pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Bed topography in the bend<br />
The superelevation of the free water surface is computed with:<br />
R o<br />
∆z = L⋅<br />
S b ⋅ ⎛-----⎞<br />
⎝ ⎠<br />
R c<br />
(3.115)<br />
Based on the analysis of field data with h smax ,<br />
⁄ h m<br />
= 1.03 ÷ 3 , BAZILEVICH established the following<br />
equation for the lateral bed slope. If the value of h smax ,<br />
is not known, he proposed to use<br />
h smax ,<br />
= 1.6 · ⋅ h m for mountain rivers (leading to a β = 1.09 = 62° ).<br />
β 0.155 h s,<br />
max<br />
= ⋅ -------------- + 0.845<br />
(3.116)<br />
Finally, BAZILEVICH compared his formula against a small set of laboratory (TALMAZA & KROSH-<br />
NIN, 1968 and VLASENKO 1 ) and field data (Tisa River near Khust, Ukraine, below the mouth of<br />
the Boroyavka River). The configuration of all data sets was a 180° meander. The results of the<br />
comparison are satisfying. PETER (1985) indicated that BAZILEVICH’S formula is quite sensitive to<br />
numerical instability and to the choice of the bed roughness. 2<br />
h m<br />
10) Peter (1986)<br />
PETER (1986) compared different scour formulae. He performed a large series of laboratory tests<br />
in a 135° bend with rectangular and trapezoidal cross-sections on a mobile bed. He varied the<br />
radius of curvature, the width of the channel, the discharge, the sediment mixture and the bed<br />
slope. Based on a dimensional analysis of his test data, PETER established an empirical formula for<br />
channels with a rectangular cross-section. The following equation gives the maximum scour<br />
depth, which can be located either at the first or second scour:<br />
h<br />
-------------- smax ,<br />
= 5.23 – 13.0<br />
h m<br />
h<br />
⋅ ----- m<br />
–<br />
B<br />
0.379 ⋅ σ + 68.4 ⋅ S e<br />
(3.117)<br />
Since the parameter R c<br />
⁄ B is not a part of this equation, the application has to be limited to examined<br />
ratios of R c<br />
⁄ B = 2 ÷ 6. Furthermore, this equation does not take into account the grain<br />
size diameter; therefore a critical attitude towards this formula is necessary.<br />
For channels with a trapezoidal cross-section, PETER found:<br />
sinβ<br />
2.95 R c<br />
----- 0.7 ⋅ σ 29.3 h m<br />
= ⎛<br />
⋅ -----<br />
⎝<br />
⋅ – – + 2.7 ⋅ Fr + 3.4⎞<br />
B<br />
B<br />
⎠<br />
(3.118)<br />
PETER also established formulae to locate the position of the first and the second scour, yet with a<br />
rather poor correlation ( r2 α1<br />
= 0.55 and r2 α2<br />
= 0.<strong>12</strong> ):<br />
α 1<br />
= 20 ⋅ σ – 0.138 ⋅ d∗ + 28<br />
(3.119)<br />
α 2<br />
= 104 + 5.66 ⋅ σ<br />
h s<br />
⋅ ----<br />
r<br />
1. Bazilevich does not give any reference for this data set.<br />
2. Bazilevich based the determination of the bed roughness on the work of Altunin & Kurganovich,<br />
which could not be found in any library.<br />
<strong>EPFL</strong> Ph.D thesis 2632 - Daniel S. Hersberger November 9, 2002 / page 55