Abstract

The present work investigates the stability properties of the flow in a 90°-bend pipe with curvature δ=R/Rc=1/3, with R being the radius of the cross-section of the pipe and Rc the radius of curvature at the pipe centreline. Direct numerical simulations (DNS) for values of the bulk Reynolds number Reb=UbD/ν between 2000 and 3000 are performed. The bulk Reynolds number is based on the bulk velocity Ub, the pipe diameter D, and the kinematic viscosity ν. The flow is found to be steady for Reb⩽2500, with two main pairs of symmetric, counter-rotating vortices in the section of the pipe downstream of the bend. The presence of two recirculation regions is detected inside the bend: one on the outer wall and the other on the inner side. For Reb⩾2550, the flow exhibits a periodic behaviour, oscillating with a fundamental non-dimensional frequency St=fD/Ub=0.23. A global stability analysis is performed in order to determine the cause of the transition from the steady to the periodic regime. The spectrum of the linearised Navier-Stokes operator reveals a pair of complex conjugate eigenvalues with positive real part, hence the transition is ascribed to a Hopf bifurcation occurring at Reb,cr≈2531, a value much lower than the critical Reynolds number for the flow in a torus with the same curvature. The velocity components of the unstable direct and adjoint eigenmodes are investigated, and they display a large spatial separation, most likely due to the non-normality of the linearised Navier-Stokes operator. Thus, the core of the instability, also known in the literature as the wavemaker, is sought performing an analysis of the structural sensitivity of the unstable eigenmode to spatially localised feedbacks. The region located 15° downstream of the bend inlet, on the outer wall, is the most receptive to this kind of perturbations, and thus corresponds to where the instability originates. Since this region coincides with the outer-wall separation bubble, it is concluded that the instability is linked to the strong shear by the backflow phenomena. The present results are relevant for technical applications where bent pipes are frequently used, and their stability properties have hitherto not been studied.

Highlights

  • The main peculiarity of the flow in curved pipes, when compared to that in a straight one, is the occurrence of a secondary motion consisting of a pair of symmetric, counter-rotating vortices

  • The onset of transition in a 90◦-bend pipe with curvature 1/3 is investigated by means of direct numerical simulations

  • The flow is found to be steady for Reb⩽2500, and two separation bubbles are observed inside the bend, one on the outer wall and another on the inner side

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Summary

Introduction

The main peculiarity of the flow in curved pipes, when compared to that in a straight one, is the occurrence of a secondary motion consisting of a pair of symmetric, counter-rotating vortices. Dean (1927) and Dean (1928) studied the flow analytically and found a solution of the incompressible NavierStokes equations valid in the small-curvature assumption In this way, a mathematical proof of the existence of the secondary motion in the form of two symmetric counter-rotating vortices, named after Dean, was given. In a recent numerical study, Rinaldi et al (2019) observed that, for curved pipes with δ = 0.01 and 2950≲Reb≲3100, subcritical transition occurs as the intermittent coex­ istence of laminar flow and turbulent puffs, a behaviour in agreement with the experimental results by Sreenivasan and Strykowski (1983) and Kühnen et al (2015).

Numerical method
Instantaneous flow fields
Base flow
Global stability analysis
Findings
Summary and conclusions

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