Hemes and hemoproteins. 1: Preparation and analysis of the heme-containing octapeptide (microperoxidase-8) and identification of the monomeric form in aqueous solution

The heme-octapeptide from cytochrome c, Microperoxidase-8 (MP-8), was prepared by peptic and tryptic digestion of horse heart cytochrome c and purified by gel permeation chromatography in about 50% yield. Conditions for the identification of MP-8 by TLC and analysis by HPLC are described. Study of the concentration-dependence of the absorption spectrum showed that at concentrations of less than or equal to 2.5 X 10(-5) M in aqueous solution at pH 7, 25 degrees C and mu = 0.1, MP-8 exists as an equilibrium mixture of monomers and dimers with KD = 1.17 +/- 0.02 X 10(5) M-1, decreasing to 1.21 +/- 0.02 X 10(4) M-1 and 2.16 +/- 0.21 X 10(3) M-1 in 20% and 50% (v/v) methanol:water mixtures, respectively. Comparison of the Soret region spectrum of monomeric MP-8 with other hemoproteins suggests that it is six-coordinate in aqueous solution with water and His as axial ligands.     

Quenching of the zinc-protoporphyrin triplet state as a measure of small-molecule diffusion through the structure of myoglobin

The diffusion of small molecules through the myoglobin structure was studied. It has been shown that the fluorescent Zn-protoporphyrin substitutes easily for the native nonfluorescent Fe-protoporphyrin in myoglobin. The quenching rate of the E-type delayed fluorescence of Zn-protoporphyrin in a substituted myoglobin by the quenchers oxygen and anthraquinonesulfonate was used to measure their diffusion from the ambient solution through the protein to the ligand binding site. The quenching rate constant (at 21 degrees C) for oxygen is kq = (9.6 +/- 0.9) X 10(7) M-1 S-1, only 1 order of magnitude less than that for Zn-hematoporphyrin quenching in aqueous solution. The activation energy in the range between 2 and 40 degrees C is Ea = 6.0 +/- 0.6 kcal/mol. The corresponding data for anthraquinonesulfonate are kq = (2.1 +/- 0.3) X 10(8) M-1 S-1 and Ea = 5.8 +/- 0.6 kcal/mol. Taking into account the statistical factor involved in the oxygen quenching of the Zn-porphyrin triplet, the quenching rates are very similar. The data are discussed in terms of the "gated reaction" theory of Northrup and McCammon. The similar rate constants and activation energies indicate that the diffusion rate in the protein is determined by the frequency of the conformational changes that open "gates" for the passage of the quencher through the protein.     

Proton magnetic relaxation dispersion in human fluoromethaemoglobin solutions.

The solvent proton spin-lattice relaxation time of high spin Fe3+ (S=5/2) human A fluoromethaemoglobin aqueous solutions was measured at 14 Larmor frequencies in the range from 2.2 to 96 MHz. The observed paramagnetic relaxation rates are analysed in terms of the Solomon-Bloembergen theory, with the g-tensor value of 2 based on the consideration of the protein tertiary structure. From the H2O (pH 6) haemoprotein solution relaxation data, tau(c) =(9.3+/-0.3) X 10(-10) sec. If the total relaxation rates are corrected for the "outer-sphere" paramagnetic contribution, tau(c)=(6.5+/-0.4) X 10(-10) sec. The latter correction is obtained from the p.m.r. of the non-exchangeable aliphatic protons of C2H4(OD)2 added to the D2O-solution of fluoromethaemoglobin. Assuming that single proton transfer is taking place through the protein channel along the axis normal to the haem (g=2), the protein "binding" site is at a distance of 3.93 to 3.98 A from the haem Fe3+ ion.     

Thyroxine-protein interactions. Interaction of thyroxine and triiodothyronine with human thyroxine-binding globulin.

