平行板通道中因压力梯度突然消失而产生的耦合应力流体的非稳态流动

Pub Date : 2024-07-12 DOI:10.24425/ather.2024.151220
Donga Anjali, Naresh Reddimalla, J. V. Ramana Murthy
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引用次数: 0

摘要

本研究考虑了在压力梯度突然停止的情况下,两平行板之间耦合应力流体的流动特性。最初,耦合应力流体在恒定压力梯度下在两个平行板之间流动。突然,施加的压力梯度停止,由此产生的非稳态流动被研究。这种类型的流动在文献中被称为 "上升流动"。现在,预计流动将在很长时间内停止。通常,这类问题采用拉普拉斯变换技术来解决。由于难以获得反拉普拉斯变换,许多研究人员采用了拉普拉斯变换的数值反演。本文采用变量分离法来解决问题。这种方法比变换法简单。通过在板上应用通常的无滑动条件和超粘性条件,分析得到速度场,从而得出随后时间的体积流量。压力梯度撤消前的稳态解与时间上的初始条件相匹配。计算静止时间,即压力梯度撤消后流体静止所需的时间。绘制不同时间和不同耦合应力参数下的速度场图。在耦合应力参数接近无穷大的特殊情况下,耦合应力流体会变成粘性流体。我们的结果与这种特殊情况非常吻合。
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Unsteady flow of a couple stress fluid due to sudden withdrawal of pressure gradient in a parallel plate channel
The investigation of the couple stress fluid flow behaviour between two parallel plates under sudden stoppage of the pressure gradient is considered. Initially, a flow of couple stress fluid is developed between the two parallel plates under a constant pressure gradient. Suddenly, the applied pressure gradient is stopped, and the resulting unsteady flow is studied. This type of flow is known as run-up flow in the literature. Now the flow is expected to come to rest in a long time. Usually, these types of problems are solved by using the Laplace transform technique. There are difficulties in obtaining the inverse Laplace transform; hence, many researchers adopt numerical inversions of Laplace transforms. In this paper, the problem is solved by using the separation of variables method. This method is easier than the transform method. The velocity field is analyti-cally obtained by applying the usual no-slip condition and hyper-stick conditions on the plates, and hence the volumetric flow rate is derived at subsequent times. The steady state solution before the withdrawal of the pressure gradient is matched with the initial condition on time. The rest time, i.e. the time taken by the fluid to come to rest after the pressure gradient is withdrawn is calculated. The graphs for the velocity field at different times and different couple stress parameters are drawn. In the special case when a couple stress parameter approaches infinity, couple stress fluid becomes a viscous fluid. Our results are in good agreement with this special case.
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