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Laboratory and field comparison of measurements obtained using the available diffusive samplers for ozone and nitrogen dioxide in ambient air.

This study presents an evaluation of the extent of differences between measurements performed by O(3) and NO(2) diffusive samplers and by the reference methods for diffusive samplers commercially available. The tests were performed in an exposure chamber under extreme conditions of controlling factors and under field conditions. For NO(2), the results of the laboratory experiments showed that most of the diffusive samplers were affected by extreme exposure conditions. The agreement between the samplers and the reference method was better for the field tests than for the laboratory ones. The estimate of the uptake rate for the exposure conditions using a model equation improved the agreement between the diffusive samplers and the reference methods. The agreement between O(3) measured by the diffusive samplers and by the reference method was satisfactory for 1-week exposure. For 8-hour exposures, the diffusive samplers with high uptake rates quantified better the O(3) concentration than the samplers with low uptake rates. As for NO(2), the results of the O(3) field tests were in better agreement with the reference method than the ones of the laboratory tests. The field tests showed that the majority of diffusive samplers fulfils the 25% uncertainty requirement of the NO(2) European Directive and the 30% uncertainty requirement of the O(3) European Directive for 1-week exposure.

Air Pollutants↗

Fast grain boundary diffusion and surface exchange reactions at active surface sites of polycrystalline materials.

Analytical solutions to the diffusion equations for fast grain boundary diffusion and surface exchange reactions at active surface sites are derived. The microstructure of the polycrystalline sample of finite thickness is modelled by parallel grain boundaries. The ratio between the surface exchange coefficient and the diffusion coefficient for the grain boundaries is assumed to be greater than or equal to that for the bulk. The analytical solutions allow the calculation of diffusion profiles for thin films. Special emphasis is laid on a detailed analysis of the time dependence of the total amount of diffusant exchanged between the constant diffusion source (e.g. gas phase) and the polycrystalline sample (e.g. oxide ceramics) which corresponds to relaxation curves obtained from, e.g., oxygen exchange measurements. The calculated relaxation curves refer to Harrison's type-A kinetics where homogeneous medium solutions are satisfactorily applicable, introducing effective kinetic parameters. Apart from expressions for the effective diffusion coefficient analogous relations for the effective surface exchange coefficient are proposed, depending on the microstructure of the polycrystalline material and the corresponding kinetic parameters of bulk and grain boundary regions, respectively.

Ceramics↗

Changes in diffusion through the brain extracellular space.

ECS (extracellular space) works as the microenvironment of brain cells. Diffusion through ECS may be described through an effective diffusion coefficient, D (e), which in turn depends on ECS porosity, epsilon, and tortuosity, T. In the present research, diffusion data together with epsilon and T were collected from the specialized literature and analysed to seek a correlation of T versus epsilon. On the basis of D (e) data, upper and lower T boundaries were defined and related to topologically 'dense' and 'loose' cell arrangement. A possible range for T variation was obtained for ECS, with epsilon ranging from 0.05 to 0.6. A tortuosity index ( n ) in the form of T and epsilon logarithmic ratio was introduced. This index may be adopted for recalculation of T or epsilon if only one of these parameters is known. As a result of data analysis and modelling, it was concluded that, upon different external conditions, for instance oxygen depletion, the ECS porosity decreases and cells (presumably through membrane rearrangements) adjust the void space to keep the diffusion within a defined range, which gives the living tissue the ability to maintain the diffusion level up to two or more times higher than in conventional granular bed packing. Thus, even with a dramatic ECS decrease, the cellular system is still able to support a given diffusion by decreasing the value of T. The obtained results clearly show the existence of three data clusters: a region of normal brain functioning, both for young and adult brains, for values of epsilon comprised between 0.15 and 0.30, and two regions of abnormal brain behaviour to the left and to the right of the normal region, corresponding to different states (aging, tumours, anoxia, brain death, etc.). The present approach allows defining the optimal range of epsilon and T to assure the best ECS diffusion efficiency for a specified macromolecule. This might be important in brain clinical treatment.

