Infinite cis influx of cyclic AMP into human erythrocyte ghosts

Infinite cis uptake of cyclic AMP into red blood cell ghosts has been measured. The $\text{K}{}_{\mathrm{<mtext>i</mtext><mtext>c</mtext>}}{}^{\mathrm{<mtext>oi</mtext>}}$ is calculated from two different integrated rate equations that are applicable when the substrate concentration is unsufficient to cause volume changes. Values of 0.69 mM and 0.66 mM are obtained for the infinite cis$\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ at 30°C using these procedures. These values are only slightly higher than that predicted from zero trans net flux experiments.Lowering the temperature reduces $\text{K}{}_{\mathrm{<mtext>i</mtext><mtext>c</mtext>}}{}^{\mathrm{<mtext>oi</mtext>}}$ from 0.69 mM at 30°C to 0.478 mM at 20°C, 0.108 mM at 10°C and 0.072 mM at 4°C ($\text{Q}{}_{10}\text{= 2.4}$). The $\text{Q}{}_{10}$ for activation of influx permeability of 10^?5 M cyclic AMP is 1.55.     

The polymorphic phase behaviour and miscibility properties of synthetic phosphatidylethanolamines

(1) The polymorphic phase behaviour of aqueous dispersions of various synthetic phosphatidylethanolamines, both singly and in mixtures, has been investigated by ³¹P-NMR. (2) $\text{14:0}\text{14:0}$ PE remains in the lamellar phase up to 90°C. $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibits a lamellar to hexagonal (H_II) transition between 60°C and 63°C. For $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE, the lamellar to hexagonal (H_II) transition occurs between 7 and 12°C, whereas for $\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}$ PE, the hexagonal (H_II) phase is the preferred structure above ?15°C. (3) Mixtures of $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibit near-ideal miscibility behaviour. For mixtures of $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{14:0}\text{14:0}$ PE there is evidence of fluid-solid immiscibility at temperatures below the gel-liquid crystalline transition temperature of the $\text{14:0}\text{14:0}$ PE component. Mixtures of $\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibit complex phase behaviour involving limited fluid-solid immiscibility at low temperatures and formation of a phase allowing isotropic motional averaging at higher temperatures. (4) ³¹P-NMR provides a graphic method for investigating the miscibility properties of mixed PE systems.     

Correlation of the perceived texture of random coil polysaccharide solutions with objective parameters

A wide range of concentrated random coil polysaccharide solutions have been assessed for textural attributes by a trained sensory panel. The only textural terms invoked to describe these model systems were ‘thickness’ and ‘stickiness’, which were shown to be highly correlated, and essentially identical numerically, using a ratio scaling technique. Viscosity (η) measurements over a wide range of shear rates (γ) for all these samples gave flow curves (log η versus log γ) of the same form. Differences in flow behaviour between samples could then be characterised completely by two parameters, the maximum viscosity at low shear rates (η₀), and the shear rate ($\text{γ}\text{?}{}_{\mathrm{0·1}}$) at which $\text{η =}\text{solη}{}_0\text{10}$. A simple linear relationship was demonstrated between these two parameters and perceived thickness (T) or stickiness (S), irrespective of polysaccharide type. For Newtonian liquids, log T (or log S) varied linearly with log η. Hence the effective ‘in-mouth’ thickness of random coil polysaccharide solutions, in normal viscosity units, may be predicted directly from η₀ and $\text{γ}\text{?}{}_{\mathrm{0·1}}$ by the simple relationship: $\text{log}\text{η}{}_{\mathrm{N}}\text{= 1·13}\text{log}\text{η}{}_0\text{+ 0·45}\text{log}\text{γ}\text{?}{}_{\mathrm{0·1}}\text{? 1·72}$ where η_N is the viscosity of a Newtonian solution which would be perceived as identical in thickness (and stickiness) to the polysaccharide solution.     

