pdf, 12 MiB - Infoscience - EPFL
pdf, 12 MiB - Infoscience - EPFL
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Chapter 6 - Analysis of the test results<br />
6.6 Analysis of the flow field<br />
The presence of the macro-roughness influences the scour process by modifying the velocity distribution<br />
in the bend. It is well known that the velocity is higher on the outside of the bend and<br />
that there is a secondary circulation also. Both factors combine to give a large scour on the outside<br />
of the bend. A brief description of the flow field was already given in the paragraph discussing the<br />
preliminary tests (§ 5.2.1/2)e). The analysis of the main tests is presented here.<br />
a) Tangential velocities<br />
The velocities in tangential direction (along the channel axis) are somewhat modified in the bend.<br />
Instead of a classical “log”-velocity profiles as it can be seen on top of Table 6.6 1 undergoes the<br />
following modifications in a curved channel. The maximum velocity is no longer found close to<br />
the free water surface but close to the bed surface, particularly in the scour holes; this can be seen<br />
very well in cross-section 40° in the second profile from the left. The highest tangential velocities<br />
( ) are now found in the outer half of the cross-section.<br />
V θ<br />
B01−Q210−F06<br />
0<br />
0<br />
100<br />
X<br />
200 800<br />
300<br />
600<br />
400<br />
0 200 400 600 800 1000<br />
Distance to outer bank (mm)<br />
400<br />
With macro-roughness, the previously mentioned increase of the water depth in the inlet reach<br />
(§ 6.2.2) is well visible. But this has no influence on the shape of the velocity profile in this zone.<br />
In the bend and especially in the scour holes, the near bed velocity is reduced and the maximum<br />
velocity shifts towards the free water surface (Table 6.6 at 40°, first two profiles at the outer bank).<br />
Appendix 11.1 shows that the highest velocities are located in a straight reach next to the free<br />
water surface. In the bend, this zone of maximum velocity first shifts towards the outer side wall<br />
and then down the wall towards the channel ground. At the maximum scour location, high (tangential)<br />
velocities can be observed near the bottom (Figure 6.22).<br />
100<br />
200<br />
300<br />
400<br />
Figure 6.22: Tangential velocities at 40° without macro-roughness (left) and with ribs spaced every 2° (right); view<br />
in the downstream direction (see also Appendix 11.4)<br />
X = max. velocity<br />
With macro-roughness (Appendix 11.4), the zone of maximum velocity remains all over the bend<br />
close to the surface for the ribs spaced every 4°. Introducing additional ribs (every 2°) the maximum<br />
velocity moves towards the channel ground, but at a significant distance from the outer wall<br />
(about 20 cm, that is about the average flow depth). For the smallest rib-spacing, the high-velocity<br />
zone gets even closer to the ground, but again at about 20 cm from the outer side wall.<br />
Distance to free water surface (mm)<br />
<strong>12</strong>00<br />
1000<br />
X<br />
B03−Q210−F06<br />
0 200 400 600 800 100<br />
200<br />
Distance to outer bank (mm)<br />
1400<br />
<strong>12</strong>00<br />
1000<br />
800<br />
600<br />
400<br />
1. Table 6.6 gives the raw velocity profiles. It shows that the first 2 cm from the free water surface<br />
are strongly influenced by the measurement, since the velocity probe had to touch the fluid.<br />
page 138 / November 9, 2002<br />
Wall roughness effects on flow and scouring