The effect of temperature on the binding of thyroxine and triiodothyronine to thyroxine-binding globulin has been studied by equilibrium dialysis. Inclusion of ovalbumin in the dialysis mixture stabilized thyroxine-binding globulin against losses in binding activity which had been found to occur during equilibrium dialysis. Ovalbumin by itself bound the thyroid hormones very weakly and its binding could be neglected when analyzing the experimental results. At pH 7.4 and 37 degrees in 0.06 M potassium phosphate/0.7 mM EDTA buffer, thyroxine was bound to thyroxine-binding globulin at a single binding site with apparent association constants: at 5 degrees, K = 4.73 +/- 0.38 X 10(10) M-1; at 25 degrees, K = 1.55 +/- 0.17 X 10(10) M-1; and at 37 degrees, K = 9.08 +/- 0.62 X 10(9) M-1. Scatchard plots of the binding data for triiodothyronine indicated that the binding of this compound to thyroxine-binding globulin was more complex than that found for thyroxine. The data for triiodothyronine binding could be fitted by asuming the existence of two different classes of binding sites. At 5 degrees and pH 7.4 nonlinear regression analysis of the data yielded the values n1 = 1.04 +/- 0.10, K1 = 3.35 +/- 0.63 X 10(9) M-1 and n2 = 1.40 +/- 0.08, K2 = 0.69 +/- 0.20 X 10(8) M-1. At 25 degrees, the values for the binding constants were n1 = 1.04 +/- 0.38, K1 = 6.5 +/- 2.8 X 10(8) M-1 and n2 = 0.77 +/- 0.22, K2 = 0.43 +/- 0.62 X 10(8) M-1. At 37 degrees where less curvature was observed, the estimated binding constants were n1 = 1.02 +/- 0.06, K1 = 4.32 +/- 0.59 X 10(8) M-1 and n2K2 = 0.056 +/- 0.012 X 10(8) M-1. When n1 was fixed at 1, the resulting values obtained for the other three binding constants were at 25 degrees, K1 = 6.12 +/- 0.35 X 10(8) M-1, n2 = 0.72 +/- 0.18, K2 = 0.73 +/- 0.36 X 10(8) M-1; and at 37 degrees K1 = 3.80 +/- 0.22 X 10(8) M-1, n2 = 0.44 +/- 0.22, and K2 = 0.43 +/- 0.38 X 10(8) M-1. The thermodynamic values for thyroxine binding to thyroxine-binding globulin at 37 degrees and pH 7.4 were deltaG0 = -14.1 kcal/mole, deltaH0 = -8.96 kcal/mole, and deltaS0 = +16.7 cal degree-1 mole-1. For triiodothyronine at 37 degrees, the thermodynamic values for binding at the primary binding site were deltaG0 = -12.3 kcal/mole, deltaH0 = -11.9 kcal/mole, and deltaS0 = +1.4 cal degree-1 mole-1. Measurement of the pH dependence of binding indicated that both thyroxine and triiodothyronine were bound maximally in the region of physiological pH, pH 6.8 to 7.7.     

Impulse photoconductance of solutions of chlorophyll and its analogs. IV. Absolute quantum yield of ion radical formation during photooxidation of chlorophyll a by n-benzoquinone

The values of absolute quantum yield phi of the formation of free ion-radicals during the illumination of alkohol solutions of chlorophyll alpha (Chl) and rho-benzoquinone (Q) at room temperature were obtained by the method of impulse photoconductance. With an increase of the dielectric constant epsilon of the solvent from approximately 6 to approximately 25 phi increases by two orders ( approximately 10(-3)--approximately 10(-1). That obtained relationship phi (epsilon) is explained by epsilon effect on the efficiency of dissociation of "solvent-shared" ion-radical pair Chls+. Os-. The comparison of experimental data and theoretically expected ones allowed the estimation of some parameters to be obtained which characterize the ion-radical pair: interionic distance (10 A), the dissociation velocity constant ( approximately 10(5)--10(8) s-1), the velocity constant of reverse electron transfer (10(8) s-1), the life time approximately 10(-8) s).     

