Rabbit and rat hepatic lectins have two sugar-combining sites per monomeric unit

Binding characteristics of the galactose/N-acetylgalactosamine-specific, hepatic lectins of rabbit and rat were studied using small, high-affinity ligands containing two and three N-acetylgalactosamine residues per molecule [Lee, R. T. and Lee, Y. C. (1987) Glycoconjugate J. 4, 317-328]. These N-acetylgalactosamine cluster ligands have the receptor-ligand dissociation constants in nanomolar range, so that the lectin-ligand interaction can easily studied by an equilibrium (gel chromatography) or non-equilibrium (fast filtration assay) method. The results suggest that there exist on the average two N-acetylgalactosamine-combining sites per monomeric unit of both the rabbit and rat lectins.     

Effect of metal ions on the adaptive response induced by N-methyl-N-nitrosourea in Escherichia coli

Induction of the adaptive response was quantified by analysis of beta-galactosidase released after the treatment of Escherichia coli CHS26/pYM3 (ada'-lacZ') with N-methyl-N-nitrosourea (MNU). Of the 15 metal ions examined, only Cd++ and Hg++ inhibited induction of the adaptive response with neither severe suppression of cell growth nor inhibition of the induction of the SOS response by MNU. Mutagenicity of MNU was potentiated by the presence of these metal ions in an E. coli strain. These results suggest that the inhibition mechanism involves a specific interaction of Cd++ or Hg++ with O6-methyl-guanine-DNA methyltransferase.     

1,25-Dihydroxyvitamin D stimulates sodium-dependent phosphate transport by renal outer cortical brush-border membrane vesicles by directly affecting membrane fluidity

We examined the effects of several forms of vitamin D added to renal brush-border membrane suspensions on phosphate and glucose transport and on membrane fluidity. The 1,25-D stimulated and the other vitamin D decreased phosphate uptake. In contrast, glucose uptake was not affected by the treatment of vitamin D. The 1,25-D resulted in a significant shift of the lower transition temperature in Arrhenius plots for phosphate, but not for glucose uptakes, from 15 degrees C to 11.5 degrees C. These data indicate that the 1,25-D may alter membrane fluidity, limited to the phosphate transporter, thus affecting the phosphate uptake.     

Molecular cloning of a cDNA coding for 70 kilodalton subunit of soluble guanylate cyclase from rat lung

A complementary DNA clone corresponding to the 70 kDa subunit of soluble guanylate cyclase (EC 4.6.1.2) of rat lung has been isolated. The primary structure of the cDNA consisted of 3063 nucleotides including a 1857-nucleotide coding region for 619 amino acids, and the calculated molecular weight was 70476. Blot hybridization of total poly(A)+RNAs from rat tissues detected a mRNA of about 3.4 kilobases. The amount of mRNA was abundant in lung, cerebrum and cerebellum, moderate in heart and kidney, and low in liver and muscle. Southern blot analysis of high molecular weight genomic DNA from rat liver indicated the presence of one gene in the rat haploid genome. The amino acid sequence of the 70 kDa subunit has partial homology with particulate guanylate cyclase from sea-urchin sperm, and protein phosphatase inhibitor I.     

Effect of pH on the mechanism of actin polymerization

The effect of pH on the Mg2+-induced polymerization of rabbit skeletal muscle G-actin at 20 degrees C was examined. Polymerization data were obtained at various initial concentrations of Mg2+, Ca2+, and G-actin between pH 6 and 7.5. The data were found to fit a kinetic mechanism for actin polymerization previously proposed at pH 8 in which Mg2+ binding at a moderate-affinity site on actin induces an isomerization of the protein enabling more favorable nucleation [Frieden, C. (1982) J. Biol. Chem. 257, 2882-2886]. The data also suggest the formation of actin dimers induced by Mg2+ binding is over 2 orders of magnitude more favorable at pH 6 than at pH 8. Little effect on trimer formation is found over this pH range. In addition, the conformation induced by nonspecific binding of metal to low-affinity sites becomes more favorable as the pH is lowered. The critical concentration for filament formation is also decreased at lower pH. The kinetic data do not support fragmentation occurring under any of the conditions examined. Furthermore, as Mg2+ exchange for Ca2+ at a high-affinity site (Kd less than 10(-9) M) fails to alter significantly the polymerization kinetics, Ca2+ release from this site appears unnecessary for either the nucleation or the elongation of actin filaments.     