Animals↗

[Value of diffusion-weighted imaging for diagnosing vertebral metastases due to prostate cancer in comparison to other primary tumors].

PURPOSE: Several publications have reported that the apparent diffusion coefficient is generally lower in metastatically affected vertebrae. Therefore, metastases are represented in diffusion-weighted images by increased signal intensity in comparison to unaffected vertebrae. However, there were indications that metastases due to prostate cancer may differ from this. Therefore, the contrast behavior of vertebral metastases due to prostate cancer or tumors with another histology are to be systematically studied using diffusion-weighted images. The present study is intended to examine whether the two groups differed and whether possible differences depended on the degree of sclerosis. MATERIALS AND METHOD: In a retrospective study the vertebral metastases of patients with prostate cancer (n = 18) were compared to those of patients with tumors of another histology (n = 20). A steady-state free precession sequence was used for the diffusion-weighted imaging. Additionally, a T1 weighted sequence before and after administration of contrast agent as well as a fat suppressed T2 weighted sequence were performed. The contrast behavior of the metastases was evaluated for all four sequences and was compared to that of the unaffected parts of the vertebra. RESULTS: In 18 patients of the tumor group, the vertebral metastases showed positive contrast in the diffusion-weighted images, and 2 had minimally negative contrast up to - 0.04. In the prostate cancer group, the contrast was positive in 9 patients and negative in 9. 6 of the metastases with negative contrast had an osteoblastic metastasization, 1 had an osteolysis, and 1 had a normal finding in the conventional X-ray image. Between the tumor group and the prostate cancer group, the medians of the contrasts were not significantly different (p = 0.054). CONCLUSION: In general, the metastatically affected vertebrae appear hyperintense in the diffusion-weighted images. This observation is only true for some vertebral metastases due to prostate cancer. The cause for this seems to be the degree of sclerosis of the metastases. Thus, it cannot be generally deduced from the hypointensity in diffusion-weighted images that a lesion is benign.

Bone Marrow↗

Influence of exercise intensity and duration on post-exercise pulmonary diffusion capacity.

Pulmonary diffusion capacity has been observed to be reduced by approximately 14% 2h after 4-6 min of maximal exercise. The purpose of this study was to determine if the decrease in pulmonary diffusion capacity also occurs when the duration of exercise intensity is shorter or when the exercise intensity is lower. We measured pulmonary diffusion capacity using the single breath method in 12 competitive rowers 22 (16-31) years old, 70 (56-100) kg body weight, and 180 (171-193) cm body height under two conditions: (1) 2h after 6 min of rowing at both 61% (58%-68%) and 76% (73%-78%) of maximal oxygen uptake; (2) 2h after 1, 2, or 3 min of all-out rowing. Values are presented as medians with ranges. Pulmonary diffusion capacity was reduced by 6% (2%-17%) after 6 min of rowing at 61% and by 10% (-7%-21%) after 6 min of rowing at 76% of maximal oxygen uptake (p < 0.03). Pulmonary diffusion capacity was reduced by 7% (3%-19%), 8% (2%-17%) and 7% (1%-16%) after 1, 2, and 3 min of all-out rowing (p < 0.01). We conclude that submaximal exercise at 61% of maximal oxygen uptake will affect pulmonary diffusion capacity following exercise as will shorter duration of maximal exercise. Although the mechanism for this fall in pulmonary diffusion capacity is unclear, the fact that it occurs after even mild exercise makes a significant change in pulmonary capillary membrane integrity or subclinical pulmonary edema unlikely.(ABSTRACT TRUNCATED AT 250 WORDS)

Adolescent↗

Anisotropic diffusion of n-butane and n-decane on a stepped metal surface.

