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二维曲线粘弹性流动中伴随流动阻力突然增大的流动模式转变。

Flow pattern transition accompanied with sudden growth of flow resistance in two-dimensional curvilinear viscoelastic flows.

作者信息

Yatou Hiroki

机构信息

Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Sep;82(3 Pt 2):036310. doi: 10.1103/PhysRevE.82.036310. Epub 2010 Sep 14.

DOI:10.1103/PhysRevE.82.036310
PMID:21230174
Abstract

We numerically find three types of steady solutions of viscoelastic flows and flow pattern transitions between them in a two-dimensional wavy-walled channel for low to moderate Weissenberg (Wi) and Reynolds (Re) numbers using a spectral element method. The solutions are called "convective," "transition," and "elastic" in ascending order of Wi. In the convective region in the Wi-Re parameter space, convective effect and pressure gradient balance on average. As Wi increases, elastic effect becomes comparable, and the first transition sets in. Through the transition, a separation vortex disappears, and a jet flow induced close to the wall by the viscoelasticity moves into the bulk; the viscous drag significantly drops, and the elastic wall friction rises sharply. This transition is caused by an elastic force in the streamwise direction due to the competition of the convective and elastic effects. In the transition region, the convective and elastic effects balance. When the elastic effect becomes greater than the convective effect, the second transition occurs but it is relatively moderate. The second transition seems to be governed by the so-called Weissenberg effect. These transitions are not sensitive to driving forces. By a scaling analysis, it is shown that the stress component is proportional to the Reynolds number on the boundary of the first transition in the Wi-Re space. This scaling coincides well with the numerical result.

摘要

我们使用谱元法,在二维波浪壁通道中,针对低到中等的魏森贝格数(Wi)和雷诺数(Re),通过数值方法找到了粘弹性流动的三种稳态解以及它们之间的流动模式转变。这些解按照Wi从小到大的顺序分别称为“对流型”、“过渡型”和“弹性型”。在Wi-Re参数空间的对流区域,对流效应和压力梯度平均而言相互平衡。随着Wi增大,弹性效应变得相当,首次转变开始。通过这次转变,一个分离涡消失,由粘弹性在壁面附近诱导出的射流进入主流;粘性阻力显著下降,而弹性壁面摩擦力急剧上升。这种转变是由于对流和弹性效应的竞争导致的流向弹性力引起的。在过渡区域,对流和弹性效应相互平衡。当弹性效应大于对流效应时,第二次转变发生,但相对较为平缓。第二次转变似乎由所谓的魏森贝格效应主导。这些转变对驱动力不敏感。通过标度分析表明,在Wi-Re空间中首次转变的边界上,应力分量与雷诺数成正比。这种标度关系与数值结果吻合得很好。

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