The concept of high- and low-affinity reactions in bovine cytochrome c oxidase steady-state kinetics

(1) Analysis of the data from steady-state kinetic studies shows that two reactions between cytochrome c and cytochrome c oxidase sufficed to describe the concave Eadie-Hofstee plots ($\text{K}{}_{\mathrm{<mtext>m</mtext>}}\text{? 1 · 10}{}^{\mathrm{?8}}\text{M}$ and $\text{K}{}_{\mathrm{<mtext>m</mtext>}}\text{? 2 · 10}{}^{\mathrm{?5}}\text{M}$). It is not necessary to postulate a third reaction of $\text{K}{}_{\mathrm{<mtext>m</mtext>}}\text{? 10}{}^{\mathrm{?6}}\text{M}$. (2) Change of temperature, type of detergent and type of cytochrome c affected both reactions to the same extent. The presence of only a single catalytic cytochrome c interaction site on the oxidase could explain the kinetic data. (3) Our experiments support the notion that, at least under our conditions (pH 7.8, low-ionic strength), the dissociation of ferricytochrome c from cytochrome c oxidase is the rate-limiting step in the steady-state kinetics. (4) A series of models, proposed to describe the observed steady-state kinetics, is discussed.     

Molecular arrangements in sphingolipids. The crystal structure of cerebroside

The single crystal analysis of a complex, membrane glycolipid is described. Cerebroside (β-D-galactosyl-N-(2-D-hydroxyoctadecanoyl)-D-dihydrosphingosine, $\text{C}{}_{42}\text{H}{}_{32}\text{O}{}_9\text{N}\text{·}\text{1}\text{2}\text{C}{}_2\text{H}{}_5\text{OH}$) — an important constituent of plasma membranes — crystallizes in the monoclinic spacegroup P2, with a = 11.202, b = 9.262, c = 46.46 A and β = 99.00^°. There are two independent molecules in the asymmetric unit partly related by a non-crystallographic symmetry. The structure was determined by direct methods and refined to R = 0.116.The molecules pack in a typical bilayer arrangement with adjacent double layers separated by ethanol molecules of crystallization. The planes of the sugar rings are turned almost parallel to the layer interface which gives the molecules the shape of a shovel. Together with the polar ceramide part, the galactose head groups form an extensive lateral network of hydrogen bonds within the polar region of each layer. The chains tilt by an angle of 49^° towards this polar boundary. A parallel stacking of the chains is achieved by a bend of the sphingosine chain as far up as carbon atom 5 and 6 in the two independent molecules. The lateral hydrocarbon chain packing is of an earlier unknown hybrid type (HS2). Chains with parallel zigzag planes are arranged in pleated shoets. These sheets contain alternatively fatty acid and sphingosine chains which have a mutually perpendicular chain plane orientation.     

High-molecular-weight carrier ampholytes for isoelectric focusing of peptides

A method is described for the synthesis of high-molecular-weight carrier ampholytes for preparative isoelectric focusing of peptides. A giant polyethylene imine ($\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{40 000–60 000}$) is mixed with a linear gradient of acrylic acid in a flow-through system and let to react at 80°C for 70 h. Giant carrier ampholytes ($\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{range}\text{50 000–90 000}$) are thus obtained. These compounds interact very strongly among themselves, probably not by hydrogen bonds or hydrophobic interactions but ionic bonds. In fact, the aggregates are split by high salt (NaCl) or by zwitterionic compounds (Gly, taurine) or at acidic or alkaline pHs. They appear to interact only weakly and reversibly with proteins and no interactions are apparent with model dipeptides (His-Ser, His-Met, His-Phe and His-Lys).     