Hemes and hemoproteins. 3. The reaction of microperoxidase-8 with cyanide: comparison with aquocobalamin and hemoproteins

The monomeric heme octapeptide from cytochrome c, microperoxidase-8, (MP-8), coordinates CN- with log K = 7.55 +/- 0.04 at 25 degrees C in 20% (v/v) aqueous methanol. Log K values are independent of pH between 6 and 9. A spectrophotometric titration of cyanoMP-8 between pH 5.5 and 13.8 gave a single pKa greater than or equal to 13.5 ascribed to ionization of the proximal His ligand. A study of the kinetics of the reaction of MP-8 with cyanide between pH 5.5 and 12, at 25 degrees C and mu = 0.1, indicates that formation of cyanoMP-8 occurs via three routes: attack of CN- on Fe(III) (k1 = 6.0 +/- 0.3 X 10(5) M-1 sec-1); attack of HCN on Fe(III) (k2 = 4.8 +/- 2.0 X 10(3) M-1 sec-1), followed by deprotonation and isomerization to form the C-bound species; and displacement of OH- by CN- when the proximal His ligand is ionized (k5 = 1.8 +/- 0.1 X 10(5) M-1 sec-1). These results are compared with available data for the reaction of cyanide with aquocobalamin and with various hemoproteins.     

Size and Surface Charge Properties of Myelin Vesicles from Normal and Diseased (Multiple Sclerosis) Brain

Differences have been observed between myelin vesicles prepared from normal human central nervous system and from white matter of patients who died with multiple sclerosis (MS). The mean cross-sectional area of the vesicles was 5.69 +/- 0.17 micron 2 from normal myelin and 3.71 +/- 0.28 micron 2 for diseased myelin. Vesicle size was reduced to 4.08 +/- 0.21 micron 2 when normal myelin vesicles were prepared in the presence of 0.1 mM EDTA. The presence of Ca2+ during the preparation of the vesicles had no effect on the mean cross-sectional area. In the case of MS myelin vesicles, 0.1 mM EDTA had no effect on vesicle size, whereas the presence of Ca2+ increased the vesicle size from 3.71 +/- 0.28 to 5.40 +/- 0.31 micron 2. Electrokinetic analysis revealed that the electrophoretic mobility of normal myelin vesicles was -5.169 +/- 0.193 X 10(-8) compared with -6.093 +/- 0.202 X 10(-8) m2 s-1 V-1 for the MS myelin vesicles. The presence of 0.1 mM EDTA increased the electrophoretic mobility of the normal vesicles to -6.483 +/- 0.151 X 10(-8) m2 s-1 V-1 but did not significantly affect that of the MS vesicles. Addition of 0.1 mM Ca2+ decreased the electrophoretic mobility of both normal and MS vesicles to similar mobilities. From these data, the surface charge densities were calculated for both normal and MS myelin vesicles and found to be -2.93 and -5.39 mV m-1, respectively. The phase transition temperature determined by wide-angle x-ray diffraction studies was 63 degrees C for normal myelin vesicles and 43 degrees C for MS myelin vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)     

Ca2+-dependent facilitated shortening in isotonic contraction of trachealis muscle

We compared isotonic shortening with isometric force generation as a function of external Ca2+ in 166 tracheal smooth muscle (TSM) strips from 27 mongrel dogs in vitro. Concentration-response curves were generated with muscarinic stimulation (acetylcholine, ACh), alpha-adrenergic receptor activation (norepinephrine after beta-adrenoceptor blockade, NE), serotonin (5-HT), and KCl-substituted Krebs-Henseleit solution. The concentrations of 5-HT causing half-maximal shortening (ECS50, 1.54 +/- 0.14 X 10(-7) M) and half-maximal active isometric tension (ECT50, 1.72 +/- 0.30 X 10(-7) M) were similar (P = NS). Likewise, ECS50 (21.9 +/- 0.7 mM) and ECT50, (22.0 +/- 0.9 mM) were similar for KCl. In contrast, facilitated isotonic shortening (i.e., greater isotonic shortening for comparable degrees of force generation) was elicited with ACh and NE for all levels of force generation between 15 and 85% of maximum and for all concentrations of ACh from 3 X 10(-8) to 3 X 10(-5) M (P less than 0.05 for all points). Facilitated isotonic shortening also was elicited for all concentrations of NE from 10(-8) to 10(-6) M (P less than 0.05 for all points). Removal of Ca2+ from the perfusate substantially reduced the potency of ACh (P less than 0.001) and abolished differences between ECS50 (2.23 +/- 0.28 X 10(-5) M) and ECT50 (2.50 +/- 0.46 X 10(-5) M, P = NS). We demonstrate that for comparable degrees of force generation, muscarinic and alpha-adrenergic receptor activation cause greater isotonic shortening than KCl or 5-HT and that this facilitated shortening is associated with the concentration of external Ca2+.     

