Abstract

It is widely acknowledged that streamwise ridges on the bed of open-channel flows generate secondary currents (SCs). A recent discovery of meandering long streamwise counter-rotating vortices in open-channel flows, known as very-large-scale motions (VLSMs), raises a question regarding the interrelations between VLSMs and SCs in flows over ridge-covered fully rough beds. To address it, we conducted long-duration experiments using stereoscopic particle image velocimetry, covering a range of ridge spacings ( ) from to flow depths ( ). For a benchmark no-ridge case, the flow is quasi-two-dimensional in the central part of the channel, exhibiting a strong spectral signature of VLSMs, as expected. With ridges on the bed at , two SC cells are formed between neighbouring ridges and VLSMs are entirely suppressed, suggesting that ridge-induced SCs prevent the formation of VLSMs by absorbing their energy or overpowering their formation. At the same time, velocity auto- and cross-spectra reveal a new feature that can be explained by low-amplitude meandering of the alternating low- and high-momentum flow regions associated with instantaneous manifestations of SCs. Two-point velocity correlations and smooth velocity field reconstructions using proper orthogonal decomposition further support the validity of this effect. Its origin is probably due to the instability related to the presence of inflection points in the spanwise distribution of the streamwise velocity within the SC cells. These results have implications for bed friction in open channels, where the friction factor may increase if depth-scale SCs are present, or decrease under conditions of sub-depth-scale SCs and suppressed VLSMs.

Highlights

  • Streamwise time-averaged vortices, known as secondary currents (SCs), can often be observed in straight open-channel flows (OCFs), where they are generated near the sidewalls due to the effects of turbulence anisotropy (e.g. Nezu & Nakagawa 1993)

  • The objective of this study is to explore SCs and very-large-scale motions (VLSMs) in OCFs over hydraulically rough beds covered by streamwise ridges, for a range of ridge spacings

  • Velocity spectra and co-spectra showed that the ≈25H long VLSMs identifiable in the case without ridges are absent once ridges are added to the bed at s 2H

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Summary

Introduction

Streamwise time-averaged vortices, known as secondary currents (SCs), can often be observed in straight open-channel flows (OCFs), where they are generated near the sidewalls due to the effects of turbulence anisotropy (e.g. Nezu & Nakagawa 1993). Streamwise time-averaged vortices, known as secondary currents (SCs), can often be observed in straight open-channel flows (OCFs), where they are generated near the sidewalls due to the effects of turbulence anisotropy Nezu & Nakagawa 1993). SCs can emerge within the flow cross-section if the bed is spanwise heterogeneous Such heterogeneities can be associated with changes in bed topography (variations in bed elevation comparable to the flow outer scale, i.e. the flow depth in OCFs) and/or in bed surface roughness. Mobile-bed open channels may be characterised by the natural appearance of spanwise-periodic streamwise sand or gravel ridges Colombini & Parker 1995), continuous protrusions along the flow that generally feature different surface roughness from the rest of the bed Mobile-bed open channels may be characterised by the natural appearance of spanwise-periodic streamwise sand or gravel ridges (e.g. Colombini & Parker 1995), continuous protrusions along the flow that generally feature different surface roughness from the rest of the bed

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