Experimentally Determined Plasma Perturbation by a Probe
The perturbation of a plasma by a probe with radius large in comparison to a mean free path is examined with a small movable probe. Electron density, electron temperature, and plasma potential are determined as a function of distance from the large probe. The experimental conditions corresponded wel...
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Veröffentlicht in: | Physics of Fluids (U.S.) 1966-04, Vol.9 (4), p.801-808 |
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Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The perturbation of a plasma by a probe with radius large in comparison to a mean free path is examined with a small movable probe. Electron density, electron temperature, and plasma potential are determined as a function of distance from the large probe. The experimental conditions corresponded well to those assumed by Waymouth; Waymouth's theory applied to the large‐probe electron current characteristic yields a value for electron density in the unperturbed plasma that is correct within a few percent. The electron temperature so determined is too low by 19%. A fundamental assumption of all theories, that electron temperature in the perturbed volume of plasma is independent of position, is found to be incorrect, at least in a plasma containing drift currents. |
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ISSN: | 0031-9171 2163-4998 |
DOI: | 10.1063/1.1761747 |