Characteristics of leucine transport by isolated hepatocytes of antarctic fish at low temperatures

Hepatocytes prepared by collagenase perfusion from Antarctic nototheniid fish of genus Trematomus are active in uptake of [¹⁴C]leucine at 0, 5, and 10°C. The system is saturable with apparent $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ about 1.0 mM. Isoleucine and phenylalanine were major competitors, valine was about one-half as effective, while alanine, glycine and histidine had no effect. Temperature dependency of rates in the 0–10°C range yielded $\text{E}{}_{\mathrm{<mtext>a</mtext>}}\text{= 65}\text{kJ/mol}$ ($\text{Q}{}_{10}\text{= 2.7}$). The average first-order rate constant at 0°C was 0.1 min^?1, one-third the value of 0.3 min^?1 estimated for clearance of [¹⁴C]leucine by liver of these species in vivo. Affinity and specificity agreed well with in vivo data on liver clearance of leucine, both in Antarctic fish at 0°C and in temperate fish acclimated to 10°C and 20°C. The results indicate similar modifications of leucine transport associated with evolutionary cold adaptation and seasonal acclimation in fish.     

Studies on NADPH-cytochrome c reductase I: Isolation and several properties of the crystalline enzyme from ale yeast.

NADPH-cytochrome c reductase has been isolated from a top-fermenting ale yeast, Saccharomyces cerevisiae (Narragansett strain), after ca. a 240-fold purification over the initial extract of an acetone powder, with a final specific activity (at pH 7.6, 30 °C) of ca. 150 μmol cytochrome c reduced min^?1mg^?1 protein. The preparation appears to be homogeneous by the criteria of: sedimentation velocity; electrophoresis on cellulose acetate in buffers above neutrality; and by polyacrylamide gel electrophoresis. Although the reductase appeared to partially separate into species “A” and “B” on DEAE-cellulose at pH 8.8, the two species have proven to be indistinguishable electrophoretically (above pH 8) and by sedimentation. By sedimentation equilibrium at 20 °C, a molecular weight of ca. 6.8 (± 0.4) × 10⁴ was obtained with use of a $\text{V}\text{?}{}_{\mathrm{20\; °}}\text{= 0.741}$ calculated from its amino acid composition. After disruption in 4 m guanidinium chloride- 10 mm dithioerythritol- 1 mm EDTA, pH 6.4 at 20 °C, an $\text{M}\text{?}{}_{\mathrm{<mtext>r</mtext>}}$ of 3.4 (± 0.1) × 10⁴ resulted, which points to a subunit structure of two polypeptide chains per mole. Confirmatory evidence of the two-subunit structure with similar, if not identical, polypeptide chains was obtained by polyacrylamide gel electrophoresis in dodecyl-sulfate, after disruption in 4 m urea and 2% sodium dodecyl sulfate, and yielded a subunit molecular weight of ca. 4 × 10⁴. Sulfhydryl group titration with 4,4′-dithiodipyridine under acidic conditions revealed one sulfhydryl group per monomer, which apparently is necessary for the catalytic reduction of cytochrome c. NADPH, as well as FAD, protects this-SH group from reaction with 5,5′-dithiobis (2-nitrobenzoate). The visible absorption spectrum of the oxidized enzyme (as prepared) has absorption maxima at 383 and 455 nm, typical of a flavoprotein. Flavin analysis (after dissociation by thermal denaturation of the “A” protein) conducted fluorometrically, revealed the presence of 2.0 mol of FAD per 70,000 g, in confirmation of the deduced subunit structure. The identity of the FAD dissociated from either “A” or “B” protein was confirmed by recombination with apo-d-amino acid oxidase and by thin-layer chromatography. A kinetic approach was used to estimate the dissociation constant for either FAD or FMN (which also yields a catalytically active enzyme) to the apoprotein reductase at 30 °C and pH 7.6 (0.05 m phosphate) and yielded values of 4.7 × 10^?8m for FAD and 4.4 × 10^?8m for FMN.     

