Bruce A. Cornell

Membrane thickness and acyl chain length.

It appears reasonable to expect that the primary result of a change in the length of the acyl chains within a lipid bilayer is a similar change in the bilayer thickness. In the present communication we draw attention to the somewhat more complicated effects which are found experimentally for phosphatidylcholine bilayers as the hydrocarbon chain is varied from twelve to eighteen carbons in length. The major change in dimension which occurs with variation in acyl chain length is the area occupied per molecule rather than the bilayer thickness. The same effect is seen with solute hydrocarbon such as hexane which partition into the membrane and cause only a small variation in membrane thickness but a large increase in the molecular area of the lipid. The origin of this effect arises from the almost isotropic distribution of the additional hydrocarbon to the lipid core of the membrane.

The molecular packing and stability within highly curved phospholipid bilayers.

It is shown that the area occupied per phospholipid molecule and the thickness of the bilayer are the same in vesicles as in a planar bilayer. From this it is concluded thtat the lower limit to the size of a vesicle depends on the packing of the head groups of the inner monolayer.

The lower limit to the size of small sonicated phospholipid vesicles

The effective hydrodynamic radius of small sonicated phospholipid vesicles has been measured by photon correlation laser light scattering. It is found that the minimum radius obtained for these vesicles is within the range 10.25 +/- 0.55 nm independent of the phospholipid hydrocarbon chain length for synthetic phosphatidylcholines in the even numbered series of 12 to 18 carbons per hydrocarbon chain. The minimum radius of vesicles of egg yolk phosphatidylcholine is 10.7 +/- 0.3 nm.

Sodium ion binding in the gramicidin A channel. Solid-state NMR studies of the tryptophan residues

Gramicidin A analogs, labeled with 13C in the backbone carbonyl groups and the C-2 indole carbons of the tryptophan-11 and tryptophan-13 residues, were synthesized using t-Boc-protected amino acids. The purified analogs were incorporated into phosphatidylcholine bilayers at a 1:15 molar ratio and macroscopically aligned between glass coverslips. The orientations of the labeled groups within the channel were investigated using solid-state NMR and the effect of a monovalent ion (Na+) on the orientation of these groups determined. The presence of sodium ions did not perturb the 13C spectra of the tryptophan carbonyl groups. These results contrast with earlier results in which the Leu-10, Leu-12, and Leu-14 carbonyl groups were found to be significantly affected by the presence of sodium ions and imply that the tryptophan carbonyl groups are not directly involved in ion binding. The channel form of gramicidin A has been demonstrated to be the right-handed form of the beta 6.3 helix: consequently, the tryptophan carbonyls would be directed away from the entrance to the channel and take part in internal hydrogen bonding, so that the presence of cations in the channel would have less effect than on the outer leucine residues. Sodium ions also had no effect on the C-2 indole resonance of the tryptophan side chains. However, a small change was observed in Trp-11 when the ether lipid, ditetradecylphosphatidylcholine, was substituted for the ester lipid, dimyristoylphosphatidylcholine, indicating some sensitivity of the gramicidin side chains to the surrounding lipid.

Low-frequency motion in membranes. The effect of cholesterol and proteins

Nuclear magnetic resonance (NMR) relaxation techniques have been used to study the effect of lipid-protein interactions on the dynamics of membrane lipids. Proton enhanced (PE) 13C-NMR measurements are reported for the methylene chain resonances in red blood cell membranes and their lipid extracts. For comparison similar measurements have been made of phospholipid dispersions containing cholesterol and the polypeptide gramicidin A+. It is found that the spin-lattice relaxation time in the rotating reference frame (T1 rho) is far more sensitive to protein, gramicidin A+ or cholesterol content than is the laboratory frame relaxation time (T1). Based on this data it is concluded that the addition of the second component to a lipid bilayer produces a low-frequency motion in the region of 10(5) to 10(7) Hz within the membrane lipid. The T1 rho for the superimposed resonance peaks derived from all parts of the phospholipid chain are all influenced in the same manner suggesting that the low frequency motion involves collective movements of large segments of the hydrocarbon chain. Because of the molecular co-operativity implied in this type of motion and the greater sensitivity of T1 rho to the effects of lipid-protein interactions generally, it is proposed that these low-frequency perturbations are felt at a greater distance from the protein than those at higher frequencies which dominate T1.

