Dipolar interactions, molecular flexibility, and flexoelectricity in bent-core liquid crystals

被引:20
作者
Dewar, A [1 ]
Camp, PJ [1 ]
机构
[1] Univ Edinburgh, Sch Chem, Edinburgh EH9 3JJ, Midlothian, Scotland
关键词
D O I
10.1063/1.2062007
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The effects of dipolar interactions and molecular flexibility on the structure and phase behavior of bent-core molecular fluids are studied using Monte Carlo computer simulations. Some calculations of flexoelectric coefficients are also reported. The rigid cores of the model molecules consist of either five or seven soft spheres arranged in a "V" shape with external bend angle gamma. With purely repulsive sphere-sphere interactions and gamma=0 degrees (linear molecules) the seven-sphere model exhibits isotropic, uniaxial nematic, and untilted and tilted smectic phases. With gamma >= 20 degrees the untilted smectic phases disappear, while the system with gamma >= 40 degrees shows a direct tilted smectic-isotropic fluid transition. The addition of electrostatic interactions between transverse dipole moments on the apical spheres is generally seen to reduce the degree of molecular inclination in tilted phases, and destabilizes the nematic and untilted smectic phases of linear molecules. The effects of adding three-segment flexible tails to the ends of five-sphere bent-core molecules are examined using configurational-bias Monte Carlo simulations. Only isotropic and smectic phases are observed. On the one hand, molecular flexibility gives rise to pronounced fluctuations in the smectic-layer structure, bringing the simulated system in better correspondence with real materials; on the other hand, the smectic phase shows almost no tilt. Lastly, the flexoelectric coefficients of various nematic phases-with and without attractive sphere-sphere interactions-are presented. The results are encouraging, but a large computational effort is required to evaluate the appropriate fluctuation relations reliably.
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页数:12
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共 46 条
[11]  
Emelyanenko AV, 2004, PHYS REV E, V70, DOI 10.1103/PhysRevE.70.021704
[12]  
Frenkel D., 2000, Computational Science Series
[13]   Molecular dynamics simulation study on the phase behavior of the Gay-Berne model with a terminal dipole and a flexible tail [J].
Fukunaga, H ;
Takimoto, J ;
Doi, M .
JOURNAL OF CHEMICAL PHYSICS, 2004, 120 (16) :7792-7800
[14]   Computer simulation study of the global phase behavior of linear rigid Lennard-Jones chain molecules: Comparison with flexible models [J].
Galindo, A ;
Vega, C ;
Sanz, E ;
MacDowell, LG ;
de Miguel, E ;
Blas, FJ .
JOURNAL OF CHEMICAL PHYSICS, 2004, 120 (08) :3957-3968
[15]   Chain and ring structures in smectic phases of molecules with transverse dipoles [J].
GilVillegas, A ;
McGrother, SC ;
Jackson, G .
CHEMICAL PHYSICS LETTERS, 1997, 269 (5-6) :441-447
[16]  
Gray G.W.J.W.G. Goodby., 1984, SMECTIC LIQUID CRYST
[17]   Molecular dynamics simulation study of a liquid crystal model: Gay-Berne particles with transverse dipole moments [J].
Gwozdz, E ;
Brodka, A ;
Pasterny, K .
CHEMICAL PHYSICS LETTERS, 1997, 267 (5-6) :557-562
[18]  
Hansen J.-P., 2013, Theory of Simple Liquids
[19]   Uniform textures of smectic liquid-crystal phase formed by bent-core molecules [J].
Jakli, A ;
Rauch, S ;
Lotzsch, D ;
Heppke, G .
PHYSICAL REVIEW E, 1998, 57 (06) :6737-6740
[20]   Computer simulation of polar bent-core molecules [J].
Johnston, SJ ;
Low, RJ ;
Neal, MP .
PHYSICAL REVIEW E, 2002, 66 (06) :14