Ubisemiquinone radicals from the cytochrome b-c1 complex of the mitochondrial electron transport chain--demonstration of QP-S radical formation

Stable ubisemiquinone radical(s) in the cytochrome $\text{b}\text{?}\text{c}{}_1$-II complex of bovine heart was observed following reduction by succinate in the presence of catalytic amounts of succinate dehydrogenase. The radical was abolished by addition of antimycin A, but a residual radical remained in the presence of excess exogenous Q₂. The radical showed an EPR signal of g = 2.0046 ± .003 at X band (～9.4 GHz) with no resolved hyperfine structure and had a line width of 8.1 ± .5 Gauss at 23°C. The Q band (35 GHz) spectra showed wellresolved $\text{g}$-anisotropy and had a field separation between derivative extrema of 26 ± 1 Gauss. This radical is evidently from QP-C. These observations substantiate that the radical is immobilized and bound to a protein. The QP-S radical was demonstrated in the cytochrome $\text{b}\text{-}\text{c}{}_1$-II complex only in the presence of more than a catalytic amount of succinate dehydrogenase and cytochrome $\text{b}\text{-}\text{c}{}_1$. This signal was not antimycin a inhibitory. The signal amplitude paralleled the reconstitutive enzymic activity of succinate-cytochrome $\text{c}$ reductase from succinate dehydrogenase and the cytochrome $\text{b}\text{-}\text{c}{}_1$-II complex.     

Studies on glutathione transport utilizing inside-out vesicle prepared from human erythrocytes

Adenosine triphosphate-dependent glutathione transport was characterized using inside-out vesicles made from human erythrocytes. Kinetic analysis of the glutathione disulfide (GSSG) transport showed a biphasic Line-weaver-Burk plot as a function of GSSG concentration suggesting the operation of two different processes. One phase had a high affinity for GSSG and a low transport velocity. Most active at acidic pH and at 25°C, this transport activity was easily lost during the storage of vesicles at 4°C. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for Mg-ATP was 0.63 mM; guanosine triphosphate (GTP) substituted for ATP gave a 340% stimulation of transport activity. Neither dithiothreitol nor thiol reagents affected this transport process. The other phase had a low affinity for GSSG and a high transport velocity. Most active at pH 7.2 and 37°C, this transport activity was stable during storage of vesicles at 4°C for several days. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for Mg-ATP was 1.25 mM; GTP substituted with no change in activity. Dithiothreitol increased the V but did not alter the $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$, and thiol reagents inhibited the transport. These findings suggest that there are two independent transfer processes for GSSG in human erythrocytes.     

Preferential solvation of methylmercurated calf thymus deoxyribonucleic acid.

The changes in polymer-solvent interactions that occur when native calf thymus DNA is dialyzed against Na₂SO₄ solutions of a given ionic strength and buffer concentration but of varying concentrations in methylmercuric hydroxide have been investigated with the help of solution density measurements at 25 °C and pH 6.8–7.0. From measurements executed under equilibrium dialysis conditions at the three salt levels 5 mm, 0.05 m, and 0.5 m Na₂SO₄ (m refers to molality) and in the presence of 5 mm cacodylic acid buffer, the density increments $\text{(}\text{??}\text{?c}{}_2\text{)}{}_{\mathrm{\mu }}{}^0$ for native calf thymus DNA were determined as a function of CH₃HgOH concentration. $\text{(}\text{??}\text{?c}{}_2\text{)}{}_{\mathrm{\mu }}{}^0$ was found not to vary with organomercurial concentration, irrespective of the concentration of supporting electrolyte, until a certain CH₃HgOH concentration level has been reached, viz., , beyond which $\text{(}\text{??}\text{?c}{}_2\text{)}{}_{\mathrm{\mu }}{}^0$ increases strongly with increasing concentration of CH₃HgOH. As is shown by optical melting, $\text{(}\text{??}\text{?c}{}_2\text{)}{}_{\mathrm{\mu }}{}^0$ becomes a function of organomercurial concentration the moment DNA undergoes denaturation brought about by the complexing of CH₃HgOH with the various N-binding sites of the base residues in the DNA double helix.Polymer-solvent interactions, expressed in terms of preferential water interactions (“net hydration”) and preferential salt interactions (“salt solvation”), were derived from the $\text{(}\text{??}\text{?c}{}_2\text{)}{}_{\mathrm{\mu }}{}^0$ data in combination with data obtained on the preferential interaction of CH₃HgOH with denatured DNA and data on the partial specific volumes of all major solution components, gathered from density measurements on solutions with fixed concentrations of diffusible components. Evidence is presented which shows that denaturation in general decreases the net hydration while salt becomes preferentially associated with the polyelectrolyte. This process is further amplified by the interaction of CH₃HgOH with denatured DNA: Methylmercurated DNA alters the redistribution of diffusible components at dialysis equilibrium to such an extent that in a formal sense large amounts of water are rejected from the immediate vicinity of the polymer. The molecular implications of these findings are explored. The results are further discussed in the light of previous findings where the methylmercury-induced denaturation of DNA had been studied with the help of buoyant density measurements in a Cs₂SO₄ density gradient and by velocity-sedimentation in a variety of sulfate media.     

