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. 2006 Oct 15;91(8):2936-42.
doi: 10.1529/biophysj.106.088716. Epub 2006 Jul 28.

Pressure tuning of the morphology of heterogeneous lipid vesicles: a two-photon-excitation fluorescence microscopy study

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Pressure tuning of the morphology of heterogeneous lipid vesicles: a two-photon-excitation fluorescence microscopy study

Chiara Nicolini et al. Biophys J. .

Abstract

We used a technique that allows us to visualize local and morphological changes of the membrane of more component giant unilamellar vesicles due to high pressure perturbation. Under these conditions, thermally induced processes are largely suppressed, and the bending rigidity and line tension are influenced by pressure-induced changes in lipid molecular packing and shape only. We studied the effect of pressure on the lateral organization and morphology of the model raft system DOPC (1,2-dioleoyl-sn-glycero-3-phosphocholine)/sphingomyelin/cholesterol as well as of the fluid mixture POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine)/DLPC (1,2-dilauroyl-sn-glycero-3-phosphocholine) by two-photon excitation fluorescence microscopy. The pressure-dependent experiments were carried out using a sample cell made from a thin fused silica capillary. The use of Laurdan as fluorescence label allowed us to also follow the lipid phase state by calculating the generalized polarization (GP) values of the vesicles and extracting their average value. During the compression cycle, a reduction in the volume of the vesicles is observed, accompanied by an increase of the average GP value, indicating an increasingly tighter packing of the lipids. Interestingly, the two systems studied show phenomena of budding and fission, and these at surprisingly low pressures of 200-300 bar. Moreover, these budding processes are not directly related to phase transitions to an overall ordered conformational state of the lipid membrane, which occur at much higher pressures. The topological changes of the lipid vesicles are irreversible and exhibit a different behavior depending on whether the pressure is increased or decreased. The results are discussed in light of the various contributions to the free energy functional of lipid vesicles. Finally, the biological relevance of these studies is highlighted.

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Figures

FIGURE 1
FIGURE 1
Two-photon excitation fluorescence intensity images of a Laurdan-labeled GUV (of ∼30-μm diameter) composed of DOPC/SM/Chol (33:33:33) at selected pressures (T = 20°C). The GP images were taken at the top of the vesicle. The white arrows indicate conditions where budding of small vesicles and loss of lipid material occur.
FIGURE 2
FIGURE 2
(a) Average GP value (GP center) of the lipid mixture DOPC/SM/Chol (33:33:33) in excess water as a function of pressure during a compression cycle at T = 20°C. (b) Average GP value of the lipid mixture POPC/DLPC (50:50) in excess water as a function of pressure during a compression cycle at T = 20°C.
FIGURE 3
FIGURE 3
Selected two-photon excitation fluorescence intensity images of Laurdan-labeled GUVs of the system POPC/DLPC (50:50) at T = 20°C taken during the compression cycle. At 250 bar, a bud develops, which grows upon further pressurization. At ∼400 bar, fission occurs. The white arrows indicate budding and fission processes. The GP images are taken at the equatorial section for the pressures at 100, 250, and 350 bar and at the top of the GUV for 400 bar. The variations in GP values are here due to the imperfect circular polarization of the excitation light.
FIGURE 4
FIGURE 4
Selected two-photon excitation fluorescence intensity images of Laurdan-labeled GUVs of the system POPC/DLPC (50:50) at T = 20°C taken during the decompression cycle from 2 kbar to 1 bar. The white arrows at 1100 bar indicate conditions where budding of small vesicles and pinching-off of lipid material occur. As the pressure is released, the GUVs start wobbling. Another interesting observation is that the GP is not homogeneous throughout the vesicle anymore.

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