Diana Bach

Phospholipid/cholesterol model membranes: formation of cholesterol crystallites.

Experimental data that define conditions under which cholesterol crystallites form in cholesterol/phospholipid model membranes are reviewed. Structural features of the phospholipids that determine cholesterol crystallization include the length and degree of unsaturation of the acyl chains, the presence of charge on the headgroups and interheadgroup hydrogen bonds.

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.

Phase behaviour of heteroacid phosphatidylserines and cholesterol

Abstract The phase behavior of mixtures of cholesterol with 1-palmitoyl-2-oleoyl phosphatidylserine or with 1-stearoyl-2-oleoyl phosphatidylserine has been examined using differential scanning calorimetry and X-ray diffraction. We found that the miscibility of cholesterol in the bilayer is strongly affected by the small difference in length between the fully saturated fatty acid chains of the two phospholipids. Cholesterol crystallites are detected in the 1-palmitoyl-2-oleoyl-phosphatidylserine/cholesterol mixtures at a mol fraction of cholesterol of approximately 0.36, whereas for the mixtures with 1-stearoyl-2-oleoyl-phosphatidylserine they appear at a cholesterol mol fraction of approximately 0.2. A phase diagram, based on differential scanning calorimetry experiments without cryoprotectant, is presented for the 1-stearoyl-2-oleoyl phosphatidylserine/cholesterol system. This phase diagram indicates the marked immiscibility of cholesterol with either the gel or the liquid crystalline phase of this phospholipid.

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.

X-ray diffraction study of cholesterol−phosphatidylserine mixtures

Phosphatidylserine-cholesterol mixtures at a molar ratio of 2:1 were investigated by X-ray diffraction. Phase separation of cholesterol independent of temperature was detected, indicating limited solubility of cholesterol in phosphatidylserine bilayers. The second phase present, the mixed phospholipid-cholesterol phase, continued to undergo melting as determined by changes with temperature in both the small angle scattering profile and in the acyl chain packing.

Interaction of basic polypeptides with phospholipid monolayers

Abstract Adsorption of the polylysine and of the copolypeptides: L-lysine/L-serine and L-lysine/L-phenylalanine on phospholipid monolayers has been investigated. The charge density of the monolayers was varied by using the negatively charged phosphatidyl serine and the neutral phosphatidyl choline at different ratios. The surface concentrations of the adsorbed polypeptides was determined by measuring the surface radiation of their radioactive label. The adsorbing capacity of the monolayer surfaces increases with their negative charge, however with respect to polypeptides the surface activity sequence is pL

Interaction of 7-ketocholesterol with two major components of the inner leaflet of the plasma membrane: phosphatidylethanolamine and phosphatidylserine.

7-Ketocholesterol is one of the major forms of oxidized cholesterol found in vivo. Several toxic effects of this sterol have been documented, and it is suggested to have a role in atherosclerosis. We have studied how this oxysterol modifies the physical properties of bilayers composed of the major lipid components of the cytoplasmic leaflet of the plasma membrane. 7-Ketocholesterol is much less effective in promoting the formation of the H ii phase in phosphatidylethanolamines than cholesterol. This is likely due to the fact that 7-ketocholesterol is more polar than cholesterol and hence would be located closer to the membrane interface. However, in ternary mixtures of dipalmitoleoylphosphatidylethanolamine with low concentrations of both sterols, the effect of 7-ketocholesterol on lowering T H is enhanced. Both cholesterol and 7-ketocholesterol are very soluble in bilayers of phosphatidylethanolamine, particularly with 1-palmitoyl-2-oleoylphosphatidylethanolamine. There is, however, a much greater solubility of 7-ketocholesterol in bilayers of 1-stearoyl-2-oleoylphosphatidylserine than is the case for cholesterol. In ternary mixtures of 1-stearoyl-2-oleoylphosphatidylserine with both sterols, it appears that the solubility of cholesterol is enhanced by the presence of 7-ketocholesterol. It is thus to be expected that several of the biophysical properties of a membrane would change as a result of the oxidation of cholesterol to 7-ketocholesterol.

