TY - GEN
T1 - Development of Kelvin Helmholtz coherent structures over a rough bed
AU - Bastien, Cerino
AU - Sébastien, Proust
AU - Céline, Berni
AU - Vladimir, Nikora
PY - 2023/8/25
Y1 - 2023/8/25
N2 - The Kelvin-Helmholtz Coherent Structures (KHCSs) that can populate Shallow Mixing Layers (SMLs) over a hydraulically rough bed are investigated in an 18 m long and 1.98 m wide tilted open-channel flume. A comparison with SMLs developing over a smooth bed is also carried out. A total of eight transversely sheared flows are studied by varying: (1) the total discharge, i.e. the flow depth; and (2) the flow partition from either side of the splitter plate, i.e. the initial shear parameter (λ=(U2-U1)/ (U2+U1) (where U2 and U1 are streamwise time-averaged velocities characterizing the high-speed and low-speed streams, respectively). The potential impact of the bed roughness on the emergence and fate of the KHCSs is discussed. The emergence of KHCSs is found to be controlled by the shear parameter, with the same threshold- value (λ>0.3) required over rough and smooth beds. Over a smooth bed, it was observed that the longitudinal stretching and final decay of the KHCSs were controlled by the bed friction number, S= (Cfδv/4hλ) (with cf = friction coefficient, δv = mixing layer width, and h = water depth). The longitudinal stretching starts S >~ 0.01 and the KHCSs vanish when S> ~. 0.1.Over the rough bed, two threshold values of S-parameter are also observed, which are of the same order of magnitude as the smooth-bed values.
AB - The Kelvin-Helmholtz Coherent Structures (KHCSs) that can populate Shallow Mixing Layers (SMLs) over a hydraulically rough bed are investigated in an 18 m long and 1.98 m wide tilted open-channel flume. A comparison with SMLs developing over a smooth bed is also carried out. A total of eight transversely sheared flows are studied by varying: (1) the total discharge, i.e. the flow depth; and (2) the flow partition from either side of the splitter plate, i.e. the initial shear parameter (λ=(U2-U1)/ (U2+U1) (where U2 and U1 are streamwise time-averaged velocities characterizing the high-speed and low-speed streams, respectively). The potential impact of the bed roughness on the emergence and fate of the KHCSs is discussed. The emergence of KHCSs is found to be controlled by the shear parameter, with the same threshold- value (λ>0.3) required over rough and smooth beds. Over a smooth bed, it was observed that the longitudinal stretching and final decay of the KHCSs were controlled by the bed friction number, S= (Cfδv/4hλ) (with cf = friction coefficient, δv = mixing layer width, and h = water depth). The longitudinal stretching starts S >~ 0.01 and the KHCSs vanish when S> ~. 0.1.Over the rough bed, two threshold values of S-parameter are also observed, which are of the same order of magnitude as the smooth-bed values.
KW - Kelvin-Helmholtz coherent structures
KW - rough bed
KW - shallow shear flows
KW - shear layer turbulence
UR - https://www.scopus.com/pages/publications/85187698979
U2 - 10.3850/978-90-833476-1-5_iahr40wc-p0193-cd
DO - 10.3850/978-90-833476-1-5_iahr40wc-p0193-cd
M3 - Published conference contribution
AN - SCOPUS:85187698979
SN - 9789083347615
T3 - Proceedings of the IAHR World Congress
SP - 33
EP - 37
BT - Proceedings of the 40th IAHR World Congress
A2 - Habersack, Helmut
A2 - Tritthart, Michael
A2 - Waldenberger, Lisa
PB - International Association for Hydro-Environment Engineering and Research -IAHR
T2 - 40th IAHR World Congress, 2023
Y2 - 21 August 2023 through 25 August 2023
ER -