We wish to communicate results from studies of the vibrational deactivation of chemically activated molecules [ 11. The present measurements are for CHaCFZ with a wide variety of bath gases which include inefficient rare gases as well as polyatomic gases ranging up to the efficiency of those investigated by Chang, Craig, and Setser [2]. The results consist of comparisons of data at high pressure, which give a measure of relative collisional deactivation efficiencies, and of extensive low-pressure data, which permit approximate assignment of a collisional transition probability model and the average energy ( A E ) lost per collision according to that model. For several bath gases experiments were done at 300°K and 195°K. The important general conclusions are (a) there is a wide spread in collisional efficiencies for various bath gases, and (b) CH 3CF 3 is particularly difficult to deactivate relative to 1,2-dichloroethane [3] and cyclopropane [4].The photolysis [5] of CF3N2CH3 generates CH3 and CF3 radicals from which chemically activated CHBCF3" molecules are formed, with an average energy of 102 kcal/rnole [Z]. The critical energy for H F elimination producing CHz=CF2 is -68 kcal/mole [6]. Chemically activated CH3CF3* may either undergo unimolecular reaction or collisional stabilization. The nonequilibrium rate constant for this process is defined by k, = wD/S, where D is the number of molecules decomposing per unit time, S is the number of molecules stabilized per unit time, and w is the collision frequency. The proportionality between w and pressure allows the rate constant to be initially recorded as k, = P(D/S); conversion to sec-' units was done in the usual manner. The experiments consisted of mapping the increase in k, with decreasing pressure by gas chromatographic measurement of D / S over a wide pressure range. For a particular bath gas the mole ratio of bath gas to CH 3N2CF 3 was constant and sufficiently high that collisions with CH3N2CF3 could be neglected. The experimental results for SFs, CFr, CH4, and N P are presented in Figure 1. The limiting high-pressure rate constants k,", the standard deviations, and the "best fit" curves were cjbtained by polynomial regression analysis. Table I presents a summary of the results.The competition between unimolecular reaction and cascade deactivation for the i t h energy increment can be represented by the master equation [1,2,4]. Computational solution of the master equation to obtain steady-state concentra-
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