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胶体悬浮液启动流动中的接触和应力各向异性

Contact and stress anisotropies in start-up flow of colloidal suspensions.

作者信息

Martys Nicos S, Lootens Didier, George William, Hébraud Pascal

机构信息

National Institute of Standards and Technology, 100 Bureau Drive, Stop 8615, Gaithersburg, Maryland 20899-8615, USA.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Sep;80(3 Pt 1):031401. doi: 10.1103/PhysRevE.80.031401. Epub 2009 Sep 11.

Abstract

Spatiotemporal correlations in start-up flows of attractive colloids are explored by numerical simulations as a function of their volume fraction and shear rate. The suspension is first allowed to flocculate during a time tw, then the stress necessary to induce its flow is computed. We find that, at low volume fractions, the stress is a universal function of the strain. On the contrary, at high volume fractions, this scaling behavior is no longer observed and a supplementary stress becomes necessary to induce flow. To better understand the physical origin of the supplementary stress, we examine the creation, disruption, and orientation of contacts between the particles and the corresponding contribution to stress as a function of strain. Our simulations show that the onset of flow is dominated by the creation of contacts between the particles at low shear rates and by their disruption at high shear rates. However, neither the evolution of the number of contacts with strain nor their orientation can fully account for the nonscaling behavior of the stress at high volume fractions. At small strains, the relative importance of forcing in the compression quadrant increases with volume fraction and with flocculation time. This mechanism of stress transmission through the compression quadrant is not accounted for in the usual description of yield stress, which considers the breaking of bonds oriented in the extension quadrant.

摘要

通过数值模拟研究了吸引性胶体启动流中的时空相关性,作为其体积分数和剪切速率的函数。首先让悬浮液在时间(t_w)内絮凝,然后计算诱导其流动所需的应力。我们发现,在低体积分数下,应力是应变的通用函数。相反,在高体积分数下,不再观察到这种标度行为,并且需要额外的应力来诱导流动。为了更好地理解额外应力的物理起源,我们研究了颗粒之间接触的产生、破坏和取向以及它们对应力随应变的贡献。我们的模拟表明,在低剪切速率下,流动的开始由颗粒之间接触的产生主导,而在高剪切速率下由它们的破坏主导。然而,接触数随应变的演变及其取向都不能完全解释高体积分数下应力的非标度行为。在小应变下,压缩象限中强迫的相对重要性随体积分数和絮凝时间增加。通过压缩象限的这种应力传递机制在通常的屈服应力描述中没有考虑,后者考虑的是在拉伸象限中取向的键的断裂。

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