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Membranes

Current Opinion in Structural Biology, 2011
This is a time of critical increases in understanding membrane protein structures and their mechanisms in biology. As the first structures of membrane proteins determined by X ray crystallography from rich natural sources bovine rhodopsin bovine aquaporin from eye lens and proteins from mammalian tissues the advent of cloning and expression opened a ...
Stroud Robert M, Schertler Gerhard F X
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Membrane fusion

Advanced Drug Delivery Reviews, 1999
Although catalyzed by different proteins, the energy barriers for lipid bilayer fusion in exocytosis, viral fusion, and trafficking seem to be the same as those for the fusion of protein-free phospholipid membranes. To minimize this energy, fusion will proceed through a minimal number of lipid molecules, probably localized in bent non-bilayer ...
, Zimmerberg, , Chernomordik
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Membrane proteins and membrane proteomics

PROTEOMICS, 2008
Abstract Biological membranes form an essential barrier between living cells and their external environments, as well as serve to compartmentalize intracellular organelles within eukaryotes. The latter includes membranes that envelope the nucleus, the outer and inner membranes of the mitochondria, membrane cisternae complex of the ER,
Sandra, Tan   +2 more
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Membrane-membrane interactions: parallel membranes or patterned discrete contacts

Biochimica et Biophysica Acta (BBA) - Biomembranes, 1990
Theoretical and experimental studies of thin liquid films show that, under certain conditions, the film thickness can undergo a sudden transition which gives a stable narrower film or ends in film rupture at spatially periodic points. Theoretical analysis have also indicated that similar transitions might arise in the thin aqueous layer separating ...
H, Darmani, W T, Coakley
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Mechanics of membrane–membrane adhesion

Mathematics and Mechanics of Solids, 2011
Curvature elasticity is used to derive the equilibrium conditions that govern the mechanics of membrane–membrane adhesion. These include the Euler–Lagrange equations and the interface conditions which are derived here for the most general class of strain energies permissible for fluid surfaces.
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