Squeezing of Oil-Swollen Surfactant Bilayers by a Membrane Protein

Compact polar moieties induce lipid-water systems to form discontinuous reverse micellar phase

The role of molecular interactions in governing lipid mesophase organization is of fundamental interest and has technological implications. Herein, we describe an unusual pathway for monoolein/water reorganization from a bicontinuous mesophase to a discontinuous reverse micellar assembly, directed by the inclusion of polar macromolecules. This pathway is very different from those reported earlier, wherein the Fd3m phase formed only upon addition of apolar oils. Experiments and molecular dynamics simulations indicate that hydrophilic ternary additives capable of inducing discontinuous phase formation must (i) interact strongly with the monoolein head group and (ii) have a compact molecular architecture. We present a detailed investigation that contrasts a monoolein-water system containing polyamidoamine (PAMAM) dendrons with one containing their linear analogs. The Fd3m phase forms only on the addition of PAMAM dendrons but not their linear analogs. Thus, the dendritic architecture of PAMAM plays an important role in determining lipid mesophase behavior. Both dendrons and their linear analogs interact strongly with monoolein through their amine groups. However, while linear polymers adsorb and spread on monoolein, dendrons form aggregates that interact with the lipid. Dendrons induce formation of an intermediate reverse hexagonal phase, which subsequently restructures into the Fd3m phase. Finally, we demonstrate that other additives with compact structures that are known to interact with monoolein, such as branched polyethylenimine and polyhedral silsesquioxane cages, also induce the formation of the Fd3m phase.

Effects of grafted polymer chains on lamellar membranes

We have investigated the effects of grafted polymer chains [poly(ethylene oxide)-poly(propylene oxide)-poly(ethylene oxide)] on the bending modulus and the intermembrane interactions of lamellar membranes (C(12)E(5) water) by means of a neutron spin-echo and a small-angle x-ray scattering technique. In this study the hydrophilic chain takes the mushroom configuration on the membrane. The bending modulus of the polymer-grafted membranes increases in proportion to the square of the end to end distance of the polymer chain, which agrees well with the theoretical prediction of Hiergeist and Lipowsky [J. Phys. II 6, 1465 (1996)]. From the interlamellar interaction point of view, the mushroom layer is renormalized to the membrane thickness, which enhances the repulsive Helfrich interaction. When the size of the decorated polymer chain increases to the interlamellar distance, however, the mushroom is squeezed so as to optimize the interlamellar potential. Further increase of the grafted polymer size brings a lamellar-lamellar phase separation, where the grafted polymer chains are localized in the dilute lamellar phase and the concentrated lamellar phase forms the onionlike texture.

Dramatic rigidification of a peptide-decorated lamellar phase

We have performed small-angle x-ray scattering on a lamellar (L(alpha)) phase made of a nonionic surfactant (C12E4), decane, and water, after the insertion of a triblock peptide. The hydrophilic part of the peptide is rigid and organized in an alpha helix in the presence of membranes. Surface tension measurements and spectrofluorometry show that the peptide lies on the membrane surface. The Caillé parameter eta and the smectic compressibility modulus (-)B decrease with peptide concentration, whereas the membrane bending rigidity kappa increases threefold for mole ratio of peptide to surfactant as low as 5.2 x 10(-4). The published models for rigid inclusions in membranes cannot account for this dramatic rigidification. However, experimental results are well fitted by a Heuristic renormalization of the membrane thickness.

Unbinding-binding transition induced by molecular snaps in model membranes

We have used a lamellar phase made of a nonionic surfactant, dodecane and water, as a model membrane to investigate its interactions with macromolecular inclusions bringing together two membranes, i.e., acting as macromolecular snaps. In systems devoid of inclusions, the interlamellar distance depends on the total volume fraction of membranes Phi. We show that, in presence of a transmembrane protein, or of several de novo designed peptides of different length and composition, the lamellar phase undergoes a binding transition. Under such conditions, the interlamellar distance is no longer proportional to Phi(-1), but rather to the surface concentration of snaps within the membrane. It also appears that, in the presence of the hydrophobic segment of peptide snaps, the length of the inclusions must be at least equal to the hydrophobic length of the membrane to be active. Experimental results have been precisely fitted to a model of thermally stabilized membranes, decorated with snaps. However, in the presence of inclusions, the parameter describing the interactions between membranes, has to take into account the length of the inclusion to preserve good predictive capabilities.

Inclusions on fluid membranes anchored to elastic media

We model theoretically the effect of localized forces on a fluid membrane anchored to a uniform elastic medium. We use this as a simple model for the plasma membrane of a cell. The atomic force microscope (AFM) has been used to apply such forces, but large membrane perturbations occurring in vivo are also treated within the same framework. Inclusions of this nature may include cell junctions, filipodia, caveolae, and similar membrane invaginations. The breakdown of linear elastic response, as observed by AFM, is predicted to occur for forces as small as 10 pN. We estimate the position of this crossover and the subsequent nonlinear behavior and make encouraging quantitative comparison with experiments. Intrinsic membrane inclusions interact through their overlapping strain fields. For similar, point force-like inclusions at large separations, this yields an attractive potential that scales like the inverse of their separation. For membranes that are intrinsically stiff or under tension, the binding force between inclusions can depend on the properties of the membrane and may be large enough to induce aggregation of inclusions, as observed experimentally. For inclusions that fix the magnitude of the membrane deformation, rather than the applied force, we demonstrate the possibility of metastable states, corresponding to finite separations. Finally, we discuss briefly the case in which inclusions couple to the membrane in more complex ways, such as via a torque (twist). In such cases, the interaction scales like a higher power of the separation, depends on the orientation of the inclusions, and can have either sign.