124 resultados para Monte-carlo-simulation
Resumo:
The pulsed-laser polymerization in emulsions has been simulated by the Monte Carlo method. Our simulation shows that the best measure of the propagation rate coefficients K-p is the peak maximum of molecular weight distribution for microemulsions when the droplets are small. However, the inflection point at the low-molecular-weight side of the peaks provides the best measure of K-p of bigger droplets. (C) 2000 Elsevier Science Ltd. All rights reserved.
Resumo:
Monte Carlo method has been applied to investigate the kinetic of grafting reaction in free radical copolymerization. The simulation is quits in agreement with that of theoretical and experimental results. It proves that the Monte Carlo simulation is an effective method for investigating the grafting reaction of free radical copolymerization. (C) 2000 Elsevier Science Ltd. All rights reserved.
Resumo:
Full Paper: The phase, behavior of A-B-random copolymer/C-homopolymer, blends with special interaction was studied by a. Monte, Carlo simulation in two dimensions. The interaction between I segment A and segment C was repulsive, whereas it was attractive between segment B and segment C. The simulation results showed that the blend became two large co-continuous phase domains at lower segment-B component compositions, indicating that the blend showed spinodal decomposition. With an increase of the segment-B component, the miscibility between the copolymer,and the polymer was gradually improved up to being miscible. In addition, it was found that segment B tended to move to the surface of the copolymer phase in the case of a lower component of segment B. On the other hand, if was observed that the average, end-to-end distances ((h) over bar) for both copolymer and polymer changed slowly with increasing segment-B component of the copolymer up to 40%, thereafter they increased considerably with increasing segment B component. Moreover, it was found that the (h) over bar of the copolymer was obviously shorter than that of the homopolymer for the segment-B composition, region from 0% to 80%. Finally, a, phase diagram showing I phase and - II phase regions under the condition of constant-temperature is presented.
Resumo:
Monte Carlo simulations were used to model A/B/A-B ternary mixtures with different AB diblock copolymer volume fractions for which both the dispersed and continuous phase volume fractions were kept constant. For concentrations of the diblock copolymer below a critical value, the domain size increment of the dispersed phase decreases linearly with the copolymer concentration. This is in agreement with the predictions of Noolandi and Hong. The dependence of the domain size as a function of the copolymer volume fraction can also be fitted by the equation of Tang and Huang. Our simulations indicate, for the first time, that the micelles form before saturation of the interface occurs. This means that the formation of the micelles is not a result of the saturation of the interface.
Resumo:
高分子凝胶广泛地存在于自然界以及日常生活中,按其形成作用力不同分为化学凝胶和物理凝胶两大类。由于高分子物理凝胶具有凝胶化的可逆性及其对环境条件强烈的响应性,因此,在近半个世纪的研究与应用中受到极大的关注。高分子溶液中的物理凝胶因其结构及形成机制复杂,在实验方面,除了散射技术及流变技术能够有效地揭示它的部分信息外,其它的实验手段很难用于这个领域的研究;在理论方面,化学凝胶的理论已经比较成熟,而物理凝胶的粘弹性质以及凝胶化是一个远离平衡态的松弛过程,除了一些特征的标度指数外,人们还没有得到适用于高分子物理凝胶的普适规律。当前,由于计算机模拟理论及模拟方法的发展,使得计算机模拟成为除了实验和理论研究方法之外的第三个重要的研究方法。但是,由于物理凝胶化行为的复杂性,用实验和理论获得的信息很难较好地描述凝胶化过程,而计算机模拟的高度透明性及反映信息的完整性,有助于理解这一复杂过程中所涉及的物理本质。因此,利用计算机模拟结合实验及理论方法深入研究高分子物理凝胶的形成机制、结构与性能关系已成为目前最有效的手段之一。 本论文主要运用Monte Carlo模拟方法,并结合小角中子散射(Small-Angle Neutron Scattering, SANS)和流变(Rheology)等实验手段从多个角度探讨了以下几类典型的高分子溶液物理凝胶化行为。 1. 温度对遥爪型三嵌段共聚物在选择性溶剂中的自组装及凝胶化行为影响的研究:采用二维简单方格子Monte Carlo模拟方法,结合逾渗(Percolation)理论,建立了溶胶-凝胶转变相图在统计热力学中的确定方法;甄别了具有特征构象的链,讨论了链及胶束的聚集,明晰了相互作用(体现为约化温度)、构象转变、聚集与凝胶化的一致的关联关系;提出了构象转变模型,进而明确了此体系的凝胶化过程,在微观尺度上表现为桥型链和环型链之间的竞争。 2. 模拟模型改进及其应用到持续长度对稀溶液中高分子链构象影响的研究:考虑到原始八位置键涨落模型效率低,实现复杂且不能应用到复杂的高分子体系,对该模型进行了改进,使其实现简单、效率高,并拓宽了该模型的应用范围。然后,以刚性对均聚物构象的影响为例,发现随着刚性增加,均聚物构象从球形椭球到棒状椭球的转变,并对比了自由连接链(Free Joint Chain, FJC)模型和蠕虫链(Wormlike Chain, WLC)模型在不同刚性范围内对高分子链末端距预测的偏差,首次给出了这两个经典模型的半定量的适用边界。 3. 溶剂尺寸对遥爪型三嵌段共聚物在选择性溶剂中的自组装及凝胶化行为影响的研究:用改进后的八位置键涨落Monte Carlo模型,研究了遥爪型三嵌段共聚物在选择性溶剂条件下的聚集和凝胶化对溶剂尺寸的依赖性,发现溶剂尺寸效应对凝胶化的作用是非单调的。由一个均聚物体系的对比模拟证明这种作用主要是由熵驱动的,并给出了中分子溶剂的半定量定义。在均聚物和嵌段共聚物溶液中,不同尺寸的溶剂分子可以使溶液由于高分子聚集不同而具有不同的微结构,并影响高分子链构象和溶液的性质。从多个角度研究了三嵌段共聚物在不同尺寸溶剂的溶液中所遵循的三种不同的凝胶化机理。 4. 聚氧化乙烯-氧化丙稀-氧化乙烯三嵌段共聚物(poly(ethylene oxide)-poly (propylene oxide)-poly-(ethylene oxide), PEO-PPO-PEO)重水溶液凝胶化的小角中子散射(SANS)和Monte Carlo研究:结合Pluronic F127(EO65PO99EO65)/D2O三嵌段共聚物溶液的特征,对照SANS数据,用改进后的八位置键涨落模型成功地从模拟中获得了F127/D2O的溶胶-凝胶转变相图。详细地考察了体系的微观结构,提出此类高分子溶液中形成的物理凝胶包含高分子逾渗网络的生成,以及被束缚溶剂(Bound Solvent)必须超过离散组分体系逾渗的临界体积分数的机理。着重研究了一定浓度的F127水溶液随温度升高引起的溶胶-凝胶转变以及凝胶-溶胶转变的Reentrant相行为,发现体系在低温区域的溶胶-凝胶转变遵循相同的机理,而在中等温度和较高温度以及不同浓度区域中的凝胶-溶胶转变遵循不同的机理。 5. 极性基团饱和度和溶剂条件对两亲性聚合物在溶液中的聚集行为和凝胶化影响的研究:用改进后的八位置键涨落模型,针对两亲性聚合物在不同溶剂条件的溶液建立了粗粒化模型,以两亲性聚合物中极性基团的饱和度,溶剂条件和高分子浓度为变量,考察了其对链构象、聚集及其凝胶化的影响。 6. 多糖水溶液凝胶化的流变和小角中子散射研究:用流变和SANS考察了两个多糖水溶液中物理凝胶化过程,针对由氢键主导的水基凝胶体系的典型特征进行了讨论,从分子链构象,聚集体结构及其关联以及流变特征等方面对聚强电解质角叉胶(Carrageenan)水溶液和聚弱电解质明胶(Pectin)水溶液进行了详细的讨论。考察了不同多糖的种类(聚合物链的电荷密度),盐的种类和浓度,溶液温度等对凝胶化和凝胶结构的影响,分析了不同多糖溶液的凝胶化机理。
