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arXiv 1302.4518physics.flu-dynmath.APmath.DSmath.OC
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粘弹性流体无惯性Couette流中扰动的最坏情况放大

Worst-case amplification of disturbances in inertialess Couette flow of viscoelastic fluids

Binh K. Lieu, Mihailo R. Jovanović, Satish Kumar

摘要:

通过分析时空体积力对速度和聚合物应力波动的频率响应,研究了粘弹性流体无惯性剪切驱动槽道流中确定性扰动的放大。在强弹性流中,我们表明,即使在没有惯性的情况下,大流向长度尺度的扰动也可能被显着放大。对于没有流向变化的波动,我们推导出明确的解析表达式的依赖性的最坏情况下的放大(从不同的迫使不同的速度和聚合物应力分量)的韦森伯格数($We$),聚合物链($L$)的最大可延伸性,粘度比,和展向波数。对于Oldrophil-B模型,速度和聚合物应力场的最高能量分量的放大比例为$We^2$和$We^4$。另一方面,聚合物分子的有限延伸性限制了即使在具有无限大的Weissenberg数的流动中也可实现的最大放大:在壁法线和展向力的存在下,流向速度和聚合物应力波动的放大受$L$的二次和四次函数的约束。这种高放大率表明对粘弹性流体的无惯性通道流的建模缺陷的鲁棒性低。潜在的物理机制涉及聚合物应力波动与基底剪切的相互作用,并且它代表了在牛顿流体的惯性流中启动旁路转变的提升机制的密切类似物。

英文摘要:

Amplification of deterministic disturbances in inertialess shear-driven channel flows of viscoelastic fluids is examined by analyzing the frequency responses from spatio-temporal body forces to the velocity and polymer stress fluctuations. In strongly elastic flows, we show that disturbances with large streamwise length scales may be significantly amplified even in the absence of inertia. For fluctuations without streamwise variations, we derive explicit analytical expressions for the dependence of the worst-case amplification (from different forcing to different velocity and polymer stress components) on the Weissenberg number ($We$), the maximum extensibility of the polymer chains ($L$), the viscosity ratio, and the spanwise wavenumber. For the Oldroyd-B model, the amplification of the most energetic components of velocity and polymer stress fields scales as $We^2$ and $We^4$. On the other hand, finite extensibility of polymer molecules limits the largest achievable amplification even in flows with infinitely large Weissenberg numbers: in the presence of wall-normal and spanwise forces the amplification of the streamwise velocity and polymer stress fluctuations is bounded by quadratic and quartic functions of $L$. This high amplification signals low robustness to modeling imperfections of inertialess channel flows of viscoelastic fluids. The underlying physical mechanism involves interactions of polymer stress fluctuations with a base shear, and it represents a close analog of the lift-up mechanism that initiates a bypass transition in inertial flows of Newtonian fluids.

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