TY - JOUR
T1 - Water proton configurations in structures I, II, and H clathrate hydrate unit cells
AU - Takeuchi, Fumihito
AU - Hiratsuka, Masaki
AU - Ohmura, Ryo
AU - Alavi, Saman
AU - Sum, Amadeu K.
AU - Yasuoka, Kenji
PY - 2013/3/28
Y1 - 2013/3/28
N2 - 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 kJmol. The total Coulomb potential on a test unit charge placed in the cage center for the minimum energyminimum 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 kJmol, while the potential energy spread increases to values up to 6 kJmol in sH and 15 kJmol 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.
AB - 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 kJmol. The total Coulomb potential on a test unit charge placed in the cage center for the minimum energyminimum 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 kJmol, while the potential energy spread increases to values up to 6 kJmol in sH and 15 kJmol 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.
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U2 - 10.1063/1.4795499
DO - 10.1063/1.4795499
M3 - Article
C2 - 23556733
AN - SCOPUS:84875783121
SN - 0021-9606
VL - 138
JO - Journal of Chemical Physics
JF - Journal of Chemical Physics
IS - 12
M1 - 124504
ER -