Structural mechanisms in the abolishment of VEGF-induced microvascular hyperpermeability by cAMP

To investigate the structural mechanisms by which elevation of the intraendothelial cAMP levels abolishes or attenuates the transient increase in microvascular permeability by vascular endothelial growth factor (VEGF), we examined cAMP effect on VEGF-induced hyperpermeability to small solute sodium fluorescein (Stokes radius = 0.45 nm) P(sodium fluorescein), intermediate-sized solute alpha-lactalbumin (Stokes radius = 2.01 nm) P(alpha-lactalbumin), and large solute albumin (BSA, Stokes radius = 3.5 nm) P(BSA) on individually perfused microvessels of frog mesenteries. After 20 min pretreatment of 2 mM cAMP analog, 8-bromo-cAMP, the initial increase by 1 nM VEGF was completely abolished in P(sodium fluorescein) (from a peak increase of 2.6+/-0.37 times control with VEGF alone to 0.96+/-0.07 times control with VEGF and cAMP), in P(alpha-lactalbumin) (from a peak increase of 2.7+/-0.33 times control with VEGF alone to 0.76+/-0.07 times control with VEGF and cAMP), and in P(BSA) (from a peak increase of 6.5+/-1.0 times control with VEGF alone to 0.97+/-0.08 times control with VEGF and cAMP). Based on these measured data, the prediction from our mathematical models suggested that the increase in the number of tight junction strands in the cleft between endothelial cells forming the microvessel wall is one of the mechanisms for the abolishment of VEGF-induced hyperpermeability by cAMP.     

Structural mechanisms of acute VEGF effect on microvessel permeability

To investigate the ultrastructural mechanisms of acute microvessel hyperpermeability by vascular endothelial growth factor (VEGF), we combined a mathematical model (J Biomech Eng 116: 502-513, 1994) with experimental data of the effect of VEGF on microvessel hydraulic conductivity (L(p)) and permeability of various-sized solutes. We examined the effect of VEGF on microvessel permeability to a small solute (sodium fluorescein, Stokes radius 0.45 nm), an intermediate solute (alpha-lactalbumin, Stokes radius 2.01 nm), and a large solute [albumin (BSA), Stokes radius 3.5 nm]. Exposure to 1 nM VEGF transiently increased apparent permeability to 2.3, 3.3, and 6.2 times their baseline values for sodium fluorescein, alpha-lactalbumin, and BSA, respectively, within 30 s, and all returned to control within 2 min. On the basis of L(p) (DO Bates and FE Curry. Am J Physiol Heart Circ Physiol 271: H2520-H2528, 1996) and permeability data, the prediction from the model suggested that the most likely structural changes in the interendothelial cleft induced by VEGF would be a approximately 2.5-fold increase in its opening width and partial degradation of the surface glycocalyx.     

Lack of effect of rat atrial natriuretic factor (rANF) on the renal function in frogs

1. The aim of the present experiments was to examine the question whether the rat atrial natriuretic factor (rANF 1-28) could alter the fractional excretion of sodium (FENa) and other solutes in the frog (Rana esculenta). 2. Although experiments were performed throughout the year possible seasonal changes in the animals were considered in particular. 3. In all frogs, a hypotonic diuresis was induced. 4. Under these conditions in winter frogs, the control FENa was 8.8 +/- 5.8% (15) [means +/- SD (n)], and during rANF administration 7.7 +/- 6.6% (13) (NS). 5. In summer frogs, the control and experimental FENa was 5.2 +/- 2.8% (5) and 6.0 +/- 2.5% (5), respectively (NS). 6. These results show that there was no significant effect of this polypeptide on the fractional excretion of sodium in the frog.     

Diffusion profiles of Na+-fluorescein in frog ventricular muscle.