The diffusion of single n-butane and n-decane molecules on a model stepped surface, Pt655, and on a corresponding flat surface, Pt111, is investigated using molecular-dynamics simulations and anisotropic united atom model. The surface step on Pt655 causes the alkane molecules to adsorb on the lower terrace in all-trans conformations with their long molecular axes adjacent and parallel to the step edge, and to diffuse anisotropically along the surface step via a constant wiggly motion without rotation or marked deviation from the parallel adsorption configuration. At relatively high temperatures, the alkane molecules can temporarily break away from the step edge but cannot migrate across the step edge in either the downstair or upstair direction. In comparison with the diffusion on Pt111, the diffusivity of n-decane is reduced by the surface step but its diffusion barrier is hardly affected. In the case of the shorter n-butane, however, the surface step significantly reduces the diffusion energy barrier and gives rise to higher diffusion coefficients at lower temperatures. Important implications of the simulation results are discussed.

Adsorption↗

Concentrations of glycolytic enzymes and other cytosolic proteins in the diffusible fraction of a vertebrate muscle proteome.

We used a novel microvolumetric technique based on protein diffusion to characterize the subproteome of muscle that consists of diffusible proteins, including those involved in cell metabolism. Muscle fiber segments were mechanically demembranated under mineral oil and transferred into drops of relaxing solution. After the fiber segment was depleted of diffusible proteins, the content of each drop and residual segment was analyzed by one-dimensional polyacrylamide gel electrophoresis. Proteins were identified through peptide mass fingerprinting and quantified using purified protein standards. Ten of the most abundant cytosolic proteins, distinguished by their ability to readily diffuse out of the skinned fiber, were glycolytic enzymes whose concentrations ranged from 2.6+/-1.0 g liter-1 (phosphoglucose isomerase) to 12.8+/-1.1 g liter-1 fiber volume (pyruvate kinase). The concentrations of the other five most abundant cytosolic proteins were as follows: glycogen phosphorylase, 6.0+/-2.3 g liter-1; phosphoglucose mutase, 2.2+/-0.2 g liter-1; adenylate kinase, 1.6+/-1.3 g liter-1; phosphocreatine kinase, 6.6+/-2.6 g liter-1; and parvalbumin, 0.7+/-0.4 g liter-1. Given the molecular weight and subunit number of each enzyme, the combined concentration of the 15 most abundant cytosolic proteins was 82.3 g liter-1; the volume fraction was 0.093. The large volume fraction of diffusible proteins favors nonspecific interactions and associations, particularly if the glycolytic enzymes and diffusible phosphocreatine kinase are restricted to the I-band as previous studies suggest. The relative molar concentration of glycolytic enzymes is roughly consistent with a stoichiometry of 1:2 for enzymes catalyzing the hexose and triose sugar reactions, respectively, a stoichiometry that may favor metabolic channeling of intermediates during glycolysis. Our results indicate that subcellular fractionation of muscle proteins, in which cytosolic constituents are distinguished by their ability to diffuse readily from demembranated cells, is a promising microvolumetric technique that allows conclusions to be drawn about native protein-protein interactions based on concentration and stoichiometry.

Animals↗

Diffusion coefficients of retinoids.

PURPOSE: Diffusion coefficients of various retinoids have not been measured previously. It is important to know the diffusion coefficients of the retinoids because this property might be rate-limiting in dark adaptation. Also, retinoid diffusion is important to explore given that rhodopsin regeneration is not impaired in IRBP knockout mice. METHODS: Measurements of lateral diffusion coefficients (D) of 9-cis-retinal, all-trans-retinal, and all-trans-retinol were made by Fourier transform pulsed-gradient spin-echo NMR measurements (FT-PGSE NMR) in several solvents. Also,(3)H-all-trans-retinoic acid was used to measure diffusion from an aqueous agarose matrix and absorption into a toluene based scintillation fluid in a biphase assay. RESULTS: In a 1:1 mixture of CD(3)OD:D(2)O the D's of the retinoids were, 2.4 to 3.0 x 10(-6)cm( 2)/s. In the biphase assay,(3)H-all trans-retinoic acid exhibited a diffusion coefficient of 2.3 x 10(-6)cm(2)/s. CONCLUSIONS: The lower than expected D for retinoids and our calculations suggest that mechanisms in addition to pure aqueous diffusion may be needed to account for normal rhodopsin regeneration rates in the mammalian retina.

