Comparison between molecular geometry and harmonic vibrational frequency predictions from CISD[TQ] and CISDTQ wave functions for hydrogen sulfide

1997 ◽  
Vol 107 (24) ◽  
pp. 10616-10619 ◽  
Author(s):  
Brian C. Hoffman ◽  
C. David Sherrill ◽  
Henry F. Schaefer
2020 ◽  
Vol 73 (8) ◽  
pp. 734
Author(s):  
W. A. Monika Madhavi ◽  
Samantha Weerasinghe ◽  
Konstantin I. Momot

Rotational motion of molecules plays an important role in determining NMR spin relaxation properties of liquids. The textbook theory of NMR spin relaxation predominantly uses the assumption that the reorientational dynamics of molecules is described by a continuous time rotational diffusion random walk with a single rotational diffusion coefficient. Previously we and others have shown that reorientation of water molecules on the timescales of picoseconds is not consistent with the Debye rotational-diffusion model. In particular, multiple timescales of molecular reorientation were observed in liquid water. This was attributed to the hydrogen bonding network in water and the consequent presence of collective rearrangements of the molecular network. In order to better understand the origins of the complex reorientational behaviour of water molecules, we carried out molecular dynamics (MD) simulations of a liquid that has a similar molecular geometry to water but does not form hydrogen bonds: hydrogen sulfide. These simulations were carried out at T=208K and p=1 atm (~5K below the boiling point). Ensemble-averaged Legendre polynomial functions of hydrogen sulfide exhibited a Gaussian decay on the sub-picosecond timescale but, unlike water, did not exhibit oscillatory behaviour. We attribute these differences to hydrogen sulfide’s absence of hydrogen bonding.


1989 ◽  
Vol 43 (6) ◽  
pp. 1053-1055 ◽  
Author(s):  
R. A. Nyquist ◽  
T. M. Kirchner ◽  
H. A. Fouchea

Variation in the correlations obtained between electron acceptor number (AN) values for each solvent versus the vC=O frequencies for acetone and tetramethylurea in solution with these solvents suggests that the AN values are not a precise measure of solute/solvent interaction for all solute/solvent systems. Factors such as intermolecular hydrogen bonding between solute and solvent and the differences between molecular geometry of the solutes and solvents most likely account for differences in the solute/solvent interaction for different solutes in the same solvents.


2007 ◽  
Vol 111 (45) ◽  
pp. 11683-11700 ◽  
Author(s):  
Jeffrey P. Merrick ◽  
Damian Moran ◽  
Leo Radom

1983 ◽  
Vol 48 (2) ◽  
pp. 504-510
Author(s):  
Jiří Krechl ◽  
Josef Kuthan

Molecular geometry of ribofuranoses I - VIII has been optimized with respect to all degrees of freedom on the basis of CNDO/2 wave functions. The results obtained are confronted with previous results of partial optimizations.


2013 ◽  
Vol 2013 ◽  
pp. 1-11 ◽  
Author(s):  
Morteza Vahedpour ◽  
Reza Baghary ◽  
Freshte Khalili

Ozone and hydrogen sulfide reaction mechanism including a complex was studied at the B3LYP/6-311++G(3df,3pd) and CCSD/6-311++G(3df,3pd)//B3LYP/6-311++G(3df,3pd) levels of computation. The interaction between sulfur atom of hydrogen sulfide and terminal oxygen atom of ozone produces a stable H2S-O3complex with no barrier. With the decomposition of this complex, four possible product channels have been found. Intrinsic reaction coordinate, topological analyses of atom in molecule, and vibrational frequency calculation have been used to confirm the suggested mechanism. Thermodynamic data atT= 298.15 K and the atmospheric pressure have been calculated. The results show that the production of H2O + SO2is the main reaction channel with ΔG° = −645.84 kJ/mol. Rate constants of H2S + O3reaction show two product channels, SO2 + H2O and HSO + HOO, which compete with each other based on the temperature.


2007 ◽  
Vol 105 (19-22) ◽  
pp. 2597-2605 ◽  
Author(s):  
Z. A. Fekete ◽  
E. A. Hoffmann ◽  
T. Körtvélyesi ◽  
B. Penke

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