pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Establishment of the scour formula<br />
7.3.3 Approach based on the bed shape of the cross-section<br />
In a typical cross-section profile, the following three important points can be found (Fig. 7.3):<br />
1. In general, the maximum scour depth can be found at the outer side wall. For some tests,<br />
especially the ones with thick vertical ribs (test series E), the maximum scour was sometimes<br />
located close to the outer side wall but not at the wall 1 . For practical reasons, these eventual<br />
depositions (or less scour) were not considered.<br />
2. Somewhere in the outer half of the cross-section, the maximum lateral bed slope can be<br />
found. Since sinβ is an approximation of the lateral bed slope, the highest point on the vertical<br />
axis corresponds to this maximum transversal bed slope (Fig. 7.3).<br />
3. Close to the inner side wall, the highest point in the cross-section can be found (location<br />
with maximum depositions).<br />
The idea explored in this paragraph is to fit a function to the cross-section, passing through the<br />
above mentioned characteristic points. The boundary conditions are given in the following way:<br />
• At the inflection point (steepest transversal bed slope), the first derivative is equal to the<br />
friction slope. The following assumptions are made: (1) the angle of repose of coarse gravel<br />
is the same with dry material as with wet sediments, (2) the maximum transversal bed slope<br />
reaches its maximum possible value φ∗ and (3) this maximal possible value is equal to the<br />
fraction angle multiplied with a factor depending on the main parameters.<br />
• For some functions, the inflection point is assumed being at the center of the channel, for<br />
other ones it is assumed being at a distance ξ ⋅ B from the channel axis.<br />
• Other functions fix the transversal bed slope either at the inner or outer bank equal to zero<br />
(translated by a first derivative of the function being equal to zero).<br />
Looking at the right part of Figure 7.3, the elliptic shape of the curve is obvious. Therefore, functions<br />
fitting that kind of curve were searched. Possible functions are a semi-ellipse, the cosines<br />
hyperbolical (cosh) function or a quadratic polynomial function.<br />
Elliptic and the cosh functions have a solution for y = fct( h s ⁄ r)<br />
, but they cannot be integrated.<br />
Therefore polynomial functions were chosen. The following paragraphs summarize the investigated<br />
functions. Out of a large number of tested parameters, only the best solutions are documented<br />
for each case.<br />
1. This can be explained by some coarse sediments remaining next to the outer wall. In addition,<br />
the secondary current may be less important in the “corner” between the vertical side wall and the<br />
channel bed, leaving coarse sediments in this zone.<br />
<strong>EPFL</strong> Ph.D thesis 2632 - Daniel S. Hersberger November 9, 2002 / page 159