Absorption↗

The effects of diffusion and viscosity on ruminant faecal excretion of markers in a simple compartmental model.

Using equations obtained in a previous analysis, results are computed numerically which illustrate the effects of diffusion and viscosity on faecal excretion patterns of markers in ruminants. Results are first given for plug flow, a velocity gradient produced by viscosity, and diffusion, each mechanism operating alone. Plug flow gives a period during which no marker appears in the faeces, then a sharp increase in faeces marker concentration, followed by rapid washout. A velocity gradient gives a more gradual appearance of marker in the faeces followed by a slower washout. Diffusion alone (although not realistic for ruminant marker kinetics) can give early appearance of marker followed by slow washout. Combining diffusion with a velocity gradient produced by viscosity can give a range of behaviour, depending on the effective diffusion coefficient, D'; an approximate method is used to compute these solutions. Because plug flow with no velocity gradient plus diffusion gives results similar to convective flow with a velocity gradient plus diffusion, we believe it will not be possible to determine the main mechanisms defining marker outflow patterns from observations of marker kinetics alone, and more detailed investigations will be needed. Although estimates of quantities such as mean transit time are unaffected by detailed mechanism, the interpretations of measures such as sigmoidicity, sharpness of the faecal marker concentration v. time curve, and length and nature of the washout tail are highly dependent on mechanism.

Animals↗

In vivo sugar diffusion in the ileal epithelium of spontaneously hypertensive rats.

BACKGROUND: D-glucose absorption, distinguishing between active and diffusive components, was studied in the ileum of spontaneously hypertensive rats (SHR) and their normotensive control Wistar-Kyoto (WKY) rats. Net water transport was also determined. METHODS: A perfusion system in vivo with ileum loops was used, and experiments with phlorizin, phloretin and 2,4,6-triaminopyrimidine (TAP) were performed in order to discriminate between active and diffusive components and between transcellular and paracellular routes. RESULTS: A significant decrease in total D-glucose absorption was found in SHR compared to WKY rats, this reduction being due to a lower SGLT1-mediated component. The effect was not compensated by the total diffusive component, since the phlorizin-insensitive D-glucose absorption did not significantly change between rat strains. However, the diffusive component of D-glucose transport was relatively more important in hypertensive than in normotensive rats. The use of 2,4,6-triaminopyrimidine (TAP), which blocks the transport across the paracellular route, showed that the paracellular diffusion of D-glucose was higher in SHR than in WKY rats. Intestinal net water absorption was not modified between either group of animals, though the presence of phlorizin in the perfusate decreased the ileal water absorption to a greater extent in normotensive rats. CONCLUSION: The observed reduction in D-glucose absorption in vivo in the ileum of SHR was due to a decrease in the SGLT1-active component. Despite the paracellular diffusion of D-glucose being higher in hypertensive than in normotensive rats, the total diffusion component was not high enough to compensate this alteration.

Animals↗

Diffusion-weighted MR imaging of acute cerebral ischemia.

Diffusion-weighted MR imaging has been used in studies on experimental animal models and on patients with acute cerebral ischemia. Compared with CT and conventional MR techniques, diffusion-weighted imaging can provide earlier and more precise detection of the location and the extent of an ischemic lesion during the critical first few hours after the onset of stroke. Quantitative apparent diffusion coefficient (ADC) mapping of the brain water can also be carried out by recording a series of diffusion-weighted images with different amplitudes of the displacement encoding gradients. ADC maps can provide important information about the extra- and intracellular water homeostasis. ADC reduction of the tissue water is one of the early signals of the pathophysiological cascade resulting from ischemic tissue injury. Diffusion MR imaging has become a valuable tool in stroke research. It may also prove a valuable tool in monitoring the efficiency of therapeutic effects in stroke patients. It is our intention to provide an overview of the recent development in this area with emphasis on the diffusion-weighted MR techniques, and to discuss the possible underlying biophysical mechanisms responsible for the contrast of diffusion-weighted imaging.

