Hao Xiaobin, Wang Baojun, Wang Qiang, Zhang Riguang, Li Debao
Key Laboratory of Coal Science and Technology of Ministry of Education and Shanxi Province, Taiyuan University of Technology, No. 79 Yingze West Street, Taiyuan 030024, Shanxi, P. R. China.
State Key Laboratory of Coal Conversion, Institute of Coal Chemistry, Chinese Academy of Sciences, Taiyuan 030001, Shanxi, P. R. China.
Phys Chem Chem Phys. 2016 Jun 29;18(26):17606-18. doi: 10.1039/c6cp01689h.
CO adsorption and activation on Ni(100), (110) and (111) surfaces have been systematically investigated to probe the effect of coverage and surface structure on CO adsorption and activation. Herein, dispersion-corrected density functional theory calculations (DFT-D) were employed, and the related thermodynamic energies at 523 K were calculated by including the zero-point energy, thermal energy and entropic corrections; the results show that the saturated coverage of CO on the Ni(111), (100) and (110) surfaces correspond to 8/9, 9/12 and 9/9 ML, respectively. As the coverage increases, the stepwise adsorption free energies decrease on the flat (111) and (100) surfaces, whereas small changes occur on the corrugated (110) surface. CO migrates from the three-fold hollow site to the top site on the (111) surface, and from the four-fold hollow to the two-fold bridge site on the (100) surface, while all the CO molecules remain at the short-bridge site on the (110) surface. As a result, the obtained intermolecular CO-CO repulsive interactions on the flat surface are stronger than the interactions on the corrugated surface. Furthermore, the computed CO vibrational frequencies at different levels of coverage over the Ni surfaces agree well with the experimental results. On the other hand, kinetic analyses were utilized to compare the stepwise CO desorption with the dissociation at different degrees of coverage on the three Ni surfaces. CO desorption is more favorable than its dissociation at all coverage levels on the most exposed Ni(111) surface. Analogously, CO desorption becomes more favorable than its dissociation on the Ni(110) surface at higher coverage, except for coverage of 1/9 ML, in which CO desorption competes with its dissociation. However, on the Ni(100) surface, CO dissociation is more favorable than its desorption at 1/12 ML; when the coverage increases from 2/12 to 3/12 ML, equilibrium states exist between dissociation and desorption over the surface; when the coverage is greater than or equal to 4/9 ML, CO desorption becomes more favorable than dissociation. By applying the atomistic thermodynamics method, the determination of stable coverage as a function of temperature and partial pressure provides useful information, not only for surface science studies under ultrahigh vacuum conditions, but also for practical applications at high temperature and pressure in exploring reactions.
系统研究了CO在Ni(100)、(110)和(111)表面的吸附和活化,以探究覆盖度和表面结构对CO吸附和活化的影响。在此,采用了色散校正密度泛函理论计算(DFT-D),并通过纳入零点能、热能和熵校正来计算523 K时的相关热力学能;结果表明,CO在Ni(111)、(100)和(110)表面的饱和覆盖度分别对应8/9、9/12和9/9 ML。随着覆盖度的增加,平整的(111)和(100)表面上逐步吸附自由能降低,而起伏的(110)表面上变化较小。CO在(111)表面从三重中空位点迁移到顶位,在(100)表面从四重中空位点迁移到二重桥位,而所有CO分子都保留在(110)表面的短桥位。结果,在平整表面上获得的分子间CO-CO排斥相互作用比在起伏表面上的相互作用更强。此外,计算得到的Ni表面不同覆盖度下的CO振动频率与实验结果吻合良好。另一方面,利用动力学分析比较了在三种Ni表面不同覆盖度下CO的逐步脱附与解离。在最暴露的Ni(111)表面,在所有覆盖度下CO脱附都比其解离更有利。类似地,在较高覆盖度下,CO在Ni(110)表面的脱附比其解离更有利,但覆盖度为1/9 ML时除外,此时CO脱附与其解离相互竞争。然而,在Ni(100)表面,CO在1/12 ML时解离比脱附更有利;当覆盖度从2/12增加到3/12 ML时,表面上解离和脱附之间存在平衡状态;当覆盖度大于或等于4/9 ML时,CO脱附比解离更有利。通过应用原子热力学方法,确定作为温度和分压函数的稳定覆盖度不仅为超高真空条件下的表面科学研究提供了有用信息,也为高温高压下探索反应的实际应用提供了有用信息。