A single lipid molecular bilayer of 17 or 18 carbon chain phosphocholines, floating in water near a flat wall, is prepared in the bilayer gel phase and then heated to the fluid phase. Its structure (electron density profile) and height fluctuations are determined by using x-ray reflectivity and nonspecular scattering. By fitting the offspecular signal to that calculated for a two-dimensional membrane using a Helfrich Hamiltonian, we determine the three main physical quantities that govern the bilayer height fluctuations: The wall attraction potential is unexpectedly low; the surface tension, roughly independent on chain length and temperature, is moderate (Ϸ5 ؋ 10 ؊4 J⅐m ؊2 ) but large enough to dominate the intermediate range of the fluctuation spectrum; and the bending modulus abruptly decreases by an order-of-magnitude from 10 ؊18 J to 10 ؊19 J at the bilayer gel-to-fluid transition. L ipid bilayers (1, 2) have been often studied as models of two-dimensional soft systems (3). They are increasingly used as controlled idealized models of cell membranes for biophysical studies of membrane-membrane and membrane-protein interactions (1, 4). Lipid bilayers can be characterized by their static structure and dynamic, equilibrium thermal fluctuations. Structural measurements yield information on the variation of chemical composition (using neutrons) or electron density (using x-rays) along the z axis normal to the bilayer plane (for a review, see ref. 5). Thermal fluctuations of the bilayer plane are classically described (6) within the harmonic approximation originally proposed by Helfrich (3) with three physical quantities: (i) The intrinsic bilayer bending modulus stabilizes fluctuations with short in-plane (x, y) wavelengths; (ii) the surface tension ␥, if strong enough, dominates the intermediate scales; and (iii) an external potential per unit surface, U, due, for instance, to the attraction by a nearby surface or neighboring bilayers, stabilizes (through its second derivative UЉ ϭ d 2 U͞dz 2 ) large in-plane wavelength fluctuation modes. The cross-over between these regimes is usually [with few exceptions (7)] at submicronic scales and more accessible to x-ray off-specular surface scattering than to optical microscopy measurements.A considerable effort has been devoted to the measurement of the bending rigidity , which controls both the physical properties (bilayer fluctuations and vesicle shape) and biophysical properties (adhesion, invagination, and membrane-protein interactions) of the bilayers (2,4,8). Experiments have been based on indirect effects (9, 10) or on the direct determination (7) of the fluctuation spectrum, usually on vesicles (7, 11) or on multilayer stacks (5, 12). They have yielded results mostly in the fluid phase (7, 9, 11, 13-16) but also in the gel phase (17) and, more recently, as a function of temperature across the melting transition (10,18,19).We report an experimental determination of the structure and fluctuations of a lipid bilayer, in a planar configuration (in the vicinity of an...
The phase behavior of a supported dimyristoylphosphatidylcholine (DMPC) bilayer system has been investigated using neutron reflectivity. The bilayer is fabricated by a combination of Langmuir-Blodgett, Langmuir-Schaeffer, and self-assembly techniques, and while robustly associated with the substrate, the bilayer remains separated from it by a substantial layer of water, due to a Helfrich type entropic repulsion. The reflectivity data have been analyzed using a quasi-molecular model, similar to that used by Wiener and White (Wiener et al. Biophys. J. 1992, 61, 434-447) allowing easy comparison of the bilayer structure with other systems such as vesicles. The area per molecule (APM) and bilayer thickness in the gel phase are found to be identical to those in DMPC vesicles. In going from the gel phase to the fluid phase, the bilayer thickness decreases and the APM increases due to chain melting. This suggests that the bilayer is minimally constrained, since the bilayer structure seems to be determined by the packing requirements of the phospholipids rather than any influence of the substrate. The hydrating layer is thicker than in vesicles, and we suggest that this may be due to differences in the confinement regime. That is, a bilayer in a multilamellar vesicle is constrained on both sides, whereas the bilayer studied here is confined on one side only. Nevertheless, the thickness of the intervening water layer decreases across the main transition in the same way as is seen in multilamellar systems.
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