2006
DOI: 10.1109/tps.2006.872189
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On the effective diffusion length for microwave breakdown

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Cited by 25 publications
(24 citation statements)
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“…We will see that Equation (3) provides a good description of breakdown in the pressure region above P t with the assumption that D1/P.  is the effective diffusion length in cm, which depends on pressure 25 (1), but providing additional confirmation that the high threshold electric field and extremely high pressure of this branch appears to correspond to a low collision frequency per Torr at breakdown. Two distinctions between Equations (1) and (3) are the power law m and the ratio D/ 2 .…”
Section: Resultsmentioning
confidence: 75%
“…We will see that Equation (3) provides a good description of breakdown in the pressure region above P t with the assumption that D1/P.  is the effective diffusion length in cm, which depends on pressure 25 (1), but providing additional confirmation that the high threshold electric field and extremely high pressure of this branch appears to correspond to a low collision frequency per Torr at breakdown. Two distinctions between Equations (1) and (3) are the power law m and the ratio D/ 2 .…”
Section: Resultsmentioning
confidence: 75%
“…[5,6] and references therein. In addition we will generalize the analysis in [1] by including the influence of attachment on the breakdown threshold.…”
Section: Formulation and Solution Of Eigenvalue Problemmentioning
confidence: 99%
“…An often used way of characterizing the breakdown threshold condition is by means of the effective diffusion length, L eff , defined as, cf [1,3,5,6]…”
Section: Effective Diffusion Lengthmentioning
confidence: 99%
“…[1][2][3][4][5][6][7][8][9][10][11][12][13] Spaceships are subject to the risk of microwave breakdown occurring on the aperture of slot antennas 3,6,7 and/or inside microwave satellite payloads. [9][10][11][12][13] The risk of breakdown appears during the atmospheric entry of space vehicles in planet exploratory missions or during Earth's atmospheric re-entry, as well as in the Telemetry Tracking and Control (TTC) launching phase. The resulting partially ionized gas leads to strong absorption and/or reflection of the incident microwave signal, what can lead to a dramatic increase of the ohmic losses and to a noticeable temperature rise, with the subsequent permanent damage of the instruments.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we apply the Rayleigh-Ritz method to solve the eigenvalue problem of the corona equation. 10,12,28 The results obtained are compared with the circular waveguide, which serves as a reference when the eccentricity of the ellipse tends to zero.…”
Section: Introductionmentioning
confidence: 99%