On the π-Donating Abilities of Sulfur and Oxygen. A Comparative Quantum Chemical Investigation of the Static and Dynamic Properties and Gas Phase Acidities of and

1975 ◽  
Vol 53 (8) ◽  
pp. 1144-1153 ◽  
Author(s):  
Fernando Bernardi ◽  
Imre G. Csizmadia ◽  
H. Bernhard Schlegel ◽  
Saul Wolfe

Nonempirical SCF-MO computations have been performed on CH2O, CH2S, and their protonated derivatives [Formula: see text] and [Formula: see text]. The methylene group of CH2O is strongly positive and that of CH2S is slightly negative, because oxygen in CH2O behaves towards carbon as a π-donor and σ-acceptor, but sulfur in CH2S behaves as both a π- and σ-donor. The total π-overlap in CH2O is greater than that in CH2S.The stable conformations of [Formula: see text] and [Formula: see text] correspond in each case to a structure in which all atoms lie in the same plane. In this conformation, both the C—O and C—S bond lengths are substantially shorter than those of methanol and methanethiol, indicative of conjugative interaction between the cationic center and the adjacent heteroatom. From the results of a Mulliken-type population analysis it is found that, relative to hydrogen, OH and SH behave towards an adjacent [Formula: see text] group as electron-withdrawing and electron-releasing ligands, respectively. When [Formula: see text] is considered to form from [Formula: see text] and OH fragments, π-donation from O to C amounts to 0.38 electron, but σ-donation in the opposite direction amounts to 0.35 electron; the π-overlap population is 0.1496. A similar analysis of [Formula: see text] reveals π- and σ-donation from S to C of 0.53 and 0.15 electron, respectively, and a π-overlap population of 0.1734, so that sulfurformsastronger π-bondtotheadjacentcationiccenter.Geometrical isomerization of [Formula: see text] proceeds by linear inversion at oxygen, with a barrier of 13.98 kcal/mol; but that of [Formula: see text] proceeds by rotation about the C—S bond, with a barrier of 36.47 kcal/mol. This latter value is substantially higher than that (23 kcal/mol ) computed for [Formula: see text] with a rigid rotor model, and reflects the greater strength of the π-bond between sulfur and the adjacent cationic center.

2019 ◽  
Author(s):  
Javad Noroozi ◽  
William Smith

We use molecular dynamics free energy simulations in conjunction with quantum chemical calculations of gas phase reaction free energy to predict alkanolamines pka values. <br>


Molecules ◽  
2020 ◽  
Vol 25 (17) ◽  
pp. 3963
Author(s):  
Jizhou Wu ◽  
Jie Ma ◽  
Yuqing Li ◽  
Wenliang Liu ◽  
Peng Li ◽  
...  

This article demonstrates new observation of the high-resolution ro-vibrational bichromatic photoassociation spectra (BPAS) of Cs2 in the 0u+ long-range state below the asymptotes 6S1/2 + 6P1/2. By combining with a modulation spectroscopic technique, precise references of the frequency differences have been engineered through the BPAS, with which the rotational constants of low-lying vibrational levels of the Cs20u+ long-range state have been accurately determined by fitting the frequency differences to the non-rigid-rotor model. The rotational constants for the newly observed seven ro-vibrational levels are summarized and disagreement for the level ῦ = 498 is clarified. The rotational constants of different vibrational levels demonstrate strong perturbations of the related energy structures. A simple analysis is performed and shows good agreement with experimental results.


2021 ◽  
pp. 1-24
Author(s):  
Gudeta Berhanu Benti ◽  
David Jose Rondon ◽  
Rolf Gustavsson ◽  
Jan-Olov Aidanpää

Abstract In this paper, the dynamics of tilting pad journal bearings with four and eight pads are studied and compared experimentally and numerically. The experiments are performed on a rigid vertical rotor supported by two identical bearings. Two sets of experiments are carried out under similar test setup. One set is performed on a rigid rotor with two four-pad bearings, while the other is on a rigid rotor with two eight-pad bearings. The dynamic properties of the two bearing types are compared with each other by studying the unbalance response of the system at different rotor speeds. Numerically, the test rig is modeled as a rigid rotor and the bearing coefficients are calculated based on Navier-Stokes equation. A nonlinear bearing model is developed and used in the steady state response simulation. The measured and simulated displacement and force orbits show similar patterns for both bearing types. Compared to the measurement, the simulated mean value and range (peak-to-peak amplitude) of the bearing force deviate with a maximum of 16 % and 38 %, respectively. It is concluded that, unlike the eight-pad TPJB, the four-pad TPJB excite the system at the third and fifth-order frequencies, which are due to the number of pads, and the amplitudes of these frequencies increase with the rotor speed.


2014 ◽  
Vol 554 ◽  
pp. 170-174 ◽  
Author(s):  
Ken Tokunaga ◽  
Shigekazu Ohmori ◽  
Hiroshi Kawabata

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