pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Chapter 7 - Establishing an empirical formula<br />
which is correct. The ratio friction velocity to mean velocity has no significant influence on the<br />
scour but is almost constant at about 0.1.<br />
7<br />
6<br />
5<br />
h <strong>12</strong>,max<br />
Computed<br />
4<br />
3<br />
2<br />
Table 7.5:<br />
1<br />
ID 101<br />
0<br />
0 1 2 3 4 5 6 7<br />
0 1 2 3 4 5 6 7<br />
Plots of the maximum relative scour depth obtained with GPKernel with macro-roughness<br />
(ID 101 corresponds to eq. 7.58, ID 1<strong>12</strong> to eq. 7.59, ID <strong>12</strong>4)<br />
ID 1<strong>12</strong><br />
Replacing V∗ ⁄ V by a constant of 0.2, leads to almost the same correlation ( R 2 = 0.885 ). If we<br />
regroup the two terms θ to form Cst + θ 2 , and adjust the constant, the correlation is even<br />
increased to R 2 = 0.887 . The constant has a value of 0.002. Since the square of θ cr = 0.047<br />
gives exactly the same result, it is tempting to write:<br />
h<br />
-------------- smax ,<br />
0.95 e s<br />
= ⋅ ----- ⋅( θ2 , (7.62)<br />
h m<br />
R cr + θ 2 ) ⋅Fr<br />
+ 1.83 R 2 = 0.887<br />
h<br />
The problem is that θ2 cr + θ 2 has not directly a physical signification. But if we write<br />
( θ–<br />
θ cr ) 2 = θ 2 – 2 ⋅θ⋅θ cr + θ2<br />
cr , we find a physical explanation (unfortunately with a worse<br />
correlation). Some additional simplifications and optimizations result in:<br />
h<br />
-------------- smax ,<br />
7.7 e s<br />
= ⋅ ----- ⋅ Fr ⋅( 0.001 + ( θ–<br />
θ , (7.63)<br />
h m<br />
R cr ) 2 ) + 1.7 R 2 = 0.876<br />
h<br />
If we check this equation with the data set without macro-roughness, (admitting e s = 11.3 m for<br />
the tests without ribs), we find R 2 = 0.766 . Considering only the data set with macro-roughness,<br />
the correlation is rather poor ( R 2 = 0.537 ) (see Figure 7.<strong>12</strong>) but still much better compared to<br />
directly computed scour depth (see § 7.4). This poor correlation is due to the fact that the tests<br />
performed with ribs cover only a limited range of the hydraulic parameters. In average, the prediction<br />
capability is quite well (see Figure 7.<strong>12</strong>).<br />
All parameters in equation 7.63 have a physical meaning. The scour depth grows with increasing<br />
rib spacing, Froude number and Shields parameter. A possible explanation for the constant 0.001<br />
is that the Shields parameter θ is computed in the inlet reach; but in the bend, the erosive power<br />
is more important, which is translated by the constant 0.001.<br />
page 180 / November 9, 2002<br />
Wall roughness effects on flow and scouring