Transport of ions across lipoprotein monolayers adsorbed at the polarized mercury/water interface☆

Abstract The permeability of pig serum lipoprotein monolayers adsorbed at the polarized mercury/water interface to anionic and cationic depolarizers was investigated polarographically. Information on the structure of the lipoprotein monolayer at different polarizations of the surface was obtained from differential capacitance measurements at different pHs and different concentrations of lipoprotein and salt in the aqueous phase. At a low surface concentration, the lipoprotein molecules are spread out in the surface, occupying an area of 9 × 105 A2. At higher bulk concentrations of the lipoprotein and for longer exposure times of the surface after a monolayer of the molecules has spread out, the continuing adsorption results in compression and rearrangement of the monolayer, which is accompanied by a reduction in permeability. The permeability decreases with crossectional area of the permeants; it is dependent on their charge and on the electrical potential on the monolayer, contributed by the charges on the lipoprotein and on the polarized mercury surface. The permeability rate constants around the electrocapillary maximum of the different depolarizers investigated are in the following order of magnitude: T1+ > S2O−8 > CuEDTA. At high negative polarizations (- 1.05 V relative to N calomel electrode) the sequence is as follows: T1+ > CuEDTA > NAD > S2O−8.

In vitro determination of the solubility limit of cholesterol in phospholipid bilayers.

Cholesterol has limited solubility in phospholipid bilayers. The solubility limit is strongly dependent on the nature of the lipid with which the cholesterol is mixed while properties of the crystals formed can be modified by phospholipid-cholesterol interactions. In this review we summarize the various methods that have been developed to prepare hydrated mixtures of cholesterol and phospholipid. We point out some of the factors that determine the form adopted when cholesterol crystallizes in such mixtures, i.e. two- or three-dimensional, monohydrate or anhydrous. These differences can greatly affect the ability to experimentally detect the presence of these crystals in a membrane. Several methods for detecting cholesterol crystals are discussed and compared including DSC, X-ray and GIXRD diffraction methods, NMR and EPR spectroscopy. The importance of the history of the sample in determining the amount and nature of the cholesterol crystals formed is emphasized.

Interrelation between hydration and interheadgroup interaction in phospholipids.

The stability and the ionic conductivity of biological membranes and of lipid bilayers depend on their hydration. A small number of water molecules adhere strongly to the different residues of the lipid headgroups and are oriented by them. An additional number of water molecules adhere more weakly, preserving their freedom of rotation, but are essential for bestowing the thermodynamic properties of hydrated bilayers and of biological membranes. Around six water molecules are attached so strongly to the headgroups of different phospholipids (PL) that they are rendered unfreezable, or their freezing is extended over such a wide range of temperatures that it cannot be detected by differential scanning calorimetry (DSC). If cholesterol is added to the PL above the concentration at which phase separation of the cholesterol phase occurs, the number of unfreezable water molecules per PL increases, indicating that the PL molecules on the border line between the two phases attach nearly twice as many water molecules as those in the middle of the phase. The orientation of about seven or eight water molecules attached to PL headgroups (seven to phosphatidyl serine (PS)) can be detected by polarized FTIR. The dichroic ratio of the successively adhering water molecules to the headgroup of PS fluctuates between 2.6 and 2.9, with the cumulative value of about 2.8 for the seven water molecules adhering to the headgroup of PS. In addition, in this case, the number of water molecules oriented by PL molecule residues on the border line of the two phases is much larger ( approximately 13 for PS). Interaction between two opposite negatively charged layers containing PS approaching each other may lead, after correlated electrostatic attraction, to change in the conformation of the headgroups with concomitant dehydration. This process is enhanced by Ca(+) and by Li(+), but it may also occur with Na(+) and K(+) as counter-ions if the layers are mutually aligned. This process may be important in the fusion mechanism of biological membranes, and its molecular modeling has been carried out.