Stability and dynamics of the flow past of a bullet-shaped blunt body moving in a pipe

TL;DR

This study investigates the flow stability and nonlinear dynamics of a bullet-shaped body in a pipe using linear stability analysis and numerical simulations, revealing bifurcation behaviors and flow regimes across various parameters.

Contribution

It provides a comprehensive bifurcation map for flow past a blunt body in a pipe, combining stability analysis with nonlinear simulations to understand flow transitions.

Findings

First bifurcation is a steady mode with azimuthal wavenumber m=±1.

Weak confinement leads to oscillating second bifurcation; strong confinement causes different mode destabilizations.

Nonlinear dynamics include steady, periodic, and complex aperiodic states depending on confinement.

Abstract

The flow past a bullet-shaped blunt body moving in a pipe is investigated through global linear stability analysis (LSA) and direct numerical simulation (DNS). A cartography of the bifurcation curves is provided thanks to LSA, covering the range of parameters corresponding to Reynolds number $Re = [50-110]$, confinement ratio $a/A = [ 0.01 - 0.92]$ and length-to-diameter ratio $L/d = [ 2-10]$. Results show that the first bifurcation is always a steady bifurcation associated to a non-oscillating eigenmode with azimuthal wavenumber $m=\pm 1$ leading to a steady state with planar symmetry. For weakly confined cases ($a/A<0.6$) the second bifurcation is associated to an oscillating mode with azimuthal wavenumber $m=\pm 1$, as in the unconfined case. On the other hand, for the strongly confined case ($a/A>0.8$), on observes destabilization of non-oscillating modes with $|m| =2,3$ and a restabilization of the $m=\pm1$ eigenmodes. The aspect ratio $L/d$ is shown to have a minor influence for weakly confined cases and almost no influence for strongly confined cases. DNS is subsequently used to characterize the nonlinear dynamics. The results confirm the steady bifurcation predicted by LSA with excellent agreement for the threshold Reynolds. For weakly confined cases, the second bifurcation is a Hopf bifurcation leading to a periodic, planar-symmetric state in qualitative accordance with LSA predictions. For more confined cases, more complex dynamics is obtained, including a steady state with $|m|=3$ geometry and aperiodic states.