A thermodynamic model for the monoclinic (ripple) phase of hydrated phospholipid bilayers

A thermodynamic model for the formation of the ripple phase of hydrated phospholipid bilayers is proposed based on the idea of a spontaneous local curvature free energy. It is suggested that this arises from electrostatic coupling between water dipoles and the dipolar head groups of the lipid molecules. A bilayer profile for the ripple phase is calculated using the model and agrees qualitatively with x‐ray structure measurements. The premelting transition is discussed in terms of a repulsive coupling between the spontaneous curvature free energy and the free energy of ordering of the head group array in the Lβ′ phase. This leads to a mechanism for the premelting transition based on the competition between head group ordering, which softens with increasing temperature, and the free energy of ripple formation, which is favored by an increase in the bilayer polarisability when the head groups become disordered.

[1]  J. Nagle,et al.  Lecithin bilayers. Density measurement and molecular interactions. , 1978, Biophysical journal.

[2]  T. Mitsui,et al.  Structural Parameters of Dipalmitoyl Phosphatidylcholine Lamellar Phases and Bilayer Phase Transitions , 1978 .

[3]  G. Zaccai,et al.  Neutron diffraction studies on selectively deuterated phospholipid bilayers , 1978, Nature.

[4]  K. Larsson Folded bilayers — an alternative to the rippled lamellar lecithin structure , 1977 .

[5]  E. Sackmann,et al.  On Domain Structure and Local Curvature in Lipid Bilayers and Biological Membranes , 1977, Zeitschrift fur Naturforschung. Section C, Biosciences.

[6]  H. Mcconnell,et al.  The intermediate monoclinic phase of phosphatidylcholines. , 1977, Biochimica et biophysica acta.

[7]  I. W. Levin,et al.  Hydrocarbon chain trans-gauche isomerization in phospholipid bilayer gel assemblies , 1977 .

[8]  G. Shipley,et al.  Nature of the Thermal pretransition of synthetic phospholipids: dimyristolyl- and dipalmitoyllecithin. , 1976, Biochemistry.

[9]  Jacques Prost,et al.  Flexoelectricity in Nematic and Smectic-A Liquid Crystals , 1976 .

[10]  S. Kohler,et al.  31P nuclear magnetic resonance chemical shielding tensors of phosphorylethanolamine, lecithin, and related compounds: Applications to head-group motion in model membranes. , 1976, Biochemistry.

[11]  J. Seelig,et al.  Conformation and motion of the choline head group in bilayers of dipalmitoyl-3-sn-phosphatidylcholine. , 1975, Biochemistry.

[12]  N. Clark,et al.  Preparation of large monodomain phospholipid bilayer smectic liquid crystals. , 1975, Proceedings of the National Academy of Sciences of the United States of America.

[13]  W. Helfrich The size of bilayer vesicles generated by sonication , 1974 .

[14]  A. Verkleij,et al.  Analysis of the crystallization process in lecithin liposomes: a freeze-etch study. , 1973, Biochimica et biophysica acta.

[15]  V. Luzzati,et al.  Structure and polymorphism of the hydrocarbon chains of lipids: a study of lecithin-water phases. , 1973, Journal of molecular biology.

[16]  J. Sturtevant,et al.  Calorimetric studies of dilute aqueous suspensions of bilayers formed from synthetic L- -lecithins. , 1972, The Journal of biological chemistry.

[17]  M. Hénon Numerical study of quadratic area-preserving mappings , 1969 .

[18]  R. M. Williams,et al.  Physical studies of phospholipids. VI. Thermotropic and lyotropic mesomorphism of some 1,2-diacyl-phosphatidylcholines (lecithins) , 1967 .

[19]  A. Adamson Physical chemistry of surfaces , 1960 .