Interpretation of osmotic pressure in solutions of one and two nondiffusible components.

Osmotic pressure data from aqueous solutions of nondiffusible serum albumin (BSA), chondroitin sulfate (CHS), and dextran T110 (D110), taken singly and in binary combinations, were interpreted in terms of excluded volume. The principal solvent was phosphate-buffered saline, pH 7.2, at 23 degrees C. Osmotic pressures were measured with a membrane osmometer fitted with Amicon PM-10 membranes. Data from each solution were fit by stepwise regression with a three- or four-term polynomial in integral powers of total nondiffusible solute concentration in accordance with the general solution theory of McMillan and Mayer (1945, J. Chem. Phys. 13:276) as extended by Yamakawa (1971, Modern Theory of Polymer Solutions, Harper & Row, New York). The date display a high internal consistency, and the results correlate well with published molecular weights and exclusion data where available. Number average molecular weights calculated from the "first virial coefficients" are: BSA, 67,000 +/- 11%; D110, 76,000 +/- 11%, CHS, 39,000 +/- 6%. Excluded volumes (in cubic centimeters per molecule) calculated from the "second virial coefficients" are: BSA, 0.97 X 10(-18); D110, 3.04 X 10(-18); CHS, 14.3 X 10(-18); BSA-D110, 6.8 X 10(-18); BSA-CHS, 7.8 X 10(-18). Uncertainty is about 30%. An empirical model for interpretation of calculated excluded volumes is proposed. It appears that CHS has the "largest" exclusion effect of the three molecules.     

Measurement of the susceptibility of paramagnetically labeled cells with paramagnetic solutions

A method of measuring the volumetric magnetic susceptibility, in which magnetically labeled cells or other particles are suspended in a paramagnetic solution of known susceptibility over the poles of a magnet, is presented. If the cells are more magnetic than the solution, they are attracted toward the poles; if they are less magnetic, they are repelled. If they have the same susceptibility as the solution, they do not move. Under this condition, the cells are said to be "isomagnetic" with the surrounding solution. Since the volumetric susceptibility of this solution is known, the susceptibility of the cells is obtained. Using the "isomagnetic" method, the volumetric susceptibilities of test metal powders were determined within +/- 8 X 10(-6) SI units. Yeast, colonic carcinoma, and liver cells, rendered magnetic with erbium chloride, had susceptibilities ranging from 13 to 20 X 10(-6). Particles of articular cartilage treated with erbium chloride were heterogeneous, with susceptibilities ranging between 50 and 125 X 10(-6), while particles of bone had a susceptibility of 560 to 580 X 10(-6). Eukaryotic cells labeled with ferritin attained susceptibilities of less than 1 X 10(-6).     

Biostructural chemistry of magnesium ion: characterization of the weak binding sites on tRNA(Phe)(yeast). Implications for conformational change and activity

The thermodynamics and kinetics of magnesium binding to tRNA(Phe)(yeast) have been studied directly by 25Mg NMR. In 0.17 M Na+(aq), tRNA(Phe) exists in its native conformation and the number of strong binding sites (Ka greater than or equal to 10(4)) was estimated to be 3-4 by titration experiments, in agreement with X-ray structural data for crystalline tRNA(Phe) (Jack et al., 1977). The set of weakly bound ions were in slow exchange and 25Mg NMR resonances were in the near-extreme-narrowing limit. The line shapes of the exchange-broadened magnesium resonance were indistinguishable from Lorentzian form. The number of weak magnesium binding sites was determined to be 50 +/- 8 in the native conformation and a total line-shape analysis of the exchange-broadened 25 Mg2+ NMR resonance gave an association constant Ka of (2.2 +/- 0.2) X 10(2) M-1, a quadrupolar coupling constant (chi B) of 0.84 MHz, an activation free energy (delta G*) of 12.8 +/- 0.2 kcal mol-1, and an off-rate (koff) of (2.5 +/- 0.4) X 10(3) s-1. In the absence of background Na+(aq), up to 12 +/- 2 magnesium ions bind cooperatively, and 73 +/- 10 additional weak binding sites were determined. The binding parameters in the nonnative conformation were Ka = (2.5 +/- 0.2) X 10(2) M-1, chi B = 0.64 MHz, delta G* = 13.1 +/- 0.2 kcal mol-1, and koff = (1.6 +/- 0.4) X 10(3) s-1. In comparison to Mg2+ binding to proteins (chi B typically ca. 1.1-1.6 MHz) the lower chi B values suggest a higher degree of symmetry for the ligand environment of Mg2+ bound to tRNA. A small number of specific weakly bound Mg2+ appear to be important for the change from a nonnative to a native conformation. Implications for interactions with the ribosome are discussed.     

