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1.
采用布朗动力学的计算机模拟方法, 研究重力因素对于稀溶液中悬浮粒子聚集过程的影响. 通过在计算机模拟程序中加入和排除重力因素的影响, 对不同重力条件下的粒子团数量随时间的变化曲线进行对比研究, 得到了重力对溶液中的粒子团总数和不同大小的粒子团数量随时间变化的影响规律,可以总结为: 在聚集阶段初期,重力不影响粒子的聚集; 而在聚集阶段后期, 重力加快了粒子的聚集. 同时, 从动力学分析的角度出发, 对重力如何影响悬浮溶液中粒子聚集过程的机制也进行了更加深入的探讨.  相似文献   

2.
使用表征粒子簇结构的几何形状因子,通过对扩散控制聚集过程的模拟,从微观或介观层次研究了粒子簇结构对粒子簇增长速率和速率常数的影响规律,并与实验结果进行了对比分析。  相似文献   

3.
使用表征粒子簇结构的几何形状因子,通过对扩散控制聚集过程的模拟,从微观或介观层次研究了粒子簇结构对粒子簇增长速率和速率常数的影响规律,并与实验结果进行了对比分析.  相似文献   

4.
通过对胶体扩散控制聚集机理的MonteCarlo模拟,表明粒子簇的布朗扩散系数与其大小和形状有关,粒子簇的大小分布可被标度、在微观或介观的层次上,揭示了表征粒子簇结构的几何形状因子在扩散控制聚集过程中对动态标度和粒子簇分布的影响。  相似文献   

5.
通过对胶体扩散控制聚集机理的MonteCarlo模拟,表明粒子簇的布朗扩散系数与其大小和形状有关,粒子簇的大小分布可被标度.在微观或介观的层次上,揭示了表征粒子簇结构的几何形状因子在扩散控制聚集过程中对动态标度和粒子簇分布的影响.  相似文献   

6.
电解质溶液自扩散系数的布朗动力学模拟   总被引:1,自引:0,他引:1  
采用布朗动力学方法对电解质溶液进行了模拟,在传统布朗动力学的基础上综合考虑了流体力学的影响,并且引入SmartMonteCarlo方法的接受概率,避免了离子不现实的移动和位型重叠,这样不仅可以将模拟过程中的时间步长大幅度提高,而且还可使溶质在相空间的演化过程更接近实际.模拟过程以电解质溶液的原始模型为基础,将溶剂看作连续介质,溶质分子之间的相互作用采用软核加静电的势能函数模型,长程静电力采用Ewald加和的处理方法.模拟得到KCl和NaCl溶液的径向分布函数g+-(r),g++(r)和g--(r),并与文献中HNC计算以及模拟的结果进行比较,使用推广的Green-Kubo公式模拟计算溶液中各种离子的自扩散性质,计算结果与实验数据吻合良好.  相似文献   

7.
电解质水溶液传递性质的布朗动力学模拟研究   总被引:1,自引:0,他引:1  
在传统布朗动力学的基础上, 考虑流体力学的影响, 并且引入Smart Monte Carlo方法的接受概率, 对电解质溶液进行布朗动力学模拟, 得到不同浓度和温度下KCl溶液中离子间的径向分布函数, 并且与超网链积分方程理论计算结果进行了比较, 同时, 模拟了KCl和NaCl溶液的摩尔电导率. 模拟过程基于电解质溶液的原始模型, 溶剂被看作连续介质, 溶质分子之间的相互作用采用软核加静电的势能函数模型, 长程静电力的处理采用Ewald加和方法. 结果显示, 流体力学的作用对于电解质溶液的结构性质没有明显的影响, 但是对于传递性质的影响显著; 考虑流体力学作用的布朗动力学模拟结果与实验数据吻合良好.  相似文献   

