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Comparison of O_2-O vibrational relaxation and dissociation rate coefficients computed on potential energy surfaces of different fidelity

机译:在不同保真度的势能面上计算的O_2-O振动弛豫和解离速率系数的比较

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The purpose of this study is two-fold: 1) to compare the vibrational relaxation and dissociation rate coefficients for the O_2(~3∑_g~-)+O(~3P) system between the Varandas and Pais potential energy surface (PES), and the Varga et al. 1~1 A′ PES, and 2) to present a new set of state-to-state (STS) vibrational relaxation rate coefficients, state-specific dissociation rate coefficients, and total dissociation rate coefficients using all nine adiabatic ab initio PESs (1~1A′, 2~1A′, 1~1A″, 1~3A′, 2~3A′, 1~3A″, 1~5A′, 2~5A′ and 1~5A") by Varga et al.1 These rate coefficients are calculated from collisional cross-sections obtained using the Quasi-Classical Trajectory (QCT) method for a temperature range T = 2,000 K to T = 12,000 K. Translational-rotational equilibrium is assumed. It is found that using the Varandas and Pais PES leads to vibrational energy transfer rate coefficients which are at most twice higher than those calculated for Varga et al. 1JA′ PES. These differences are not very significant on the logarithmic scale of rates. STS vibrational relaxation rate coefficients for the nine Varga et al. PESs show that the PES that contributes the most towards relaxation varies significantly depending on the vibrational transition considered. This observation indicates that all 9 PESs must be taken into account to present a more complete picture of the full O2-O system. Finally, state-specific and total dissociation rate coefficients, considering cross-sections from all 9 appropriately weighted Varga et al. PESs, are calculated and reported. Contrary to vibrational relaxation, it is observed that dissociation rate coefficients are not sensitive to the 9 Varga et al. PESs.
机译:本研究的目的有两个方面:1)比较Varandas和Pais势能面(PES)之间的O_2(〜3∑_g〜-)+ O(〜3P)系统的振动弛豫和解离速率系数,以及Varga等人。 1〜1 A'PES和2)提出了一套使用所有九种绝热从头算起的PES的新状态-状态(STS)振动弛豫速率系数,特定于状态的解离速率系数和总解离速率系数(1 Varga等人[1] ~~ 1A',2〜1A',1〜1A'',1〜3A',2〜3A',1〜3A'',1〜5A',2〜5A'和1〜5A“)这些速率系数是根据在温度范围T = 2,000 K到T = 12,000 K时使用准经典轨迹(QCT)方法获得的碰撞横截面计算得出的,并假定了平移-旋转平衡。 Pais PES导致的振动能量传递速率系数最多比Varga等人的1JA′PES计算出的高两倍,这些差异在速率的对数范围内不是很显着,九个Varga等人的STS振动弛豫速率系数。 al。PESs显示,对松弛贡献最大的PES随振动的变化而显着变化。考虑过渡。该观察表明,必须考虑所有9个PES,才能对完整的O2-O系统有一个更完整的了解。最后,考虑所有9个权重适当的Varga等人的横截面,确定特定状态和总的解离速率系数。计算并报告了PES。与振动弛豫相反,观察到解离速率系数对9 Varga等人不敏感。聚醚砜。

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