Interaction of dipalmitoyl phosphatidylserine with ethanol: induction of an ordered gel phase at room temperature.

Using differential scanning calorimetry and small and wide-angle X-ray diffraction, we show that, unlike the saturated phosphatidylcholines, for which ethanol induces chain interdigitation in the gel state, and unlike natural phosphatidylserine in which the gel state is almost unaffected by the addition of ethanol, dipalmitoyl phosphatidylserine (DPPS) assumes an ordered structure after incubation at room temperature in the presence of as little as 5% (v/v) ethanol. In the liquid crystalline state, a progressive decrease in the interbilayer spacing is observed as a function of ethanol concentration, similar to what is found for natural phosphatidylserine (PS) and 1-palmitoyl-2-oleoyl-phosphatidylserine (POPS). The 0.37 molar fraction of cholesterol in the DPPS dispersion in the presence of 10% (v/v) ethanol, does not prevent the formation of the ordered gel.

Phase separation of cholesterol and the interaction of ethanol with phosphatidylserine-cholesterol bilayer membranes.

Thermotropic and structural effects of ethanol on phosphatidylserine (PS) membranes containing up to 0.4 mol fraction cholesterol were investigated by differential scanning calorimetry, X-ray diffraction and fluorescence spectroscopy. It was found that in the presence of cholesterol, 10% (v/v) added ethanol depresses the melting temperature of the phospholipid by approximately 2 degrees C, similar to what was observed in the absence of cholesterol. Below the melting temperature the progressive disordering effect of added cholesterol is weakly enhanced by the presence of ethanol. In the liquid crystalline state, the marked decrease in the thickness of the bilayer which ethanol causes in the absence of cholesterol (Chem. Phys. Lipids 92 (1998) 127), is also observed in its presence. We conclude that, in contrast to what has been observed for zwitterionic phospholipids, high concentrations of cholesterol do not diminish the interaction of ethanol with PS membranes. With addition of 10% (v/v) ethanol, crystalline cholesterol diffraction, an indication of phase separation of the sterol, appears at mol fraction cholesterol 0.34, as compared to 0.3 in the absence of ethanol (Chem. Phys. Lipids 92 (1998) 71).

A new high-temperature transition of crystalline cholesterol in mixtures with phosphatidylserine.

Phosphatidylserine and cholesterol are two major components of the cytoplasmic leaflet of the plasma membrane. The arrangement of cholesterol is markedly affected by the presence of phosphatidylserine in model membranes. At relatively low mol fractions of cholesterol in phosphatidylserine, compared with other phospholipids, cholesterol crystallites are formed that exhibit both thermotropic phase transitions as well as diffraction of x-rays. In the present study we have observed and characterized a novel thermotropic transition occurring in mixtures of phosphatidylserine and cholesterol. This new transition is observed at 96 degrees C by differential scanning calorimetry (DSC), using a heating scan rate of 2 degrees C/min. Observation of the transition requires that the hydrated lipid mixture be incubated for several days, depending on the temperature of incubation. The rate of formation of the material exhibiting a transition at 96 degrees C is more rapid at higher incubation temperatures. At 37 degrees C the half-time of conversion is approximately 7 days. Concomitant with the appearance of the 96 degrees C peak the previously known transitions of cholesterol, occurring at approximately 38 degrees C and 75 degrees C on heating scans of freshly prepared suspensions, disappear. These two transitions correspond to the polymorphic transition of anhydrous cholesterol and to the dehydration of cholesterol monohydrate, respectively. The loss of the 75 degrees C peak takes a longer time than that of the 38 degrees C peak, indicating that anhydrous cholesterol first gets hydrated to the monohydrate form exhibiting a transition at 75 degrees C and subsequently is converted by additional time of incubation to an altered form of the monohydrate, showing a phase transition at 96 degrees C. After several weeks of incubation at 37 degrees C, only the form with a phase transition at 96 degrees C remains. If such a sample undergoes several successive heating and cooling cycles, the 96 degrees C peak disappears and the 38 degrees C transition reappears on heating. For samples of 1-palmitoyl-2-oleoyl phosphatidylserine or of 1-stearoyl-2-oleoyl phosphatidylserine having mol fractions of cholesterol between 0.4 and 0.7, the 38 degrees C transition that reappears after the melting of the 96 degrees C component generally has the same enthalpy as do freshly prepared samples. This demonstrates that, at least for these samples, the amount of anhydrous cholesterol crystallites formed is indeed a property of the lipid mixture. We have also examined variations in the method of preparation of the sample and find similar behavior in all cases, although there are quantitative differences. The 96 degrees C transition is partially reversible on cooling and reheating. This transition is also scan rate dependent, indicating that it is, at least in part, kinetically determined. The enthalpy of the 96 degrees C transition, after incubation of the sample for 3 weeks at 37 degrees C is dependent on the ratio of cholesterol to 1-palmitoyl-2-oleoyl phosphatidylserine or to 1-stearoyl-2-oleoyl phosphatidylserine, with the enthalpy per mole cholesterol increasing between cholesterol mol fractions of 0.2 and 0.5. Dimyristoyl phosphatidylserine at a 1:1 molar ratio with cholesterol, after incubation at 37 degrees C, exhibits a transition at 95 degrees C that reverses on cooling at 44 degrees C, instead of 60 degrees C, as observed with either 1-palmitoyl-2-oleoyl phosphatidylserine or 1-stearoyl-2-oleoyl phosphatidylserine. These findings along with the essential absence of the 96 degrees C transition in pure cholesterol or in cholesterol/phosphatidylcholine mixtures, indicates that the phospholipid affects the characteristics of the transition, and therefore the cholesterol crystallites must be in direct contact with the phospholipid and are not simply in the form of pure crystals of cholesterol. These observations are particularly important in view of recent observations of the presence of cholesterol crystals in biological systems.

