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pdf, 12 MiB - Infoscience - EPFL

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Chapter 7 - Establishing an empirical formula<br />

Cross section in the upper scour hole<br />

Radius from center of the bend [m]<br />

6.5<br />

6.3<br />

6.1<br />

5.9<br />

5.7<br />

5.5<br />

0.0<br />

3<br />

0.1<br />

Water depth [m]<br />

60%<br />

0.2<br />

2<br />

C01b<br />

C01c<br />

2<br />

40%<br />

0.3<br />

C01d<br />

1 1<br />

20%<br />

0.4<br />

sin(beta)<br />

0%<br />

3<br />

0.5<br />

-20%<br />

Figure 7.3: Characteristic points in a cross-section profile at the (upstream) maximum scour location<br />

on top: cross-section in the upper scour; bottom right: transversal bed slope as a function of h/r<br />

a) Polynomial function of the 3rd degree - centered<br />

First a centered polynomial function is analyzed:<br />

-40%<br />

0.00 0.02 0.04 0.06<br />

h/r<br />

h s<br />

= h s () r =<br />

c<br />

---- 1<br />

⋅ ( r–<br />

c<br />

3 2<br />

) 3 + c 3<br />

( r–<br />

c 2<br />

) + c 4<br />

(7.8)<br />

dh<br />

------- s<br />

= c (7.9)<br />

dr 1<br />

⋅ ( r – c 2<br />

) 2 + c 3<br />

The boundary conditions are:<br />

1. dh s ( R c ) ⁄ dr = tanφ∗<br />

: the maximum bed slope is tanφ∗<br />

, located on the channel axis.<br />

2. h s ( R c ) = h m : the water depth in the center of the channel is equal to the mean water<br />

depth in the cross-section.<br />

3. dh s ( r i ) ⁄ dr = dh s ( r o ) ⁄ dr = 0 : the transversal bed slope is equal to zero at the outer and<br />

inner side wall.<br />

page 160 / November 9, 2002<br />

Wall roughness effects on flow and scouring

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