The theme of the fluid mosaic membrane by Singer and Nicholson (1972), in any colored variation, is known to every student of the biosciences. Yet, there exists no complete picture of the structure and dynamics of any real biological membrane, based on a sufficient set of experimentally determined atomic coordinates and trajectories. While the paradigm of static structure as a determinant of biological function has proven extremely fruitful for nucleic acids, and to a large extent also for proteins, this seems not to be the case with biological membranes. From all we know today, the static structures and mechanistic interactions are necessary to describe the protein moiety of membranes; this could be sufficiently defined in terms of three-dimensional atomic coordinates and their dislocations on conformational changes. However, a major species of membranes constituents, the lipids, appears to be physiologically in a state of dynamic disorder within certain limits given by the overall morphology—planar, tubular, or micellar—of the membrane. This is related to the situation in liquid crystals (De Gennes, 1974), and the physical description of membrane lipids has greatly benefited from the phenomenology applied to that field.KeywordsSynchrotron RadiationElectron Density ProfileLipid Phase TransitionLipid Model MembraneHydrocarbon Chain PackingThese keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
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