The molecular packing of various fully hydrated mixed-chain phosphatidylcholines was studied by X-ray diffraction and electron microscopy. All of the mixed-chain phosphatidylcholines under study were shown to adopt a lamellar or bilayer form in aqueous media. The bilayer thickness of these mixed-chain phosphatidylcholines was determined from the lamellar repeat distance in the small-anglé X-ray diffraction region by controlled swelling experiments. At T greater than Tm, the bilayer thickness of C(18):C(12)PC and C(18):C-(10)PC is found to be comparable to that of C(14):C(14)PC. In contrast, the bilayer thickness of these highly asymmetric phosphatidylcholines is considerably less than that of the symmetric C(14):C(14)PC at temperatures below Tm. Moreover, the wide-angle X-ray diffraction patterns taken at T less than Tm consist of at least two sharp reflections at 4.2 and 4.6 A. These X-ray diffraction data suggest that these highly asymmetric mixed-chain phospholipids, in excess water, form mixed interdigitated bilayers in the gel state and that the acyl chain packing in the gel-state bilayer is not hexagonal. The freeze-fracture planes of these mixed-chain phosphatidylcholines are discontinuous at T less than Tm, supporting the conclusion drawn from X-ray diffraction data that these highly asymmetric phosphatidylcholines form interdigitated bilayers at temperatures below Tm. The molecular packing of fully hydrated C(18):C(14)PCs in bilayers is distinctively different from that of C(18):C(10)PCs or C(18):C(10)PCs.(ABSTRACT TRUNCATED AT 250 WORDS)

Fusion between bilayers of mixed egg phosphatidylcholine and soybean phosphatidylethanolamine was induced by freezing and thawing. Contact points between bilayers were observed by freeze fracture electron microscopy, and isotropic molecular motional averaging was detected by phosphorus-31 nuclear magnetic resonance under fusion conditions. A molecular model of point defect structure is proposed as an intermediate stage of fusion.

Salmon, porcine, and human calcitonins interact with phosphatidylglycerol to form water-soluble complexes, but these peptides do not interact with the zwitterionic lipids phosphatidylcholine or sphingomyelin. The calcitonins are more helical in the presence of dimyristoylphosphatidylglycerol than in its absence, but human calcitonin is considerably less helical than the other two, particularly in the presence of the lipid. This may explain the previously reported faster rate of degradation of human compared with salmon calcitonin in vivo. The ability of human calcitonin to solubilize dimyristoylphosphatidylglycerol and to alter the phase transition properties of this phospholipid while maintaining a low content of helix indicates that the presence of an amphipathic helix is not a requirement for these effects. The binding of salmon calcitonin to dimyristoylphosphatidylglycerol has been studied by determining the dependence of the circular dichroism properties of the peptide on the concentration of lipid. At 25 degrees C, salmon calcitonin binds to five molecules of dimyristoylphosphatidylglycerol with an affinity constant of 1 X 10(5) M-1. Little change in these parameters is observed at 38 degrees C, and the complex is stable over a wide range of temperatures both above and below the phase transition temperature. The rate of reaction of salmon calcitonin with dimyristoylphosphatidylglycerol is rapid at or above the phase transition temperature of the lipid but not at low temperatures. Salmon calcitonin also interacts with egg phosphatidylglycerol. These results demonstrate that salmon calcitonin can react with phosphatidylglycerol at or above its phase transition temperature to form complexes which are at least kinetically stable both above and below the phase transition temperature. Salmon calcitonin can solubilize mixtures of dimyristoylphosphatidylglycerol and dimyristoylphosphatidylcholine containing 25% or more of the former phospholipid. The helical content of the peptide in the presence of these lipid mixtures is dependent on the fraction of the lipid which is phosphatidylglycerol, with larger fractions of this lipid leading to the formation of a higher helical content. At 25% phosphatidylglycerol, salmon calcitonin can solubilize the lipid mixture without much increase in the helix content of the peptide, again demonstrating that an amphipathic helical structure is not required for the solubilization of phospholipids. Ionic bonding appears to be an important component in the binding of the cationic calcitonins to phospholipids. Salmon calcitonin binds to the acidic phospholipids phosphatidylinositol and phosphatidic acid, but not to zwitterionic phospholipids. In addition, high concentrations of NaCl cause the dissociation of the complex between salmon calcitonin and dimyristoylphosphatidylglycerol.(ABSTRACT TRUNCATED AT 400 WORDS)

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It has been shown that there is a correlation between the fusogenecity of synthetic peptides corresponding to the N-terminal segment of wild-type and mutant forms of simian immunodeficiency virus gp32 (SIV) and their mode of insertion into lipid bilayers. Fusogenic activity is only observed when the peptide inserts into the bilayer with an oblique orientation. Since bilayer destabilization is a necessary step in membrane fusion, we investigate how fusion peptides, which insert at different orientations into lipid bilayers, structurally affect model membranes. We use X-ray diffraction to investigate the structural effects of two synthetic peptides on three different lipid systems. One peptide corresponds to the wild-type sequence (SIVwt), which inserts into the membrane at an oblique angle and is fusogenic. The other peptide has a rearranged sequence (SIVmutV), inserts into the membrane along the bilayer normal, and is nonfusogenic. Our results are expressed through different structural effects, which depend on the lipid system: for example, (i) disordering of the L alpha phase as evidenced by the broadening of the diffraction peaks, (ii) morphological convertion of multilamellar vesicles into unilamellar vesicles, (iii) decrease of the hexagonal phase cell parameter when SIVwt is added, and (iv) change in the conditions for the formation of cubic phases as well as its kinetic stability over a range of temperatures. Some of these observations are explicable based on the fact that the SIVwt destabilizes bilayers by inducing a negative monolayer curvature, while the SIVmutV destabilizes bilayers by inducing a positive monolayer curvature. Finally, we present a model which describes how these findings correlate with fusogenic activity and fusion inhibitory activity, respectively.