Hexane dissolved in dioleoyllecithin bilayers has a partial molar volume of approximately zero

• Published in: Biochemistry (Easton) 1985-08, Vol.24 (17), p.4637-4645
• Main Authors: King, Glen I, Jacobs, Russell E, White, Stephen H
• Format: Article
• Language: English
• Subjects: Artificial membranes and reconstituted systems; Biological and medical sciences; dioleoyllecithin; Fundamental and applied biological sciences. Psychology; hexane; Hexanes; Lipid Bilayers; Mathematics; Membrane physicochemistry; Models, Biological; Molecular biophysics; Molecular Conformation; Neutrons; Phosphatidylcholines; Scattering, Radiation
• ISSN: 0006-2960; 1520-4995
• DOI: 10.1021/bi00338a024

Neutron diffraction has been used to measure the amount and distribution of hexane incorporated from the vapor phase into oriented dioleoylphosphatidylcholine bilayers at 66% relative humidity. We reported earlier that hexane at low concentrations is located largely in a zone 10 A wide at the center of the bilayer [White, S. H., King, G. I., & Cain, J. E. (1981) Nature (London) 290, 161-163]. Extending these studies to high hexane concentrations, we find no readily apparent change in the volume of the hydrocarbon region of the bilayer even though more than one hexane molecule per lipid enters the region. The hexane partial molar volume in the bilayer hydrocarbon region is thus approximately zero. Within our statistical confidence limits, the partial molar volume is certainly no greater than one-third the molecular volume of the hexane. Further, analysis of the data suggests that the mass density of the bilayer is considerably less than 1 in the absence of hexane. These findings are in conflict with the assumptions usually made about lipid bilayers and their interaction with nonpolar hydrophobic molecules. In the course of these experiments, we found that standard methods of interpreting diffraction results were not suitable for our purposes. We thus developed several new methods which are summarized in the text and two appendixes. One of these methods allows us to define with precision the width of the hydrocarbon core of the bilayer. The other provides a means of calculating the effects of changes in the absolute scaling of the bilayers with changes in composition without placing the structures on an absolute scattering length density scale.