Townsend discharge or Townsend avalanche is a gas ionisation process where free electrons are accelerated by an electric field, collide with gas molecules, and consequently free additional electrons.
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Townsend discharge or Townsend avalanche is a gas ionisation process where free electrons are accelerated by an electric field, collide with gas molecules, and consequently free additional electrons.
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Townsend avalanche discharge is named after John Sealy Townsend avalanche, who discovered the fundamental ionisation mechanism by his work circa 1897 at the Cavendish Laboratory, Cambridge.
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Townsend avalanche forced the cathode to emit electrons using the photoelectric effect by irradiating it with X-rays, and he found that the current flowing through the chamber depended on the electric field between the plates.
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Townsend avalanche observed currents varying exponentially over ten or more orders of magnitude with a constant applied voltage when the distance between the plates was varied.
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Townsend avalanche discovered that gas pressure influenced conduction: he was able to generate ions in gases at low pressure with a much lower voltage than that required to generate a spark.
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Townsend avalanche put forward the hypothesis that positive ions produce ion pairs, introducing a coefficient expressing the number of ion pairs generated per unit length by a positive ion moving from anode to cathode.
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Occurrence of Townsend avalanche discharge, leading to glow discharge breakdown shapes the current–voltage characteristic of a gas-discharge tube such as a neon lamp in a way such that it has a negative differential resistance region of the S-type.
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Avalanche multiplication during Townsend discharge is naturally used in gas phototubes, to amplify the photoelectric charge generated by incident radiation on the cathode: achievable current is typically 10~20 times greater respect to that generated by vacuum phototubes.
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Townsend avalanche discharges are fundamental to the operation of gaseous ionisation detectors such as the Geiger–Muller tube and the proportional counter in either detecting ionising radiation or measuring its energy.
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The electric field and chamber geometries are selected so that an "Townsend avalanche region" is created in the immediate proximity of the anode.
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