Kinetic modeling of low-pressure nitrogen discharges and post-discharges

被引:210
作者
Guerra, V [1 ]
Sá, PA
Loureiro, J
机构
[1] Inst Super Tecn, Ctr Fis Plasmas, P-1049001 Lisbon, Portugal
[2] Univ Porto, Fac Engn, Dept Fis, P-4200465 Oporto, Portugal
关键词
D O I
10.1051/epjap:2004188
中图分类号
O59 [应用物理学];
学科分类号
摘要
The kinetic modeling of low-pressure (p similar to 1-10 torr) stationary nitrogen discharges and the corresponding afterglows is reviewed. It is shown that a good description of the overall behavior of nitrogen plasmas requires a deep understanding of the coupling between different kinetics. The central role is played by ground-state vibrationally excited molecules, N-2(X (1)Sigma(g)(+), v), which have a strong influence on the shape of the electron energy distribution function, on the creation and destruction of electronically excited states, on the gas heating, dissociation and on afterglow emissions. N-2(X (1)Sigma(g)(+), v) molecules are actually the hinge ensuring a strong link between the various kinetics. The noticeable task done by electronically excited metastable molecules, in particular N-2(A (3)Sigma(u)(+)) and N-2(a' (1)Sigma(u)(-)), is also pointed out. Besides contributing to the same phenomena as vibrationally excited molecules, these electronic metastable states play also a categorical role in ionization. Furthermore, vibrationally excited molecules in high v levels are in the origin of the peaks observed in the. owing afterglow for the concentrations of several species, such as N-2(A (3)Sigma(g)(+)), N-2(B (3)Pi(g)), N-2 + (B-2 Sigma(u)(+))and electrons, which occur downstream from the discharge after a dark zone as a consequence of the V-V pumping-up mechanism.
引用
收藏
页码:125 / 152
页数:28
相关论文
共 178 条
[1]   Vibrational energy transfer rates using a forced harmonic oscillator model [J].
Adamovich, IV ;
Macheret, SO ;
Rich, JW ;
Treanor, CE .
JOURNAL OF THERMOPHYSICS AND HEAT TRANSFER, 1998, 12 (01) :57-65
[2]   Three-dimensional analytic model of vibrational energy transfer in molecule-molecule collisions [J].
Adamovich, IV .
AIAA JOURNAL, 2001, 39 (10) :1916-1925
[3]   Determination of nitrogen V-V transfer rates by stimulated Raman pumping [J].
Ahn, T ;
Adamovich, IV ;
Lempert, WR .
CHEMICAL PHYSICS, 2004, 298 (1-3) :233-240
[4]  
ALEKSANDROV NL, 1979, HIGH TEMP+, V17, P179
[5]  
ALEKSANDROV NL, 1985, HIGH TEMP+, V23, P666
[6]   CROSS-SECTION FOR EXCITATION OF N-2+ FIRST NEGATIVE BANDS IN COLLISIONS BETWEEN GROUND-STATE N-2+ IONS AND VIBRATIONALLY EXCITED N-2 MOLECULES [J].
ANKETELL, J .
CANADIAN JOURNAL OF PHYSICS, 1977, 55 (13) :1134-1136
[7]  
[Anonymous], 1956, HDB PHYS
[8]   DEACTIVATION DYNAMICS OF VIBRATIONALLY EXCITED NITROGEN MOLECULES BY NITROGEN-ATOMS - EFFECTS ON NONEQUILIBRIUM VIBRATIONAL DISTRIBUTION AND DISSOCIATION RATES OF NITROGEN UNDER ELECTRICAL DISCHARGES [J].
ARMENISE, I ;
CAPITELLI, M ;
GARCIA, E ;
GORSE, C ;
LAGANA, A ;
LONGO, S .
CHEMICAL PHYSICS LETTERS, 1992, 200 (06) :597-604
[9]   TIME EVOLUTION OF THE POPULATION VERSION BETWEEN (A(3)SIGMA(U)(+), V'') AND (B(3)PI(G), V') STATES IN THE POSITIVE-COLUMN OF A NITROGEN PULSED DISCHARGE [J].
AUGUSTYNIAK, E ;
BORYSOW, J .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1995, 28 (01) :55-60
[10]   VIBRATIONAL-STATE-TO-STATE COLLISION-INDUCED INTRAMOLECULAR ENERGY-TRANSFER N2(A(3)SIGMA(U)(+), V''-]B(3)PI(G), V') [J].
BACHMANN, R ;
LI, X ;
OTTINGER, C ;
VILESOV, AF ;
WULFMEYER, V .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (11) :8606-8626