Frog ventricular muscle strips were placed in a single sucrose-gap chamber to measure the interdiffusion of solutes across the sucrose-Ringer's solution partition. Steady-state diffusion profiles of fluorescein sodium developed along the axis of the muscle in the physiological node by continuously perfusing the sucrose pool with 210-mM sucrose plus fluorescein (5-10 mM). Fluorescein was found to diffuse freely through the extracellular space of the ventricular muscle without binding to the tissue. The fluorescence of Na+-fluorescein in the muscle (measured at 530 +/- 30 nm) varied linearly with the dye concentration in the sucrose perfusate. The diffusion profiles of dye in the test node depended on the tightness or snaring of the muscle strip by the latex diaphragms, the diameter of the muscle strip, and changes in hydrostatic pressure between the sucrose and Ringer's solution pools. Fluorescein concentration in the cross section of test node closest to the latex partition (sucrose-Ringer's solution interface) ranged between 4-13% of the dye concentration in the sucrose pool. These values are more than five times smaller than those estimated theoretically, assuming free diffusion. The experimental findings indicate that the presence of a physical barrier, such as a rubber diaphragm, limits free interdiffusion of solutes across the sucrose gap. The presence of such a barrier thus prevents large concentration gradients from occurring in the extracellular spaces along the physiological node.     

Macromolecule permeability of in situ and excised rodent skeletal muscle arterioles and venules

In microvessels, acute inflammation is typified by an increase in leukocyte-endothelial cell interactions, culminating in leukocyte transmigration into the tissue, and increased permeability to water and solutes, resulting in tissue edema. The goal of this study was to establish a method to quantify solute permeability (P(s)) changes in microvessels in intact predominantly blood-perfused networks in which leukocyte transmigratory behavior could be precisely described using established paradigms. We used intravital confocal microscopy to measure solute (BSA) flux across microvessel walls, hence P(s). A quantitative fluorescence approach (Huxley VH, Curry FE, and Adamson RH. Am J Physiol Heart Circ Physiol 252: H188-H197, 1987) was adapted to the imaged confocal tissue slice in which the fluorescent source volume and source surface area of the microvessel were restricted to the region of vessel that was contained within the imaged confocal tissue section. P(s) measurements were made in intact cremaster muscle microvasculature of anesthetized mice and compared with measurements of P(s) made in isolated rat skeletal muscle microvessels. Mouse arteriolar P(s) was 9.9 +/- 1.1 x 10(-7) cm/s (n = 16), which was not different from 8.4 +/- 1.3 x 10(-7) cm/s (n = 6) in rat arterioles. Values in venules were significantly (P < 0.05) higher: 44.4 +/- 7.9 x 10(-7) cm/s (n = 14) in mice and 25.0 +/- 3.7 x 10(-7) cm/s in rats. Convective coupling was estimated to contribute <10% to the measured P(s) in both microvessel types and both animal models. We conclude that this approach provides an appropriate quantification of P(s) in the intact microvasculature and that arteriolar P(s), while lower than in venules, is nevertheless consistent with arterioles being a significant source of interstitial protein.     

Diffusion and partition of solutes in cartilage under static load

We describe experimental apparatus, methodology and mathematical algorithms to measure diffusion and partition for typical small ionic solutes and inulin (a medium size solute) in statically loaded cartilage. The partition coefficient based on tissue water (K(H(2)O)) of Na(+) increased from 1.8 to 4.5 and for SO(4)(-2) decreased from 0.5 to 0.1, when the applied pressure was raised from zero to 22 atm K(H(2)O) of inulin decreased from 0.3 to 0.05, for an increase in pressure from zero to 11 atm. Our theoretical interpretation of the results is that the partition coefficient can be expressed as a function of fixed charge density (FCD) for both loaded and unloaded cartilage. The partition coefficient shows good agreement with the ideal Gibbs-Donnan equilibrium, particularly when FCD is based on extrafibrillar water (EFW). The diffusion coefficients, D also decreased with an increase in applied pressure; raising the pressure from 0 to 22 atm resulted in the following changes in the values of D: for Na(+) from 2.86 x 10(-6) to 1.51 x 10(-6) cm(2)/s, for SO(4)(-2) from 1.58 x 10(-6) to 7.5 x 10(-7) cm(2)/s, for leucine from 1.69 x 10(-6) to 8.30 x 10(-7) cm(2)/s and for inulin from 1.80 x 10(-7) to 3.30 x 10(-8) cm(2)/s. For the three small solutes (two charged and one neutral) the diffusion coefficient D is highly correlated with the fraction of fluid volume in the tissue. These experimental results show good agreement with the simple model of Mackie and Meares: hence solute charge does not affect the diffusion of small solutes under load. For inulin D & K show some agreement with a modified Ogston model based on two major components, viz., glycosaminoglycans (GAG) and core protein. We conclude that the changes in the partition and diffusion coefficients of small and medium size solutes in statically loaded cartilage can be interpreted as being due to the reduction in hydration and increase in FCD. The change in the latter affects the partition of small ionic solutes and the partition and diffusion of larger molecules. Our results throw light on the ionic environment of chondrocytes in loaded cartilage as well as on the transport of solutes through the matrix.     