Domain structure, stability, and interactions of human complement C1s-: characterization of a derivative lacking most of the B chain

A better understanding of the structure and function of C1 requires knowledge of the regions (domains) of the subcomponents that are responsible for Ca2+-dependent assembly. Toward this end, C1-s was digested with trypsin in the presence of Ca2+, a treatment that rapidly degraded the B chain, leaving a 56-kDa fragment comprised of a complete A chain disulfide linked to a small (less than 4-kDa) residual piece of the B chain. The purified fragment, referred to as C1-s-A, was shown by fast exclusion chromatography to be similar to C1-s in its ability to (1) reversibly dimerize in the presence of Ca2+, (2) substitute for C1-s in the formation of C1-r2-s2 tetramers, and (3) associate with C1-r and C1q to form macromolecular C1. Although C1-s-A was itself catalytically and hemolytically inactive, it competitively inhibited the expression of the hemolytic activity of C1-s in a reconstitution assay. When heated in the absence of Ca2+, C1-s exhibited a low-temperature transition (LTT) near 31 degrees C and a high-temperature transition (HTT) near 51 degrees C, similar to those previously observed in the homologous protein C1-r [Busby, T. F., & Ingham, K. C. (1987) Biochemistry 26, 5564-5571]. The midpoint of the LTT was shifted to 58 degrees C in 5 mM Ca2+ whereas the HTT was unaffected by Ca2+. C1-s-A exhibited only a LTT whose midpoint and Ca2+ dependence were similar to those of the LTT in C1-s. The HTT, which was accompanied by a loss of esterolytic activity, was reproduced in a plasmin-derived fragment representing the catalytic domain. These results provide strong support for the structural and functional independence of the catalytic and interaction domains of C1-s and strengthen current models regarding the role of these domains in various interactions. They also provide direct proof for the occurrence of Ca2+ binding sites on the A chain and demonstrate that all or most of the sites on C1-s that are responsible for its interaction with C1-r and C1q are located on the A chain.     

Studies on ras proteins. Catalytic properties of normal and activated ras proteins purified in the absence of protein denaturants

Normal (Gly12) and activated (Val12) Ha-ras proteins were produced in Escherichia coli, and purified to an apparent homogeneity without using any protein denaturants. The purified proteins contained an equimolar amount of GDP. They were stable in the presence of 5 mM Mg2+ and 25% (v/v) glycerol when incubated at 60 degrees C for 5 min. The binding of GDP to the protein was greatly stabilized by Mg2+. In the presence of 10 mM Mg2+, the bound GDP hardly exchanged with external guanine nucleotides, even at 30 degrees C. The exchange reaction was markedly enhanced in the presence of 10 mM EDTA or 120 mM ammonium sulfate. The rate-limiting step of the exchange reaction was the dissociation of the bound GDP from the ras protein, and this step was facilitated 40- to 100-fold by the addition of EDTA or ammonium sulfate. The dissociation rate of the normal (Gly12) ras protein was 2- to 3-fold faster than that of the activated (Val12) protein. The dissociation constants (Kd) for GDP of the normal and activated ras proteins were 1.2 X 10(-8) and 3.1 X 10(-9) M, respectively. The overall turnover rate of GTPase activity of the normal ras protein (10.8 mmol.mol-1.min-1) was about 10-fold higher than that of the activated protein (1.1 mmol.mol-1.min-1) in the absence of Mg2+ (less than 10(-8) M).     

Effects of shear rate on rouleau formation in simple shear flow

A kinetic equation for rouleau formation in a simple shear flow is derived, based on several assumptions. These are (a) colliding rouleaux stick to one another with a certain probability to form a single rouleau; (b) simultaneous collisions between more than two rouleaux are negligible; (c) rouleaux are broken by a viscous force exerted by the suspending fluid on the surfaces of rouleaux; (d) when a rouleau is broken by viscous forces, only two fragments are formed. Based on a simple mathematical model, collision rate, sticking probability and degradation rate are obtained as functions of applied shear rate. From the solution of the kinetic equation, the average size of rouleaux is obtained as a function of time with shear rate as a parameter. It is shown that the average size of rouleaux increases monotonically with increasing time and tends to an equilibrium size. The average size of rouleaux in a dynamical equilibrium decreases monotonically with increasing shear rate and tends to one cell as shear rate approaches infinity. It is also found that the initial rate of rouleau formation increases with increasing shear rate at very low shear rate, but this trend is reversed at higher shear rates. The theoretical results are compared quantitatively with experimental data.     

To what extent does a minimal atherosclerotic plaque alter the arterial wall shear stress distribution? A model study by an electrochemical method

An electrochemical surface shear stress measurement was applied to a model of very thin unilateral arterial stenosis (height of 1/8 of the model pipe diameter with very smooth surface). Three dimensional wall shear stress distribution was measured under steady flow field from a relatively low Reynolds number, Re = 270, to a high Reynolds number, Re = 1200. There was a characteristic high and low wall shear distribution pattern around the stenosis. There were also remarkable high shear stress areas on the opposite wall and both side walls of the stenosis. It was clearly shown that three dimensional structure of the flow field, hence, the wall shear stress distribution, is affected by a minimal change on the arterial wall.