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Physics

Cloud chamber

A line of droplets, and every answer comes out of its shape: how long, how thick, how straight, and which way it bends.

Cloud chamber — Actual application image
Actual application image

What happens

A chamber measures nothing. It draws a line of droplets and lets you read it. Length comes from the stopping power - an alpha of five MeV dies in four centimetres of air, a ten MeV proton runs a metre. Thickness carries the Bragg peak: ionisation is heaviest at the END of a heavy track, so an alpha is a blunt stub with a fat tip. Straightness is mass: a one MeV electron wanders two degrees a centimetre, a fast muon eighteen thousandths. And the bend in a field gives the momentum and the SIGN of the charge - which is how the positron was found, in a photograph, with a lead plate.

Equations used in the module
Equations
−dE/dx = K z² (Z/A) (1/β²)·[½ ln(2m_e c²β²γ²T_max/I²) − β²]
R = ∫ dE / (−dE/dx)
θ₀ = (13.6 MeV / βpc)·z·√(x/X₀)·(1 + 0.038 ln(x/X₀))
r_perp = p_perp / (|q|B)

Related experiments

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Mass spectrometer — Actual application image

Physics

Mass spectrometer

A ruler that reads mass off a position: the radius carries the square root of the mass, so every mass difference arrives halved.

Alpha decay — Actual application image

Physics

Alpha decay

Twenty-four decades of half-life out of a factor of two in energy, because the tunnelling probability sits in an exponent.

Cherenkov radiation — Actual application image

Physics

Cherenkov radiation

An optical sonic boom: a cone of blue light trailing a particle that outran the light in the medium.