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聚电解质在简单剪切流中的动力学。

Dynamics of a polyelectrolyte in simple shear flow.

机构信息

Department of Physics, Indian Institute of Technology Madras, Chennai 600 036, India.

出版信息

J Chem Phys. 2013 Dec 14;139(22):224902. doi: 10.1063/1.4837218.

Abstract

The configurational dynamics of a polyelectrolyte (PE), subjected to a simple shear flow, is studied using Brownian dynamics (BD) and Dissipative Particle Dynamics (DPD) simulations of a bead-spring model with explicit counterions. We explore the effect of counterion condensation on the tumbling and extension of PEs by varying the shear rates for a range of values of the electrostatic coupling parameter A (which is defined as the ratio of the Bjerrum length to the size of the monomer). In all cases, the power spectrum of Rs(t) (which characterizes the projected length of the PE in the flow direction as a function of time) exhibits a power law decay at high frequencies, similar to that for a dumbbell in shear flow. For lower values of A (A ~ 2), the tumbling of the PE is periodic and is always associated with folding and stretching, which is in contrast to the oscillatory transition between the extended and globular states seen at higher values of A (A ~ 15). We observe that for A ~ 2 the tumbling frequency decreases and the average tumbling time increases with hydrodynamic interaction (HI). For A > 15, we observe a critical shear rate γ[combining dot]c below which there is considerable counterion condensation and the PE remains in the globular state with a structure akin to that of a neutral polymer in poor solvent. The γ[combining dot]c and the behavior of the PE above the critical shear rate are dependent on the HI. For a given shear rate, when there is considerable condensed counterion fluctuation, the PE extends as a whole and then collapses by the formation of folds with no observable periodicity in tumbling. When the condensed counterion fluctuations are suppressed, the polymer exhibits periodic tumbling. Simulation artifacts resulting from the implicit nature of the solvent and that due to boundary conditions are discussed by comparing the BD results with that obtained from the DPD simulations incorporating Ewald summation for electrostatics.

摘要

采用布朗动力学(BD)和耗散粒子动力学(DPD)模拟带有明确抗衡离子的链球模型,研究了聚电解质(PE)在简单剪切流中的构态动力学。我们通过改变剪切速率来研究抗衡离子凝聚对聚电解质旋转和拉伸的影响,考察静电耦合参数 A 的一系列值(定义为 Bjerrum 长度与单体尺寸之比)。在所有情况下,Rs(t)(其特征为沿流方向投影的聚电解质长度随时间的变化)的功率谱在高频时呈幂律衰减,与剪切流中哑铃的情况相似。对于较小的 A 值(A2),PE 的旋转是周期性的,并且总是与折叠和拉伸相关联,这与在较高 A 值(A15)时观察到的在伸展和球状状态之间的振荡转变形成对比。我们观察到,对于 A~2,旋转频率降低,平均旋转时间随流体力学相互作用(HI)的增加而增加。对于 A>15,我们观察到临界剪切速率γ[combining dot]c 以下存在相当大的抗衡离子凝聚,PE 保持在球状状态,结构类似于不良溶剂中中性聚合物的结构。γ[combining dot]c 和临界剪切速率以上的 PE 行为取决于 HI。对于给定的剪切速率,当存在大量凝聚抗衡离子波动时,PE 整体延伸,然后通过形成无明显周期性旋转的褶皱而坍塌。当凝聚抗衡离子波动被抑制时,聚合物表现出周期性的旋转。通过将 BD 结果与包含静电学 Ewald 求和的 DPD 模拟结果进行比较,讨论了溶剂的隐式性质和边界条件引起的模拟假象。

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