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 />
The shape of the last equation gets quite close to the parabolic form of many traditional equations.<br />
To allow an appreciation of the quality of the obtained relation, an equation with corrections<br />
(eq. 7.20) is given on Fig. 7.7.<br />
The so obtained correlation for the maximum scour depth can be compared to the empirical formula<br />
of PETER (1986), who obtains a correlation of 0.87 compared to the complete data set.<br />
Hoping to obtain even higher correlations with other functions, the following two type of functions<br />
were explored: a polynomial function of the 3rd degree, but with additional terms<br />
( y = x 3 + x 2 + x ) and a polynomial function of the 5th degree.<br />
d) Polynomial function of the 3rd degree with additional terms - uncentered with vertical<br />
adjustment<br />
The following function was used with the boundary conditions mentioned in paragraph c).<br />
Solving for the different constants, leads to:<br />
h s = h m + tanφ∗<br />
⋅<br />
c 1<br />
c<br />
h s<br />
---- ⋅ ( r–<br />
c<br />
3 2<br />
) 3 3<br />
=<br />
+ ---- ( r–<br />
c<br />
2 2<br />
) 2 + c 4<br />
⋅ ( r–<br />
c 2<br />
) + c 5<br />
4<br />
--------<br />
3B 2<br />
1<br />
⋅ ----------------<br />
4ξ 2 ⋅ ( r – R<br />
– 1 c – ξB) 3 ---<br />
4 ξ<br />
+ ⋅ ----------------<br />
B 4ξ 2 ⋅ ( r– R<br />
– 1 c – ξB) 2<br />
B<br />
( r – R c – ξB)<br />
---<br />
4ξ 3 – 3ξ<br />
+ + ⋅ -------------------<br />
3 4ξ 2 – 1<br />
(7.21)<br />
(7.22)<br />
dh<br />
------- s<br />
= tanφ∗<br />
dr<br />
⋅<br />
4<br />
-----<br />
B 2<br />
1<br />
⋅ ----------------<br />
4ξ 2 ⋅ ( r – R<br />
– 1 c – ξB) 2 ---<br />
8 ξ<br />
+ ⋅ ----------------<br />
B 4ξ 2 ⋅( r– R<br />
– 1 c – ξB)<br />
+ 1<br />
(7.23)<br />
The final solution has quite a strange behavior as far as the choice of ξ is concerned. At ± 50 %<br />
the curvature (second derivative) has a discontinuity. Therefore this value had to be avoided.<br />
Without any correction factor the correlation is very low (below 0.50) and the order of magnitude<br />
of the predicted scour does not fit at all. The correlation (maximum scour) can be increased up to<br />
0.81 by introducing a correction factor c = 4.45 ⋅ ( 690 ⋅ S eall ,<br />
+ 5.8 ⋅ R c ⁄ B – 79 ⋅ h m ⁄ B)<br />
, but<br />
the shape of the predicted bed does not fit well to the measured one (Fig. 7.8). With other correction<br />
factors, the bed shape fits better, but with lower correlations up to 0.75.<br />
Rendering the function more complicated does not bring the desired effect of a better prediction<br />
of the maximum scour nor a better fit to the transversal bed topography.<br />
page 166 / November 9, 2002<br />
Wall roughness effects on flow and scouring