Influence of Lipid Membranes on the Conformational Transitions of Nucleic Acids

Abstract

The conformational transitions of nucleic acids which were enclosed in reverse phase evaporation vesicles (REV) were studied by thermal denaturation with optical recording. Cloned fragments of double-stranded DNA containing 179 base pairs and 187 base pairs, respectively, and polyA · polyU were enclosed in REV with a yield up to every vesicle containing 50 nucleic acid molecules. With the 179 base pairs DNA enclosed in the vesicle from egg lecithin two well resolved helix-coil transitions could be measured; one is very similar in the midpoint- temperature T_m and halfwidth δT_1/2 to the transition of the free nucleic acid, and the other transition occurs stabilized at a 3.5°C higher T_m-value and with a broader δT_1/2, 2.7°C instead of 0.6°C. Both transitions are from nucleic acids inside the vesicles. Varying the surface charge of the lipid membrane by adding the negatively charged phosphatidylserine or phosphatidylglycerol, an optimum in the yield of enclosure and a maximum in the increase in T_m (4.5°C) and δT_1/2 (5.5°C instead of 1.0°C) was obtained at 20% phosphatidylserine or phosphatidylglycerol. In vesicles from pure negatively charged lipids no second population of nucleic acids was observed. Qualitatively, similar effects were observed with polyA·polyU. Stabilization and broadening of the second transition is higher for nucleic acids inside vesicles from lipids with unsaturated fatty acids, as dioleoyl-phosphatidylcholine, than with saturated fatty acids, dipalmitoyl-phosphatidylcholine. Stabilization and broadening decrease with increasing ionic strength, whereas the relative contributions of both transitions to the total hypochromicity remain unchanged; the second transition coincides with the first at 90 mM Na⁺. From the experimental results it was concluded that the interaction of nucleic acids and lipid membranes is mainly of electrostatic nature. The nucleic acids exist inside the vesicles in two populations, one behaving like nucleic acid free in solution and one influenced by the contact with the membrane. All results are in accordance with a model in which the interaction between the nucleic acid and the membrane is in competition with the dipole-dipole interaction inside the membrane surface.