Directional preferences of nonbonded atomic contacts with divalent sulfur in terms of its orbital orientations. 2. Sulfur.cntdot..cntdot..cntdot.sulfur interactions and nonspherical shape of sulfur in crystals

1981 ◽  
Vol 103 (2) ◽  
pp. 477-479 ◽  
Author(s):  
T. N. Guru Row ◽  
R. Parthasarathy
1988 ◽  
Vol 53 (9) ◽  
pp. 2023-2054 ◽  
Author(s):  
Milan Randić ◽  
Sonja Nikolić ◽  
Nenad Trinajstić

The conjugated circuits model is applied to heterocycles containing divalent sulfur. A novel parametrization is introduced for 4n + 2 and 4n conjugated circuits containing a single sulfur atom. The relative aromatic stabilities of a number of heterocyclic systems containing divalent sulfur are studied. Comparison is made whenever possible with earlier reported resonance energies of these compounds, obtained by using Huckel MO and SCF π-MO models, and appropriate reference structures. Special attention is given to positional isomers. An explanation of the differences amongst such isomers is given.


Author(s):  
А.И. Грачев

AbstractThe rotation of a spherical particle in a constant electric field (an effect found earlier) has been analyzed. The particle is illuminated to induce the electric dipole moment of the sphere. The dynamics of the rotation effect has been considered in general terms to refine conditions for adiabatic rotation. The features of the particle’s nonadiabatic rotation have been demonstrated with a sphere placed in a medium with an infinitesimal viscosity. It has been shown that the nonadiabatic rotation dynamics to a great extent depends on a relationship between the electrical and photoinduced dipole moments of the sphere. The rotation dynamics of a particle with a slightly nonspherical shape has been briefly analyzed.


2020 ◽  
Vol 118 (3) ◽  
pp. 388a
Author(s):  
Rikhia Ghosh ◽  
Vahid Satarifard ◽  
Andrea Grafmüller ◽  
Reinhard Lipowsky
Keyword(s):  

1975 ◽  
Vol 6 (15) ◽  
pp. no-no
Author(s):  
HIDEKI SAKAI ◽  
TOKIO YAMABE ◽  
HIROSHI KATO ◽  
SHINICHI NAGATA ◽  
KENICHI FUKUI

1945 ◽  
Vol 67 (12) ◽  
pp. 2092-2095 ◽  
Author(s):  
Ralph Mozingo ◽  
Stanton A. Harris ◽  
Donald E. Wolf ◽  
Charles E. Hoffhine ◽  
Nelson R. Easton ◽  
...  
Keyword(s):  

2006 ◽  
Vol 291 (6) ◽  
pp. H3114-H3121 ◽  
Author(s):  
Yichun Sun ◽  
Israel Belenkie ◽  
Jiun-Jr Wang ◽  
John V. Tyberg

Diastolic suction (DS) can be defined as that property of the ventricle by means of which it tends to refill itself during early diastole, independent of any force from the atrium. Although thought to be significant in the left ventricle (LV), DS in the right ventricle (RV) has received little attention, probably because of RV geometry. Our recent LV studies have shown that DS is related to both decreased elastance (i.e., τ, the relaxation time constant) and end-systolic volume (VLVES), thus reconciling the two mechanisms that have been used to explain the concept of DS. We hypothesized that RV DS would similarly depend on τ and VRVES. In six anesthetized open-chest dogs, aortic, RV, right atrial (RA), pulmonary arterial (PA), and RV pericardial pressure, tricuspid velocity, and PA flow were measured. VRVES was calculated by measuring distances between eight ultrasonic crystals. An empirical index of relaxation, τ′, and VRVES were manipulated by volume loading/caval constriction and isoproterenol/esmolol. We calculated the total energy (IW−) of the backward expansion wave generated during RV relaxation and that component causing DS [IW−(DS)]; i.e., the energy remaining after tricuspid valve opening. IW− [IW−(DS) also] was found to be inversely related to τ′ and to VRVES {i.e., IW− = −8.85· e(−0.0423τ′)· e[−0.0665(%VRVES)]}. Thus, as for the LV, the energy of the backward-going wave generated by the RV during relaxation depends on both the rate at which elastance decreases and the completeness of ejection. Despite the thin wall and nonspherical shape of the RV, DS appears to be an important mechanism.


1977 ◽  
Vol 27 (5) ◽  
pp. 1436-1440
Author(s):  
Yu. L. Frolov ◽  
L. M. Sinegovskaya ◽  
N. K. Gusarova ◽  
S. V. Amosova ◽  
B. A. Trofimov

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