Acute Disease↗

The development of regionalized lipid diffusibility in the germ cell plasma membrane during spermatogenesis in the mouse.

The lipids and proteins of sperm cells are highly regionalized in their lateral distribution. Fluorescence recovery after photobleaching studies of sperm membrane component lateral diffusibility have shown that the sperm plasma membrane is also highly regionalized in the extents and rates of diffusion of its surface components. These studies have also shown that regionalized changes in lateral diffusibility occur during the differentiative processes of epididymal maturation and capacitation. Unlike mammalian somatic cells, sperm cells exhibit large nondiffusing lipid fractions. In this paper, we will show that both regionalized lipid diffusibility and nondiffusing lipid fractions develop with the morphogenesis of cell shape during spermatogenesis in the mouse. Pachytene spermatocytes and round spermatids show diffusion rates and the nearly complete recoveries (80-90%) typical of mammalian somatic cells. In contrast, stage 10-11 condensing spermatids, testicular spermatozoa, cauda epididymal spermatozoa, as well as the anucleate structures associated with these later stages of spermatogenesis (residual bodies and the cytoplasmic droplets of condensing spermatids and testicular spermatozoa), exhibit large nondiffusing fractions. Both the diffusion rates and diffusing fractions observed on the anterior and posterior regions of the head of stage 10-11 condensing spermatids are the same as the values obtained for these regions on testicular spermatozoa. Possible mechanisms of lipid immobilization and possible physiological implications of this nondiffusing lipid are discussed.

Animals↗

Unconfined lateral diffusion and an estimate of pericellular matrix viscosity revealed by measuring the mobility of gold-tagged lipids.

Nanovid (video-enhanced) microscopy was used to determine whether lateral diffusion in the plasma membrane of colloidal gold-tagged lipid molecules is confined or is unrestricted. Confinement could be produced by domains within the plane of the plasma membrane or by filamentous barriers within the pericellular matrix. Fluorescein-phosphatidylethanolamine (F1-PE), incorporated into the plasma membranes of cultured fibroblasts, epithelial cells and keratocytes, was labeled with 30-nm colloidal gold conjugated to anti-fluorescein (anti-F1). The trajectories of the gold-labeled lipids were used to compute diffusion coefficients (DG) and to test for restricted motion. On the cell lamella, the gold-labeled lipids diffused freely in the plasma membrane. Since the gold must move through the pericellular matrix as the attached lipid diffuses in the plasma membrane, this result suggests that any extensive filamentous barriers in the pericellular matrix are at least 40 nm from the plasma membrane surface. The average diffusion coefficients ranged from 1.1 to 1.7 x 10(-9) cm2/s. These values were lower than the average diffusion coefficients (DF) (5.4 to 9.5 x 10(-9) cm2/s) obtained by FRAP. The lower DG is partially due to the pericellular matrix as demonstrated by the result that heparinase treatment of keratocytes significantly increased DG to 2.8 x 10(-9) cm2/s, but did not affect DF. Pericellular matrix viscosity was estimated from the frictional coefficients computed from DG and DF and ranged from 0.5 to 0.9 poise for untreated cells. Heparinase treatment of keratocytes decreased the apparent viscosity to approximately 0.1 poise. To evaluate the presence of domains or barriers, the trajectories and corresponding mean square displacement (MSD) plots of gold-labeled lipids were compared to the trajectories and MSD plots resulting from computer simulations of random walks within corrals. Based on these comparisons, we conclude that, if there are domains limiting the diffusion of F1-PE, most are larger than 5 microns in diameter.

Animals↗

Lateral diffusion of H-2 antigens on mouse fibroblasts.

