Abstract

Pulsatile channel and pipe flows constitute a fundamental flow configuration with significant bearing on many applications in the engineering and medical sciences. Rotating machinery, hydraulic pumps or cardiovascular systems are dominated by time-periodic flows, and their stability characteristics play an important role in their efficient and proper operation. While previous work has mainly concentrated on the modal, harmonic response to an oscillatory or pulsatile base flow, this study employs a direct–adjoint optimisation technique to assess short-term instabilities, identify transient energy-amplification mechanisms and determine their prevalence within a wide parameter space. At low pulsation amplitudes, the transient dynamics is found to be similar to that resulting from the equivalent steady parabolic flow profile, and the oscillating flow component appears to have only a weak effect. After a critical pulsation amplitude is surpassed, linear transient growth is shown to increase exponentially with the pulsation amplitude and to occur mainly during the slow part of the pulsation cycle. In this latter regime, a detailed analysis of the energy transfer mechanisms demonstrates that the huge linear transient growth factors are the result of an optimal combination of Orr mechanism and intracyclic normal-mode growth during half a pulsation cycle. Two-dimensional sinuous perturbations are favoured in channel flow, while pipe flow is dominated by helical perturbations. An extensive parameter study is presented that tracks these flow features across variations in the pulsation amplitude, Reynolds and Womersley numbers, perturbation wavenumbers and imposed time horizon.

Highlights

  • Pulsatile flows are a common phenomenon in a variety of engineering flows, and they are ubiquitous in physiological configurations

  • The control parameters are the same as those used in figure 2 for pulsating channel flow, and it is observed that the transient growth properties are very similar

  • The optimised duration tf − ti is given in mean-flow advection units τQ in figure 19(c) and in units of the pulsation period T in figure 19(d). These plots illustrate that pulsating pipe flows display similar transient dynamics as channel flows: for Q < Qc, the optimal duration tf −ti remains close to the value prevailing for the average parabolic flow profile; for Q > Qc, when helical perturbations dominate, maximal amplification occurs over intervals corresponding approximately to half a pulsation period

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Summary

Introduction

Pulsatile flows are a common phenomenon in a variety of engineering flows, and they are ubiquitous in physiological configurations. The application of these nonmodal techniques to hydrodynamic stability calculations has resulted in a more complete understanding of shear-driven instability phenomena The generality of this approach (Schmid 2007) is well-suited for assessing pulsatile flow over a range of time scales, mapping out the optimal perturbation dynamics over partial and multiple pulsation cycles. This article follows up on and extends earlier work (Pier & Schmid 2017) that demonstrated the influence of a pulsating flow component on the stability of channel flow via a linear (Floquet) and nonlinear analysis In this present study, we focus on nonmodal effects and the occurrence of transient energy amplification mechanisms under conditions that are asymptotically stable, both for rectangular channel and cylindrical pipe flows. The present paper represents the culmination of several years of work; a preliminary version of the main results has been presented at the 12th European Fluid Mechanics Conference in Vienna (Pier & Schmid 2018)

Flow configurations and governing equations
Base flows and non-dimensional control parameters
Mathematical formulation
Numerical implementation
Pulsating channel flow
Growth of streaks
Growth of two-dimensional perturbations
Growth of three-dimensional perturbations
Maximal transient growth
Discussion of energy transfer mechanisms
Two-dimensional maximally amplified optimal perturbation
I μ2F Gnm
Pulsating pipe flow
Transient growth of streaks and helical perturbations
Optimal growth at given wavenumbers
Maximal amplification
Conclusion

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