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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

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