An electrodiffusion model for effects of surface glycocalyx layer on microvessel permeability

To investigate the charge effect of the endothelial surface glycocalyx on microvessel permeability, we extended the three-dimensional model developed by Fu et al. (J Biomech Eng 116: 502-513, 1994) for the interendothelial cleft to include a negatively charged glycocalyx layer at the entrance of the cleft. Both electrostatic and steric exclusions on charged solutes were considered within the glycocalyx layer and at the interfaces. Four charge-density profiles were assumed for the glycocalyx layer. Our model indicates that the overall solute permeability across the microvessel wall including the surface glycocalyx layer and the cleft region is independent of the charge-density profiles as long as they have the same maximum value and the same total charge. On the basis of experimental data, this model predicts that the charge density would be 25-35 meq/l in the glycolcalyx of frog mesenteric capillaries. An intriguing prediction of this model is that when the concentrations of cations and anions are unequal in the lumen due to the presence of negatively charged proteins, the negatively charged glycocalyx would provide more resistance to positively charged solutes than to negatively charged ones.     

Effect of Mercurascan on sodium transport in frog skin and bladder

The authors studied the effect of Mercurascan (MSC) (a hydroxy- mercury derivative of fluorescein) on electrical parameters, namely potential difference (P.D.) and short circuit current (S.C.C.) of frog skin and on the ability of frog bladder tissue to accumulate sodium ions in experiments in vitro. It was found that MSC, in 10(-4) mol/l concentration, reduced the S.C.C., after a brief initial increase, to 5% of the original value and that the P.D. fell steadily right from the outset. In 10(-5) mol/l concentration it raised the S.C.C. by 60% and the increase lasted several hours. The P.D. was unaffected. In 10(-7) and 10(-6) mol/l concentration MSC had no effect on the NA+ content of a nonpolarized frog bladder tissue preparation, but a 10(-5) nol/l concentration sharply reduced it. The effect of MSC on membrane Na+--K+ ATPase, i.e. on the energy metabolism of cellular tissue, is discussed with reference to these results.     

Effect of calcitonin on fractional delivery of sodium and solutes to the juxtamedullary end-descending limb of the rat

The purpose of the present studies was to examine, by micropuncture, the effect of salmon calcitonin on fractional sodium and solutes deliveries to the juxtamedullary end-descending limb of the rat. All animals were postprandial and thyroparathyroidectomized Munich-Wistar rats. Group 1 (N = 8) consisted of time control water-diuretic rats; group 2 (N = 8) received synthetic salmon calcitonin (10 mU/min) intravenously while undergoing water diuresis; group 3 (N = 8) was treated as group 2 but also received calcium intravenously to prevent the calcitonin-induced fall in plasma calcium. Calcitonin, alone and with calcium, produced a marked fall in urine flow rate and a marked increase in urinary osmolality. Concomitant fractional water delivery to the end-descending limb fell significantly (28 +/- 0.8 to 21 +/- 1.0%, p less than 0.05), while fractional solute and sodium deliveries increased significantly (36 +/- 1.3 to 55 +/- 2.6%, p less than 0.05; 34 +/- 2.0 to 48 +/- 3.5%, p less than 0.05, respectively). The three groups did not significantly differ in fractional water and sodium deliveries to the superficial end-accessible proximal tubule. We conclude that salmon calcitonin is antidiuretic in the rat and that it also produces an increase in fractional sodium and total solute deliveries to the end-descending limb, which we suggest is due to transepithelial sodium addition. The physiological significance of these observations to water homeostasis in vivo remains to be determined.     

