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在 Couette 流作用下半浓蠕虫状胶束体系中的流速分布和剪切带形成。

Flow velocity profiles and shear banding onset in a semidilute wormlike micellar system under Couette flow.

机构信息

Instituto de Física, Universidad Nacional Autónoma de México, P.O. Box 20-264, Mexico, DF, 01000.

出版信息

J Phys Chem B. 2009 Nov 26;113(47):15485-94. doi: 10.1021/jp9027996.

Abstract

Velocity profiles in Couette flow are measured in a wormlike micellar solution made of cetyltrimethylammonium bromide (CTAB), sodium salicylate (NaSal), and water, at R (= [NaSal]/[CTAB]) = 2 and at R = 4; [CTAB] = 100 mM. Velocity profiles were obtained by using a two-incident beam laser Doppler technique. Profiles reveal that one of the micellar solutions (R = 2) becomes heterogeneous a long time after flow inception, even at very low imposed shear rates. However, profiles do not correspond to what is expected for gradient shear banding, because the fluid splits in one section close to the moving cylinder where the local mean velocity depends linearly on the gap position and in a second section presenting important velocity fluctuations. Close to the static cylinder, there is a third section where the fluid does not flow; it behaves like a slipping block. On the other hand, at high imposed shear rates, the former slipping block flows and presents a linear profile. Here, velocity profiles are consistent with gradient shear banding. The onset of shear banding was observed. The picture of two stable shear bands separated by a thin steady interface is not always valid. Inhomogeneous flow could be observed, although it cannot be classified as shear banding. In addition, conditions can be found where, as shear rate is increased and before shear banding appears, instead of a thin interface, a fluctuating intermediate band can be observed. On the contrary, for the R = 4 solution, the flow never becomes heterogeneous even at high shear rates. Flow curves were measured in a Couette cell under shear rate control in two cases, when stress is sensed with the moving cylinder and when it is sensed with the static cylinder of the cell. Differences between the flow curves can be explained by using the velocity profiles for both solutions.

摘要

在由溴化十六烷基三甲铵(CTAB)、水杨酸钠(NaSal)和水组成的蠕虫状胶束溶液中测量了 Couette 流中的速度分布,R(=[NaSal]/[CTAB])=2 和 R=4;[CTAB]=100mM。通过使用双入射光束激光多普勒技术获得速度分布。结果表明,两种胶束溶液之一(R=2)在流动起始后很长时间内变得不均匀,即使在非常低的施加剪切速率下也是如此。然而,这些分布与梯度剪切带化所预期的情况并不相符,因为在靠近移动圆柱的一个区域内,流体分裂成一个局部平均速度与间隙位置呈线性关系的部分,而在另一个部分则呈现出重要的速度波动。在靠近静止圆柱的地方,还有一个第三部分,流体不流动;它表现得像一个滑动块。另一方面,在高施加剪切速率下,原来的滑动块流动并呈现线性分布。这里,速度分布与梯度剪切带化一致。观察到了剪切带化的起始。两个稳定的剪切带由一个薄的稳定界面分隔的图像并不总是有效的。尽管不能将其归类为剪切带化,但仍可以观察到不均匀流动。此外,可以发现,随着剪切速率的增加,在剪切带化出现之前,可以观察到一个波动的中间带,而不是一个薄的界面。相反,对于 R=4 的溶液,即使在高剪切速率下,也从未出现过不均匀流动。在两种情况下,即当用移动圆柱感应应力和用细胞的静止圆柱感应应力时,在 Couette 室中在剪切速率控制下测量了流动曲线。两种情况下的流动曲线之间的差异可以通过使用两种溶液的速度分布来解释。

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