8.
重质油胶体聚集结构的耗散粒子动力学模拟   总被引:1,自引:0,他引:1  
重质油是以沥青质为胶核分散于饱和油分中形成的极其复杂的胶体体系.本文采用耗散粒子动力学(DPD)方法研究重质油的胶体结构及其影响因素.根据重质油各组分的分子结构特征,构建了描述重质油组分的粗粒化模型化合物.模拟结果表明,本文构建的粗粒化模型能很好地反映重质油的胶体聚集结构.沥青质分子结构对胶体聚集结构有序性有显著影响,较高稠合程度的芳香环结构将使胶束结构有较高的有序性,烷基侧链则表现出分散作用.重质油中的胶质具有胶溶作用,胶质与沥青质的浓度比存在一个极限,当小于这个极限时,重质油将出现聚沉.  相似文献   

9.
对不同长度及不同数量的高分子链在微直通道及微缩通道中的流动进行了模拟与分析.研究表明,高分子链的伸展状态与微通道的形状密切相关,微直通道中高分子链能较充分地伸展,方形微缩通道中高分子链未能充分伸展,而斜坡微缩通道中高分子链的伸展状态介于微直通道与方形微缩通道之间.高分子的存在对微通道系统的温度没有明显影响,对密度与水平流动速度有较明显的影响.高分子链的运动直接影响到周围的简单流体粒子,降低其周围流体粒子的流动速度,对密度与速度产生局部扰动,形成"拖曳"现象.高分子链分布越密集,长度越长,高分子链的拖曳现象越明显.  相似文献   

10.
利用布朗动力学方法研究了ACB三嵌段粒子的分级自组装过程.由第一级组装得到的结构作为第二级组装的初始构型,通过调控体系中补丁B部分的吸引强度和补丁粒子的浓度,研究了第二级组装过程中形成有序结构的影响因素.通过设计组装模型、组装规则和组装路线,得到了蜂巢状网络结构和金刚石状结构.结果表明,在较高的吸引强度和适当的浓度下,可以得到更多且更规整的蜂巢状结构;较高和较低的吸引强度和浓度都不利于金刚石状结构的形成.  相似文献   

11.
We investigated the effect of hydrodynamic interaction(HI) on flow-induced polymer translocation through a nanotube by Brownian dynamics simulations. Whether there is HI in the simulation system is separately controlled by using different diffusion tensors. It is found that HI has no effect on critical velocity flux for long polymer chains due to the competition between more drag force and the hindrance of chain stretching from HI, however, HI broadens the transition interval. In addition, for flow-induced polymer translocation with HI, the critical velocity flux firstly slowly decreases with the increase of chain length and then becomes identical to that of it without HI, that is, the critical velocity flux is independent of chain length. At the same time, HI also accelerates the translocation process and makes the relative variation amplitude of single bead translocation time smaller. In fact, HI can enhance the intrachain cooperativity to make the whole chain obtain more drag force from fluid field and hinder chain stretching, both of which play an important role in translocation process.  相似文献   

12.
张勇  肖忠党 《物理化学学报》2011,27(11):2705-2710
脱氧核糖核酸(DNA)单分子链从完全拉伸状态折叠到平衡状态的动力学过程是溶液中DNA单分子力学的重要特征之一.通过构建全参数化的珠子-弹簧分子链模型,并运用一种高效平衡的半隐式预测——校验积分算法,系统研究了体积排斥作用、有限伸长弹性作用和涨落流体动力学作用等三种非线性作用对稀溶液中DNA分子链折叠过程相对回旋半径和驰豫时间的影响程度和变化趋势.模拟结果发现:体积排斥作用不影响分子链的折叠驰豫时间,但能显著减小平衡时的相对回旋半径;流体动力学作用不影响分子链的相对回旋半径,但明显缩短折叠过程的驰豫时间;有限伸长弹性作用能明显减小短链的相对回旋半径,能显著延长长链的折叠驰豫时间.模拟数据进一步表明:完全伸展的DNA分子链在折叠过程中的相对回旋半径随时间平滑变化,且折叠驰豫时间随长度的标度指数对上述三种非线性作用都具有两种不同的长度依赖性.  相似文献   

