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pdf, 12 MiB - Infoscience - EPFL

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Chapter 6 - Analysis of the test results<br />

6.2.2 Analysis of the water surface<br />

Without macro-roughness, stationary waves can be observed at the outer side wall (Figure 6.11,<br />

Appendix 6 and 8). The amplitude of these surface waves is about 10 cm and their length about<br />

60 cm to 1 m. For the highest channel slope (S 0 = 0.70%), the one or two last waves after the<br />

bend showed small surface rollers (Fig. 6.<strong>12</strong>, left).<br />

no MR e s =4° e s =2° e s =1°<br />

Figure 6.11: Water surface views for tests C1 to C4 at Q = 210 l/s<br />

With vertical ribs, the previously observed stationary waves are replaced by shock waves, resulting<br />

from the reflection of the water on the macro-roughness elements. They emerge about 0.5°<br />

upstream the ribs (Figure 6.14) and redirect the flow towards the center (with a deviation angle<br />

from the channel axis of about 50 to 55° depending on the local Froude number 1 ). The waves can<br />

be observed over the outer 70% of the channel for a rib spacing of 4° and over the outer half of<br />

the channel for 2°-spacing. If even more ribs are added (1°), these shock waves disappear and the<br />

ribs no longer work as isolated elements but rather as continuous roughness on the outer wall.<br />

The roughness is too important to observe the stationary shock waves that were observed without<br />

ribs.<br />

Figure 6.<strong>12</strong>: Stationary wave at the end of the bend with surface roller (left) and a common one (right). Picture<br />

taken across the outer side wall<br />

1. The local Froude numbers are of about 1.2 to 1.4, indicating supercritical flow conditions along<br />

the outer side wall.<br />

page <strong>12</strong>6 / November 9, 2002<br />

Wall roughness effects on flow and scouring

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