A gas discharge is electrical conduction through a gas containing mobile charged particles. An applied electric field accelerates electrons; collisions can cause ionization, generating additional electrons and ions. A sustained discharge requires charge-production and electrode-emission processes to offset losses, rather than merely the presence of a few initially charged particles.
In a uniform Townsend avalanche model, gives across a gap . If each arriving positive ion releases on average electrons from the cathode, the self-sustaining threshold is . Combining that condition with the field dependence of gives the Paschen law.[ref]
A motivating measurement fixes the gas, electrode material and gap, varies pressure and records the onset electric potential difference with a current-limited source. A pressure gauge and current measurement distinguish the breakdown threshold from the later conducting regime. At larger currents, space charge and heating can invalidate the uniform-field avalanche approximation.
The Paschen law models gas-breakdown electric potential difference as a function of pressure times electrode spacing. For a uniform gap , fixed gas conditions and effective secondary-emission coefficient , an empirical ionization law together with gives
Here , has units inverse to pressure times length, and has units of potential. The denominator must be positive. These constants and the fitted range are part of the model.[ref]
Writing and gives . Differentiation places its minimum at , with . A pressure sweep at fixed gap can therefore first lower and then raise the threshold. Nonuniform fields, changing cathode surfaces, temperature changes or microscopic gaps can break this scaling; it is not a universal law for every electrical spark.

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