Cholesterol crystalline polymorphism and the solubility of cholesterol in phosphatidylserine.

There is a marked hysteresis between the heating and cooling polymorphic phase transition of anhydrous cholesterol. At a scan rate of 0.05 degrees C/min the difference in transition temperatures between heating and cooling scans is approximately 10 degrees C. This phenomenon also occurs with mixtures of cholesterol with phosphatidylserine and can result in an underestimation of the amount of crystalline cholesterol in a sample that has not been cooled sufficiently. With 1-palmitoyl-2-oleoyl phosphatidylserine and 1-stearoyl-2-oleoyl phosphatidylserine the cholesterol crystallites form while the lipid remains in the L(alpha) phase. Sonication of dimyristoyl phosphatidylserine with a 0.4 mol fraction cholesterol results in the loss of cholesterol crystallite diffraction, but only a partial loss of the polymorphic transition detected by calorimetry. We therefore conclude that the thermal history of the sample can have profound effects on the appearance of the polymorphic phase transition of cholesterol by differential scanning calorimetry. Depending on the morphology of the vesicles, diffraction methods may underevaluate the amount of cholesterol crystallites present.

Effect of dehydroepiandrosterone on phosphatidylserine or phosphatidylcholine bilayers: DSC and X-ray diffraction study.

The effect of dehydroepiandrosterone (DHEA) on the thermotropic and structural properties of phosphatidylserine or phosphatidylcholine membranes was investigated by differential scanning calorimetry and X-ray diffraction. At molar fractions of sterol, X (sterol), less than approximately 0.2, DHEA interacts with both types of model membranes, depressing the melting temperature and reducing the enthalpy of melting. At higher concentrations, phase separation of DHEA occurs with appearance of crystallites of the S2 monohydrate form.

The effect of ethanol on the structure of phosphatidylserine bilayers.

Thermotrophic and structural effects of ethanol on phosphatidylserine (PS) membranes were investigated by differential scanning calorimetry (DSC) and X-ray diffraction. It was found that up to 15% (v/v) added ethanol, there is little change in the melting temperature of the phospholipid and no change in the interbilayer (d) spacing in the gel phase, indicating that there is no interdigitation of the hydrocarbon chains. Above the melting temperature of the phospholipid, a large decrease of the d spacing, due primarily to a decrease in the thickness of the bilayer, was found. Ethanol molecules located in the headgroup region apparently expand the area available to the headgroups with concomitant coiling of the acyl chains, resulting in marked thinning of the lipid layer.

Ligand-specific oligomerization of T-cell receptor molecules.