Quantum-chemical and empirical calculations on Phospholipids VIII. The electrostatic potential from isolated molecules up to layer systems

Using 1-6-12 empirical functions with a solvent-averaged electrostatic contribution $\text{q}{}_{\mathrm{I}}\text{q}{}_{\mathrm{j}}\text{ε(r}{}_{\mathrm{Ij}}\text{)}\text{× r}{}_{\mathrm{Ij}}$ and electrostatic potentials from CNDO-type wavefunctions, the development of specific interactions of ions visualized by the molecular electrostatic potential of PO₄-group containing molecules was studied. Going from single molecules to monolayers made up of 37 head groups of phosphatidylcholine (PC) or phosphatidylethanolamine (PE) for quantum-chemical calculations, or of 23 head groups for empirical calculations we found decreasing potential minima. Only the inclusion of the screening effect of water, simulated by a distance dependent dielectric constant, ε(r), gives an explanation of stereospecific interactions of model membranes with ions. This finding can be compared with results of simulation calculations on water structure above a PE head group layer.     

Lipid-protein interactions in membrane models fluorescence polarization study of cytochrome b5-phospholipids complexes

According to previous authors, cytochrome $\text{b}{}_5$, when extracted from bovine liver by a detergent method, is called cytochrome $\text{d-b}{}_5$. On the other hand, the protein obtained after trypsin action, which eliminates an hydrophobic peptide of about 54 residues, is called cytochrome $\text{t-b}{}_5$.Fluorescence polarization of the dansyl phosphatidylethanolamine probe inserted into phospholipid vesicles is very senstive to the binding of proteins, and so is a useful method to study lipid-protein interactions.The chromophore mobility, $\text{R}$, decreases markedly when dipalmitoyl phosphatidylcholine vesicles are incubated with cytochrome $\text{d-b}{}_5$, whereas $\text{R}$ does not change for cytochrome $\text{c}$ and cytochrome $\text{t-b}{}_5$. This can be interpreted as a strengthening of the bilayer, only due to the interaction of the hydrophobic peptide tail.Interaction of dipalmitoyl phosphatidylcholine vesicles with cytochrome $\text{d-b}{}_5$ occurs either below or above the melting temperature of the aliphatic chains (41 °C). Even for a high protein to lipid molar ratio (1 molecule of protein for 40 phospholipid molecules), the melting temperature is apparently unaffected.Phosphatidylserine and phosphatidylinositol do not interact at pH 7.7 with cytochrome $\text{d-b}{}_5$, because electrostatic forces prevent formation of complexes. At low pH, the interaction with the protein occurs, but the binding is mainly of electrostatic nature.     