Static and kinetic studies on carp muscle parvalbumins

Fluorescence titration and fluorescence stopped-flow studies were performed on carp muscle parvalbumin components 1, 2, 3, and 5 (the latter three components were modified with a SH-directed fluorescent reagent, dansyl-L-cysteine). Apparent binding constants (Kapp) of Ca2+ to these components decrease in the order of component 2 (Kapp = 2.8 +/- 0.9 X 10(8) M-1) greater than component 1 (Kapp = 1.25 +/- 0.25 X 10(8) M-1) greater than component 3 = component 5 (Kapp = 4.0 +/- 0.5 X 10(7) M-1) in 30 mM KCl, 50 mM Na-cacodylate-HCl, pH 7.0 at 20 degrees C. The rate constant of the conformational change of parvalbumin induced by Ca2+ binding or removal decreases in the order of component 2 greater than component 1 greater than component 5 greater than or equal to component 3; that is, component 2 undergoes the fastest conformational change and component 3 the slowest in response to the rapid free Ca2+ concentration ([Ca2+]) change in the protein solution. The fluorescence titration curves and [Ca2+]-dependences of the rate constants are analyzed by a simple two-state model, (partially unfolded state) k1 in equilibrium k2 (folded state). It is shown that the equilibrium constant K = k1/k2 depends on the second power of [Ca2+], the rate constant k1 on the first power of [Ca2+] and k2 on the inverse first power of [Ca2+], respectively.     

Determination of glucose oxidase oxidation-reduction potentials and the oxygen reactivity of fully reduced and semiquinoid forms.

The oxidation-reduction potential values for the two electron transfers to glucose oxidase were obtained at pH 5.3, where the neutral radical is the stable form, and at pH 9.3, where the anion radical is the stable form. The midpoint potentials at 25 degrees were: pH 5.3 EFl1ox + e- H+ equilibrium EFlH. Em1 = -0.063 +/- 0.011 V EFlH. + e- + H+ equilibrium EFlredH2 Em2 = -0.065 +/- 0.007 V pH 9.3 EFlox + e- EFi- Em1 = -0.200 +/- 0.010 V EFi- + e- + H+ equilibrium EFlredH- Em2 = -0.240 +/- 0.005 V All potentials were measured versus the standard hydrogen electrode (SHE). The potentials indicated that glucose oxidase radicals are stabilized by kinetic factors and not by thermodynamic energy barriers. The pK for the glucose oxidase radical was 7.28 from dead time stopped flow measurements and the extinction coefficient of the neutral semiquinone was 4140 M-1 cm-1 at 570 nm. Both radical forms reacted with oxygen in a second order fashion. The rate at 25 degrees for the neutral semiquinone was 1.4 X 10(4) M-1 s-1; that for the anion radical was 3.5 X 10(4) M-1 s-1. The rate of oxidation of the neutral radical changed by a factor of 9 for a temperature difference of 22 degrees. For the anion radical, the oxidation rate changed by a factor of 6 for a 22 degrees change in temperature. We studied the oxygen reactivity of the 2-electron reduced form of the enzyme over a wide wavelength range and failed to detect either oxygenated flavin derivatives or semiquinoid forms as intermediates. The rate of reoxidation of fully reduced glucose oxidase at pH 9.3 was dependent on ionic strength.     

Effect of joule temperature jump on tension and stiffness of skinned rabbit muscle fibers.