T cells initiate many immune responses through the interaction of their T-cell antigen receptors (TCR) with antigenic peptides bound to major histocompatibility complex (MHC) molecules. This interaction sends a biochemical signal into the T cell by a mechanism that is not clearly understood. We have used quasielastic light scattering (QELS) to show that, in the presence of MHC molecules bound to a full agonist peptide, TCR/peptide-MHC complexes oligomerize in solution to form supramolecular structures at concentrations near the dissociation constant of the binding reaction. The size of the oligomers is concentration dependent and is calculated to contain two to six ternary complexes for the concentrations tested here. This effect is specific as neither molecule forms oligomers by itself, nor were oligomers observed unless the correct peptide was bound to the MHC. These results provide direct evidence for models of T-cell signalling based on the specific assembly of multiple TCR/peptide-MHC complexes in which the degree of assembly determines the extent and qualitative nature of the transduced signal. They may also explain how T cells maintain sensitivity to antigens present in only low abundance on the antigen-presenting cell.

Cholesteryl hemisuccinate-cholesterol interaction: miscibility properties of the sterols.

Miscibility of cholesterol and cholesteryl hemisuccinate was investigated by differential scanning calorimetry and small-angle X-ray scattering. In an excess of cholesterol, above 2:1 mol ratio, phase separation takes place into a mixed phase and an almost pure cholesterol phase.

Phase behavior of mixtures of cholesterol and saturated phosphatidylglycerols.

The interaction of cholesterol with a series of saturated phosphatidylglycerols was investigated using differential scanning calorimetry and X-ray diffraction. We find that the miscibility of cholesterol in phosphatidylglycerol bilayers is lower than in the corresponding phosphatidylcholine bilayers and decreases with increasing acyl chain length of the phospholipid. The influence of the negative charge of the phosphatidylglycerol on cholesterol miscibility is discussed.

The effect of protons or calcium ions on the phase behavior of phosphatidylserine-cholesterol mixtures.

The influence of protons or calcium ions on the miscibility of cholesterol in phosphatidylserine has been examined using differential scanning calorimetry and X-ray diffraction. At pH 2.6, where the carboxyl group of the serine moiety is protonated, two endothermic transitions are observed in cholesterol-phosphatidylserine mixtures. The midpoint of the first is at 35 degrees C in the absence of cholesterol and decreases to approx. 15 degrees C for molar fraction of cholesterol 0.5. The second transition is centered at approx. 44 degrees C, almost independent of cholesterol content. The two lower temperature phases are lamellar and the high temperature phase has hexagonal symmetry. Cholesterol is more miscible in protonated phosphatidylserine than in the sodium form: cholesterol crystals are detected at a molar ratio of phosphatidylserine to cholesterol of about 1.7:1 as compared to about 2.3:1 at neutral pH. In the presence of calcium ions (1.3 Ca2+ per phosphatidylserine), a lamellar phase is observed with layer spacing 53 A which is independent of temperature (25 degrees C-65 degrees C) and of cholesterol content. Calcium ions cause reduced cholesterol solubility: crystallites are detected already at a molar ratio of 4:1.

Stabilization of halophilic malate dehydrogenase.

Malate dehydrogenase from the extreme halophile, Halobacterium marismortui, is stable only in highly concentrated solutions of certain salts. Previous work has established that its physiological environment is saturated in KCl; it remains soluble is saturated NaCl or KCl solutions; also it unfolds in solutions containing less than 2.5 M-NaCl or -KCl, salt concentrations which are still relatively high. New data show that the structure of this enzyme can be stabilized in a range of high concentrations of Mg2+ or other "salting-in" ions, also with exceptional protein-solvent interactions. "Salting-in" ions, contrary to stabilizing protein structure, usually favour unfolding. These, and most other results concerning the structure, stability and solvent interactions of the protein cannot be understood in terms of the usual effects of salts on protein structure. In this paper, a novel stabilization model is proposed for halophilic malate dehydrogenase that can account for all observations so far. The model results from experiments on the protein in salt solutions chosen for their different effects on protein stability (potassium phosphate, a strongly "salting-out" agent, and MgCl2, which is "salting-in"), and previously published data from NaCl and KCl solutions (mildly "salting-out"). Enzymic activity and stability measurements were combined with neutron scattering, ultracentrifugation and quasi-elastic light-scattering experiments. The analysis showed that the structure of the protein in solution as well as the dominant stabilization mechanisms were different in different salt solutions in which this enzyme is active. Thus, in molar concentrations of phosphate ions, stabilization and hydration are similar to those of non-halophilic soluble proteins, in which the hydrophobic effect dominates. In high concentrations of KCl, NaCl or MgCl2, on the other hand, solution particles are formed in which the protein dimer interacts with large numbers of salt and water molecules (the mass of solvent molecules involved depends on the nature of the salt but it is approximately equivalent to the protein mass). It is proposed that, under these conditions, the hydrophobicity of the protein core is too weak to stabilize the folded structure and the main stabilization mechanism is the formation of co-operative hydrate bonds between the protein and hydrated salt ions. Model predictions are in agreement with all experimental results, such as the different numbers of solvent molecules found in the solution particles formed with different salts, the loss of the exceptional solvent interactions concomitant with unfolding at non-physiological salt concentrations, and the different temperature denaturation curves observed for different salt solutions.(ABSTRACT TRUNCATED AT 400 WORDS)

