scholarly journals Intra-erythrocyte microviscosity and diffusion of specifically labelled [glycyl-α-13C]glutathione by using 13 C n.m.r.

1983 ◽  
Vol 216 (3) ◽  
pp. 655-660 ◽  
Author(s):  
Z H Endre ◽  
B E Chapman ◽  
P W Kuchel

[alpha-13C]Glycine was incubated with suspensions of human erythrocytes under special buffer conditions to enrich specifically intracellular glutathione with 13C. The metabolically active cells were then subjected to 13C n.m.r. spectroscopy in which the longitudinal relaxation time(s) (T1) and nuclear Overhauser enhancement(s) of the free glycine and glutathione were measured. With the appropriate analysis, assuming the molecules to be isotropic rotors, intracellular rotational correlation times were calculated. Using these data together with the Stokes-Einstein equation, viscosity and translational diffusion coefficients were calculated. The results were compared with those from cell lysates and extracts. The cytosolic microviscosity probed by glutathione was only 1.9 +/- 0.3 times that of saline, suggesting, therefore, that most enzyme reactions involving this solute are not likely to be diffusion-controlled inside the erythrocyte.

Author(s):  
Boris Gordeychik ◽  
Tatiana Churikova ◽  
Thomas Shea ◽  
Andreas Kronz ◽  
Alexander Simakin ◽  
...  

Abstract Nickel is a strongly compatible element in olivine, and thus fractional crystallization of olivine typically results in a concave-up trend on a Fo–Ni diagram. ‘Ni-enriched’ olivine compositions are considered those that fall above such a crystallization trend. To explain Ni-enriched olivine crystals, we develop a set of theoretical and computational models to describe how primitive olivine phenocrysts from a parent (high-Mg, high-Ni) basalt re-equilibrate with an evolved (low-Mg, low-Ni) melt through diffusion. These models describe the progressive loss of Fo and Ni in olivine cores during protracted diffusion for various crystal shapes and different relative diffusivities for Ni and Fe–Mg. In the case when the diffusivity of Ni is lower than that for Fe–Mg interdiffusion, then olivine phenocrysts affected by protracted diffusion form a concave-down trend that contrasts with the concave-up crystallization trend. Models for different simple geometries show that the concavity of the diffusion trend does not depend on the size of the crystals and only weakly depends on their shape. We also find that the effect of diffusion anisotropy on trend concavity is of the same magnitude as the effect of crystal shape. Thus, both diffusion anisotropy and crystal shape do not significantly change the concave-down diffusion trend. Three-dimensional numerical diffusion models using a range of more complex, realistic olivine morphologies with anisotropy corroborate this conclusion. Thus, the curvature of the concave-down diffusion trend is mainly determined by the ratio of Ni and Fe–Mg diffusion coefficients. The initial and final points of the diffusion trend are in turn determined by the compositional contrast between mafic and more evolved melts that have mixed to cause disequilibrium between olivine cores and surrounding melt. We present several examples of measurements on olivine from arc basalts from Kamchatka, and published olivine datasets from mafic magmas from non-subduction settings (lamproites and kimberlites) that are consistent with diffusion-controlled Fo–Ni behaviour. In each case the ratio of Ni and Fe–Mg diffusion coefficients is indicated to be <1. These examples show that crystallization and diffusion can be distinguished by concave-up and concave-down trends in Fo–Ni diagrams.


The electron-nuclear Overhauser effect at two magnetic fields has been investigated for solutions of 2, 4, 6-tri- tert . -butyl phenoxy radical in several protonated and fluorinated organic solvents. In some cases the enhancement of the nuclear resonance is positive in sign, and the results have been interpreted in terms of the theory of Hubbard (1966) in which both dipolar and scalar interactions between the electrons and nuclei are considered. Hubbard assumes two models for the scalar interaction which he calls the sticking and diffusion models. The experimental results may be best explained in terms of the diffusion model. The theory permits calculation of the diffusional correlation times, distances of closest approach of the nuclei to the electrons, and relative diffusion coefficients of the solvent and radical molecules. Reasonable values are obtained for the systems investigated.


2014 ◽  
Vol 43 (6-7) ◽  
pp. 331-339 ◽  
Author(s):  
Shenggen Yao ◽  
Daniel K. Weber ◽  
Frances Separovic ◽  
David W. Keizer

2004 ◽  
Vol 03 (01) ◽  
pp. 69-90 ◽  
Author(s):  
BEHZAD HAGHIGHI ◽  
ALIREZA HASSANI DJAVANMARDI ◽  
MOHAMAD MEHDI PAPARI ◽  
MOHSEN NAJAFI

Viscosity and diffusion coefficients for five equimolar binary gas mixtures of SF 6 with O 2, CO 2, CF 4, N 2 and CH 4 gases are determined from the extended principle of corresponding states of viscosity by the inversion technique. The Lennard–Jones 12-6 (LJ 12-6) potential energy function is used as the initial model potential required by the technique. The obtained interaction potential energies from the inversion procedure reproduce viscosity within 1% and diffusion coefficients within 5%.


2008 ◽  
Vol 40 (02) ◽  
pp. 529-547
Author(s):  
Francisco J. Piera ◽  
Ravi R. Mazumdar ◽  
Fabrice M. Guillemin

In this paper we consider reflected diffusions with positive and negative jumps, constrained to lie in the nonnegative orthant of ℝ n . We allow for the drift and diffusion coefficients, as well as for the directions of reflection, to be random fields over time and space. We provide a boundary behavior characterization, generalizing known results in the nonrandom coefficients and constant directions of the reflection case. In particular, the regulator processes are related to semimartingale local times at the boundaries, and they are shown not to charge the times the process expends at the intersection of boundary faces. Using the boundary results, we extend the conditions for product-form distributions in the stationary regime to the case when the drift and diffusion coefficients, as well as the directions of reflection, are random fields over space.


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