The effects of a temperature jump (T-jump) from 5-7 degrees C to 26-33 degrees C were studied on tension and stiffness of glycerol-extracted fibers from rabbit psoas muscle in rigor and during maximal Ca2+ activation. The T-jump was initiated by passing an alternating current pulse (30 kHz, up to 2.5 kV, duration 0.2 ms) through a fiber suspended in air. In rigor the T-jump induces a drop of both tension and stiffness. During maximal activation, the immediate stiffness dropped by (4.4 +/- 1.6) x 10(-3)/1 degree C (mean + SD) in response to the T-jump, and this was followed by a monoexponential stiffness rise by a factor of 1.59 +/- 0.14 with a rate constant ks = 174 +/- 42 s-1 (mean +/- SD, n = 8). The data show that the fiber stiffness, determined by the cross-bridge elasticity, in both rigor and maximal activation is not rubber-like. In the activated fibers the T-jump induced a biexponential tension rise by a factor of 3.45 +/- 0.76 (mean +/- SD, n = 8) with the rate constants 500-1,000 s-1 for the first exponent and 167 +/- 39 s-1 (mean +/- SD, n = 8) for the second exponent. The data are in accordance with the assumption that the first phase of the tension transient after the T-jump is due to a force-generating step in the attached cross-bridges, whereas the second one is related to detachment and reattachment of cross-bridges.     

Reciprocal cooperative effects of multiple ligand binding to pyruvate kinase

The formation of multiple ligand complexes with muscle pyruvate kinase was measured in terms of dissociation constants and the standard free energies of formation were calculated. The binding of Mn2+ to the enzyme (KA = 55 +/- 5 X 10(-6) M; deltaF degrees = -5.75 +/- 0.05 kcal/mol) and to the enzyme saturated with phosphoenolpyruvate (conditional free energy) KA' = 0.8 +/- 0.4 X 10(-6) M; deltaF degrees = -8.22 +/- 0.34 kcal/mol) has been measured under identical conditions giving a free energy of coupling, delta(deltaF degrees) = -2.47 +/- 0.34 kcal/mol. Such a large negative free energy of coupling is diagnostic of a strong positively cooperative effect in ligand binding. The binding of the substrate phosphoenolpyruvate to free enzyme and the enzyme-Mn2+ complex was, by necessity, measured by different methods. The free energy of phosphoenolpyruvate binding to free enzyme (KS = 1.58 +/- 0.10 X 10(-4)M; deltaF degrees = -5.13 +/- 0.04 kcal/mol) and to the enzyme-Mn2+ complex (K3 = 0.75 +/- 0.10 X 10(-6)M; deltaF degrees = -8.26 +/- 0.07 kcal/mol) also gives a large negative free energy of coupling, delta(deltaF degrees) = -3.16 +/- 0.08 kcal/mol. Such a large negative value confirms reciprocal binding effects between the divalent cation and the substrate phosphoenolpyruvate. The binding of Mn2+ to the enzyme-ADP complex was also investigated and a free energy of coupling, delta(deltaF degrees) = -0.08 +/- 0.08 kcal/mol, was measured, indicative of little or no cooperativity in binding. The free energy of coupling with Mn2+ and pyruvate was measured as -1.52 +/- 0.14 kcal/mol, showing a significant amount of cooperativity in ligand binding but a substantially smaller effect than that observed for phosphoenolpyruvate binding. The magnitude of the coupling free energy may be related to the role of the divalent cation in the formation of the enzyme-substrate complexes. In the absence of the activating monovalent cation, the coupling free energies for phosphoenolpyruvate and pyruvate binding decrease by 40-60% and 25%, respectively, substantiating a role for the monovalent cation in the formation of enzyme-substrate complexes with phosphoenolpyruvate and with pyruvate.     

Proton nuclear magnetic resonance measurement of diffusional water permeability in suspended renal proximal tubules.