Dynamic loading of immature epiphyseal cartilage pumps nutrients out of vascular canals

The potential influence of mechanical loading on transvascular transport in vascularized soft tissues has not been explored extensively. This experimental investigation introduced and explored the hypothesis that dynamic mechanical loading can pump solutes out of blood vessels and into the surrounding tissue, leading to faster uptake and higher solute concentrations than could otherwise be achieved under unloaded conditions. Immature epiphyseal cartilage was used as a model tissue system, with fluorescein (332 Da), dextran (3, 10, and 70 kDa) and transferrin (80 kDa) as model solutes. Cartilage disks were either dynamically loaded (± 10% compression over a 10% static offset strain, at 0.2 Hz) or maintained unloaded in solution for up to 20 h. Results demonstrated statistically significant solute uptake in dynamically loaded (DL) explants relative to passive diffusion (PD) controls for all solutes except unbound fluorescein, as evidenced by the DL:PD concentration ratios after 20 h (1.0 ± 0.2, 2.4 ± 1.1, 6.1 ± 3.3, 9.0 ± 4.0, and 5.5 ± 1.6 for fluorescein, 3, 10, and 70 kDa dextran, and transferrin). Significant uptake enhancements were also observed within the first 30s of loading. Termination of dynamic loading produced dissipation of enhanced solute uptake back to PD control values. Confocal images confirmed that solute uptake occurred from cartilage canals into their surrounding extracellular matrix. The incidence of this loading-induced transvascular solute pumping mechanism may significantly alter our understanding of the interaction of mechanical loading and tissue metabolism.     

Leukocyte adhesion and microvessel permeability

To investigate the direct effect of leukocyte adherence to microvessel walls on microvessel permeability, we developed a method to measure changes in hydraulic conductivity (L(p)) before and after leukocyte adhesion in individually perfused venular microvessels in frog mesentery. In 19 microvessels that were initially free of leukocyte sticking or rolling along the vessel wall, control L(p) was measured first with Ringer-albumin perfusate. Blood flow was then restored in each vessel with a reduced flow rate in the range of 30-116 microm/s to facilitate leukocyte adhesion. Each vessel was recannulated in 45 min. The mean number of leukocytes adhering to the vessel wall was 237 +/- 22 leukocytes/mm(2). At the same time, L(p) increased to 4.7 +/- 0.5 times the control value. Superfusion of isoproterenol (10 microM) after leukocyte adhesion brought the increased L(p) back to 1.1 +/- 0.2 times the control in 5-10 min (n = 9). Superfusing isoproterenol before leukocyte adhesion prevented the increase in L(p) (n = 6). However, the number of leukocytes adhering to the vessel wall was not significantly affected. These results demonstrated that leukocyte adhesion caused an increase in microvessel permeability that could be prevented or restored by increasing cAMP levels in endothelial cells using isoproterenol. Thus cAMP-dependent mechanisms that regulate inflammatory agent-induced increases in permeability also modulate leukocyte adhesion-induced increases in permeability but act independently of mechanisms that regulate leukocyte adhesion to the microvessel wall. Application of ketotifen, a mast cell stabilizer, and desferrioxamine mesylate, an iron-chelating reagent, attenuated the increase in L(p) induced by leukocyte adhesion, suggesting the involvement of oxidants and the activation of mast cells in leukocyte adhesion-induced permeability increase. Furthermore, with the use of an in vivo silver stain technique, the locations of the adherent leukocytes on the microvessel wall were identified quantitatively in intact microvessels.     

