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Response of open-channel flow to a sudden change from smooth to rough bed

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Abstract

The turbulence characteristics in open-channel flow owing to a sudden change from smooth (upstream) to rough (downstream) bed are investigated experimentally using a Particle Image Velocimetry system. The upstream flow had a shear Reynolds number of 4.86, characterizing the hydraulically smooth flow, while the downstream flow had a shear Reynolds number greater than 70, characterizing the hydraulically rough flow. The Reynolds stress results reveal that for a given vertical distance, both the Reynolds shear and normal stresses in the downstream bed increase with the streamwise distance as compared to their upstream values. Their peaks appear at a distance of one-fifth of the flow depth from the bed. In addition, the bed shear stress enhances with the streamwise distance. The stress contours corroborate that the formation of a roughness-induced layer over the downstream bed thickens with the streamwise distance. The third-order correlations reveal that an arrival of slowly moving fluid streaks associated with an outward Reynolds stress diffusion prevails in the flow on the upstream bed, while an inrush of rapidly moving fluid streaks associated with an inward Reynolds stress diffusion governs the near-bed flow zone in the downstream bed. These results are in conformity with those obtained from the turbulent kinetic energy (TKE) fluxes and the bursting events. With regard to the TKE budget, the peaks of TKE production and dissipation rates appear near the downstream bed and are greater than those in the upstream bed. However, in the downstream bed, an enhanced negative TKE diffusion prevails near the bed.

Article highlights

  • Turbulent flow field on a sudden change from smooth to rough bed converting the flow from smooth to rough.

  • Formation of a roughness-induced layer over the downstream rough bed.

  • Understanding the effects of a sudden change in bed roughness on the turbulence characteristics from the perspectives of their time-averaged spatial fields.

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Data availability

Data used in Figs. 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18 and 19 are available from the corresponding author by request.

Abbreviations

D 50 :

Median size of uniform gravel

d 50 :

Median size of sand

E D :

Normalized TKE dissipation rate

F :

Froude number

F ku :

Normalized streamwise TKE flux

F kw :

Normalized vertical TKE flux

f ku :

Streamwise TKE flux

f kw :

Vertical TKE flux

g :

Gravitational acceleration

H :

Hole size

h :

Flow depth

I :

Turbulence indicator

k :

Time-averaged TKE

k s :

Average roughness height

L :

Streamwise distance required to grow δ

m jk :

Third-order correlations

P D :

Normalized pressure energy diffusion rate

p′:

Pressure fluctuation

p d :

Pressure energy diffusion rate

Q i :

Quadrant i

R * :

Shear Reynolds number

S :

Streamwise bed slope

S i , H :

Fractional contribution of conditional Reynolds shear stress

T :

Sampling time

T D :

Normalized TKE diffusion rate

T P :

Normalized TKE production rate

t :

Time

t d :

TKE diffusion rate

t p :

TKE production rate

\(\overline{U}\) :

Time-averaged flow velocity

U a :

Depth-averaged streamwise velocity

U c :

Threshold streamwise velocity

U max :

Maximum streamwise velocity

\(\overline{u}\) :

Time-averaged streamwise velocity

u′:

Fluctuations of streamwise velocity

u * :

Shear velocity

u * x :

Local shear velocity at x

v d :

Viscous diffusion rate

\(\overline{w}\) :

Time-averaged vertical velocity

w′:

Fluctuations of vertical velocity

x :

Streamwise coordinate

z :

Vertical coordinate

z 0 :

Zero-velocity level

ν :

Coefficient of kinematic viscosity of water

Δ t :

Inter-frame time

Δz :

Depth of virtual bed level from bed surface or Nikuradse zero-plane displacement

δ :

Boundary layer thickness

δ 0 :

Roughness-induced layer thickness

ε :

TKE dissipation rate

κ :

Von Kármán coefficient

λ i , H :

Detecting function

ρ :

Mass density of water

τ 0 :

Bed shear stress

ω :

Instantaneous vorticity

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Acknowledgements

The authors acknowledge the financial support provided by the “SILA” PONa3_00341 project, “An Integrated System of Laboratories for the Environment”. SD also acknowledges the JC Bose Fellowship Award [funded by DST, Science and Engineering Research Board (SERB), Grant Reference No JCB/2018/000004] this collaborative work.

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Correspondence to Subhasish Dey.

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Rathore, V., Penna, N., Dey, S. et al. Response of open-channel flow to a sudden change from smooth to rough bed. Environ Fluid Mech 22, 87–112 (2022). https://doi.org/10.1007/s10652-021-09830-5

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