Department of Mechanical Engineering, Keio University, 3-14-1 Hiyoshi, Kohoku-Ku, Yokohama 223-8522, Japan.
J Chem Phys. 2013 Mar 28;138(12):124504. doi: 10.1063/1.4795499.
Position and orientation of water protons need to be specified when the molecular simulation studies are performed for clathrate hydrates. Positions of oxygen atoms in water are experimentally determined by X-ray diffraction analysis of clathrate hydrate structures, but positions of water hydrogen atoms in the lattice are disordered. This study reports a determination of the water proton coordinates in unit cell of structure I (sI), II (sII), and H (sH) clathrate hydrates that satisfy the ice rules, have the lowest potential energy configuration for the protons, and give a net zero dipole moment. Possible proton coordinates in the unit cell were chosen by analyzing the symmetry of protons on the hexagonal or pentagonal faces in the hydrate cages and generating all possible proton distributions which satisfy the ice rules. We found that in the sI and sII unit cells, proton distributions with small net dipole moments have fairly narrow potential energy spreads of about 1 kJ∕mol. The total Coulomb potential on a test unit charge placed in the cage center for the minimum energy∕minimum dipole unit cell configurations was calculated. In the sI small cages, the Coulomb potential energy spread in each class of cage is less than 0.1 kJ∕mol, while the potential energy spread increases to values up to 6 kJ∕mol in sH and 15 kJ∕mol in the sII cages. The guest environments inside the cages can therefore be substantially different in the sII case. Cartesian coordinates for oxygen and hydrogen atoms in the sI, sII, and sH unit cells are reported for reference.
在进行笼形水合物的分子模拟研究时,需要指定水合质子的位置和取向。水分子中氧原子的位置通过笼形水合物结构的 X 射线衍射分析实验确定,但晶格中水合质子的位置是无序的。本研究报告了满足冰规则、具有质子最低势能构型且净偶极矩为零的 sI(sI)、sII(sII)和 H(sH)笼形水合物晶胞中质子坐标的确定。通过分析水合物笼中六边形或五边形面上质子的对称性,并生成满足冰规则的所有可能质子分布,选择晶胞中的可能质子坐标。我们发现,在 sI 和 sII 晶胞中,具有小净偶极矩的质子分布具有相当窄的势能分布,约为 1 kJ/mol。计算了放置在笼中心的测试单位电荷的总库仑势能,对于最小能量/最小偶极单元胞构型。在 sI 小笼中,每个笼类的库仑势能能分布的展宽小于 0.1 kJ/mol,而在 sH 和 sII 笼中,势能能分布展宽增加到高达 6 kJ/mol 和 15 kJ/mol。因此,在 sII 情况下,笼内的客体环境可能会有很大的不同。报告了 sI、sII 和 sH 晶胞中氧和氢原子的笛卡尔坐标,以供参考。