Diffusional water permeability was measured in renal proximal tubule cell membranes by pulsed nuclear magnetic resonance using proton spin-lattice relaxation times (T1). A suspension of viable proximal tubules was prepared from rabbit renal cortex by Dounce homogenization and differential sieving. T1 measured in a tubule suspension (22% of exchangeable water in the intracellular compartment) containing 20 mM extracellular MnCl2 was biexponential with time constants 1.8 +/- 0.1 ms and 8.3 +/- 0.2 ms (mean +/- SD, n = 8, 37 degrees C, 10 MHz). The slower time constant, representing diffusional exchange of water between intracellular and extracellular compartments, increased to 11.6 +/- 0.6 ms (n = 6) after incubation of tubules with 5 mM parachloromercuribenzene sulfonate (pCMBS) for 60 min at 4 degrees C and was temperature dependent with activation energy Ea = 2.9 +/- 0.4 kcal/mol. To relate T1 data to cell membrane diffusional water permeabilities (Pd), a three-compartment exchange model was developed that included intrinsic decay of proton magnetization in each compartment and apical and basolateral membrane water transport. The model predicted that the slow T1 was relatively insensitive to apical membrane Pd because of low luminal/cell volume ratio. Based on this analysis, basolateral Pd (corrected for basolateral membrane surface convolutions) is 2.0 X 10(-3) cm/s, much lower than corresponding values for basolateral Pf (10-30 X 10(-3) cm/s) measured in the intact tubule and in isolated basolateral membrane vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of strophanthidin on intracellular Na ion activity and twitch tension of constantly driven canine cardiac Purkinje fibers.

Intracellular Na ion activity (aiNa) and twitch tension (T) of constantly driven (1 Hz) canine cardiac Purkinje fibers were measured simultaneously and continuously with neutral carrier Na+-selective microelectrodes and a force transducer. The aiNa of 8.9 +/- 1.4 mM (mean +/- SD, n = 52) was obtained in the driven fibers perfused with normal Tyrode solution. Temporary interruption of stimulation showed that aiNa of the driven fibers was approximately 1.5 mM greater than that of quiescent fibers. The constantly driven fibers were exposed to strophanthidin of 10(-8), 5 X 10(-8), 10(-7), 5 X 10(-7), and 10(-6) M for 5 min. No detectable changes in aiNa and T were observed in the fibers exposed to 10(-8) M strophanthidin, and the threshold concentration of the strophanthidin effect appeared to be approximately 5 X 10(-8) M. With concentrations greater than 5 X 10(-8) M, strophanthidin produced dose-dependent increases in aiNa and T. An increase in aiNa always accompanied an increase in T and after strophanthidin exposure both aiNa and T recovered completely. During onset and recovery periods of the strophanthidin effect the time course of change in aiNa was similar to that of change in T. A plot of T vs. aiNa during the onset and recovery periods showed a linear relationship between T and aiNa. These results indicate strongly that the positive inotropic effect of strophanthidin is closely associated with the increase in aiNa. Raising [K+]0 from 5.4 to 10.8 mM produced decreases in aiNa and T, and restoration of [K+]0 resulted in recoveries of aiNa and T. During the changes of [K+]0 the time course of change in aiNa was similar to that of the change in T. A steady-state sarcoplasmic Ca ion activity (aiCa) of 112 +/- 31 nM (mean +/- SD, n = 17) was obtained in the driven fibers with the use of neutral carrier Ca2+-selective microelectrodes. Temporary interruption produced 10-30% decreases in aiCa. No detectable changes in aiCa were observed in the fibers exposed to strophanthidin of 10(-7) M or less; 5 X 10(-7) and 10(-6) M strophanthidin produced 1.3-1.6 and 2-3-fold increases in aiCa, respectively. This result is consistent with the hypothesis that an increase in aiNa produces an increase in aiCa, which enhances Ca accumulation in the intracellular stores.     

Study of E. coli penicillin amidase. The pH dependence of the equilibrium constant of ampicillin enzymatic hydrolysis]

The equilibrium parameters of the hydrolysis of ampicillin catalysed by penicillin amidase were determined within the pH range of 4.5 to 5.5. The values of the ionization constants of the carboxy group of D-(-)-ALPHA-AMINOPHENYLACETIC ACID (PK1=1.80) and amino group of 6-aminopenicillanic acid (pK2=4.60) were estimated and pH-dependence of the effective free energy of ampicillin hydrolysis was calculated. It was shown that the thermodynamic optimum of ampicillin synthesis was at 3.20 (the value of the effective free energy under the experimental conditions was 3.27 kcal/mole). The value of the "true", pH-independent free energy of hydrolysis (deltasigma) of the amide bond in the ampicillin molecule was determined to be equal to 9.72 kcal/mole. The thermodynamic parameters of ampicillin and benzylpenicillin hydrolysis were compared. The amino group in the alpha-position of phenylacetic acid was shown to have a significant effect on the values of "true" free energy of hydrolysis of the penicillin amide bond and free ionization energy in the system.     

