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中国物理学会期刊

H2和HD分子宏观热力学性质

CSTR: 32037.14.aps.74.20241793

Macroscopic thermodynamic properties of H2 and HD

CSTR: 32037.14.aps.74.20241793
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  • 本文通过扩展的改进多参数指数型(the extended improved multiparameter exponential-type, EIMPET)势能模型, 结合实验光谱数据, 研究了H2和HD分子的热力学性质. 首先利用解析势能曲线计算得到分子的振转能级, 其次结合量子统计系综理论计算了分子在100—6000 K温度下的配分函数、摩尔热容、摩尔熵、摩尔焓以及约化摩尔吉布斯自由能. 计算结果与美国国家标准与技术研究所(National Institute of Standards and Technology, NIST)数据库中的数据具有良好的一致性. 本文的理论方法可用于预测某些气态物质的热力学性质.

     

    H2 molecule and their isotopes represent one of the modern clean energy sources. It is imperative to understand their thermodynamic properties for comprehending their behaviors under various conditions. Thereby promoting their more in-depth applications. In this paper, an extended improved multiparameter exponential-type potential (EIMPET) combined with the quantum statistical ensemble theory is used to investigate and analyze the thermodynamic properties of H2 and HD molecules. Firstly, reliable energy level data for molecules are obtained using the EIMPET potential. Subsequently, the one-dimensional Schrödinger equation is solved with the LEVEL program to determine the rovibrational energy levels of the molecules. Finally, the quantum statistical ensemble theory is integrated to determine the partition functions, molar heat capacity, molar entropy, molar enthalpy, and reduced molar Gibbs free energy of H2 and HD in a temperature range of 100–6000 K. The calculation results indicate that compared with IHH potential and IMPET potential, the EIMPET potential is closer to RKR data. A comparison of the calculated thermodynamic properties of the molecules reveals that the results from the EIMPET potential-based method accord well with those from the NIST database. Specifically, for H2, the root mean square (RMS) errors for C_\textm\left( T \right) , S_\textm\left( T \right) , G_\textr\left( T \right) , and \Delta H_\textr\left( T \right) are 0.6894 J·K–1·mol–1, 0.3824 J·K–1·mol–1, 0.1754 J·K–1·mol–1, and 0.9586 kJ·mol–1, respectively, while for HD, the RMS errors are 0.3431 J·K–1·mol–1, 0.1443 J·K–1·mol–1, 0.0495 J·K–1·mol–1, and 0.4863 kJ·mol–1, respectively. All of these results are superior to those obtained using IMPET potential, and to those obtained using IHH potential as a whole. These findings demonstrate the advantages and practical applications of the EIMPET potential in calculating the thermodynamic properties of diatomic gas molecules, providing a foundation for subsequently studying the thermodynamic properties of triatomic molecules.

     

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