The formation of supported lipid bilayers (SLBs) on glass from giant unilamellar vesicles (GUVs) was studied using fluorescence microscopy. We show that GUV rupture occurs by at least four mechanisms, including 1), spontaneous rupture of isolated GUVs yielding almost heart-shaped bilayer patches (asymmetric rupture); 2), spontaneous rupture of isolated GUVs yielding circular bilayer patches (symmetric rupture); 3), induced rupture of an incoming vesicle when it contacts a planar bilayer edge; and 4), induced rupture of an adsorbed GUV when a nearby GUV spontaneously ruptures. In pathway 1, the dominant rupture pathway for isolated GUVs, GUVs deformed upon adsorption to the glass surface, and planar bilayer patch formation was initiated by rupture pore formation near the rim of the glass-bilayer interface. Expanding rupture pores led to planar bilayer formation in approximately 10-20 ms. Rupture probability per unit time depended on the average intrinsic curvature of the component lipids. The membrane leaflet adsorbed to the glass surface in planar bilayer patches originated from the outer leaflet of GUVs. Pathway 2 was rarely observed. We surmise that SLB formation is predominantly initiated by pathway 1 rupture events, and that rupture events occurring by pathways 3 and 4 dominate during later stages of SLB formation.
The adsorption of large unilamellar vesicles composed of various combinations of phosphatidylcholine, phosphatidylethanolamine (PE), monomethyl PE, and dimethyl PE (PE-Me2) onto a glass surface was studied using fluorescence microscopy. The average lipid geometry within the vesicles, described mathematically by the average intrinsic curvature, C(0,ave), was methodically altered by changing the lipid ratios to determine the effect of intrinsic curvature on the ability of vesicles to rupture and form a supported lipid bilayer. We show that the ability of vesicles to create fluid planar bilayers is dependent on C(0,ave) and independent of the identity of the component lipids. When the C(0,ave) was approximately -0.1 nm(-1), the vesicles readily formed supported lipid bilayers with almost full mobility. In contrast, when the C(0,ave) ranged from approximately -0.2 to approximately -0.3 nm(-1), the adsorbed vesicles remained intact upon the surface. The results indicate that the average shape of lipid molecules within a vesicle (C(0,ave)) is essential for determining kinetically viable reactions that are responsible for global geometric changes.
DNA oligomers deposited on Cu(111) surfaces were observed at liquid nitrogen temperature using a scanning
tunneling microscope. The observed oligomers were pAAAAAAATTTTTTT (14mer), pTTTGGTTAACCAAA
(14mer), pGGGGGTTTTTTTTTT (15mer), and pAAAAAAAAAATTTTTTTTTT (20mer). The structure of the
isolated oligomers adsorbed on the Cu surface varies with the length of the molecular chain. The isolated
20mer is adsorbed to aggregate three-dimensionally. The isolated 14mer and 15mer are extended on the
surface, and the almost entire molecular chain touches the surface. A highly resolved image of the 20mer
shows bright spots aligned in a row along a single-stranded DNA with the same periodicity as that of the
nucleotide units, demonstrating that each bright spot is a nucleotide.
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