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Distribution of turbulent intensity in a gravel-bed flume

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Abstract

Detailed measurements have been taken for the longitudinal turbulent intensities of flow in a gravel-bed flume. The experimental results indicate that the distribution of turbulent intensity greatly depends on the relative roughness. In comparison with the smooth-bed results, the roughness makes the flow turbulence become well-distributed, especially in the region near the bed and in the case of smaller H/K s values. In addition, the cross sectional average of turbulent intensity is also discussed in this paper, and the results show that the roughness makes flow turbulence much more intense.

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Abbreviations

D u :

empirical constant

H :

flow depth

K s :

roughness height

N :

\(N = \frac{1}{H}\int\limits_0^H {\frac{{u\prime }}{{\bar U}}} {\text{ }}dy\), the mean turbulence intensity over the cross section

Re * :

\(Re* = \frac{{k_s u_* }}{\nu }\), roughness Reynolds number

u′ :

the RMS of streamwise fluctuating velocity

u * :

friction velocity

Ū :

mean bulk velocity

x :

coordinate alined with mainstream velocity (x = 0 is channel entrance)

y :

vertical coordinate to the rough bed (y = 0 is the top of the rough elements)

y + \(\frac{{yu_* }}{\nu }\) :

λ u empirical constant

v :

kinematic viscosity

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Wang, JJ. Distribution of turbulent intensity in a gravel-bed flume. Experiments in Fluids 11, 201–202 (1991). https://doi.org/10.1007/BF00190303

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  • DOI: https://doi.org/10.1007/BF00190303

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