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Shock-tube study of relaxation in HCN

机译:HCN松弛的冲击管研究

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Thermal vibrational relaxation in HCN mixtures with Kr has been observed with the laser-schlieren technique. The experiments cover the temperatures 750-2900 K and a large pressure range of 13-420 Torr in 5% and 20% HCN/Kr mixtures. Relaxation is extremely fast but appears to occur in two well-separated stages that are assigned to the vibrational transitions (000)->(010) and (000)->(100) with perhaps some lesser contribution from (000)->(001). This interpretation is strongly supported by a comparison of net density changes to thermodynamic calculations. The first and faster process shows near constant relaxation times whereas the latter slower stage has a slight decrease of these with T. Relaxation times in pure HCN obtained by neglecting the small contribution of krypton are as follows: (a) P tau(HCN-HCN)=27 exp(1.473/T-1/3) ns atm (000)->(010); (b) P tau(HCN-HCN)=11 exp(32.6/T-1/3) ns atm (000)->(100). Probabilities suggested by these results are around 0.05 for the fast step and 0.0035 to 0.005 for the slow process. These results are close to those found by laser fluorescence measurements for deactivation of levels involving excitation of the C-H stretch (001) at 3312 cm(-1). These results are also consistent with the notion of a dominance of the fast stage by T,R-V transfer (thermal relaxation) occurring in a weakly bound complex. However, the slow step most likely occurs through a V-V process (03 (1)0)->(100), Delta E=27.7 cm(-1), after multiple excitation of the (010) mode. These are the first thermal measurements of relaxation in HCN and the first to see energy transfer involving the low-frequency modes. (C) 2008 American Institute of Physics.
机译:激光-石蜡技术已观察到HCN与Kr混合物中的热振动弛豫。实验覆盖了750和2900 K的温度以及5%和20%的HCN / Kr混合物的13-420 Torr的大压力范围。弛豫非常快,但似乎在两个完全分开的阶段中发生,它们分别分配给振动跃迁(000)->(010)和(000)->(100),而从(000)->( 001)。将净密度变化与热力学计算进行比较,就可以很好地支持这种解释。第一个和较快的过程显示出几乎恒定的弛豫时间,而后一个较慢的过程则随着T的变化而略有下降。通过忽略k的少量贡献而获得的纯HCN的弛豫时间如下: )= 27 exp(1.473 / T-1 / 3)ns atm(000)->(010); (b)P tau(HCN-HCN)= 11 exp(32.6 / T-1 / 3)ns atm(000)->(100)。这些结果表明,快速步骤的概率约为0.05,而慢速过程的概率为0.0035至0.005。这些结果接近于通过激光荧光测量发现的用于在3312 cm(-1)处激发C-H拉伸(001)的水平失活的结果。这些结果也与在弱结合的复合物中发生的T,R-V转移(热弛豫)的快速阶段占优势的概念一致。但是,在多次激发(010)模式之后,最慢的步进很可能是通过V-V过程(03(1)0)->(100)发生的,Delta E = 27.7 cm(-1)。这是HCN中弛豫的第一个热测量值,也是第一个看到涉及低频模式的能量传递的测量值。 (C)2008美国物理研究所。

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