论文标题

各向同性至弦样相的动力学在纳米底底电流动流体中的动力学转换

Kinetics of isotropic to string-like phase switching in electrorheological fluids of nanocubes

论文作者

Tonti, Luca, Daza, Fabián Alonso García, Patti, Alessandro

论文摘要

将电场应用于可极化的胶体颗粒,其介电常数与分散介质的介电性不同,会产生诱导的偶极子,从而促进弦乐样簇的形成,并最终改变流体的机械和流变特性。这种复杂的系统,它们的电场引起的流变学可以在粘性和弹性材料之间操纵,被称为电子流体。通过动态蒙特卡洛模拟,我们研究了使用电场后介电纳米管自组装的动力学。切换诱导粒子内偶极子的场,并且在足够大的场强度下,会导致在体积分数频谱之间产生类似弦的长度簇。从各向同性变为弦状状态的动力学表明存在两种机制,这是与链的成核有关的第一个机制,第二个机制与进一步合并和分离之间的竞争有关。我们通过遵循链长度分布并分析纳米管从一个链到另一个链的过渡概率来表征瞬态不稳定状态。此外,我们采用被动微流行病来深入了解电场对模型流体粘弹性响应的影响。我们不仅可以观察到在田间的存在下它变得更加粘弹性,而且它的粘弹性假设具有各向异性特征,垂直于外部田地的平面中粘性和弹性模量都比沿沿田间大。

Applying an electric field to polarisable colloidal particles, whose permittivity differs from that of the dispersing medium, generates induced dipoles that promote the formation of string-like clusters and ultimately alter the fluid mechanical and rheological properties. Complex systems of this kind, whose electric-field-induced rheology can be manipulated between that of viscous and elastic materials, are referred to as electrorheological fluids. By dynamic Monte Carlo simulations, we investigate the dynamics of self-assembly of dielectric nanocubes upon application of an electric field. Switching the field on induces in-particle dipoles and, at sufficiently large field intensity, leads to stringlike clusters of variable length across a spectrum of volume fractions. The kinetics of switching from the isotropic to the string-like state suggests the existence of two mechanisms, the first related to the nucleation of chains and the second to the competition between further merging and separation. We characterise the transient unsteady state by following the chain length distribution and analysing the probability of transition of nanocubes from one chain to another over time. Additionally, we employ passive microrheology to gain an insight into the effect of the electric field on the viscoelastic response of our model fluid. Not only do we observe that it becomes more viscoelastic in the presence of the field, but also that its viscoelasticity assumes an anisotropic signature, with both viscous and elastic moduli in planes perpendicular to the external field being larger than those along it.

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