We have used fluorescence photobleaching and recovery (FPR) to measure the lateral diffusion of mouse H-2 antigens, labeled with fluorescent Fab fragments, in the membrane of cl 1d fibroblasts. Diffusion coefficients, D, vary more than 20-fold from cell to cell, though they vary no more than twofold when measured at different points on a single cell. The fraction of H-2 antigens mobile, R, also varies from cell to cell, and no lateral diffusion of H-2 antigens can be detected in approximately 20% of the cells examined. Treatment of cells with NaCN + NaF, reducing their levels of ATP reduces the proportion of cells in which no lateral diffusion can be detected. The maximum values of D seen in poisoned cells are less than those in controls. Treatment of cells with the divalent inophore, A23187, greatly increases the proportion of cells in which diffusion of H-2 is rapid, D greater than 2 x 10(-9) cm2 s-1. The data obtained on diffusion by FPR can be replotted in the form of an experiment in which lateral diffusion of H-2 antigens is measured in a population of heterokaryons. There is good agreement between this transformation and actual data on heterokaryons. Thus the two methods appear to measure the same transport process.

Animals↗

Diffusion and regionalization in membranes of maturing ram spermatozoa.

An essential feature of the "fluid mosaic model" (Singer, S. J., and G. L. Nicolson , 1972, Science (Wash. DC)., 175:720-731) of the cell plasma membrane is the ability of membrane lipids and proteins to diffuse laterally in the plane of the membrane. Mammalian sperm are capable of overcoming free random diffusion and restricting specific membrane components, both lipid and protein, to defined regions of the sperm's surface. The patterns of these regionalizations evolve with the processes of sperm differentiation: spermatogenesis, epididymal maturation, and capacitation. We have used the technique of fluorescence recovery after photobleaching to measure the diffusion of the lipid analogue 1,1'- dihexadecyl 3,3,3',3'- tetramethylindocarbocyanine perchlorate ( C16dil ) on the different morphological regions of testicular and ejaculated ram spermatozoa. We have found: (a) that the major morphologically distinct regions (head, midpiece, and tail) of the plasma membrane of both testicular and ejaculated spermatozoa are also physically distinct as measured by C16dil diffusibility; (b) that despite regional differences in diffusibility there is exchange of this lipid analogue by lateral diffusion between the major morphological regions of the plasma membrane; and (c) that epididymal maturation results in changes in C16dil diffusibility in the different regions of the sperm plasma membrane. In particular, the plasma membranes of the anterior and posterior heads become physically distinct.

Animals↗

Diffusion in the aqueous compartment.

Measurements of diffusion of molecules in cells can provide information about cytoplasmic viscosity and structure. In a series of studies electron-spin resonance was used to measure the diffusion of a small spin label in the aqueous cytoplasm of mammalian cells. Translational and rotational motion were determined from the same spectra. Based on measurements made in model systems, it was hypothesized that calculations of the apparent viscosity of the cytoplasm from both rotational and translational motion would distinguish between the effects of viscosity and structure on diffusion. The diffusion constant measured in several cell lines averaged 3.3 X 10(-6) cm2/s. It was greater in growing cells and in cells treated with cytochalasin B than in quiescent cells. The viscosity of the cytoplasm calculated from the translational diffusion constant or the rotational correlation time was 2.0-3.0 centipoise, about two to three times that of the spin label in water. Therefore, over the dimensions measured by the technique, 50-100 A, solvent viscosity appears to be the major determinant of particle movement in cells under physiologic conditions. However, when cells were subjected to hypertonic conditions, the translational motion of the spin label decreased threefold, whereas the rotational motion changed by less than 20%. These data suggest that the decrease in cell volume under hypertonic conditions is accompanied by an increase in cytoplasmic barriers and a decrease in the space between existing cytoplasmic components without a significant increase in viscosity in the aqueous phase. In addition, a comparison of reported diffusion values of a variety of molecules in water and in cells indicates that cytoplasmic structure plays an important role in the diffusion of proteins such as bovine serum albumin.

