Influence of stigmastanol and stigmastanyl-phosphorylcholine, two plasma cholesterol lowering substances, on synthetic phospholipid membranes. A 2H- and 31P-NMR study

Order parameters and areas in fluid-phase oriented lipid membranes using wide angle X-ray scattering

We used wide angle x-ray scattering (WAXS) from stacks of oriented lipid bilayers to measure chain orientational order parameters and lipid areas in model membranes consisting of mixtures of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC)/cholesterol and 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC)/cholesterol in fluid phases. The addition of 40% cholesterol to either DOPC or DPPC changes the WAXS pattern due to an increase in acyl chain orientational order, which is one of the main properties distinguishing the cholesterol-rich liquid-ordered (Lo) phase from the liquid-disordered (Ld) phase. In contrast, powder x-ray data from multilamellar vesicles does not yield information about orientational order, and the scattering from the Lo and Ld phases looks similar. An analytical model to describe the relationship between the chain orientational distribution and WAXS data was used to obtain an average orientational order parameter, S(x-ray). When 40% cholesterol is added to either DOPC or DPPC, S(x-ray) more than doubles, consistent with previous NMR order parameter measurements. By combining information about the average chain orientation with the chain-chain correlation spacing, we extended a commonly used method for calculating areas for gel-phase lipids to fluid-phase lipids and obtained agreement to within 5% of literature values.

Structure and dynamics of phospholipid bilayers using recently developed general all-atom force fields

Two fully hydrated pure-species phospholipids bilayers, 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) and 1,2-dioleoyl-sn-glycero-3-phosphorylcholine (DOPC), in the fluid phase and explicit solvent have been studied using molecular dynamics simulation. Atom interactions were modeled using recently developed force fields based on AMBER with full atomistic details. Several representative liquid phase properties for the structure and dynamics of lipids with different length of hydrocarbon chains and different level of saturation have been reproduced without artificially biasing the system in order to match experimental data. In particular, as the new GAFF (General Amber Force Field) has not been explicitly developed to reproduce lipid characteristics and is naturally compatible with standard AMBER nucleic acids and proteins parameters, it is here proven a promising tool to study mixed lipid-protein processes as protein activity dependence on membrane composition, permeation of solute across membranes, and other cellular processes.

1H-13C polarization transfer in membranes: a tool for probing lipid dynamics and the effect of cholesterol

Phospholipid bilayers with over 20% cholesterol can form a liquid-ordered (l(o)) phase, which can be found in lateral domains, called rafts, in biomembranes. We show here that high-resolution (13)C and (1)H solid-state NMR are well suited to explore this phase, intermediate between gel and fluid. This approach can be applied to artificial or natural membranes, with no isotopic enrichment and with the help of magic-angle spinning (MAS), taking advantage of the high resolution and sensitivity of these nuclei. The sensitivity of magnetization transfer schemes to different lipid states has allowed us here to discriminate between various phases. We show that the phase composed of unsaturated phospholipids and cholesterol differs, in terms of lipid dynamics, both from the previously described l(o) phase and from the liquid-disordered phase.

Order parameters of unsaturated phospholipids in membranes and the effect of cholesterol: a 1H-13C solid-state NMR study at natural abundance

Most biological phospholipids contain at least one unsaturated alkyl chain. However, few order parameters of unsaturated lipids have been determined because of the difficulty associated with isotopic labeling of a double bond. Dipolar recoupling on axis with scaling and shape preservation (DROSS) is a solid-state nuclear magnetic resonance technique optimized for measuring (1)H-(13)C dipolar couplings and order parameters in lipid membranes in the fluid phase. It has been used to determine the order profile of 1,2-dimyristoyl-sn-glycero-3-phosphocholine hydrated membranes. Here, we show an application for the measurement of local order parameters in multilamellar vesicles containing unsaturated lipids. Taking advantage of the very good (13)C chemical shift dispersion, one can easily follow the segmental order along the acyl chains and, particularly, around the double bonds where we have been able to determine the previously misassigned order parameters of each acyl chain of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC). We have followed the variation of such order profiles with temperature, unsaturation content and cholesterol addition. We have found that the phase formed by DOPC with 30% cholesterol is analogous to the liquid-ordered (l(o)) phase. Because these experiments do not require isotopic enrichment, this technique can, in principle, be applied to natural lipids and biomembranes.

Interaction of pulmonary surfactant protein SP-A with DPPC/egg-PG bilayers

In the mixture of lipids and proteins which comprise pulmonary surfactant, the dominant protein by mass is surfactant protein A (SP-A), a hydrophilic glycoprotein. SP-A forms octadecamers that interact with phospholipid bilayer surfaces in the presence of calcium. Deuterium NMR was used to characterize the perturbation by SP-A, in the presence of 5 mM Ca(2+), of dipalmitoyl phosphatidylcholine (DPPC) properties in DPPC/egg-PG (7:3) bilayers. Effects of SP-A were uniformly distributed over the observed DPPC population. SP-A reduced DPPC chain orientational order significantly in the gel phase but only slightly in the liquid-crystalline phase. Quadrupole echo decay times for DPPC chain deuterons were sensitive to SP-A in the liquid-crystalline mixture but not in the gel phase. SP-A reduced quadrupole splittings of DPPC choline beta-deuterons but had little effect on choline alpha-deuteron splittings. The observed effects of SP-A on DPPC/egg-PG bilayer properties differ from those of the hydrophobic surfactant proteins SP-B and SP-C. This is consistent with the expectation that SP-A interacts primarily at bilayer surfaces.

