Ferre-Vilaplana A
High-Performance Computing and Visualization Aided Scientific and Engineering Applications Group, Instituto Tecnológico de Informática, Ciudad Politécnica de la Innovación, Camino de Vera s/n, Edificio 8G, 46022 Valencia, Spain.
J Chem Phys. 2005 Jun 1;122(21):214724. doi: 10.1063/1.1924545.
Using relatively approximated methods, physisorption of molecular hydrogen on single-walled carbon nanotubes (SWCNTs) as a mechanism to develop hydrogen storage systems has been only partially investigated in literature. Here, we use ab initio molecular-orbital theory, at benchmark quality level, to provide a more complete description about the mentioned mechanism. Physisorption inside and outside achiral-armchair and zigzag-SWCNTs, in the range of diameters from about 6 A-chiral vectors (5,5) and (8,0)-to more than 30 A-chiral vectors (30,30) and (40,0)-was examined. Perpendicular, longitudinal, and transversal configurations, with the hydrogen molecule centered on an aromatic ring, were taken into account. SWCNTs were modeled as curved coronenelike (C24H12) graphene sheets. Local modeling strategies, using more complete basis sets for the adsorbate and for the nearest atoms to the adsorbate than for the lion's share of the substrate, at the Moller-Plesset second-order correlation level, were selected for numerical treatment. Basis-set superposition errors were corrected by means of the counterpoise method of Bois and Bernardi. It was found that physisorption of molecular hydrogen on SWCNTs would depend mainly on the diameter being virtually independent of the chirality. Lowest physisorption energies, up to 20% less than that on planar graphene, would be reached outside nanotubes in the range of diameters of 6-10 A. For hydrogen storage purposes, highest physisorption energies, up to 40% greater than that on planar graphene, but not more, would be reached inside nanotubes in the relatively narrow range of diameters of 10-20 A. Finally, for diameters from 20 A onwards physisorption of molecular hydrogen on SWCNTs would be in the range of +/-10% of that on planar graphene. To our knowledge, this would be the most complete and realistic theoretical investigation of the target physisorption mechanism to date.
使用相对近似的方法,将分子氢在单壁碳纳米管(SWCNT)上的物理吸附作为开发储氢系统的一种机制,在文献中仅得到了部分研究。在此,我们使用基准质量水平的从头算分子轨道理论,对上述机制进行更完整的描述。研究了非手性扶手椅型和锯齿型SWCNT内外的物理吸附,直径范围从约6埃(手性向量(5,5)和(8,0))到超过30埃(手性向量(30,30)和(40,0))。考虑了垂直、纵向和横向构型,氢分子以芳香环为中心。SWCNT被建模为弯曲的冠状(C24H12)石墨烯片。在数值处理中,选择了局部建模策略,在Moller-Plesset二阶相关水平下,对吸附质和与吸附质最近的原子使用比底物大部分区域更完整的基组。基组叠加误差通过Bois和Bernardi的平衡法进行校正。结果发现,分子氢在SWCNT上的物理吸附主要取决于直径,实际上与手性无关。在直径为6 - 10埃的纳米管外,物理吸附能最低,比平面石墨烯上的低20%。出于储氢目的,在直径相对较窄的10 - 20埃范围内,纳米管内的物理吸附能最高,比平面石墨烯上的高40%,但不会更高。最后,对于直径从20埃起,分子氢在SWCNT上的物理吸附将在平面石墨烯的±10%范围内。据我们所知,这是迄今为止对目标物理吸附机制最完整、最现实的理论研究。