Revisit the intrinsic features of flip-flopping flow behind side-by-side circular cylinders

TL;DR

This paper investigates the flip-flopping wake patterns behind side-by-side circular cylinders, analyzing their origins, connections across flow regimes, and mechanisms affecting their switching time scales, revealing new insights into vortex dynamics.

Contribution

The study classifies flip-flopping flow into laminar sub-classes and links turbulent flip-flopping to laminar vortex interactions, providing a comprehensive understanding of flow regime transitions.

Findings

FF flow in laminar regime arises from vortex shedding instabilities

Turbulent FF flow shares origins with laminar FF2 pattern

Switching time scales vary significantly with Reynolds number

Abstract

As one of the most intriguing wake patterns of two side-by-side circular cylinders at an intermediate gap spacing, the flip-flopping (FF) flow has attracted great attention of fundamental research interest. This FF flow is featured by the intermittently and randomly switching gap flow with correspondingly changing forces of the two cylinders. In this paper, we first present a partition map of the wake patterns behind two side-by-side circular cylinders and briefly introduce intrinsic features of each flow pattern. We focus on the FF flow aiming to explain: (i) the origin of the FF flow between laminar and turbulent regimes, (ii) their connections in different flow regimes, and (iii) mechanisms of the significantly varying flip-over time scale of the FF flows. In the laminar regime, we further divide the FF flow into the sub-classed I (FF1) and II (FF2), based on their different origins from the in-phase and anti-phase synchronized vortex shedding instabilities, respectively. By exploring the vortex interactions, we show that the FF flow in the turbulent regime has the same origin and similar vortex dynamics as the FF2 wake in the laminar regime, despite some minor disparities. Thus, a connection is established between the FF2 pattern in the laminar flow and the FF pattern in the turbulent flow. For the FF flow in the laminar regime (Re < 150-200), the mildly decreasing switching time, is several vortex shedding periods. However, for the FF flow in the weak turbulence regime (150-200 < Re < 1000-1700), the switching time scale increases significantly with Re owing to the increased vortex formation length. The FF in the strong turbulence regime (Re > 1000-1700) has a switching time scale of several orders of magnitude longer than the vortex shedding period, where the switching scale decreases gradually with Re due to the stronger Kelvin-Helmholtz vortices.