Abstract:The isotropic-nematic interface of a simple model of liquid-crystal molecules has been investigated using computer simulation, and by numerical minimization of the Onsager free-energy functional. The molecules are represented by long spherocylindrical particles interacting via the Kihara potential. The agreement between simulation and theory is excellent, apart from the bulk coexistence densities which are over estimated by the theory. Planar alignment of the molecules at the interface is preferred in all case… Show more
“…For a given value of N, equation (11) constitutes N +1 coupled nonlinear integral equations for the N +1 unknowns ρ k (z, θ ), (k = 0, 1, · · · N ). This set of equations can be solved numerically on a (z, θ ) grid, e.g.…”
Section: The Free Isotropic-nematic Interfacementioning
confidence: 99%
“…However, these findings are in disagreement with the claims in [8], where a refinement of the spatial grid yields a higher value for γ and a nonmonotonic density profile. In order to study the effect of interfacial biaxiality we consider the Euler-Lagrange equations (11) for N = 1, which we write as…”
Section: The Free Isotropic-nematic Interfacementioning
Within the Onsager theory we study the planar isotropic-nematic interface of fluids of hard rods. We present a method with which interfacial biaxiality can be dealt with efficiently and systematically, and apply it (i) to the pure hard-rod fluid and (ii) to a binary mixture of thin and thick hard rods. In the one-component system we find a surface tension that is lower by 15% than earlier estimates, and monotonic profiles of the density and the uniaxial order parameter. The biaxial order parameter profile is non-monotonic. In the twocomponent system we find the possibility of non-monotonic density profiles, and a maximum in the surface tension as a function of the pressure.
“…For a given value of N, equation (11) constitutes N +1 coupled nonlinear integral equations for the N +1 unknowns ρ k (z, θ ), (k = 0, 1, · · · N ). This set of equations can be solved numerically on a (z, θ ) grid, e.g.…”
Section: The Free Isotropic-nematic Interfacementioning
confidence: 99%
“…However, these findings are in disagreement with the claims in [8], where a refinement of the spatial grid yields a higher value for γ and a nonmonotonic density profile. In order to study the effect of interfacial biaxiality we consider the Euler-Lagrange equations (11) for N = 1, which we write as…”
Section: The Free Isotropic-nematic Interfacementioning
Within the Onsager theory we study the planar isotropic-nematic interface of fluids of hard rods. We present a method with which interfacial biaxiality can be dealt with efficiently and systematically, and apply it (i) to the pure hard-rod fluid and (ii) to a binary mixture of thin and thick hard rods. In the one-component system we find a surface tension that is lower by 15% than earlier estimates, and monotonic profiles of the density and the uniaxial order parameter. The biaxial order parameter profile is non-monotonic. In the twocomponent system we find the possibility of non-monotonic density profiles, and a maximum in the surface tension as a function of the pressure.
“…The computational model is appealing due to its relative cheapness but in this paper is shown to be rich in phase behaviour, exhibiting both the nematic and smectic liquid crystalline phases. In addition the short-range nature of this potential makes it highly suitable for use in parallel domain decomposition algorithms [14,15], which can provide for the simulation of extremely large systems [16] of mesogenic molecules.…”
Computer simulations of systems of soft repulsive spherocylinders (SRS) of aspect ratio ( L = D ) equal to 4 have been carried out using the parallel molecular dynamics program GBMOLDD. At su ciently high densities the system forms stable nematic and smectic-A liquid crystalline phases. Results are presented for a series of seven isochores in the NVE ensemble, and for isobars at T ¤ˆk T ="ˆ0:5; 1:0; 1:5 in the NpT ensemble.
IntroductionRecent years have seen substantial progress in the simulation of liquid crystal systems [1± 3]. Such simulations frequently require large numbers of mesogenic molecules. This is particularly true for the calculation of material properties, such as elastic constants that require the computation of a wavevector-dependen t ordering tensor in the low-k limit [4,5], or for the study of smectic phases where many particles are required to represent individual smectic layers. In these cases it is desirable to use models that are cheap, in terms of computer power, but which still capture the essential physics of real mesogenic molecules. The most commonly studied model systems are the hard spherocylinder model [6,7] and the soft-particle Gay± Berne mesogen [8± 10]. In this study, computer simulations of a`hybrid' system of soft repulsive spherocylinders (SRS), which have only been brie¯y examined in the past [11± 13], are carried out in order to determine the phase behaviour of the system. The computational model is appealing due to its relative cheapness but in this paper is shown to be rich in phase behaviour, exhibiting both the nematic and smectic liquid crystalline phases. In addition the short-range nature of this potential makes it highly suitable for use in parallel domain decomposition algorithms [14,15], which can provide for the simulation of extremely large systems [16] of mesogenic molecules.The layout of this paper is as follows: the computational model and simulation details are described in } 2, the results of our work are presented and discussed in } 3 and our conclusions are made in } 4.
“…Recently, a number studies have been devoted to the interface between the nematic and the isotropic phase in Gay-Berne fluids [108] and fluids of spherocylinders [110] or ellipsoids [109,111,112]. They reveal among other a rather intriguing capillary wave spectrum.…”
Section: Interfacial Propertiesmentioning
confidence: 99%
“…Therefore, a growing number of simulations are devoted to the study of model nematics at surfaces [93,94,95,96,97,98,99,100,101,102,103,104,105,106,107]. and interfaces [108,109,110,111,112] or in thin films [24,25,113,114,115,116,117,118].…”
Abstract. Computer simulations of simple model systems for liquid crystals are briefly reviewed, with special emphasis on systems of ellipsoids. First, we give an overview over some of the most commonly studied systems (ellipsoids, Gay-Berne particles, spherocylinders). Then we discuss the structure of the nematic phase in the bulk and at interfaces.
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