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pdf, 12 MiB - Infoscience - EPFL

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Chapter 3 - Theoretical considerations<br />

∆x<br />

B<br />

h<br />

p up<br />

G x<br />

z<br />

G z<br />

G<br />

p dw<br />

τ 0<br />

α<br />

Figure 3.4: Definition of the boundary shear stress as a gravity component<br />

At a given distance z of the ground, the shear stress can be obtained with:<br />

τ τ 0<br />

1<br />

z<br />

= ⋅ ⎛ – --⎞<br />

⎝ h⎠<br />

(3.22)<br />

b) Shear Reynolds number<br />

The Shear Reynolds number is composed in analogy to the Reynolds number. The velocity is<br />

replaced by the shear velocity and the flow depth by the size of the roughness ε .<br />

Re∗ = -------------<br />

V∗ ⋅ ε<br />

(3.23)<br />

ν<br />

c) Densimetric and sediment Froude number<br />

In analogy to the Froude number, two dimensionless numbers are defined to characterize the sediment<br />

transport capacity of a river. The densimetric Froude number Fr 1 d and the sediment<br />

Froude number Fr∗ are distinguished by the used velocity:<br />

Fr d<br />

= ----------------------------------<br />

V<br />

; Fr∗ = ----------------------------------<br />

V∗<br />

= θ<br />

(3.24)<br />

( s – 1) ⋅ g⋅<br />

d<br />

( s – 1) ⋅ g ⋅ d<br />

1. The densimetric Froude number - combining the flow velocity with sediment related characteristics<br />

- is frequently used in literature despite a less explicit physical meaning (compared to Fr∗ ).<br />

page 30 / November 9, 2002<br />

Wall roughness effects on flow and scouring

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