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APS -APS March Meeting 2017 - Event - Stress correlations in the transition region of discontinuously thickening suspension flows

机译:APS -APS 2017年3月会议-事件-悬浮液不连续增稠过渡区域的应力相关

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In concentrated suspensions of particles in liquids, the apparent viscosity and the normal stresses are often found to undergo an abrupt transition from a low-viscosity to a high-viscosity state. This behavior happens in a range of materials, for example dispersions of sub-micron spheres in organic liquids to 20-micron diameter corn starch particles in water. While the mechanism may differ for different materials, one scenario which is able to explain this type of behavior is that as the shear stress increases, a stabilizing force which maintains liquid-filled gaps between the particles transitions to one in which contact occurs and frictional interactions between the particles plays a role. par This lubricated-frictional transition is explored using an established simulation approach for spherical particles in viscous liquid [1,2]. The behavior will first be shown to exhibit a shear rate- or stress-induced transition which has features of a classical phase transition. The point equivalent to a critical point is thus the point at which the variation of the shear stress (and typically also the mean particle normal stress) with respect to the shear rate becomes infinite. This point is associated with a pairing of solid fraction and friction coefficient , $phi$ and $mu$ respectively. The temporal fluctuations and spatial correlations of the mixture stress are examined and shown to exhibit a striking change as this transition is crossed.par1. R. Mari, R. Seto, J. F. Morris & M. M. Denn 2014 “Shear thickening, frictionless and frictional rheologies in non-Brownian suspensions” {emph J. Rheol.} {f 58}, 1693.par 2. R. Mari, R. Seto, J. F. Morris & M. M. Denn 2015 Discontinuous shear thickening in Brownian suspensions by dynamic simulation. {emph Proc. National Acad. Sci.} {f 112}, 15326.
机译:在液体中颗粒的浓缩悬浮液中,通常发现表观粘度和法向应力经历了从低粘度状态到高粘度状态的突然转变。此行为发生在多种材料中,例如亚微米球在有机液体中的分散体到直径为20微米的玉米淀粉颗粒在水中的分散体。尽管对于不同的材料其机理可能有所不同,但一种能够解释这种行为的方案是,随着切应力的增加,一种稳定力会保持颗粒之间的液体填充间隙过渡到发生接触和摩擦相互作用的一种粒子之间起着作用。 par该润滑-摩擦转变是通过使用已建立的模拟方法研究粘性液体中球形颗粒的方法[1,2]。首先将显示该行为表现出剪切速率或应力引起的转变,该转变具有经典的相变特征。因此,等于临界点的点是剪切应力(通常还包括平均粒子法向应力)相对于剪切速率的变化变为无限大的点。这一点分别与固体分数和摩擦系数分别配对。检查了混合应力的时间波动和空间相关性,结果表明,随着这种转变的进行,其表现出惊人的变化。 R. Mari,R. Seto,JF Morris和MM Denn 2014“非布朗悬浮液中的剪切增稠,无摩擦和摩擦流变学” {emph J. Rheol。} {f 58},1693.par 2. R. Mari,R Seto,JF Morris和MM Denn 2015年通过动态模拟对布朗悬浮液进行不连续剪切增稠。 {Emph Proc。国家科学院。 {f 112},15326。

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