The effect of gramicidin A on phospholipid bilayers

The helical polypeptide, gramicidin A has been widely studied as a model for the interactions of hydrophobic proteins with lipid bilayer membranes. Many reports are now available of the physical effects of mixing gramicidin A with phospholipid membranes, however, the interpretation of these data remains unclear. The purpose of this communication is to examine the controversial claim that high concentrations of gramicidin A′ cause disorder within the Lα phase of phosphatidylcholine-water dispersions. Solid-state nuclear magnetic resonance (NMR), density gradient and X-ray diffraction techniques are used to confirm the existence of such an effect and mechanisms are discussed which account for the known effects of gramicidin A on lipid bilayers.

NMR study of synthetic lecithin bilayers in the vicinity of the gel-liquid--crystal transition.

1H, 2H, and 31P NMR methods have been employed in the study of dimyristoyl lecithin bilayers hydrated with D2O in the gel (L beta), intermediate (P beta) and liquid-crystalline (L alpha) phases. For D2O/lipid molar ratios, n, in the range 7 less than or equal to n less than or equal to 11 discontinuities are observed in the deuterium NMR splittings at both main and pretransitions. A partial phase diagram based on NMR and differential scanning calorimetry data is presented. 1H NMR dipolar splittings are observed for macroscopically oriented samples in all three phases. Changes in the 1H splittings are correlated with 2H and 31P data and interpreted to show that the chain tilt in the gel phase undergoes a discontinuous change on transition to the intermediate phase, which brings the chain axes closer to the bilayer normal. An estimate of chain tilt in the gel phase is made on the basis of NMR data and found to be approximately 23 degrees for a sample with n = 11 at 18 degrees C.

NMR order parameter analysis of a peptide plane aligned in a lyotropic liquid crystal

A full order parameter analysis has been carried out on a peptide plane of gramicidin A in aligned phospholipid bilayers. The most ordered molecular axis was determined to be the helical long axis of the molecule, possessing an order parameter of 0·93 ± 0·03 parallel to the bilayer normal, and an axial symmetry of -0·06 ± 0·04.

Biological membranes are rich in low-frequency motion

Using 13C cross-polarization NMR techniques, we have found that the effect of protein on the dynamics of the hydrocarbon interior of a series of biological membranes is to depress the intensity of motion on the nanosecond timescale (i.e., T1 becomes longer) and to enhance the intensity of motion on the timescale of tens of microseconds (i.e., T1p becomes shorter.)

Small unilamellar phospholipid vesicles and the theories of membrane formation

Small unilamellar phospholipid vesicles (SUVs) are widely used as a model system in which to study the molecular interactions which occur in biological membranes. Israelachvili et al. and Mitchell and Ninham argue that provided the phospholipid concentration is sufficiently low, lipid aggregates will spontaneously form into SUVs which represent the equilibrium state of the lipid in water. Helfrich, Fromherz and Lasic adopt an alternative model and picture the phospholipid vesicle as a distortion of a planar membrane which requires energy for its formation and is inherently unstable.In the present work we examine these two approaches and their consequences in explaining the physical properties of SUVs. A quantitative basis for our discussion has been devised by adapting a recently published data set of Parsegian et al. to permit an approximate estimate of the curvature energy associated with vesicle formation. We conclude that the spontaneous vesicle formation model only applies to a limited class of molecules where the electrostatic term is the dominant free-energy contribution which drives the bilayer to a more curved geometry. In the case of phosphatidylcholine we propose that the flexibility of the zwitterion eliminates this term causing the planar geometry to be the preferred state. Based on our calculation of curvature energy we are able to predict the diameter of SUVs of phosphatidylcholines to within 10% of the experimental value and to account for the effects of lysolecithin and cholesterol on the size of such vesicles.