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| | [No title] (Site not responding. Last check: 2007-10-20) |
 | | Before reaching the first Paschen minimum A (0.6 mbar) in the absence of magnetic field, we can say that for high pressures and short mean free paths, the combined effects of decreasing the pressure with higher B fields could produce the electric crossing conditions (D, E and F). |
 | | For pressures lower than 10-1 mbar (the Paschen minima are reached for the B field curves) there are electric inversions points at approximately 8 INCRUSTAR Equation.3 10-2 mbar (point G) and 3,5 INCRUSTAR Equation.3 10-2 mbar (point H). |
 | | These phenomena are due to the anomalous diffusion characteristics of the glow discharge with a longitudinal magnetic field centered at the cathode fall [5], observed experimentally at the positive column by Hoh and Lehnert [6], Allen, Paulikas and Pyle [7], and explained theoretically by Kadomtsev and Nedospadov [8] and Johnson, et al, [9, 10]. |
| www.pucp.edu.pe /~gip/articles/articulo_paschen.doc (887 words) |
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