Role of V1- and V2-receptors in mechanism of physiological paradox--an increase of reabsorption of the solute free water and simultaneous rise of diuresis

In experiments on non-anesthetized rats with administration into stomach of water (5 ml/100 g body mass) direct correlation has been found between an increase of diuresis and excretion of solute free water (r = 0.98, p < 0.01), while after injection to these animals of 5 x 10(-11) M arginine-vasotocin - between an increase of diuresis and simultaneous rise reabsorption of solute free water (r = 0.8, p < 0.01). The rise of diuresis after the vasotocin injection is due to inhibition of sodium re- absorption, with the solute excretion fraction increasing from 2.6 +/- 0.2 % to 11.9 +/- 1.2, p < 0.001. A similar physiological paradox - an increase of diuresis with the simultaneous increase of reabsorption of solute free water - has been revealed at night hours in children with tendency for nocturnal enuresis (r = 0.64, p < 0.01). Mechanism responsible for this phenomenon consists in a rise of diuresis due to a decrease of sodium ion reabsorption in the ascending Henle loop limb. A problem is discussed of the homeostatic significance of a decrease of sodium reabsorption combined with an increase of solute-free water reabsorption; it is suggested that this phenomenon is based on a redistribution of reabsorption inside the nephron - a decrease of ion and water reabsorption in the initial parts of the nephron distal segment and an increase of solute free water reabsorption with the antidiuretic hormone-stimulated high osmotic permeability of terminal parts of renal tubules. An intraperitoneal injection of V1-anatagonist (OPC-21268) decreased the natriuretic component of response to arginine-vasotocin, while injection of V2-antagonist (OPC-31260) eliminated the antidiuretic component.     

Physical and kinetic properties of homogenous bovine lens aldose reductase.

Aldose reductase from calf lens was purified 15,000-fold. The homogeneity of the final preparation was demonstrated by molecular sieve chromatography, analytical ultracentrifugation, sodium dodecyl sulfate gel electrophoresis, Ouchterlony immunodiffusion, and polyacrylamide gel electrophoresis at three pH values. The monomeric nature of the enzyme is suggested by the molecular weight of 37,000 from both molecular sieve chromatography and sodium dodecyl sulfate-gel electrophoresis with beta-mercaptoethanol. This closely corresponds with a molecular weight of 40,400 estimated by using calculate physical constants in the Svedberg equation. The S20,w was 3.6 to 3.7 as determined from ultracentrifuge and sucrose density gradient data. The Stokes radius was found to be 2.5 +/- 0.2 nm and 2.75 +/- 0.15 nm by two different methods. The diffusion constant D20,w is (7.8 +/- 10(-7) +/- 0.45 X 10(-7) cm2/s). The molecule is nearly spherical as indicated by a frictional ratio f/fo = 1.14. The alpha-helical content was estimated from circular dichroism data to be 5% and did not change in the presence of added substrates, products, and some enzyme inhibitors. Homotropic cooperative effects were observed as shown by the concave downward curvature of the reciprocal plots.     

Transport of water and solutes across bullfrog alveolar epithelium

Water and solute transport properties of the alveolar epithelium of isolated bullfrog lungs were studied. Lungs from Rana catesbeiana were removed and mounted in an Ussing chamber. Unstirred layers on both sides of the tissue were estimated from the time courses of dilution potential development, and the measured transport parameters were corrected for the effect of the unstirred layers. Spontaneous potential difference, short-circuit current, tissue resistance, instantaneous voltage-current relationships, diffusional permeabilities of water and hydrophilic solutes, and hydraulic conductivities were determined. The hydraulic conductivity obtained from hydrostatically driven water flow anomalously decreased with time, and was initially 100 -1,000 times higher than osmotically determined hydraulic conductivity. The equivalent pore radius of the bullfrog alveolar epithelium was estimated to be 0.8-0.9 nm. We conclude that the alveolar epithelium is extremely tight, presenting a major barrier to water and solute flow. This high resistance to water and solute flow may be helpful in maintaining the alveolar lumen relatively free of fluid under normal physiological conditions.     

