The dynamic stress responses to area change in planar lipid bilayer membranes

被引:8
作者
Jeon, JG
Voth, GA
机构
[1] Univ Utah, Dept Chem, Salt Lake City, UT 84112 USA
[2] Univ Utah, Ctr Biophys Modeling & Simulat, Salt Lake City, UT 84112 USA
关键词
D O I
10.1529/biophysj.104.052183
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
The viscoelastic properties of planar phospholipid (dimyristoylphosphatidylcholine) bilayer membranes at 308 K are studied, many of them for the first time, using the nonequilibrium molecular dynamics simulation ( NEMD) method for membrane area change. First, we present a unified formulation of the intrinsic three-dimensional (3D) and apparent in-plane viscoelastic moduli associated with area change based on the constitutive relations for a uniaxial system. The NEMD simulations of oscillatory area change process are then used to obtain the frequency-domain moduli. In the 4 - 250 GHz range, the intrinsic 3D elastic moduli of 20 - 27 kbar and viscous moduli of 0.2 - 9 kbar are found with anisotropy and monotonic frequency dispersion. In contrast, the apparent in-plane elastic moduli ( 1 - 9 kbar) are much smaller than, and the viscous moduli ( 2 - 6 kbar) comparable to, their 3D counterparts, due to the interplay between the lateral and normal relaxations. The time-domain relaxation functions, separately obtained by applying stepwise strains, can be fit by 4 - 6 exponential decay modes spanning subpicosecond to nanosecond timescale and are consistent with the frequency-domain results. From NEMD with varying strain amplitude, the linear constitutive model is shown to be valid up to 6 and 20% area change for the intrinsic 3D elastic and viscous responses, respectively, and up to 20% area change for the apparent in-plane viscoelasticity. Inclusion of a gramicidin A dimer (similar to1 mol %) yields similar response properties with possibly smaller (<10%) viscous moduli. Our results agree well with available data from ultrasonic experiments, and demonstrate that the third dimension ( thickness) of the planar lipid bilayer is integral to the in-plane viscoelasticity.
引用
收藏
页码:1104 / 1119
页数:16
相关论文
共 54 条
[1]  
Almeida P.F. F., 1995, STRUCTURE DYNAMICS M, V1, P305, DOI [10.1016/S1383-8121, DOI 10.1016/S1383-8121]
[2]  
[Anonymous], 1980, MINPACK PROJECT
[3]   Bridging microscopic and mesoscopic simulations of lipid bilayers [J].
Ayton, G ;
Voth, GA .
BIOPHYSICAL JOURNAL, 2002, 83 (06) :3357-3370
[4]   Calculating the bulk modulus for a lipid bilayer with nonequilibrium molecular dynamics simulation [J].
Ayton, G ;
Smondyrev, AM ;
Bardenhagen, SG ;
McMurtry, P ;
Voth, GA .
BIOPHYSICAL JOURNAL, 2002, 82 (03) :1226-1238
[5]   PHYSICAL-PROPERTIES OF THE FLUID LIPID-BILAYER COMPONENT OF CELL-MEMBRANES - A PERSPECTIVE [J].
BLOOM, M ;
EVANS, E ;
MOURITSEN, OG .
QUARTERLY REVIEWS OF BIOPHYSICS, 1991, 24 (03) :293-397
[6]   NEW VIEW OF LIPID BILAYER DYNAMICS FROM H-2 AND C-13 NMR RELAXATION-TIME MEASUREMENTS [J].
BROWN, MF ;
RIBEIRO, AA ;
WILLIAMS, GD .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA-BIOLOGICAL SCIENCES, 1983, 80 (14) :4325-4329
[7]  
Chaikin P., 2000, Principles of Condensed Matter Physics
[8]  
CORNELL WD, 1995, J AM CHEM SOC, V117, P5197
[9]  
de Gennes P.-G., 1993, PHYS LIQUID CRYSTALS
[10]  
de Gennes P. G., 1969, J PHYS C SOLID STATE, V30, pC4, DOI DOI 10.1051/JPHYSCOL:1969415