Resumo:
We studied the self-assembly of polydisperse diblock copolymers under various confined states by Monte Carlo simulation. When the copolymers were confined within two parallel walls, it was found that the ordered strip structures appeared alternately with the increase in wall width. Moreover, the wall width at which the ordered structure appeared tended to increase with an increase in the polydispersity index (PDI). On the other hand, the simulation results showed that the copolymers were likely to form ordered concentric strip structures when they were confined within a circle wall.
Resumo:
Monte Carlo simulation was used to study the graft of maleic anhydride (MAH) onto linear polyethylene (PE-g-MAH) initiated by dicumyl peroxide (DCP). Simulation results revealed that major MAH monomers attached onto PE chains as branched graft at higher MAH content. However, at extremely low MAH content, the fraction of bridged graft was very close to that of branched graft. This conclusion was somewhat different from the conventional viewpoint, namely, the fraction of bridged graft was always much lower than that of branched graft under any condition. Moreover, the results indicated that the grafting degree increased almost linearly to MAH and DCP concentrations. On the other hand, it was found that the amount of grafted MAH dropped sharply with increasing the length of grafted MAH, indicating that MAH monomers were mainly attached onto the PE chain as single MAH groups or very short oligomers. With respect to the crosslink of PE, the results showed that the fraction of PE-(MAH)(n)-PE crosslink structure increased continuously, and hence the fraction of PE-PE crosslink decreased with increasing MAH concentration.
Resumo:
The conventional direct simulation Monte Carlo (DSMC) method has a strong restriction on the cell size because simulated particles are selected randomly within the cell for collisions. Cells with size larger than the molecular mean free path are generally not allowed in correct DSMC simulations. However, the cell-size induced numerical error can be controlled if the gradients of flow properties are properly involved during collisions. In this study, a large cell DSMC scheme is proposed to relax the cell size restriction. The scheme is applied to simulate several test problems and promising results are obtained even when the cell size is greater than 10 mean free paths of gas molecules. However, it is still necessary, of course, that the cell size be small with respect to the flow field structures that must be resolved.
Resumo:
The direct simulation Monte Carlo (DSMC) method is a widely used approach for flow simulations having rarefied or nonequilibrium effects. It involves heavily to sample instantaneous values from prescribed distributions using random numbers. In this note, we briefly review the sampling techniques typically employed in the DSMC method and present two techniques to speedup related sampling processes. One technique is very efficient for sampling geometric locations of new particles and the other is useful for the Larsen-Borgnakke energy distribution.
Resumo:
The permeability of the fractal porous media is simulated by Monte Carlo technique in this work. Based oil the fractal character of pore size distribution in porous media, the probability models for pore diameter and for permeability are derived. Taking the bi-dispersed fractal porous media as examples, the permeability calculations are performed by the present Monte Carlo method. The results show that the present simulations present a good agreement compared with the existing fractal analytical solution in the general interested porosity range. The proposed simulation method may have the potential in prediction of other transport properties (such as thermal conductivity, dispersion conductivity and electrical conductivity) in fractal porous media, both saturated and unsaturated.