pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Chapter 3 - Theoretical considerations<br />
b) Formulae based on equilibrium considerations<br />
The analytical formulae of VAN BENDEGOM, ENGELUND AND BRIDGE are valid for small bed<br />
slopes, high width to depth ( B ⁄ h) ratios and for small curvatures of the bend ( R c » h ). VAN<br />
BENDEGOM and ENGELUND established their equations for partially developed secondary flow<br />
conditions. The equation of van Bendegom is based on equilibrium conditions of spherical grains<br />
which are completely exposed to the flow. This leads to an underestimation of the bed slope in<br />
radial direction. Furthermore the static lift was neglected leading to an additional underestimation<br />
of the lateral bed slope. The formula of Engelund considered a rectangular cross-section with a<br />
fixed bed and slightly meandering bends. Bridge adjusted the formula of Engelund, integrating the<br />
results of the research works of Rozovskii; he assumed the ratio between tangential and radial<br />
velocity components to be equal to 11.<br />
KIKKAWA ET AL. introduced a flow model, which allows to determine the drag and lift force as a<br />
function of characteristic flow and bed parameters. REINDL observed that the maximum flow also<br />
depends on the sediment saturation Gs for river reaches influenced by a backwater curve. He<br />
modified KIKKAWA’S formula, in order to take into account the quantity of sediment available for<br />
transport.<br />
c) Formulae based on control volume considerations<br />
ZIMMERMANN, FALCON & KENNEDY and ODGAARD considered control volumes of different<br />
size, but always with the thickness of the armoring layer. ZIMMERMANN used the whole cross-section<br />
at the maximum scour location, while FALCON & KENNEDY and ODGAARD used a local control<br />
volume. Since ZIMMERMANN’s equation is a function of h / R c , the bed geometry in the<br />
cross-section is a straight line, which does not fit with the observed geometry of the cross-section.<br />
All three formulae were established for sand bed rivers.<br />
BAZILEVICH’S formula is very sensitive to the chosen parameters (see PETER, 1985). Since the<br />
flow and geometric characteristics of a river often contain (considerable) uncertainties, this equation<br />
does not seem very appropriate for engineering practice.<br />
d) Empirical formula<br />
PETER gives an empirical formula based on a dimensional analysis. In general, his formula gives<br />
good results for alpine rivers (see PETER, REINDL). But unfortunately, it does not take into<br />
account the sediment size. Therefore the formula should be used with care within the authorized<br />
domain of radius to with ratios ⁄ B = 2 ÷ 6.<br />
R c<br />
3.5.4 Comparison with experimental data<br />
In this paragraph, the mentioned scour formulae are compared to laboratory experiments for<br />
smooth walls performed in the frame set of this study (also published in HERSBERGER &<br />
SCHLEISS, 2002). The laboratory tests of PETER (1986), performed at the VAW (ETHZ) were<br />
added to this data set. The so obtained extension of the data set (39 tests) to 71 tests covers a wide<br />
page 58 / November 9, 2002<br />
Wall roughness effects on flow and scouring