Shape and quaternary structure of alpha-globulin from sesame (Sesamum indicum L.) seed as revealed by small angle x-ray scattering and quasi-elastic light scattering

The alpha-globulin from sesame seed has a molar mass of 2.7 X 10(5) g mol-1, determined by x-ray scattering, and (2.8 +/- 0.3) 10(5) g mol-1, determined by quasi-elastic light scattering. The radius of gyration RG amounts to (4.1 +/- 0.1) nm and (3.9 +/- 0.2) nm as determined by Guinier approximation and from the distribution function D(x), respectively. The molecule has a Stokes radius Rs of (5.4 +/- 0.15) nm and a maximum dimension L of (11 less than L less than 15) nm. The translational diffusion coefficient D0(20),w and the ratio of fractional coefficients f/fmin amount to (3.95 +/- 0.12) X 10(-7) cm2 s-1 and 1.25, respectively. The quaternary structure of the protein molecule is approximated by a model consisting of six spherical subunits situated at the vertices of an octahedron having the symmetry 32.     

Structure and function of the Ah receptor for 2,3,7,8-tetrachlorodibenzo-p-dioxin. Species difference in molecular properties of the receptors from mouse and rat hepatic cytosols

Molecular properties of cytosolic Ah receptors from livers of Sprague-Dawley rats and C57BL/6N mice were assessed by velocity sedimentation on sucrose gradients and by gel permeation chromatography on Sephacryl S-300. Analyses were done under conditions of both moderate ionic strength (presence of 0.1 M KCl) and high ionic strength (0.4 M KCl). [3H] 2,3,7,8-Tetrachlorodibenzo-p-dioxin (TCDD) was used as the radioligand. In conditions of moderate ionic strength the receptor from Sprague-Dawley rat liver sedimented at 8.8 +/- 0.05 S, had a Stokes radius of 7.0 +/- 0.21 nm, and an apparent relative molecular mass (Mr) of 257,000 +/- 7,700. In conditions of high ionic strength the Ah receptor from rat hepatic cytosol dissociated to a [3H]TCDD-binding subunit which sedimented at 5.6 +/- 0.58 S, had a Stokes radius of 5.2 +/- 0.24 nm, and an apparent Mr of 121,000 +/- 5,600. The Ah receptor from liver of C57BL/6N mice, in moderate ionic strength conditions, sedimented at 9.4 +/- 0.54 S, had a Stokes radius of 7.1 +/- 0.12 nm, and an apparent Mr of 277,000 +/- 4,800. Whereas the Ah receptor from rat liver readily dissociated into a [3H]TCDD-binding subunit during brief exposure to 0.4 M KCl, the mouse Ah receptor resisted dissociation. When exposed to 0.4 M KCl for 2 h, the mouse Ah receptor remained at the same molecular size that it had exhibited in moderate ionic strength conditions. Prolonged exposure (16 h) to 0.4 M KCl prior to analysis partially converted the mouse Ah receptor into a smaller [3H]TCDD-binding subunit which sedimented at 4.9 +/- 0.07 S, had a Stokes radius of 5.2 +/- 0.19 nm, and an apparent Mr of 105,000 +/- 3,800. The potency of seven different Ah receptor agonists in competing with [3H]TCDD for specific receptor sites was slightly different in mouse cytosol than in rat cytosol. By criteria of size, response to high ionic strength environments, and ligand binding preferences the mouse and rat Ah receptors appear to be similar but not identical molecular species.     

Physicochemical characterization of the nuclear form of Ah receptor from mouse hepatoma cells exposed in culture to 2,3,7,8-tetrachlorodibenzo-p-dioxin

