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首页> 外文期刊>Physics of fluids >Planar non-Newtonian confined laminar impinging jets: Hysteresis, linear stability, and periodic flow
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Planar non-Newtonian confined laminar impinging jets: Hysteresis, linear stability, and periodic flow

机译:平面非牛顿限制层撞击喷射:滞后,线性稳定性和周期性流动

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摘要

This paper considers the linear stability of confined planar impinging jet flow of a non-Newtonian inelastic fluid. The rheology is shear rate dependent with asymptotic Newtonian behavior in the zero shear limit, and the analysis examines both shear thinning and shear thickening behavior. The planar configuration is such that the width of the inlet nozzle is smaller than the distance from the jet exit to the impinging surface, giving an aspect ratio e = 8 for which two-dimensional time dependent flowis readily manifest. For values of the power-lawindex n in the range 0.4 = n = 1.1, the bi-global linear stability of the laminar flow is analyzed for Newtonian Reynolds numbers Re. 200. The calculations show that for certain values of n, including the Newtonian value n = 1, the steady flow exhibits multiplicity leading to hysteresis in the primary separation vortex reattachment point and a consequent jump in stability behavior. Even in the absence of hysteresis, relatively small changes in viscosity significantly affect stability characteristics. For Newtonian and mildly shear thinning or shear thickening fluids, an unstable flow shows a decaying perturbation growth rate as Re is increased, and for certain values of n, the flow may be restabilized at a larger Re before eventually becoming unstable again. This decay in the growth rate of the critical antisymmetric mode may be correlated as a function of the reattachment point RP of the primary separation vortex in the underlying steady flow. Representative results are analyzed in detail and discussed in the context of some experimental observations of time-dependent Newtonian impinging flow. The stability results are used to construct the neutral stability curve (n, Re) that displays multiplicity and contains several cusp points associated with flow restabilization and hysteresis. Integration of the full nonlinear equation reveals the structure of the time periodic flow field for both Newtonian and non-Newtonian
机译:本文考虑了狭窄的平面撞击非牛顿非弹性流体的射流流动的线性稳定性。流变学是沉秒剪切极限的渐近牛顿行为的剪切速率,分析检查了剪切稀释和剪切增厚行为。平面配置使得入口喷嘴的宽度小于从射流出口到撞击表面的距离,给出纵横比E = 8,其二维时间依赖于其易于清单。对于0.4℃的功率-AtawIndex n的值,对于0.4 = 1.1,分析了层流的双全局线性稳定性,用于牛顿雷诺数RE。计算结果表明,对于N的某些值,包括牛顿值n = 1,稳定流量显示出初级分离涡流重新连接点中的滞后和随后的稳定行为跳跃。即使在没有滞后的情况下,粘度的相对较小的变化也显着影响稳定性特征。对于牛顿和轻度剪切稀释或剪切增稠流体,不稳定的流动显示出RE增加的衰减扰动生长速率,并且对于N的某些值,该流动可以在最终再次变得不稳定之前在更大的RE处重新缩放。在临界反对法模式的生长速率中的这种衰减可以作为底层稳定流动中的初级分离涡流的重新定位点Rp的函数相关。分析了代表性结果,并在一些实验观察时间依赖于牛顿撞击流的情况下进行了讨论。稳定性结果用于构造显示多重性的中性稳定性曲线(n,Re),并包含与流程恢复和滞后相关的几个尖端点。完全非线性方程的集成揭示了牛顿和非牛顿的时间级流动场的结构

著录项

  • 来源
    《Physics of fluids》 |2017年第10期|共19页
  • 作者

    Chatterjee Ajay; Fabris Drazen;

  • 作者单位

    Santa Clara Univ Dept Mech Engn 500 El Camino Real Santa Clara CA 95053 USA;

    Santa Clara Univ Dept Mech Engn 500 El Camino Real Santa Clara CA 95053 USA;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 流体力学;
  • 关键词

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