13.
凝并和成核机理下颗粒尺度分布的Monte Carlo求解   总被引:2,自引:0,他引:2  
颗粒的凝并和成核现象影响其尺度分布,现有的MonteCarlo方法描述颗粒尺度分布的时间演变过程存在若干困难.提出了一种新的多重MonteCarlo(MMC)算法,基于时间驱动,利用加权的虚拟颗粒的思想,在模拟过程中保持虚拟颗粒总数不变和计算区域体积不变.利用该算法对“常凝并核,一阶成核”的情况下颗粒尺度分布的时间演变过程进行了数值求解,所得结果与数值解相符,表明MMC算法具有高且稳定的计算精度.另外,MMC算法由于跟踪比实际颗粒数目少得多的虚拟颗粒而具有较低的计算代价.  相似文献   

14.
15.
《Soft Materials》2013,11(2):185-202
A new Brownian dynamics code was developed that is capable of computing trajectories of several spherical particles in the presence of a charged planar surface. The code takes into account electrostatic, van der Waals, and hydrodynamic interactions. In this work we describe the methods used in the program and show results from calculations for cytochrome cmolecules interacting with a negatively charged lipid bilayer. This system is of particular biological interest since these molecules play a major role as electron carriers, e.g., in photosynthesis. The shape and charge distribution of cytochrome cmolecules can be well approximated as spherical particles with an embedded monopole and dipole and can therefore easily be handled by the program. That level of approximation makes it possible to study large systems with many (up to 100) particles over time scales up to milliseconds, which would be computationally too expensive using detailed atomistic models.  相似文献   

16.
Summary: We have shown that the components of Cartesian rotation vectors can be used successfully as generalized coordinates describing angular orientation in Brownian dynamics simulations of non‐spherical nanoparticles. For this particular choice of generalized coordinates, we rigorously derived the conformation‐space diffusion equations from kinetic theory for both free nanoparticles and nanoparticles interconnected by springs or holonomic constraints into polymer chains. The equivalent stochastic differential equations were used as a foundation for the Brownian dynamics algorithms. These new algorithms contain singularities only for points in the conformation‐space where both the probability density and its first coordinate derivative equal zero (weak singularities). In addition, the coordinate values after a single Brownian dynamics time step are throughout the conformation‐space equal to the old coordinate values plus the respective increments. For some parts of the conformation‐space these features represent a major improvement compared to the situation when Eulerian angles describe rotational dynamics. The presented simulation results of the equilibrium probability density for free nanoparticles are in perfect agreement with the results from kinetic theory.

Simulation of p(eq)(Φ) for free nanoparticles.  相似文献   


17.
We have recently developed a new singularity‐free algorithm for Brownian dynamics simulation of free rotational diffusion. The algorithm is rigorously derived from kinetic theory and makes use of the Cartesian components of the rotation vector as the generalized coordinates describing angular orientation. Here, we report on the application of this new algorithm in Brownian dynamics simulations of transient electro‐optical properties. This work serves two main purposes. Firstly, it demonstrates the integrity of the new algorithm for BD‐simulations of the most common transient electro‐optic experiments. Secondly, it provides new insight into the performance of the new algorithm compared to algorithms that make use of the Euler angles. We study the transient electrically induced birefringence in dilute solutions of rigid particles with anisotropic polarization tensor in response to external electric field pulses. The use of both one single electric pulse and two electric pulses with opposite polarity are being analyzed. We document that the new singularity‐free algorithm performs flawlessly. We find that, for these types of systems, the new singularity‐free algorithm, in general, outperforms similar algorithms based on the Euler angles. In a wider perspective, the most important aspect of this work is that it serves as an important reference for future development of efficient BD‐algorithms for studies of more complex systems. These systems include polymers consisting of rigid segments with single‐segment translational–rotational coupling, segment–segment fluid‐dynamic interactions and holonomic constraints.

  相似文献   


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