The conformation and motion of the choline head group in lipid bilayers above and below the gel-to-liquid crystal transition point are studied by means of deuterium and phosphorus magnetic resonance. For this purpose dipalmitoyl-3-sn-phosphatidylcholine is selectively deuterated at various positions on the choline and glycerol constituents. The residual deuteron quadrupole couplings and the phosphorus chemical-shift anisotropy of the corresponding lipid-water mixtures yield quantitative information on the segmental motions. The choline methyl group is only slightly hindered in its movement, but the motional freedom becomes increasingly restricted the closer the segment is located to the glycerol backbone. The average value of the OC-CN bond rotation angle changes with temperature. Increasing the temperature rotates the choline methyl group into the vicinity of the phosphorus atom. The choline group as a whole is thus characterized by a flexible, temperature-dependent structure. Its orientation in space is not fixed, either parallel or perpendicular to the bilayer surface. Instead all segments execute angular oscillations with varying degrees of restriction around the normal on the bilayer surface. The gel-to-liquid crystal phase transition at 41 degrees is clearly reflected in the deuterium and phosphorus resonance spectra of the choline moiety, while no change is observed at 34 degrees. The calorimetric pretransition at 34 degrees seems not to be associated with a conformational change in the choline group.
The motion of the ethanolamine head group in unsonicated lipid bilayers above and below the phase transition is studied by means of deuterium and phosphorus magnetic resonance. For this purpose, dipalmitoyl-3-sn-phosphatidylethanolamine is selectively deuterated at the two ethanolamine carbon atoms. The deuterium quadrupole splittings of the corresponding bilayer phases are measured at pH 5.5 as a function of temperature. In addition, the phosphorus-31 chemical shift anisotropies of planor-oriented and randomly dispersed samples of dipalmitoyl-3-sn-phosphatidylethanolamine are measured at pH 5.5 and 11 by applying a proton-decoupling field. The knowledge of the static chemical shift tensor (Kohler, S.J., and Klein, M.P. (1976), Biochemistry 15, 967) provides the basis for a quantitive analysis of the head-group motion. The nuclear magnetic resonance data are consistent with a model in which the ethanolamine group is rotating flat on the surface of the bilayer with rapid transitions occurring between two enantiomeric conformations.
Glycerol selectively deuterated at various positions was synthesized and supplied to the growth medium of Escherichia coli strain T131 GP, which is defective in endogenous glycerol synthesis as well as glycerol degradation and lacks the ability to synthesize cardiolipin. The procedure enables the stereospecific labeling of the membrane phospholipids (approximately 80% phosphatidylethanolamine, approximately 20% phosphatdylglycerol). Deuterium magnetic resonance spectra were obtained for cell membranes and lipid dispersions either from total lipid extractions or from purified phosphitidylglycerol or -ethanolamine. When glycerol deuterated at various positions was used, all resonances of the phospholipid glycerol backbone and the terminal glycerol moiety in phosphatidylglycerol could be assigned. The results indicate that the molecular conformation of the glycerol backbone is independent of the phospholipid species investigated and is also not altered by the presence of high amounts of membrane proteins. For the quantitative interpretation of the deuterium magnetic resonance splittings, a model is proposed which assumes essentially free rotation around the glycerol C(2)-C(3) bond combined with an asymmetric and restricted jump process around the C(1)-C(2) bond. This model is compatible with known X-ray structures of phospholipids molecules. The two deuterons of both the glycerol backbone C(1) and C(3) segments were found to be magnetically inequivalent. Stereoselective monodeuteration eliminated one set of quadrupole splittings in both cases.
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