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An electrical discharge transfers electric charge through a medium or gap. A gas discharge can begin when accelerated charge carriers produce enough further ionization to sustain an electric current. An electron avalanche describes multiplication by successive ionizing collisions; the supply and loss processes determine whether it becomes a sustained conducting state.

A motivating gas-breakdown experiment varies pressure while keeping the gas, electrode separation and electrode geometry specified. The required electric potential difference does not generally decrease monotonically with pressure. At very low density, an electron encounters too few molecules to sustain multiplication; at higher density, collisions can interrupt acceleration before sufficient ionizing energy is acquired. The resulting dependence on pressure and gap is summarized, within its assumptions, by the Paschen law.^[ref]

The experimental apparatus therefore needs electrodes with a known separation, pressure control and measurement, and a current-limited electrical source with current and potential measurements. Geometry and electrode surfaces must be recorded along with the gas conditions. A measured onset threshold and the later current–potential characteristic answer different questions; the existence of a glowing plasma is not itself a measurement of its onset threshold.

An ionization chamber measures ionizing radiation by collecting the electric charge that it creates in a gas. Two electrodes establish an electric field; liberated electrons and positive ions move toward opposite electrodes. In the chamber's intended operating regime the field collects the initial charge with negligible electron avalanche multiplication, distinguishing it from a proportional counter.

Varying the applied electric potential difference while holding the incident radiation fixed produces a collection curve. Too weak a field allows electron-ion recombination before collection; an approximately flat region indicates near-complete collection under those conditions. Increasing the field far enough can instead cause gas multiplication. A 2013 synchrotron radiation experiment compared free-air chambers with different electrode gaps and chopped the X-ray beam, showing that collection depends on both geometry and the temporal delivery of radiation.^[ref]

For a simple counting model, let each interacting particle create on average $n$ electron-ion pairs and let $f$ be their collected fraction. An interaction rate $r$ then gives mean electric current $I=efnr$, where $e$ is the elementary charge. This accounting explains why loss of charge can mimic a reduced incident particle flux; converting a current to absorbed dose requires additional information about energy deposition and the irradiated mass.

A multiwire proportional chamber is a proportional counter: parallel anode wires between cathodes in a gas. Charged particle ionization frees electrons; an electric field drives them toward wires, triggering an electron avalanche read by electronic amplifiers.^[ref]

Georges Charpak's electronic readout avoided film scanning and full spark chamber discharge.^[ref]

Opposite polarities identify the avalanche wire. Positive ion motion dominates integrated signal; detection precedes complete collection. Calibrated electron travel times enable drift chambers.^[ref]

A gas-filled particle detector using electron avalanche multiplication. Within its proportional operating range, the collected electric charge tracks the initial ionization, allowing more than a yes-or-no count.