Time-Resolved CRDS Measurements of the N2(A3Σu+) Density Produced by Nanosecond Discharges in Atmospheric Pressure Nitrogen and Air

被引:48
作者
Stancu, Gabi D. [1 ]
Janda, Mario [1 ]
Kaddouri, Farah [1 ]
Lacoste, Deanna A. [1 ]
Laux, Christophe O. [1 ]
机构
[1] Ecole Cent Paris, Lab EM2C, CNRS, UPR 288, F-92295 Chatenay Malabry, France
关键词
RADIATIVE TRANSITION-PROBABILITIES; ENERGY-POOLING REACTIONS; RING-DOWN SPECTROSCOPY; RATE CONSTANTS; STATE; O-2; NO; MOLECULES; N-2; N2;
D O I
10.1021/jp9075383
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Cavity ring-down spectroscopy (CRDS) is used to measure the number density of N-2(A(3)Sigma(+)(u)) metastables produced by nanosecond repetitively pulsed discharges in nitrogen and air preheated at 1000 K and atmospheric pressure. The densities of N2(A) are inferred from the absorbance of the Q(1)(22) and Q(3)(16) lines of the (2 <- 0) vibrational band of the first positive system (B-3 Pi g - A(3)Sigma(+)(u)) of N-2 at 769.945 nm. The procedure for determining the temporal evolution of the density of metastable from the measured ring down signals is presented. The maximum number densities are in the range of 10(14)-10(15) molecules cm(-3) for air and nitrogen discharges, respectively. In nitrogen, the decay of the N2(A) density is shown to be a second-order process with a rate coefficient of 1.1 x 10(-9) cm(3) s(-1) at 1600 K with a factor of 2 uncertainty. In air, the decay is estimated to be I order of magnitude faster than that in nitrogen owing to quenching by atomic and molecular oxygen. Furthermore, the rotational temperature is determined by comparison of CRDS measurements and simulations of several rotational lines of the (2 <- 0) band of the first positive system of N-2 between 769.8 and 770.7 nm. The rotational and vibrational temperatures are also determined by comparison of optical emission measurements and simulations of the second positive system of N-2 between 365 and 385 nm. In these CRDS measurements, we achieved a temporal resolution down to 50 ns.
引用
收藏
页码:201 / 208
页数:8
相关论文
共 47 条
[1]   KINETICS OF THE (A(3)SIGMA(U)+, V=0) STATE OF N-2 IN THE NEAR AFTERGLOW OF A NITROGEN PULSED DISCHARGE [J].
AUGUSTYNIAK, E ;
BORYSOW, J .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1994, 27 (03) :652-660
[2]  
Bachir IH, 1997, CHEM PHYS LETT, V270, P533, DOI 10.1016/S0009-2614(97)00387-4
[3]  
Becker KH., 2005, Non-Equilibrium Air Plasmas at Atmospheric Pressure
[4]   Simultaneous kinetics and ring-down: Rate coefficients from single cavity loss temporal profiles [J].
Brown, SS ;
Ravishankara, AR ;
Stark, H .
JOURNAL OF PHYSICAL CHEMISTRY A, 2000, 104 (30) :7044-7052
[5]  
BUSCH KW, 1999, ACS SYM SER, V720, DOI DOI 10.1021/BK-1999-0720
[6]  
Capitelli M., 2000, Plasma kinetics in atmospheric gases
[7]   Experimental study and modelling of a low-pressure N2-O2 time afterglow [J].
Cartry, G ;
Magne, L ;
Cernogora, G .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1999, 32 (15) :1894-1907
[8]   VIBRATIONAL POPULATIONS OF N-2(A 3-SIGMA-U+) IN A PURE NITROGEN GLOW-DISCHARGE [J].
CERNOGORA, G ;
FERREIRA, CM ;
HOCHARD, L ;
TOUZEAU, M ;
LOUREIRO, J .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 1984, 17 (21) :4429-4437
[9]   ENERGY-TRANSFER REACTIONS OF N-2(A3SIGMA-UT) .5. QUENCHING BY HYDROGEN HALIDES, METHYL HALIDES, AND OTHER MOLECULES [J].
CLARK, WG ;
SETSER, DW .
JOURNAL OF PHYSICAL CHEMISTRY, 1980, 84 (18) :2225-2233
[10]   LASER-INDUCED FLUORESCENCE DETECTION AND CHARACTERIZATION OF IONIC AND METASTABLE REACTION-PRODUCTS [J].
COOK, JM ;
MILLER, TA ;
BONDYBEY, VE .
JOURNAL OF CHEMICAL PHYSICS, 1978, 69 (06) :2562-2568