Research Institute of Petroleum Industry(RIPI), West Side of Azadi Complex, Tehran, 1485733111, Iran.
J Mol Graph Model. 2018 May;81:86-96. doi: 10.1016/j.jmgm.2018.02.015. Epub 2018 Mar 2.
In this study, pure and ternary adsorption of hydrogen sulfide (HS), ethylbenzene (EB), and carbon monoxide (CO) on different arrays of zigzag double wall carbon nanotube was investigated using grand canonical Monte Carlo simulations. The internal diameters of nanotube were fixed at 2r = 50.17 Å while nanotube wall distances were different values from d = 0 Å to d = 150 Å. Pure simulation results indicated that adsorption quantity of HS and EB in low pressure ranges of P = 1.9 bar to P = 3.1 bar was at least 100% more than CO adsorption quantities. At high pressure ranges of P = 23.1 bar to P = 38.2 bar HS adsorption was greater than EB and CO by about 200 molecules per unit cell (UC) at low nanotube distances. This was related to smaller kinetic diameter and greater dipole moment of HS compared to EB and CO. At higher nanotube distance the effect of size however disappears and all three gases approach to adsorption quantity of about 800 molecules/UC. Graphical representation of adsorption areas showed that HS and CO form multilayer adsorption around nanotube inner and outer walls while EB fill the whole space uniformly without any congestion around the walls. Ternary adsorption results EB/CO and HS/CO selectivity are greater than EB/HS selectivity. In addition, at smaller nanotube distances HS/CO selectivity is generally higher than EB/CO selectivity, which at higher nanotube distance the order becomes revers suggesting that size dependent effects on adsorption vanishes. Isosteric heat of adsorption shows that the order of EB > HS > CO suggesting that ethylbenzene interaction with nanotube arrays was strongest. Although HS has a greater dipole moment and smaller molecular dimension, EB adsorption at higher nanotube distance is greater than HS by at least 50% probably because EB is less volatile.
在这项研究中,使用巨正则蒙特卡罗模拟研究了纯态和三元态下硫化氢(HS)、乙苯(EB)和一氧化碳(CO)在不同排列的锯齿形双壁碳纳米管上的吸附。纳米管的内径固定在 2r=50.17Å,而纳米管壁之间的距离从 d=0Å到 d=150Å不等。纯吸附模拟结果表明,在 P=1.9 到 3.1 巴的低压范围内,HS 和 EB 的吸附量至少比 CO 多 100%。在 P=23.1 到 38.2 巴的高压范围内,在低纳米管距离下,HS 的吸附量比 EB 和 CO 多约 200 个单位细胞(UC)。这与 HS 相比 EB 和 CO 具有更小的动力学直径和更大的偶极矩有关。在更高的纳米管距离下,尺寸的影响消失,所有三种气体的吸附量都接近 800 个分子/UC。吸附面积的图形表示表明,HS 和 CO 在外壁和内壁周围形成多层吸附,而 EB 均匀地填充整个空间,没有任何在壁周围的拥挤。三元吸附结果表明,EB/CO 和 HS/CO 的选择性大于 EB/HS 的选择性。此外,在较小的纳米管距离下,HS/CO 的选择性通常高于 EB/CO 的选择性,而在较高的纳米管距离下,顺序相反,表明吸附的尺寸依赖性效应消失。等吸附热表明,EB>HS>CO,这表明乙苯与纳米管阵列的相互作用最强。尽管 HS 具有更大的偶极矩和更小的分子尺寸,但在较高的纳米管距离下,EB 的吸附量至少比 HS 多 50%,这可能是因为 EB 的挥发性较低。