PACS. 68.10 -Fluid surfaces and interfaces with fluids (inc. surface tension, capillarity, wetting and related phenomena).
FACS. 68.80 -Dynamics of solid surfaces and interface vibrations.Abstract. -We detennine the dispersion relation for a fluid bilayer membrane, taking into account the coupling between bending and the local density of the two monolayers. Apart from important corrections to the conventional bending mode, we obtain a second slow mode which is essentially a fluctuation in the density difference of the two monolayers, damped by inter-monolayer friction. Estimates for a stack of membranes show reasonable agreement with a recent spin-echo study of membrane undulations.The traditional model for fluid phospholipid membranes treats them as a single incompressible sheet with bending rigidity [1). Actually, of course, they consist of a pair of slightly compressible monolayers bound tightly together. This bilayer structure implies that bending a membrane necessarily leads to a stretching of one monolayer and a compression of the other. Since the membrane is fluid, density inhomogeneities can relax within each monolayer by lateral lipid flow. For the investigation of static equilibrium phenomena, one ean therefore assume that the lipid density within each monolayer is homogeneous. The only effect of the bilayer structure is to add a global term to the energy, the area difference elasticity [2-4), which is important for calculating the phase diagram of vesicle shapes.Evans and Yeung [5, 6) recently stressed that for the dynamics of conformational changes of membranes the coupling between bending and relative compression is crucial, and demonstrated this in the analysis of a tether fonnation experiment. The purpose of this paper is, first, to analyse this coupling for the much simpler but paradigmatic case of the dynamical equilibrium fluctuations of an almost planar bilayer embedded in a viscous medium and then, briefly, to discuss these fluctuations for the experimentally relevant case of membrane stacks.The standard treatment [7) of the fluctuating single membrane leads to a relaxation rate y, = "q'/4~ for a plane wave excitation with wave number q within the membrane. The bending rigidity" provides the driving force, while the viscosity ~ of the surrounding liquid provides the dissipation. Does this relation hold for a bilayer in which the lipids can