Nitric Oxide Vibrational Relaxation and Decomposition Rate Measurements in Shock-Heated NO-Ar and NO-N2Mixtures

2022 ◽  
Author(s):  
Jesse W. Streicher ◽  
Ajay Krish ◽  
Efaine Chang ◽  
Ronald K. Hanson
Nature ◽  
1969 ◽  
Vol 224 (5216) ◽  
pp. 268-268 ◽  
Author(s):  
W. D. BRESHEARS ◽  
P. F. BIRD

The first excited vibrational level of the ground electronic states of nitric oxide was popu­lated above its equilibrium value by flash photolysis of nitric oxide + inert gas mixtures, under isothermal conditions. Electronic excitation NO 2 II ( v = 0) + hv → NO 2 Ʃ ( v = 0, 1, 2) was followed either by fluorescence NO 2 Ʃ ( v = 0, 1, 2) → NO 2 II ( v = 0, 1, 2...) + hv , or by quenching NO 2 Ʃ ( v = 0, 1, 2) + M → NO 2 II( v = 0, 1, 2...) + M , causing a non-equilibrium population of the vibrational levels of the ground electronic states. Subsequently, the reactions NO 2 II ( v = 1) + M → NO 2 II ( v = 0) + M and NO 2 II ( v = 1) + NO 2 II ( v = 0) → 2NO 2 II ( v = 1) caused a decay of the vibrationally excited molecules with time; this was followed in absorption by kinetic spectroscopy. Because of the rapidity of the last reaction, bands of NO2 II with v >1 were usually observed only in the fluorescence spectrum. In mixtures of 1 to 5 mm of NO with a large excess of nitrogen or krypton, the con­centration of NO2 II ( v = 1) produced by the flash was of the order of 10-1 mm pressure, i. e. about the same concentration which is present in one atmosphere pressure of NO at room temperature. The absolute concentration of NO2 II ( v = 1) was measured accurately by plate photometry, high pressures of NO being used for calibration. The recorded probabilities of vibrational relaxation, P1-0, for NO2 II ( v = 1), and radii for electronic quenching, σ e , by NO, N 2 , CO, H 2 O and CO 2 , are P 1-0 σ e (Å) NO 3.55 x 10 -4 14 N 2 4 x 10 -7 ≤ 2x 10 -2 CO 2.5 x 10 -5 0.6 H 2 O 7 x 10 -3 30 CO 2 1.7 x 10 -4 5 With the use of an analytic form for the flash duration, the entire rise and fall of the concentration of excited species was quantitatively interpreted. A very small fraction of the NO was decomposed by the flash, due either to absorption of radiation below 1900 Å or by reaction of metastable NO molecules with each other or with ground state molecules. Abnormal effects were observed in NO+ H 2 +inert gas mixtures and chemical reaction occurred.


Vibrationally excited carbon monoxide was produced by flashing mixtures of nitric oxide, carbon monoxide and nitrogen. The rate of formation and decay of the vibrationally excited molecules was interpreted by means of the processes: NO ( X 2 I I , υ = 0 ) + h v → NO ( A 2 ∑ + , υ = 0 , 1 , 2 ) , NO ( A 2 ∑ + , υ = 0 , 1 , 2 ) + M →→ NO ( X 2 I I , υ = 1 ) + M , NO ( A 2 ∑ + , υ = 0 , 1 , 2 ) →→ NO ( X 2 I I ) , υ = 1 ) + h v , NO ( X 2 I I , υ = 1 ) + CO X 1 ∑ + ( υ = 0 ) → ← NO ( X 2 I I , υ = 0 ) + CO ( X 1 ∑ + , υ = 1 ) , CO ( X 1 ∑ + , υ = 1 ) + N 2 X 1 ∑ V + ( υ = 0 ) → ← CO ( X 1 ∑ + , υ = 0 ) + N 2 ( X 1 ∑ V + , υ = 1 ) , NO ( X 2 I I , υ = 1 ) + NO X 2 I I ( υ = 0 ) → 2 NO ( X 2 I I , υ = 0 ) .


1970 ◽  
Vol 53 (10) ◽  
pp. 3987-3989 ◽  
Author(s):  
Goro Kamimoto ◽  
Hiroyuki Matsui

1960 ◽  
Vol 33 (2) ◽  
pp. 630-630 ◽  
Author(s):  
Frank Robben ◽  
Philip R. Monson ◽  
John J. Allport

Nature ◽  
1969 ◽  
Vol 224 (5220) ◽  
pp. 687-688 ◽  
Author(s):  
J. BILLINGSLEY ◽  
A. B. CALLEAR

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