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Extra resources for Rarefied Gas Dynamics: Volume 2
Previously, Derwent and Thrush gave successively two different analysis. In the first one, they reported a fairly even distribution2; in the second one, they found a peak near V' = 2018. However, the peak near V'= 40 does not appear, and that is in agreement with their observed spectrum which does not exhibit a second maximum near 520 nm. This diversified behaviour of the B-state vibrational distribution can be explained by the collisional relaxation, the distribution at p = 0,04 Torr giving the real excitation processes of the A and B state of iodine.
ENTAL APPARATUS (VARIABLE P 0 ) Fig. 1. SECOND DEGREE OF FREEDOM OF EXPERIMENTAL APPARATUS (VARIABLE x/D) L. APPARATUS (VARIABLE DETECTOR PosiTION, e) Schematic Diagram of Principal Components of Molecular-Beam System Used in Velocity-Distribution Measurements. 12(l-1) Tu 1 ( TJ. 3--2 )(T~)z - r.. r.. ....... - ) +4 (li- - 4 +3 r.. T• Tu r.. z 0 ;::: a:: ... 4 z Q ..... 0. 2 3 A ~ ~ TEMPERATURE RATIO, T,IT, 1 Fig. 2. 0 Relaxation Function Appearing in Equation Used in Deducing Effective Hard-Sphere Diameter.
Soc. Faraday Trans. , 53 : 162 (1972). J. Tellinghuisen, Resolution of the visible infrared absorption spectrum of L~ into three contributing transitions, J. of Chem. , 58 : 2821 (1973). A. P. N. K. v Physico-Technica1 Institute Do1goprudny 1 141700 1 USSR INTROIJlCI'IOO The mixing of co2 into a supersonic flow of vibrated-exci ted nitrogen for increasing efficiency and specific ch~2cteristics of gasdynamic 1asers (GDL) is wide1y used at present 1 • The main characterization of a 1aser media is i ts energy reserve 1 the detennination of which opens a nurober of advantages as canpared wi th the traditiona1 detennination of co2 vibrationa1 terrperature.