Numéro |
J. Phys. II France
Volume 3, Numéro 12, December 1993
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Page(s) | 1795 - 1805 | |
DOI | https://doi.org/10.1051/jp2:1993230 |
J. Phys. II France 3 (1993) 1795-1805
Bending stiffness of lipid bilayers. V. Comparison of two formulations
Thoms M. FischerInstitut für Physiologie, Medizinische Einrichtungen der Rheinisch-Westfälischen Technischen Hochschule Aachen, D-52057 Aachen, Germany
(Received 30 July 1993, Received in final form 23 August 1993, accepted 30 August 1993)
Abstract
Two formulations of the intrinsic bending elasticity of lipid bilayers are compared which are based on (A) the mean and the
Gaussian curvature and (B) the mean and the deviatoric curvature. It is shown that (i) formulation A contains implicitly the
elasticity associated with the deviatoric curvature even if the topology of the membrane does not change, (ii) the deviatoric
elasticity is responsible for the change in elastic energy that comes with a change in membrane topology, (iii) the elastic
constant associated with the Gaussian curvature is negative, and (iv) the spontaneous-curvature model may be extended by a
curvature-independent term which becomes relevant when the membrane surface area changes. Formulation B is then (for the special
case of symmetric bilayers) refined in that the curvatures of the two monolayers are accounted for separately. This leads
to a curvature independent term and a correction of the elastic constants of the bilayer which both depend on the value of
the monolayer-curvature. A continuum mechanical model for the bending elasticity of a lipid monolayer is developed. By comparison
of this model to experimental data (i) the elastic constant associated with the deviatoric curvature is estimated and (ii)
the decrease in experimentally determined elastic constants with increasing lipid unsaturation is traced back to the change
in area compressibility and a trend in the spontaneous curvature of the monolayers. Finally it is shown that upon a change
in temperature the change in elastic energy of a lipid vesicle due to the curvature-independent term is much larger than the
concomitant change in elastic energy due to the shape change but only a small fraction of the total change in internal energy.
87.20 - 62.20D
© Les Editions de Physique 1993