Macromolecular assemblies of myosin.

The self-assembly of myosin into filamentous structures is a highly cooperative and rapid process. Nevertheless, the presence of nonequivalent bonding interactions within the filament permits differential stabilization of several macromolecular assemblies of myosin under well-controlled ionic conditions in citrate/Tris buffer at pH 8.0. We have detected and characterized bipolar myosin minifilaments, myosin octamers, and tetramers by using light scattering, analytical ultracentrifugation, and viscosity techniques. These structures have molecular weights of 8.0 X 10(6), 3.9 X 10(6) g/mol, sedimentation coefficients of 32S, 22S, and 18S, and radii of gyration of 990 A, 890 A and 790, A, respectively. The similar radii of gyration indicate similar bipolar geometry for all these particles. The 32S minifilaments in 10 mM citrate/Tris buffer (pH 8.0) are the most stable species. The smaller 18S and 22S assemblies in 2 mM and 5 mM citrate/Tris, pH 8.0, are readily affected by low concentrations of KCl and fuse into the minifilament particles. The instability of the 18S and 22S forms of myosin assembly is also revealed by their titration with ATP. These structures are dissociated at lower ATP concentrations than the minifilaments and do not show the cooperative dissociation transitions characteristic of filaments and minifilaments. Sedimentation velocity analysis of the 18S and 22S species in the presence of ATP reveals the involvement of 10S myosin dimer in the dissociation of assembled myosin. The different forms of assembled myosin are discussed in the context of formation of myosin minifilaments.

Monomers, dimers, and minifilaments of vertebrate skeletal myosin in the presence of sodium pyrophosphate.

The self-assembly of myosin in the presence of sodium pyrophosphate was studied in the pH range between 7.0 and 8.5. As evidenced by sedimentation velocity (S0(20,w) = 6.30 S) and light-scattering measurements (molecular weight of 470 000; radius of gyration = 45 nm), myosin existed in a predominantly monomeric form in the presence of 5 mM sodium pyrophosphate at pH 8.5 and above. The concentration-dependent monomer-dimer equilibrium could be easily shifted toward dimeric species at pH 8.0 in the presence of 5 mM sodium pyrophosphate and 5 mM 2-[bis(2-hydroxyethyl)amino]-2-(hydroxymethyl)-1,3-propanediol. The estimated parameters of the dimeric particles were S0(20,w) between 10 and 11 S, molecular weight of 1.1 X 10(6), and radius of gyration = 52 nm. These results are consistent with a head to tail (parallel) arrangement of staggered myosin molecules in the dimer. At lower pH values (7.5), and in the presence of 10 mM sodium pyrophosphate, the monomer-dimer species were in dynamic equilibrium with myosin minifilaments. At pH 7.0, the minifilaments appeared to be the only detectable species present in solutions of myosin in 5 mM sodium pyrophosphate. The molecular parameters of these minifilaments, including sedimentation and viscosity coefficients, molecular weight, radius of gyration, and morphological appearance, were almost indistinguishable from those obtained for myosin minifilaments prepared in 10 mM citrate-tris(hydroxymethyl)aminomethane at pH 8.0 [Reisler, E., Smith, C., & Seegan, G. (1980) J. Mol. Biol. 143, 129-145]. The equilibrium polymerization reactions of myosin in sodium pyrophosphate are discussed in the context of minifilament assembly.

Interaction of chromatin with NaCl and MgCl2. Solubility and binding studies, transition to and characterization of the higher-order structure.

