Abstract

We present a new application of Lagrangian Perturbation Theory (LPT): the stability analysis of fluid flows. As a test case that demonstrates the framework we focus on the plane Couette flow. The incompressible Navier-Stokes equation is recast such that the particle position is the fundamental variable, expressed as a function of Lagrangian coordinates. The displacement due to the steady state flow is taken to be the zeroth order solution and the position is formally expanded in terms of a small parameter (generally, the strength of the initial perturbation). The resulting hierarchy of equations is solved analytically at first order. We find that we recover the standard result in the Eulerian frame: the plane Couette flow is asymptotically stable for all Reynolds numbers. However, it is also well established that experiments contradict this prediction. In the Eulerian picture, one of the proposed explanations is the phenomenon of `transient growth' which is related to the non-normal nature of the linear stability operator. The first order solution in the Lagrangian frame also shows this feature, albeit qualitatively. As a first step, and for the purposes of analytic manipulation, we consider only linear stability of 2D perturbations but the framework presented is general and can be extended to higher orders, other flows and/or 3D perturbations.

Highlights

  • Understanding the transition of fluid flows from the stable to turbulent regime is one of the central questions in the studies of turbulence

  • We examine the stability of laminar flows using a perturbative scheme in the Lagrangian frame i.e., Lagrangian Perturbation Theory (LPT)

  • In addition it recovers the feature of transient growth, which in the Eulerian case is attributed to the nonnormality of the linear stability operator

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Summary

INTRODUCTION

Understanding the transition of fluid flows from the stable to turbulent regime is one of the central questions in the studies of turbulence. One way is to computationally investigate the full non-linear Navier-Stokes equation as was done by Orszag and collaborators [14, 15] who showed that the energy growth in the system corresponds to a sub-critical bifurcation Another is to look for finite amplitude equilibrium states near the transition and examine their stability against two and three dimensional perturbations [16]. The linear analysis using LPT analytically confirms the linear Eulerian stability result that the plane Couette flow is asymptotically stable at all Reynolds numbers. In addition it recovers the feature of transient growth, which in the Eulerian case is attributed to the nonnormality of the linear stability operator.

EQUATIONS IN THE LAGRANGIAN FRAME
Zeroth Order
First Order Equations
Initial and Boundary Conditions
First Order Solution
Discussion
TRANSFORMING BACK TO THE EULERIAN FRAME
CONCLUSION
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