The average energy difference method for calculation of line broadening of asymmetric tops

2015 ◽  
Vol 28 (6) ◽  
pp. 503-509 ◽  
Author(s):  
A. S. Dudaryonok ◽  
N. N. Lavrentieva ◽  
Q. Ma
2021 ◽  
Vol 129 (10) ◽  
pp. 1244
Author(s):  
Н.Н. Лаврентьева ◽  
А.С. Дударёнок

The averaged energy difference method has been applied to calculate the broadening coefficients of rotation vibration water vapor lines induced by helium pressure. The calculations have been performed for a wide range of rotational quantum numbers (the averaged energy difference method have been applied for J from 0 to 20, interpolation of the J-dependence have been used for J from 20 to 50) in the spectral range from 500 to 10000 cm-1. We compared the calculated H2O-He line broadening coefficients with the literature data, and a good agreement have been obtained. The temperature dependence for linewidths are calculated.


2006 ◽  
Vol 317-318 ◽  
pp. 683-688
Author(s):  
Fumihiro Wakai ◽  
Yutaka Shinoda ◽  
Takashi Akatsu

The sintering stress is related to the thermal stability of porous structure. The sintering stress for a given porous structure in equilibrium can be calculated by three methods theoretically; the energy difference method, the curvature method, and the force balance method. The sintering stresses by three different methods were exactly the same for the idealized porous materials in equilibrium, in which the pore surface had a constant curvature at any point. The porous material does not spontaneously shrink when the sintering stress becomes zero or negative. The sintering stress will be used to design optimal porous structures with improved thermal stability.


Molecules ◽  
2018 ◽  
Vol 23 (12) ◽  
pp. 3308 ◽  
Author(s):  
Giovanni La Penna ◽  
Fabrizio Machetti

Proton transfer in water involving C–H bonds is a challenge and nitro compounds have been studied for many years as good examples. The effect of substituents on acidity of protons geminal to the nitro group is exploited here with new p K a measurements and electronic structure models, the latter including explicit water environment. Substituents with the amide moiety display an exceptional combination of acidity and solubility in water. In order to find a rationale for the unexpected p K a changes in the (ZZ ′ )NCO- substituents, we measured and modeled the p K a with Z=Z ′ =H and Z=Z ′ =methyl. The dominant contribution to the observed p K a can be understood with advanced computational experiments, where the geminal proton is smoothly moved to the solvent bath. These models, mostly based on density-functional theory (DFT), include the explicit solvent (water) and statistical thermal fluctuations. As a first approximation, the change of p K a can be correlated with the average energy difference between the two tautomeric forms (aci and nitro, respectively). The contribution of the solvent molecules interacting with the solute to the proton transfer mechanism is made evident.


2018 ◽  
Vol 62 ◽  
pp. 02010
Author(s):  
Anna S. Dudaryonok ◽  
Nina N. Lavrentieva ◽  
Nikolai A. Lavrentiev

Calculations of the CO2-broadening coefficients of sulfur oxide lines by the semi-empirical method [Mol. Phys. 102 (2004) 1653] and averaged energy difference method [Atmosph. Ocean. Optics 28 (2015) 403] are presented. In this work, 41 lines are considered, the rotational quantum number J varies from 14 to 51. Calculations of the line widths are carried out for room temperature (296 K), and also for the temperature range typical for the Ears atmosphere. There is good agreement with the literature data. The carbon dioxide lines broadening coefficients induced by nitrogen, nitrogen oxide, carbon monoxide and carbon dioxide at room temperature (T = 296 K) are obtained for a wide range of the rotational quantum number J (up to 100). The temperature exponents are calculated for every line widths. The calculations were performed by a semi-empirical method, based on the semiclassical impact theory of line broadening and modified by introducing additional correction factor whose parameters can be determined by fitting the broadening or shifting coefficients to the experimental data.


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