John Bettina S, Escobedo Fernando A
School of Chemical and Biomolecular Engineering, Cornell University, Ithaca, New York 14853-5201, USA.
J Phys Chem B. 2005 Dec 8;109(48):23008-15. doi: 10.1021/jp0551521.
The impact of particle geometry on the phase behavior of hard colloidal tetragonal parallelepipeds (TPs) was studied by using Monte Carlo simulations in continuum space. TPs or "cuboids" of aspect ratios varying from 0.25 to 8 were simulated by approximating their shapes with multisite objects, i.e., via rigid clusters of hard spheres. Using equation of state curves, order parameters, radial distribution functions, particle distribution functions along three directions, and visual analysis of configurations, an approximate phase diagram for the TPs was mapped out as a function of aspect ratio (r) and volume fraction. For r > 3 and intermediate concentrations, the behavior of the TPs was similar to that of spherocylinders, exhibiting similar liquid crystalline mesophases (e.g., nematic and smectic phases). For r = 1, a cubatic phase occurs with orientational order along the three axes but with little translational order. For 1 < r < 4, the TPs exhibit a cubatic-like mesophase with a high degree of order along three axes where the major axes of the particles are not all aligned in the same direction. For r < 1, the TPs exhibit a smectic-like phase where the particles have rotational freedom in each layer but form stacks with tetratic order. The equation of state for perfect hard cubes (r = 1) was also simulated and found to be consistent with that of the rounded-edge r = 1 TPs, except for its lack of discontinuity at the cubatic-solid transition.
通过在连续空间中使用蒙特卡罗模拟,研究了颗粒几何形状对硬胶体四方平行六面体(TPs)相行为的影响。通过用多位点物体(即硬球的刚性簇)近似其形状,模拟了长宽比从0.25到8的TPs或“长方体”。利用状态方程曲线、序参量、径向分布函数、沿三个方向的粒子分布函数以及构型的可视化分析,绘制了TPs的近似相图,作为长宽比(r)和体积分数的函数。对于r>3和中等浓度,TPs的行为类似于球柱体,表现出类似的液晶中间相(如向列相和近晶相)。对于r = 1,出现立方相,沿三个轴具有取向序,但平移序很小。对于1<r<4,TPs表现出类似立方的中间相,沿三个轴具有高度有序,其中粒子的主轴并非都沿同一方向排列。对于r<1,TPs表现出类似近晶的相,其中粒子在每层中具有旋转自由度,但形成具有四方序的堆叠。还模拟了完美硬立方体(r = 1)的状态方程,发现除了在立方-固体转变处缺乏不连续性外,它与圆角r = 1的TPs的状态方程一致。