use real values for alpha and beta particles in air, and the beta momenta allow for relativity; p = BQr still holds. Real school chambers use permanent magnets of about 0.1 T or less; the slider goes higher so that the alpha trails can be seen to curve.