pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Chapter 2 - State of the art<br />
complex flow structure (Figure 2.1). On the upstream face of the abutment the flow plunges down<br />
towards the bottom, where the principal vortex along the scour hole is located. Behind the abutment,<br />
the wake vortex can be found. Some small surface rollers can be seen upstream of the<br />
obstacle.<br />
MELVILLE & RAUDKIVI (1984) summarized studies performed at the University of Oakland. An<br />
important result of their study is the conclusion that the abutment scour depth can be up to 2 to 5<br />
times the mean flow depth.<br />
Semi-empirical formulae to estimate the equilibrium scour depth are given by INGLIS (1949),<br />
AHMAD (1953), LIU ET AL (1961) and many others. Inglis found the scour depth to depend on the<br />
flow characteristics (mean water depth and discharge) and the with of the channel. Ahmad introduced<br />
correction factors depending on the channel bend, the shape of the abutment structure, the<br />
angle of attack and the porosity of the abutment. Liu et al. found the abutment scour to depend<br />
also on the Froude number. A recent review of local abutment scour equations is presented in<br />
PRZEDWOJSKI ET AL. (1995).<br />
MOLINAS, KHEIRELDIN & WU (1998) determined the necessary rip-rap size for protection of<br />
bridge abutments. The phenomenon at the downstream side of such a narrow cross-section can<br />
be compared to the one observed behind an element of macro-roughness. From their results, it<br />
can be supposed that the elements of macro-roughness might have a significant influence on the<br />
flow structure. However, it is important to note that these experiments were not carried out in a<br />
bend.<br />
c) Bed sills<br />
GAUDIO ET.AL. (2000) performed experiments on scour downstream of bed sills in uniform sediment<br />
and obtained empirical formulae to predict the dimensions of the scour hole. An important<br />
result is that the Froude number does not seem to influence the dimensions of the scour hole.<br />
2.3.3 Bridge scour<br />
An overview of the phenomena influencing bridge scour related formulae can be found in textbooks<br />
like BREUSERS & RAUDKIVI (1991), MELVILLE & COLEMAN (1999). The large number of<br />
studies on bridge scour identified the following main parameters to influence the maximum scour<br />
depth: the particle Reynolds number, a particle Froude number, the ratios mean water depth to<br />
channel width and characteristic grain size to channel width and the ratio of sediment to water<br />
density. Furthermore the pier dimensions and placement in the flow field and the sediment grading<br />
play a role.<br />
Some recent studies on scour in cohesive material were undertaken by TING, BRIAUD,& CHEN<br />
(2001) who found that the equilibrium scour depth in cohesive material is of the same order of<br />
magnitude as the one in a sand bed.<br />
page 14 / November 9, 2002<br />
Wall roughness effects on flow and scouring