| 2H-nuclear magnetic resonance investigations on phospholipid acyl chain order and dynamics in the gramicidin-induced hexagonal HII phase Biophysical Journal, Volume 51, Issue 3, 1 March 1987, Pages 395-405 V. Chupin, J.A. Killian and B. de Kruijff Abstract The following results are reported in this paper: The interaction of gramicidin with [11,11–2H2]dioleoylphosphatidylcholine (DOPC) and [11,11–2H2]dioleoylphosphatidylethanolamine (DOPE) at different stages of hydration was studied by 2H- and 31P-nuclear magnetic resonance. In the L alpha phase in excess water the acyl chains of phosphatidylethanolamine (PE) are more ordered than phosphatidylcholine (PC) most likely as the result of the lower headgroup hydration of the former lipid. In excess water gramicidin incorporation above 5 mol % in DOPC causes a bilayer----hexagonal HII phase change. In the HII phase acyl chain order is virtually unaffected by gramicidin but the peptide restricts the fast chain motions. At low water content gramicidin cannot induce the HII phase but it markedly decreases chain order in the DOPC bilayer. Increasing water content results in separation between a gramicidin-poor and a gramicidin-rich L alpha phase with decreased order of the entire lipid molecule. Further increase in hydration reverts at low gramicidin contents the phase separation and at high gramicidin contents results in a direct change of the disordered lamellar to the hexagonal HII phase. Gramicidin also promotes HII phase formation in the PE system but interacts much less strongly with PE than with PC. The results support our hypothesis that gramicidin, by a combination of strong intermolecular attraction forces and its pronounced cone shape, both involving the four tryptophans at the COOH-terminus, has a strong tendency to organize, with the appropriate lipid, in intramembranous cylindrical structures such as is found in the HII phase. Abstract | PDF (1037 kb) |
| X-Ray Diffraction Structures of Some Phosphatidylethanolamine Lamellar and Inverted Hexagonal Phases* Biophysical Journal, Volume 81, Issue 5, 1 November 2001, Pages 2693-2706 Paul E. Harper, David A. Mannock, Ruthven N.A.H. Lewis, Ronald N. McElhaney and Sol M. Gruner Abstract X-ray diffraction is used to solve the low-resolution structures of fully hydrated aqueous dispersions of seven different diacyl phosphatidylethanolamines (PEs) whose hydrocarbon chains have the same effective chain length but whose structures vary widely. Both the lower-temperature, liquid-crystalline lamellar (L) and the higher-temperature, inverted hexagonal (H) phase structures are solved, and the resultant internal dimensions (d-spacing, water layer thickness, average lipid length, and headgroup area at the lipid–water interface) of each phase are determined as a function of temperature. The magnitude of the L and H phase d-spacings on either side of the L/H phase transition temperature () depends significantly on the structure of the PE hydrocarbon chains. The L phase d-spacings range from 51.2 to 56.4Å, whereas those of the H phase range from 74.9 to 82.7Å. These new results differ from our earlier measurements of these PEs (Lewis et al., , 28:541–548, 1989), which found near constant d-spacings of 52.5 and 77.0–78.0Å for the L and H phases, respectively. In both phases, the d-spacings decrease with increasing temperature independent of chain structure, but, in both phases, the rate of decrease in the L phase is smaller than that in the H phase. A detailed molecular description of the L/H phase transition in these PEs is also presented. Abstract | Full Text | PDF (455 kb) |
| Comparative Study of the Effects of Several n-Alkanes on Phospholipid Hexagonal Phases Biophysical Journal, Volume 74, Issue 2, 1 February 1998, Pages 944-952 Z. Chen and R.P. Rand Abstract The effects of a series of normal alkanes (decane, dodecane, tetradecane, hexadecane, and octadecane) on the hexagonal H structures containing dioleoylphosphatidylethanolamine (DOPE) and dioleoylphosphatidylcholine (DOPC) were studied using x-ray diffraction and osmotic stress. The alkanes affect structural dimensions and the monolayer intrinsic curvature and bending modulus. The alkane effects are chain-length dependent and are attributed to their different distribution within the H structure. The data suggest that short-chain alkanes are more uniformly distributed within the H hydrocarbon regions and change the curvature and bending modulus of the monolayer, whereas longer-chain alkanes appear confined more to the interstitial region and do not change the curvature and bending modulus. Abstract | Full Text | PDF (222 kb) |
Copyright © 1996 The Biophysical Society. All rights reserved.
Biophysical Journal, Volume 70, Issue 5, 2248-2255, 1 May 1996
doi:10.1016/S0006-3495(96)79790-4
Research Article
D. Marsh
The intrinsic or spontaneous radius of curvature, R(o), of lipid monolayer assemblies is expressed in terms of a lipid molecular packing parameter, V/AI, for various geometries. It is shown that the equivalent lipid length, 1, in inverted hexagonal (HII) phases, defined by a cylindrical shell of equal total lipid volume, yields an expression for R o identical to that for inverted cylindrical micelles (or, equivalently, HII phases in the presence of excess hydrocarbon). This identity is used to obtain values of the effective packing parameter for various phosphatidylethanolamines. The temperature dependence of the intrinsic radius of curvature is predicted to be negative and to be considerably greater than that for the lipid length in nearly all cases. The thermal expansion coefficient is not constant but is found to vary, depending on the value of the lipid packing parameter. A possible addition rule is constructed for the intrinsic radius of curvature of lipid mixtures, based on the linear additivity of the effective molecular volumes, V, and molecular areas, A. This relation is found to hold for mixtures of dioleoyl phosphatidylcholine (DOPC) with dioleoyl phosphatidylethanolamine, and a value of R(o) of > or = 9 A (V/AI = 1.08) is obtained for DOPC. The energetics of the intrinsic curvature and lamellar-nonlamellar transitions are also discussed within the framework of the model.