Hypoxia-induced activation in small isolated pulmonary arteries from the cat

Effects of hypoxia on force development and membrane potential were studied in isolated small (less than 300 microns diam) and large (greater than 500 microns diam) pulmonary arteries from cats. There was a consistent and reproducible hypoxic constrictor response in small pulmonary arteries that began at PO2 values between 350 and 300 Torr and reached a maximum at PO2 between 50 and 30 Torr. In the small artery smooth muscle cell the membrane potential, which was -51 +/- 1.4 mV at a PO2 of 400 Torr, was depolarized to -37 +/- 2 mV at a PO2 of 50 Torr. In contrast, larger arteries did not exhibit significant hypoxic constriction or depolarization upon exposure to low PO2. Constriction in small arteries was not blocked by phentolamine. Treatment with a low dose of indomethacin (10(-9) M) augmented the response; however, a larger dose of indomethacin (10(-3) M) blocked the constriction to hypoxia but not to 30 mM KCl. Depolarization during hypoxia was not blocked by ouabain. Results of this study suggest that the hypoxic response of these isolated small pulmonary vessels may be like that seen in the intact lung. Furthermore, these data suggest that hypoxic vasoconstriction may be mediated by electrical events occurring at the pulmonary arterial muscle cell membrane either directly or via mediators released from the vessel wall.     

Competitive inhibition evidence for specific intermolecular interactions in hyaluronate solutions

Intermolecular associations in hyaluronate systems have been investigated by a competitive inhibition approach, monitored by low deformation oscillatory measurements of dynamic viscosity and rigidity. Solutions of sodium hyaluronate isolated by a mild procedure from rooster combs showed, under physiological conditions of pH and ionic strength, coupling behaviour typical of a transient polymer network. On addition of an equal concentration of hyaluronate segments (~60 disaccharide units), all evidence of coupling is lost and the solution rheology approximates closely to that typical of isolated chains. Such behaviour is clearly incompatible with entanglement coupling, such as occurs between synthetic polymers in solution, but parallels the behaviour of gelling polysaccharides, where co-operative interchain association is known to occur. Similar inhibition is observed in hyaluronate viscoelastic “putties” and “gels”, where further intermolecular association is promoted by suppression of interchain electrostatic repulsion and reduction of water activity. The effects are particularly pronounced for hyaluronate of lower molecular weight, where crosslinking in putties and gels may approach the minimum requirements for a cohesive network. No inhibition is observed with very short chain segments (~4 disaccharide residues) nor with longer segments (~400 disaccharides). On the basis of this evidence we suggest that hyaluronate chains interact by formation of specific co-operative junctions analogous to those characterised for plant structural polysaccharides, but having substantially shorter lifetimes. The magnitude of rheological changes on suppression of these fleeting associations by competitive inhibition suggests that they are likely to dominate the physical properties of hyaluronate in vivo.     

Specification of sites for polarized growth in Saccharomyces cerevisiae and the influence of external factors on site selection.

Many eucaryotic cell types exhibit polarized cell growth and polarized cell division at nonrandom sites. The sites of polarized growth were investigated in G1 arrested haploid Saccharomyces cerevisiae cells. When yeast cells are arrested during G1 either by treatment with alpha-factor or by shifting temperature-sensitive cdc28-1 cells to the restrictive temperature, the cells form a projection. Staining with Calcofluor reveals that in both cases the projection usually forms at axial sites (i.e., next to the previous bud scar); these are the same sites where bud formation is expected to occur. These results indicate that sites of polarized growth are specified before the end of G1. Sites of polarized growth can be influenced by external conditions. Cells grown to stationary phase and diluted into fresh medium preferentially select sites for polarized growth opposite the previous bud scar (i.e., distal sites). Incubation of cells in a mating mixture results in projection formation at nonaxial sites: presumably cells form projections toward their mating partner. These observations have important implications in understanding three aspects of cell polarity in yeast: 1) how yeast cell shape is influenced by growth conditions 2) how sites of polarized growth are chosen, and 3) the pathway by which polarity is affected and redirected during the mating process.