Chicken erythrocyte chromatin containing histones H1 and H5 was carefully separated into a number of well-characterized fractions. A distinction could be made between chromatin insoluble in NaCl above about 80 mM, and chromatin soluble at all NaCl concentrations. Both chromatin forms were indistinguishable electrophoretically and both underwent the transition from the low salt "10 nm" coil to the "30 nm" higher-order structure solenoid by either raising the MgCl2 concentration to about 0.3 mM or the NaCl concentration to about 75 mM. The transitions were examined in detail by elastic light-scattering procedures. It could be shown that the 10 nm form is a flexible coil. For the 30 nm solenoid, the assumption of a rigid cylindrical structure was in good agreement with 5.7 nucleosomes per helical turn. However, disagreement of calculated frictional parameters with values derived from quasielastic light-scattering and sedimentation introduced the possibility that the higher-order structure, under these conditions, is more extended, flexible, or perhaps a mixture of structures. Values for density and refractive index increments of chromatin are also given. To understand the interaction of chromatin with NaCl and with MgCl2, a number of experiments were undertaken to study solubility, precipitation, conformational transitions and binding of ions over a wide range of experimental conditions, including chromatin concentration.

Interaction and conformational changes of chromatin with divalent ions.

We have investigated the interaction of divalent ions with chromatin towards a closer understanding of the role of metal ions in the cell nucleus. The first row transition metal ion chlorides MnCl2, CoCl2, NiCl2 and CuCl2 lead to precipitation of chicken erythrocyte chromatin at a significantly lower concentration than the alkali earth metal chlorides MgCl2, CaCl2 and BaCl2. A similar distinction can be made for the compaction of chromatin to the "30 nm" solenoid higher order structure which occurs at lower MeCl2 concentration in the first group but at the same MeCl2 concentration within each group. In other experiments in which mixed solutions of NaCl and of MgCl2 were examined, it is shown that increasing NaCl concentration leads to increasing solubility in the presence of MgCl2. Best compaction of chromatin was obtained at 40 mM NaCl and 0.8 mM MgCl2 at a value A260 approximately 0.8. Similar experiments were undertaken with mixtures of NaCl and MnCl2.

Isolation and physical studies of the intact supercoiled, the open circular and the linear forms of ColE1-plasmid DNA.

For the study of DNA conformations, conformational transitions, and DNA-protein interactions, covalently closed supercoiled ColE1-plasmid DNA has been purified from cultures of Escherichia coli harboring this plasmid and grown in the presence of chloramphenicol according to the method of D.B. Clewell [J. Bact. 110 (1972)667]. The open circular and linear forms of the plasmid were prepared by digestion of the covalently closed, supercoiled form with pancreatic deoxyribonuclease and EcoRI-restriction endonuclease, respectively. The linear form was found to be very homogeneous by electron microscopy and sedimenting boundary analysis. Its physical properties (s0 20,w=16.3 S,D0 20,W=1.98 X 10(-8) cm2 s-1 and [eta]=2605 ml g-1) have been carefully determined in 0.2 M NaCl, 0.002 M NaPO4 pH 7.0,0.002 M EDTA, at 23 degrees C. Combination of s0 20, w (obtained by quasielastic laser light scattering) gave Ms,D=4.39 x 10(6). This value is in reasonable agreement with the molecular weight from total intensity laser light scattering M=4.30 x 10(6). The covalently closed and open circular forms of the ColE1-plasmid are less homogeneous due to slight cross-contamination and the presence of small amounts of dimers in these preparations. The weight fractions of the various components as determined by boundary analysis or electron microscopy are given together with the average quantities obtained in the same solvent for the supercoiled form ((s0 20,w)w=25.4 S, (D0 20,w)z=2.89 x 10(-8) cm2 s-1, [eta]= 788 ML G-1,Ms,D=4.69 x 10(6) and Mw=4.59 x 10(6)) and the open circular form (s0 20, w)w=20.1 S, (D0 20,w)z=2.45 x 10(-8) cm2 s-1, [eta]=1421 ml g-1,Ms,D=4.37 x 10(6) and Mw=4.15 x 10(6)). Midpoint analysis of the sedimenting boundaries allows unambiguous determination of the sedimentation coefficients of these two forms: s0 20,w=24.5 S and s0 20,w=18.8 S, respectively. Also deduced from total intensity light scattering were radii of gyration Rg (103.5, 134.2 and 186 nm) and second virial coefficients A2 (0.7, 4.8 AND 5.4 x 10(-4) mole ml/g2) for the supercoiled, the open circular and linear forms, respectively. The data presented are discussed in relation to the conformational parameters for the three forms in solution.