Giant vesicles formed by gentle hydration and electroformation: a comparison by fluorescence microscopy.

Giant unilamellar vesicles (diameter of a few tens of micrometers) are commonly produced by hydration of a dried lipidic film. After addition of the aqueous solution, two major protocols are used: (i) the gentle hydration method where the vesicles spontaneously form and (ii) the electroformation method where an ac electric field is applied. Electroformation is known to improve the rate of unilamellarity of the vesicles though it imposes more restricting conditions for the lipidic composition of the vesicles. Here we further characterize these methods by using fluorescence microscopy. It enables not only a sensitive detection of the defects but also an evaluation of the quantity of lipids in these defects. A classification of the defects is proposed and statistics of their relative importance in regard to both methods and lipid composition are presented: it shows for example that 80% of the vesicles obtained by electroformation from 98% 1,2-dioleoyl-sn-glycero-3-phosphocholine are devoid of significant defects against only 40% of the vesicles with the gentle hydration method. It is also shown that the presence of too many negatively charged lipids does not favor the formation of unilamellar vesicles with both methods. For the gentle hydration, we checked if the negatively charged lipids were inserted in the vesicles membrane in the same proportion as that of the lipid mixture from which they are formed. The constant incorporation of a negatively charged labeled lipid despite an increasing presence of negatively charged 1,2-dioleoyl-sn-glycero-3-[phospho-l-serine] tends to confirm that the composition of vesicles is indeed close to that of the initial mixture.

[1]  Petra Schwille,et al.  Probing Lipid Mobility of Raft-exhibiting Model Membranes by Fluorescence Correlation Spectroscopy* , 2003, Journal of Biological Chemistry.

[2]  Mark Ellisman,et al.  Reassembly of protein-lipid complexes into large bilayer vesicles: perspectives for membrane reconstitution. , 1980, Proceedings of the National Academy of Sciences of the United States of America.

[3]  R. Waugh,et al.  Local and nonlocal curvature elasticity in bilayer membranes by tether formation from lecithin vesicles. , 1992, Biophysical journal.

[4]  P. Devaux,et al.  Shape change and physical properties of giant phospholipid vesicles prepared in the presence of an AC electric field. , 1996, Biophysical journal.

[5]  E. Evans,et al.  Thermomechanical and transition properties of dimyristoylphosphatidylcholine/cholesterol bilayers. , 1988, Biochemistry.

[6]  H. Itoh,et al.  Preparation of giant liposomes in physiological conditions and their characterization under an optical microscope. , 1996, Biophysical journal.

[7]  I. Bivas,et al.  Bending elasticity and thermal fluctuations of lipid membranes. Theoretical and experimental requirements , 1989 .

[8]  P. Bassereau,et al.  A minimal system allowing tubulation with molecular motors pulling on giant liposomes , 2001, Proceedings of the National Academy of Sciences of the United States of America.

[9]  E Gratton,et al.  Giant phospholipid vesicles: comparison among the whole lipid sample characteristics using different preparation methods: a two photon fluorescence microscopy study. , 2000, Chemistry and physics of lipids.

[10]  M. Angelova,et al.  Preparation of giant vesicles by external AC electric fields. Kinetics and applications , 1992 .

[11]  Faraday Discuss , 1985 .

[12]  E. Evans,et al.  Thermoelasticity of large lecithin bilayer vesicles. , 1981, Biophysical journal.

[13]  R. Dowben,et al.  Formation and properties of thin‐walled phospholipid vesicles , 1969, Journal of cellular physiology.

[14]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[15]  R M Hochmuth,et al.  Measurement of the elastic modulus for red cell membrane using a fluid mechanical technique. , 1973, Biophysical journal.