1971
DOI: 10.1002/ctpp.19710110408
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Berechnung der Ionisationswellen in der Edelgas‐Starkstromsäule bei niedrigen Drücken

Abstract: InhaltsubersichtDie lineare Theorie der Ionisationswellen wird in quasihomogener Naherung u n k r besonderer Berucksichtigung der Temperatur-und Konzentrationsabhiingigkeit der Energieverlustrate, der Temperaturabhangigkeit der Elektronenbeweglichkeit sonie der Thermodiffusion ausgebaut. Es wird gezeigt, wie man aus der komplexen Dispersionsgleichung 4. Grades auf einfache Weise auf die Selbsterregungsgrenze und das Verhalten der Ionisationswellen bei der Grenzstromstarke schlieBen kann. Die gefundenen Zusamme… Show more

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Cited by 27 publications
(10 citation statements)
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“…The competition of electron-atom and electron-electron collisions results in strongly nonlinear (exponential) dependences of the ionization rates on electron density [14]. These nonlinearities may be the reason for the occurrence of ionization waves within the framework of local hydrodynamic model of stratification at low pressure and large currents in argon [15,16].…”
Section: Introductionmentioning
confidence: 99%
“…The competition of electron-atom and electron-electron collisions results in strongly nonlinear (exponential) dependences of the ionization rates on electron density [14]. These nonlinearities may be the reason for the occurrence of ionization waves within the framework of local hydrodynamic model of stratification at low pressure and large currents in argon [15,16].…”
Section: Introductionmentioning
confidence: 99%
“…Webb's Fig. 11 ( p = 0.5 Torr), the h i c k appeared a t I = 2.3 A while the critical current for Rp = 0.075 cm Torr is 2.26 A, which is obtained by extrapolating the data in [16]. The value of 0.26 A in Fig.…”
Section: Sat0mentioning
confidence: 77%
“…Since the basic equations used by Wojaczek (1971) are simpler than those used by others (Duncan and Forrest 1971), his equations are here modified to include the metastable atoms to explain the r and p waves. The following assumptions are used: (1) the charged particles diffuse ambipolar to the tube wall and disappear there; (2) the charged particles are treated as being quasi-neutral; Since the disturbance by the wave is treated in the axially uniform positive column without ends, V e along the tube axis is expressed by (Wojaczek 1971) The radial distribution of metastable atoms is assumed to be governed by the 0th order Bessel function as that of electrons or ions. 20, and Zom are expanded by U, (Duncan and Forrest 1971).…”
Section: Basic Equationsmentioning
confidence: 99%