Bross David H, Yu Hua-Gen, Harding Lawrence B, Ruscic Branko
Chemical Sciences and Engineering Division , Argonne National Laboratory , Lemont , Illinois 60439 , United States.
Division of Chemistry, Department of Energy and Photon Sciences , Brookhaven National Laboratory , Upton, New York 11973 , United States.
J Phys Chem A. 2019 May 16;123(19):4212-4231. doi: 10.1021/acs.jpca.9b02295. Epub 2019 May 7.
The best currently available set of temperature-dependent nonrigid rotor anharmonic oscillator (NRRAO) thermochemical and thermophysical properties of hydroxymethyl radical is presented. The underlying partition function relies on a critically evaluated complement of accurate experimental and theoretical data and is constructed using a two-pronged strategy that combines contributions from large amplitude motions obtained from direct counts, with contributions from the other internal modes of motion obtained from analytic NRRAO expressions. The contributions from the two strongly coupled large-amplitude motions of CHOH, OH torsion and CH wag, are based on energy levels obtained by solving the appropriate two-dimensional projection of a fully dimensional potential energy surface that was recently obtained at the CCSD(T)/cc-pVTZ level of theory. The contributions of the remaining seven, more rigid, vibrational modes and of the external rotations are captured by NRRAO corrections to the standard rigid rotor harmonic oscillator (RRHO) treatment, which include corrections for vibrational anharmonicities, rotation-vibration interaction, Coriolis effects, and low temperature. The basic spectroscopic constants needed for the construction of the initial RRHO partition function rely on experimental ground-state rotational constants and the best available experimental fundamentals, additionally complemented by fundamentals obtained from the variational solution of the full-dimensional potential energy surface using a recently developed two-component multilayer Lanczos algorithm. The higher-order spectroscopic constants necessary for the NRRAO corrections are extracted from a second-order variational perturbation treatment (VPT2) of the same potential energy surface. The Lanczos solutions of the fully dimensional surface are validated against available experimental data, and the VPT2 results and the solutions of the reduced dimensionality surface are validated both against the Lanczos solutions and available experiments. The NRRAO thermophysical and thermochemical properties, given both in tabular form and as seven- and nine-coefficient NASA polynomials, are compared to previous results. In addition, the latest ATcT values for the enthalpy of formation of CHOH at 298.15 K (0 K), -16.75 ± 0.27 kJ/mol (-10.45 ± 0.27 kJ/mol), and of other related CH O species ( n = 0-4, m = 0,1) are reported, together with a plethora of related bond dissociation enthalpies (BDEs), such as the C-H, O-H, and C-O bond dissociation enthalpies of methanol, 402.16 ± 0.26 kJ/mol (395.61 ± 0.26 kJ/mol), 440.34 ± 0.26 kJ/mol (434.86 ± 0.26 kJ/mol), and 384.85 ± 0.15 kJ/mol (377.14 ± 0.15 kJ/mol), respectively, and analogous BDEs for hydroxymethyl, 343.67 ± 0.37 kJ/mol (339.16 ± 0.37 kJ/mol), 125.54 ± 0.28 kJ/mol (121.11 ± 0.28 kJ/mol), and 445.86 ± 0.29 kJ/mol (438.76 ± 0.29 kJ/mol), respectively. The reasons governing the alternation between strong and weak sequential H atom BDEs of methanol are also discussed.
本文给出了目前可用的关于羟甲基自由基的温度相关非刚性转子非谐振荡器(NRRAO)热化学和热物理性质的最佳数据集。基础的配分函数依赖于对准确实验和理论数据的严格评估补充,并采用双管齐下的策略构建,该策略将直接计数得到的大幅度运动的贡献与从解析NRRAO表达式获得的其他内部运动模式的贡献相结合。CHOH的两个强耦合大幅度运动,即OH扭转和CH摆动的贡献,基于通过求解最近在CCSD(T)/cc-pVTZ理论水平获得的全维势能面的适当二维投影得到的能级。其余七个更刚性的振动模式和外部旋转的贡献通过对标准刚性转子谐振荡器(RRHO)处理的NRRAO修正来捕捉,其中包括振动非谐性、转动-振动相互作用、科里奥利效应和低温的修正。构建初始RRHO配分函数所需的基本光谱常数依赖于实验基态转动常数和最佳可用实验基频,此外还辅以使用最近开发的双组分多层兰索斯算法从全维势能面的变分解中获得的基频。NRRAO修正所需的高阶光谱常数从同一势能面的二阶变分微扰处理(VPT2)中提取。全维表面的兰索斯解根据可用实验数据进行验证,VPT2结果和降维表面的解则根据兰索斯解和可用实验进行验证。以表格形式以及七系数和九系数NASA多项式给出的NRRAO热物理和热化学性质与先前结果进行了比较。此外,还报告了298.15 K(0 K)时CHOH生成焓的最新ATcT值,为-16.75±0.27 kJ/mol(-10.45±0.27 kJ/mol),以及其他相关CH O 物种(n = 0 - 4,m = 0,1)的生成焓,同时还报告了大量相关的键解离焓(BDE),例如甲醇的C - H、O - H和C - O键解离焓分别为402.16±0.26 kJ/mol(395.61±0.26 kJ/mol)、440.34±0.26 kJ/mol(434.86±0.26 kJ/mol)和384.85±0.15 kJ/mol(377.14±0.15 kJ/mol),以及羟甲基的类似BDE分别为343.67±0.37 kJ/mol(339.16±0.37 kJ/mol)、125.54±0.28 kJ/mol(121.11±0.28 kJ/mol)和445.86±0.29 kJ/mol(438.76±0.29 kJ/mol)。还讨论了甲醇中强、弱顺序H原子BDE交替的原因。