Phenomenology and kinetics of lipid bilayer spreading on hydrophilic surfaces
We studied the spreading of phospholipid bilayer membranes and the conditions for the
formation of continuous bilayers on rough (glass, glass-MgF2, glass-MgF2-SiC> 2) and
smooth (mica) solids using reflection interference contrast microscopy as an analytical tool.
We show that two fundamentally different spreading mechanisms are possible:(i) The sliding
of a single bilayer on a thin lubricating water film and (ii) the rolling of thin lobes of two
juxtaposed bilayers in a tank tread type motion. In the first mechanism the spreading velocity …
formation of continuous bilayers on rough (glass, glass-MgF2, glass-MgF2-SiC> 2) and
smooth (mica) solids using reflection interference contrast microscopy as an analytical tool.
We show that two fundamentally different spreading mechanisms are possible:(i) The sliding
of a single bilayer on a thin lubricating water film and (ii) the rolling of thin lobes of two
juxtaposed bilayers in a tank tread type motion. In the first mechanism the spreading velocity …
We studied the spreading of phospholipid bilayer membranes and the conditions for the formation of continuous bilayers on rough (glass, glass-MgF2, glass-MgF2-SiC> 2) and smooth (mica) solids using reflection interference contrast microscopy as an analytical tool. We show that two fundamentally different spreading mechanisms are possible:(i) The sliding of a single bilayer on a thin lubricating water film and (ii) the rolling of thin lobes of two juxtaposed bilayers in a tank tread type motion. In the first mechanism the spreading velocity of a straight interface exhibits a square root behavior, v~ f~ y2, allowing an estimate of the frictional coupling of the membrane to the substrate. On smooth surfaces (eg, freshly cleaved mica) the dissipation is dominated by shear flow in the ultrathin water film separating the bilayer from the substrate. On rough surfaces in contrast (eg, glass) friction is caused by two-dimensional flow of pinning centers through the spreading membrane. In the latter case the advancing front exhibits a self-similar interface roughness which grows with time. The growth of the roughness is analyzed, and a static roughness exponent£= 0.61±0.04 is found. The rolling of membranes occurs on dehydrated solid-bilayer interfaces with the substrateadjacent bilayer being immobilized. In this case a viscous fingering type spreading pattern is observed. From a practical point of view the rolling motion results in separated lipid patches with intermediate uncovered spots, while spreadingby membrane sliding leads to continuous substratesupported bilayers.
ACS Publications
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