The CD24 antigen discriminates between pre-B and B cells in human bone marrow.

When bone marrow (BM) lymphoid cells from 12 adult healthy donors were labeled by CD24 antibodies and analyzed by flow cytometry, two positive populations of cells were demonstrated in each sample (by a separated bimodal specific immunofluorescence). One population had intermediate CD24-Ag density (termed CD24+ cells) whereas the other had high CD24-Ag density (termed CD24(2+) cells). CD24+ cells represented 5.8 +/- 2.7% of the total lymphoid BM cells and CD24(2+) cells 5.6 +/- 2.5%. Using dual fluorescence analysis on eight samples, all CD24+ cells expressed the CD21 and CD37 mature B cell Ag and also surface IgM (sIgM), but this population lacked CD10 Ag. These cells also expressed CD19 Ag, and at a higher density than CD24(2+) cells. They were also positive for HLA-DR Ag. Conversely, CD24(2+) cells were shown to be early cells of the B cell lineage. While all the CD24(2+) cells were HLA-DR+ and CD19+, 64 +/- 16% of them expressed CD20 Ag (at a lower density than CD24+ cells), 65 +/- 21% CD10 Ag, and 22 +/- 8% were positive for cytoplasmic mu-chains (c mu). None of these cells expressed the CD21 and CD37 mature B cell Ag or sIgM. Additional experiments on four different healthy donors demonstrated that 30 +/- 9% of the CD24(2+) cells expressed the CD34 Ag and that the CD24+ cells did not express it. Thus, the CD24 Ag permits discrimination between two populations of the B cell lineage present in adult BM: 1) A CD24(2+) cell population including "pre" pre-B cells (HLA-DR+, CD19+, CD10+/-, CD20-, CD21-, CD34+, CD37-, c mu-), "intermediate" pre-B cells (HLA-DR+, CD19+, CD10+, CD20+, CD21-, CD34-, CD37-, c mu-), and "true" pre-B cells (HLA-DR+, CD19+, CD10+, CD20+, CD21-, CD34-, CD37-, c mu+). 2) A CD24+ cell population including B cells of the standard phenotype (HLA-DR+, CD19+, CD10-, CD20+, CD21+, CD34-, CD37+, c mu-, sIgM+).     

The magnetic and electronic properties of Methanobacterium thermoautotrophicum (strain delta H) methyl coenzyme M reductase and its nickel tetrapyrrole cofactor F430. A low temperature magnetic circular dichroism study

Variable temperature magnetic circular dichroism (MCD) spectroscopy has been used to characterize the magnetic and electronic properties of the Ni(II) tetrapyrrole, F430, which is the cofactor of the S-methyl coenzyme M methylreductase enzyme from Methanobacterium thermoautotrophicum (strain delta H). 4-Coordinate forms are found to be diamagnetic (S = 0 ground state), whereas 6-coordinate forms are paramagnetic (S = 1 ground state). MCD studies, together with parallel low temperature UV-visible absorption and resonance Raman investigations, show that the equilibrium distribution of 4-coordinate square-planar and 6-coordinate bis-aquo forms of the native isomer of F430 in aqueous solution is affected by both temperature and the presence of glycerol. In the presence of 50% glycerol, the 12,13-diepimer of F430 is shown to be partially 6-coordinate in frozen solution at low temperature. Low temperature MCD magnetization data allow the determination of the axial zero-field splitting (D) of the S = 1 ground state of bis-ligand complexes of F430. The value of D is sensitive to the nature of the Ni(II) axial ligands: bis-aquo F430, D = +9 +/- 1 cm-1; bis-imidazole F430, D = -8 +/- 2 cm-1. Measurement of D = +10 +/- 1 cm-1 for F430 in the methylreductase holoenzyme argues strongly against histidine imidazole coordination to Ni(II) in the enzyme. The possible existence of alcoholic or phenolic oxygen-containing ligands (serine, threonine, tyrosine, water) to Ni(II) in the enzyme-bound cofactor is discussed.