The laminar flow past rectangular prisms is studied in the space of length-to-height ratio , width-to-height ratio and Reynolds number; and are the streamwise and cross-flow dimensions of the prisms. The primary bifurcation is investigated with linear stability analysis. For large, an oscillating mode breaks the top/bottom planar symmetry. For smaller, the flow becomes unstable to stationary perturbations and the wake experiences a static deflection, vertical for intermediate and horizontal for small. Weakly nonlinear analysis and nonlinear direct numerical simulations are used for and larger. For and 2.25, the flow recovers the top/bottom planar symmetry but loses the left/right one, via supercritical and subcritical pitchfork bifurcations, respectively. For even larger, the flow becomes unsteady and oscillates around either the deflected (small) or the non-deflected (intermediate) wake. For intermediate and, a fully symmetric periodic regime is detected, with hairpin vortices shed from the top and bottom leading-edge (LE) shear layers; its triggering mechanism is discussed. At large and for all, the flow approaches a chaotic state characterised by the superposition of different modes: shedding of hairpin vortices from the LE shear layers, and wake oscillations in the horizontal and vertical directions. In some portions of the parameter space the different modes synchronise, giving rise to periodic regimes also at relatively large.

Stability and dynamics of the laminar flow past rectangular prisms

Chiarini, Alessandro;
2025-01-01

Abstract

The laminar flow past rectangular prisms is studied in the space of length-to-height ratio , width-to-height ratio and Reynolds number; and are the streamwise and cross-flow dimensions of the prisms. The primary bifurcation is investigated with linear stability analysis. For large, an oscillating mode breaks the top/bottom planar symmetry. For smaller, the flow becomes unstable to stationary perturbations and the wake experiences a static deflection, vertical for intermediate and horizontal for small. Weakly nonlinear analysis and nonlinear direct numerical simulations are used for and larger. For and 2.25, the flow recovers the top/bottom planar symmetry but loses the left/right one, via supercritical and subcritical pitchfork bifurcations, respectively. For even larger, the flow becomes unsteady and oscillates around either the deflected (small) or the non-deflected (intermediate) wake. For intermediate and, a fully symmetric periodic regime is detected, with hairpin vortices shed from the top and bottom leading-edge (LE) shear layers; its triggering mechanism is discussed. At large and for all, the flow approaches a chaotic state characterised by the superposition of different modes: shedding of hairpin vortices from the LE shear layers, and wake oscillations in the horizontal and vertical directions. In some portions of the parameter space the different modes synchronise, giving rise to periodic regimes also at relatively large.
2025
vortex shedding
wakes
File in questo prodotto:
File Dimensione Formato  
CHIAA01-25.pdf

accesso aperto

: Publisher’s version
Dimensione 6.69 MB
Formato Adobe PDF
6.69 MB Adobe PDF Visualizza/Apri

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11311/1291206
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 3
  • ???jsp.display-item.citation.isi??? 3
social impact