Pulse-length dependence of the electrical breakdown in lipid bilayer membranes

Charge-pulse experiments were performed on artificial lipid bilayer membranes with charging times in the range between 10 ns and 10 μs. If the membranes are charged to voltages in the order of 100 mV, the membrane voltage at the end of the charge pulse is a linear function of the injected charge. However, if the membranes are charged to voltages in the range of 1 V, this relationship no longer holds and a reversible high conductance state occurs. This state is defined as an electrical breakdown and it does not allow the membranes to charge to higher voltages than the breakdown voltage, $\text{V}{}_{\mathrm{<mtext>c</mtext>}}$. Between charging times of 300 ns and 5 μs at 25°C and between 100 ns and 2 μs at 40°C, $\text{V}{}_{\mathrm{<mtext>c</mtext>}}$ showed a strong dependence on the charging time of the membrane and decreased from 1.2 to 0.5 V (25°C) and from 1 to 0.4 V (40°C). For other charging times below and above these ranges, the breakdown voltage seemed to be constant. The results indicate that the breakdown phenomenon occurs in less than 10 ns.The pulse-length dependence of the breakdown voltage is consistent with the interpretation of the electrical breakdown mechanism in terms of the electromechanical model. However, it seems possible that below a charging time of the membrane of 300 ns (25°C) and 100 ns (40°C) other processes (such as the Born energy) become possible.     

The influence of cholesterol on head group mobility in phospholipid membranes

The dielectric dispersion in the MHz range of the zwitterionic dipolar phosphocholine head groups has been measured from 0–70°C for various mixtures of $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycero-3-phosphocholine}$ (DPPC) and cholesterol. The abrupt change in the derived relaxation frequency $\text{f}{}_2$ observed for pure DPPC at the gel-to-liquid crystalline phase transition at 42°C reduces to a more gradual increase of frequency with temperature as the cholesterol content is increased. In general the presence of cholesterol increases the DPPC head group mobility due to its spacing effect. Below 42°C no sudden changes in $\text{f}{}_2$ are found at 20 or 33 mol% cholesterol, where phase boundaries have been suggested from other methods. Above 42°C, however, a decrease in $\text{f}{}_2$ at cholesterol contents up to 20–30 mol% is found. This is thought to be partly due to an additional restricting effect of the cholesterol on the number of hydrocarbon chain conformations and consequently on the area occupied by the DPPC molecules.     

Chloroplast membrane damage during freezing: the lipid phase

In order to study the effect of freeze damage to chloroplast membranes microviscosity of spinach thylakoids was probed by stearic acid spin labels. Changes in ESR parameters have been determined either as a function of temperature or during freezing at ?15 °C as a function of time. An empirical parameter $\text{h}{}_{\mathrm{+}}\text{h}{}_0$ (ratio of height of a low field line component h₊ over height of the central line h₀) proved to be very sensitive to minute changes in membrane structure.In cryoprotected chloroplast membranes Arrhenius plot breaks indicative of phase changes are observed at +15 and ?10 °C. Breaks in the Arrhenius plots were not observed in vesicles prepared from chloroplast lipids by sonication. Instead, a melting zone was indicated below ?30 °C.Freeze damage of thylakoids during storage at ?15 °C is reflected in an increase of $\text{h}{}_{\mathrm{+}}\text{h}{}_0$ and a decrease in central line width W₀. At +20 °C, differences between the ESR parameters of active as compared to freeze-damaged membranes could be detected, if the osmolarity of the suspending medium exceeded 200 mosm. The observed changes in line shapes are interpreted as an increase in mobility and/or orientation of the lipids following the swelling of thylakoids. They do not indicate a disorganization of the lipid phase. Sedimentation experiments indicated that the freeze-damaged swollen membranes still exhibited osmotic responses. It is suggested that freezing which is known to dissociate proteins from the membranes altered the charge distribution of the membranes leading first to membrane swelling and finally, by the opening of hydrophilic channels, to membrane collapse.