Animals↗

Lateral diffusion of an 80,000-dalton glycoprotein in the plasma membrane of murine fibroblasts: relationships to cell structure and function.

The lateral diffusion of an 80,000-dalton major cell surface glycoprotein of murine fibroblasts has been measured. This antigen, identified through the use of monoclonal antibodies, is an integral glycoprotein distributed through the plasma membrane as judged by immunofluorescence and immunoelectron microscopy (see preceding paper). Measurements of fluorescence recovery after photobleaching were performed on the antigen-antibody complex within the plasma membrane of C3H/10T1/2 and NIH/3T3 cells after labeling the monoclonal antibody with fluorescein. Measurements were performed as a function of temperature, for interphase, mitotic, and G0 C3H/10T1/2 cells. The mean lateral diffusion coefficients (D) for the antibody-protein complex in interphase cells were in the range of 0.7-3.5 X 10(-10) cm2/s between 9 degrees and 37 degrees C, while that for the lipid analog probe, dihexadecylindocarbocyanine was about two orders of magnitude greater. This comparison indicates that peripheral interactions other than bilayer fluidity limit the lateral mobility of the antigen. The mobile fraction of mitotic, G0, and interphase cells showed a monotonic increase with temperature with most of the antibody-antigen complexes being free to move about 25 degrees C. Semi-quantitative interpretations of both the slow glycoprotein diffusion and the immobile fraction are offered. Comparison of diffusion coefficients for cells in different phases of the cell cycle does not reveal striking differences. Mobile fractions for G0 cells at 25 degrees C or less are substantially lower than in interphase cells. In all cases, there was a remarkably broad range of the fluorescence recovery data between different cells, resulting in up to a 10-fold variation in diffusion coefficients, which is far greater than the precision limits of the experiment. Diffusion values and mobile fractions were generally well within a factor of two when measured at several arbitrary points on a single cell. The origins of this cellular heterogenity remain to be elucidated. Lateral mobility in cell fragments and specific regions of single cells was also examined. The glycoprotein was mobile in ventral surface cell fragments. Its mobility was not altered in regions of cell-cell underlapping. However, the diffusion coefficient was threefold higher near the leading edge of motile cells compared to the trailing region. This difference may reflect weaker coupling of the glycoprotein to the underlying cytoskeleton in the dynamic leading edge region.

Animals↗

Diffusion of water in cat ventricular myocardium.

The rates of diffusion of tritiated water (THO) and [14C]sucrose across cat right ventricular myocardium were studied at 23 degrees C in an Ussing-type diffusion cell, recording the time-course of increase in concentration of tracer in one chamber over 4--6 h after adding tracers to the other. Sucrose data were fitted with a model for a homogeneous sheet of uneven thickness in which the tissue is considered to be an array of parallel independent pathways (parallel pathway model) of varying length. The volume of the sucrose diffusion space, presumably a wholly extracellular pathway, was 23% of the tissue or 27.4 +/-1.7% (mean +/- SEM; n=11) of the tissue water. The effective intramyocardial sucrose diffusion coefficient, D8, was 1.51 +/- 0.19 X 10(-6)cm2.s-1 (n=11). Combining these data with earlier data, D8 was 22.6 +/- 1.1% (n=95) of the free diffusion coefficient in aqueous solution D degrees 8. The parallel pathway model and a dead-end pore model, which might have accounted for intracellular sequestration of water, gave estimates of DW/D degrees W (observed/free) of 15%. Because hindrance to water diffusion must be less than for sucrose (where D8/D degrees 8=22.6%), this showed the inadequacy of these models to account simultaneously for the diffusional resistance and the tissue water content. The third or cell-matrix model, a heterogeneous system of permeable cells arrayed in the extracellular matrix, allowed logical and geometrically reasonable interpretations of the steady-state data and implied estimates of DW in the cellular and extracellular fluid of approximately 25% of the aqueous diffusion coefficient.

Animals↗