Molecular properties of nuclear aromatic hydrocarbon (Ah) receptor from Hepa-1c1c9 (Hepa-1) cells were assessed by velocity sedimentation on sucrose gradients and by gel permeation chromatography on Sephacryl S-300. Nuclear Ah receptor was obtained by exposing intact cells to [3H]-2,3,7,8-tetrachlorodibenzo-p-dioxin (TCDD) for 1 h at 37 degrees C in culture followed by extraction of receptor from nuclei with buffers containing 0.5 M KCl. The nuclear Ah receptor was compared to the cytosolic Ah receptor from the same cells. Under conditions of low ionic strength, the Ah receptor from Hepa-1 cytosol sedimented as a single 9.4 +/- 0.63 S binding peak that had a Stokes radius of 7.1 +/- 0.12 nm and an apparent relative molecular mass of 271,000 +/- 16,000. After prolonged (24 h) exposure to high ionic strength (0.5 M KCl), cytosol labeled with [3H]TCDD exhibited two specific binding peaks. The large form of cytosolic Ah receptor seen under high ionic strength conditions sedimented at 9.4 +/- 0.46 S, had a Stokes radius of 6.9 +/- 0.19 nm, and an apparent Mr 267,000 +/- 15,000. The smaller ligand-binding subunit generated by exposing cytosol to 0.5 M KCl sedimented at 4.9 +/- 0.62 S, had a Stokes radius of 5.0 +/- 0.14 nm, and an apparent Mr 104,000 +/- 12,000. Nuclear Ah receptor, analyzed under high ionic strength conditions, sedimented at 6.2 +/- 0.20 S, had a Stokes radius of 6.8 +/- 0.19 nm, and an apparent Mr 176,000 +/- 7000. Nuclear Ah receptor from rat H4IIE hepatoma cells was analyzed and found to have physicochemical characteristics identical to those of nuclear Ah receptor from the mouse Hepa-1 cells. The molecular mass of Hepa-1 nuclear Ah receptor was found to be statistically different from both the Mr approximately 267,000 cytosolic Ah receptor and the Mr approximately 104,000 subunit which were present in cytosol under high ionic strength conditions. Hepa-1 nuclear Ah receptor could not be converted to a smaller ligand-binding subunit by treatment with alkaline phosphatase, ribonuclease, or sulfhydryl-modifying reagents or prolonged exposure to 1.0 M KCl. Cytosolic Ah receptor from Hepa-1 cells was "transformed" by heating at 25 degrees C in vitro into a form with high affinity for DNA-cellulose. The transformed cytosolic Ah receptor, when analyzed under conditions of high ionic strength, sedimented at approximately 6 S, had a Stokes radius of approximately 6.7 nm, and an apparent Mr approximately 167,000.(ABSTRACT TRUNCATED AT 400 WORDS)     

Permeability properties of the subepithelial tissues of Necturus gallbladder

The permeability properties of the subepithelial connective tissue of Necturus gallbladder were evaluated by measurement of electrical resistance, dilution potentials and hydraulic water permeability. The gallbladder epithelial cells were removed by scraping and the underlying connective tissue placed in an Ussing chamber. The electrical resistance was 2.2 +/- 0.8 omega X cm2; the tissue was slightly cation selective relative to free solution. The subepithelial tissues restricted the rate of diffusion of small solutes to 50% of the free solution value. The hydraulic water permeability averaged 2.1 X 10(-2) cm/s per atm. We conclude that limitations of the area of subepithelium available for fluid movement are the most important factors in determining the restrictions to solute and water flow offered by the subepithelial tissues.     

Starling forces that oppose filtration after tissue oncotic pressure is increased

We tested the hypothesis that the effective oncotic force that opposes fluid filtration across the microvessel wall is the local oncotic pressure difference across the endothelial surface glycocalyx and not the global difference between the plasma and tissue. In single frog mesenteric microvessels perfused and superfused with solutions containing 50 mg/ml albumin, the effective oncotic pressure exerted across the microvessel wall was not significantly different from that measured when the perfusate alone contained albumin at 50 mg/ml. Measurements were made during transient and steady-state filtration at capillary pressures between 10 and 35 cmH(2)O. A cellular-level model of coupled water and solute flows in the interendothelial cleft showed water flux through small breaks in the junctional strand limited back diffusion of albumin into the protected space on the tissue side of the glycocalyx. Thus oncotic forces opposing filtration are larger than those estimated from blood-to-tissue protein concentration differences, and transcapillary fluid flux is smaller than estimated from global differences in oncotic and hydrostatic pressures.