Interactions of cyclosporines with lipid membranes as studied by solid-state nuclear magnetic resonance spectroscopy and high-sensitivity titration calorimetry

Cyclosporin A (CyA) interacts with lipid membranes. Binding reaction and membrane location of CyA and analogs were examined with 2H-NMR, high-sensitivity isothermal titration calorimetry (ITC), and CD spectroscopy. Effects of CyA and charged analogs on the phosphocholine head group and on the membrane interior were investigated using selectively deuterated phospholipids. Incorporation of cyclosporin generated small disordering of the lipid acyl chains. Binding of CyA and neutral and positively charged analogs to lipid membranes showed endothermic heats of reaction between + 5.9 and + 11.3 kcal/mol, whereas enthalpy of binding was close to zero for the negatively charged derivative. Binding constants of cyclosporines to liposomal membranes were in the range of K(P) = 1650-5560 M(- 1) depending on the cholesterol content. (2)H-NMR provides evidence that CyA is essentially located in the interior of the bilayer membrane. For the charged analogs an additional interaction occurs at the head group level, placing the polar groups of these CyA analogs in the vicinity of the phosphocholine dipoles. The association of CyA and its analogs is accompanied by a positive enthalpy change, which is overcompensated by positive entropy changes. Binding of CyA to lipid membranes thus follows the classical hydrophobic effect, which is in contrast to many other peptide-lipid binding reactions.

Interaction of the neuronal marker dye FM1-43 with lipid membranes. Thermodynamics and lipid ordering

The fluorescent dye FM1-43 labels nerve terminals in an activity-dependent fashion and has been found increasingly useful in exploring the exo- and endocytosis of synaptic vesicles and other cells by fluorescence methods. The dye distributes between the aqueous phase and the lipid membrane but the physical-chemical parameters characterizing the adsorption/partition equilibrium have not yet been determined. Fluorescence spectroscopy alone is not sufficient for a detailed elucidation of the adsorption mechanism since the method can be applied only in a rather narrow low-concentration window. In addition to fluorescence spectroscopy, we have therefore employed high sensitivity isothermal titration calorimetry (ITC) and deuterium magnetic resonance (2H-NMR). ITC allows the measurement of the adsorption isotherm up to 100 microM dye concentration whereas 2H-NMR provides information on the location of the dye with respect to the plane of the membrane. Dye adsorption/partition isotherms were measured for neutral and negatively-charged phospholipid vesicles. A non-linear dependence between the extent of adsorption and the free dye concentration was observed. Though the adsorption was mainly driven by the insertion of the non-polar part of the dye into the hydrophobic membrane interior, the adsorption equilibrium was further modulated by an electrostatic attraction/repulsion interaction of the cationic dye (z=+2) with the membrane surface. The Gouy-Chapman theory was employed to separate electrostatic and hydrophobic effects. After correcting for electrostatic effects, the dye-membrane interaction could be described by a simple partition equilibrium (Xb=Kcdye) with a partition constant of 103-104 M-1, a partition enthalpy of DeltaH=-2.0 kcal/mol and a free energy of binding of DeltaG=-7.8 kcal/mol. The insertion of FM1-43 into lipid membranes at room temperature is thus an entropy-driven reaction following the classical hydrophobic effect. Deuterium nuclear magnetic resonance provided insight into the structural changes of the lipid bilayer induced by the insertion of FM1-43. The dye disturbed the packing of the fatty acyl chains and decreased the fatty acyl chain order. FM1-43 also induced a conformational change in the phosphocholine headgroup. The -P-N+ dipole was parallel to the membrane surface in the absence of dye and was rotated with its positive end towards the water phase upon dye insertion. The extent of rotation was, however, much smaller than that induced by other cationic molecules of similar charge, suggesting an alignment of FM1-43 such that the POPC phosphate group is sandwiched by the two quaternary FM1-43 ammonium groups. In such an arrangement the two cationic charges counteract each other in a rotation of the -P-N+ dipole.

Plant sterols: a neutron diffraction study of sitosterol and stigmasterol in soybean phosphatidylcholine membranes

Neutron scattering experiments have been performed on oriented Soybean phosphatidylcholine (SPC) bilayers, containing sitosterol or stigmasterol, two major sterols of plant plasma membranes. Sitosterol and stigmasterol were either protonated or deuterated on position C25 of the lateral chain. Incorporation of sitosterol leads to an increase of the hydrophobic thickness of SPC bilayers of 1.2 and 2 A when present, at 16 and 30 mol%, respectively. On the other hand, no change was observed when stigmasterol is present in the bilayer at its maximal solubility of 16 mol%. These results are in agreement with the fact that sitosterol is more efficient than stigmasterol to order acyl chains of SPC, as already shown with other biophysical techniques. In order to get more insight into the behavior of the lateral chains of the two sterols, the proton-deuterium contrast method was used in order to locate the (2)H25 atoms of the two sterols. For sitosterol, this atom was found close to the center of the bilayer at +/-(1.6+/-0.2 A), with a width, nu=2.5+/-0.5 A. For stigmasterol, the difference profile could be fitted in two different ways: either two possible locations are found at +/-(2.3+/-0.2 A) and +/-(10+/-0.2 A) with the same width, nu=2.5+/-0.5 A or only one broad distribution at +/-(6.1+/-0.3 A), nu=8.5+/-0.7 A. The results are discussed in terms of difference of dynamics for the lateral chain of the two sterols.