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Computer simulation of polymer surfaces.

机译:聚合物表面的计算机模拟。

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One of the main objectives of computer simulation is to isolate the effect of a specific variable in a physical or chemical system of interest, but with ambiguity in experimental interpretation. The area of polymer surface or interface contains such an ambiguity due to absence of a major thermodynamic driving force and difficulty of the complete control of experimental design.; Considering the length and the time scales that define a phenomenon observed in polymeric systems, the appropriate choice of a method among the currently available methodologies in computational chemistry that have been developed mostly for small molecules is very demanding because of the Imitation of computational resources.; In this study, a computationally efficient Monte Carlo simulation on a high coordination lattice employing the RIS scheme for short range interactions and a Lennard-Jones potential for long-range interaction has been applied to various boundary situations which define the material status and distinguish the properties of the material at an interface or surface from those in the bulk state. The polymer surfaces of interest in this study include a free polymer surface, a surface near an attractive solid substrate, a polymer surface generated by compression between two repulsive hard walls, and a polymer-polymer interface.; Several focuses are on the change of the static properties and dynamic properties at the interfaces, which includes density profiles, distribution of a specific constituent of a polymer chain at the interfaces, chain orientation, local conformational state, and chain diffusivity. Each property at an interface is greatly affected by the characteristic of the imposed heterogeneity. One common feature is that the chains are confined at an interface along the direction normal to a surface regardless of the detailed nature of the surface. In addition, the effect of a surface gradually diminishes toward a bulk region and each property has its own effective range in which the properties are different from those in the bulk state. The length scale over which the effect of a free surface can extend in terms of a macroscopic property like density is related to the chain dimension as around 2 Rg where Rg is the radius of gyration of the chain. This length varies with the introduction of a strong boundary such as a solid substrate. With a strongly attractive interaction between polymer chains and a solid substrate, the effect can extend much farther than 2 Rg. The length scale can be easily changed by a perturbation such as a small change of chemical constituents of chain ends.; The simulation method is also used to elucidate a microscopic cause for the decrease of chain mobility of polybutadiene with increase of its 1,2-units, in conjunction with an experimental observation and a theoretical interpretation. After ruling out other possible causes, the simulation reproduces the experimental trend with the lower rate of the transitional jump between rotational states of sp3-sp3 bonds in 1,2-units.
机译:计算机模拟的主要目标之一是隔离特定变量在感兴趣的物理或化学系统中的作用,但在实验解释上存在歧义。聚合物表面或界面的面积由于缺乏主要的热力学驱动力和难以完全控制实验设计而含糊不清。考虑到定义在聚合物系统中观察到的现象的时间长度和时间尺度,由于模仿了计算资源,因此在目前主要用于小分子的计算化学中,从目前可用的计算化学方法中适当选择一种方法非常困难。在这项研究中,采用RIS方案进行短距离相互作用和Lennard-Jones电位进行长距离相互作用的高配位晶格的高效计算蒙特卡罗模拟已应用于各种边界条件,这些边界条件定义了材料状态并区分了性质处于界面或表面的材料与处于散装状态的材料之间的差异。在这项研究中,感兴趣的聚合物表面包括一个自由的聚合物表面,一个吸引人的固体基质附近的表面,通过两个排斥性硬壁之间的压缩产生的聚合物表面以及一个聚合物-聚合物界面。几个焦点集中在界面的静态和动态特性的变化上,包括密度分布,界面上聚合物链特定成分的分布,链取向,局部构象态和链扩散性。界面上的每个属性都受到所施加的异质性特征的极大影响。一个共同的特征是,无论表面的详细性质如何,链条都沿垂直于表面的方向限制在界面处。另外,表面的效果朝着块状区域逐渐减小,并且每种性质具有其自身的有效范围,在该有效范围内,该性质不同于块状状态的性质。自由表面的影响可以在宏观尺度上扩展的长度尺度,例如密度,与链的大小有关,大约为2 R g ,其中R g 为链条的回转半径。该长度随引入强边界(例如固体基材)而变化。由于聚合物链和固体底物之间具有很强的吸引力,因此这种作用可以扩展到比2 R g 更远的距离。长度标度可以容易地通过扰动来改变,例如链端的化学成分的微小变化。结合实验观察和理论解释,该模拟方法还用于阐明导致聚丁二烯链迁移率降低的微观原因,即其1,2-单元的增加。在排除了其他可能的原因之后,该模拟重现了实验趋势,即在1,2-中,sp 3 -sp 3 键的旋转状态之间的过渡跳变速率较低。单位。

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