The concentration of cholesterol in cell membranes affects membrane fluidity and thickness, and might regulate different processes such as the formation of lipid rafts. Since interpreting experimental data from biological membranes is rather intricate, investigations on simple models with biological relevance are necessary to understand the natural systems. We study the effect of cholesterol on the molecular structure of multi-lamellar vesicles (MLVs) composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), a phospholipid ubiquitous in cell membranes, with compositions in the range 0-60 mol% cholesterol. Order parameters, |S(CH)|, are experimentally determined by using (1)H-(13)C solid-state nuclear magnetic resonance (NMR) spectroscopy with segmental detail for all parts of both the cholesterol and POPC molecules, namely the ring system and alkyl chain of the sterol, as well as the glycerol backbone, choline headgroup and the sn-1 and sn-2 acyl chains of POPC. With increasing cholesterol concentration the acyl chains gradually adopt a more extended conformation while the orientation and dynamics of the polar groups are rather unaffected. Additionally, we perform classical molecular dynamics simulations on virtual bilayers mimicking the POPC-cholesterol MLVs investigated by NMR. Good agreement between experiments and simulations is found for the cholesterol alignment in the bilayer and for the |S(CH)| profiles of acyl chains below 15 mol% cholesterol. Deviations occur for the choline headgroup and glycerol backbone parts of POPC, as well as for the phospholipid and cholesterol alkyl chains at higher cholesterol concentrations. The unprecedented detail of the NMR data enables a more complete comparison between simulations and experiments on POPC-cholesterol bilayers and may aid in developing more realistic model descriptions of biological membranes.
Although it is well described in model membranes, little is known about phase separation in biological membranes. Here, we provide evidence for a coexistence of at least two different lipid bilayer phases in the apical plasma membrane of epithelial cells. Phase connectivity was assessed by measuring long-range diffusion of several membrane proteins by fluorescence recovery after photobleaching in two polarized epithelial cell lines and one fibroblast cell line. In contrast to the fibroblast plasma membrane, in which all of the proteins diffused with similar characteristics, in the apical membrane of epithelial cells the proteins could be divided into two groups according to their diffusion characteristics. At room temperature (Ϸ25°C), one group showed fast diffusion and complete recovery. The other diffused three to four times slower and, more importantly, displayed only partial recovery. Only the first group comprises proteins that are believed to be associated with lipid rafts. The partial recovery is not caused by topological constraints (microvilli, etc.), cytoskeletal constraints, or protein-protein interactions, because all proteins show 100% recovery in fluorescence recovery after photobleaching experiments at 37°C. In addition, the raft-associated proteins cannot be coclustered by antibodies on the apical membrane at 12°C. The interpretation that best fits these data is that the apical membrane of epithelial cells is a phaseseparated system with a continuous (percolating) raft phase <25°C in which isolated domains of the nonraft phase are dispersed, whereas at 37°C the nonraft phase becomes the continuous phase with isolated domains of the raft phase dispersed in it.fluorescence recovery after photobleaching ͉ rafts ͉ paurdan ͉ liquid-ordered ͉ Madin-Darby-canine kidney T he domain organization of biological membranes is presently under intense scrutiny. In particular, the existence and role of sphingomyelin-and cholesterol-rich lipid bilayer phases, commonly known as rafts, have drawn much attention (1-5). Phase diagrams of model membrane systems made from ternary mixtures of sphingomyelin, 1-palmitoyl-2-oleoylphosphatidylcholine, and cholesterol show regions of fluid-fluid phase coexistence (6). The two fluid phases of special relevance are a liquid-ordered phase, characterized by high conformational and low translational order, and a liquid-disordered phase, characterized by low conformational and translational order (7,8). The coexistence of these two phases has been visualized by several laboratories in giant unilamellar vesicles and supported lipid bilayers prepared from synthetic lipids. More importantly, giant unilamellar vesicles prepared from cell membrane lipid extracts (9) also show visible fluid-fluid phase coexistence. However, there was no direct evidence for phase separation in native cell membranes (2, 5). Glycosylphosphatidylinositol (GPI)-anchored proteins in the exoplasmic leaflet (10, 11) and lipid-anchored proteins in the cytoplasmic leaflet (12-14) of cell membranes were shown to b...
One of the great challenges in membrane biophysics is to find a means to foster the transport of drugs across complex membrane structures. In this spirit, we elucidate methodological challenges associated with free energy computations of complex chainlike molecules across lipid membranes. As an appropriate standard molecule to this end, we consider 7-nitrobenz-2-oxa-1,3-diazol-4-yl-labeled fatty amine, NBD-Cn, which is here dealt with as a homologous series with varying chain lengths. We found the membrane-water interface region to be highly sensitive to details in free energy computations. Despite considerable simulation times, we observed substantial hysteresis, the cause being the small frequency of insertion/desorption events of the amphiphile's alkyl chain in the membrane interface. The hysteresis was most pronounced when the amphiphile was pulled from water to the membrane and compromised the data that were not in line with experiments. The subtleties in umbrella sampling for computing distance along the transition path were also observed to be potential causes of artifacts. With the PGD (pull geometry distance) scheme, in which the distance from the molecule was computed to a reference plane determined by an average over all lipids in the membrane, we found marked deformations in membrane structure when the amphiphile was close to the membrane. The deformations were weaker with the PGC (pull geometry cylinder) method, where the reference plane is chosen based on lipids that are within a cylinder of radius 1.7 nm from the amphiphile. Importantly, the free energy results given by PGC were found to be qualitatively consistent with experimental data, while the PGD results were not. We conclude that with long amphiphiles there is reason for concern with regard to computations of their free energy profiles. The membrane-water interface is the region where the greatest care is warranted.
The interaction of small molecules, such as drugs or metabolites, with proteins and biomembranes is of fundamental importance for their bioavailability. The systematic characterization of the binding affinity for structurally related ligands may provide rules that allow its prediction for any other relevant molecule. In this work we have studied a homologous series of fluorescent fatty amines with the fluorescent moiety 7-nitrobenz-2-oxa-1,3-diazol-4-yl covalently bound to the amine group (NBD-C(n); n = 4, 6, 8, 10, 12, 14, and 16) in aqueous solution and associated with BSA or lipid bilayers. We have found a linear dependence with the length of the alkyl chain, up to NBD-C(10), for the Gibb's free energy of partition between the aqueous solution and 1-palmitoyl-2-oleoyl phosphatidylcholine bilayers equal to ΔΔG = -2.5 ± 0.3 kJ/mol per methylene group. Additionally, the amphiphiles interacted efficiently with bovine serum albumin, and it was inhibited by fatty acids indicating that binding occurs to the fatty acids highest affinity binding site. The association of the amphiphiles with BSA and POPC bilayers was performed at different temperatures (15-35 °C) allowing for the calculation of the enthalpic and entropic contributions. A value of ΔH = -15 ± 4 kJ/mol was obtained for all amphiphiles and binding agents. The entropy contribution was always positive and increased with the length of the alkyl chain. The location of the ligand in the biological membrane is also of high relevance, namely because this will determine its effect on biomembrane properties at high ligand concentrations. With this goal, we have measured some photophysical properties of the amphiphiles inserted in POPC bilayers, and we found no significant variation along the series, indicating that the NBD group is located in a region with similar properties regardless of the length of the nonpolar group. An exception was noted for the case of NBD-C(14) whose parameters were somewhat different from the trend observed.
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