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pdf, 12 MiB - Infoscience - EPFL

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Chapter 4 - Experimental setup and test procedure<br />

During the measurements, the (water and bed) levels were recorded in an Excel file. For each<br />

measurement point, 32 values were recorded at 5 Hz and stored in a spreadsheet. The average of<br />

these 32 values was computed in a further step (Visual Basic Macro) and recorded in a file summarizing<br />

all data points over the whole channel. The coordinates were transformed from the local<br />

measurement frame coordinates to absolute frame coordinates relative to the bend (Fig. 4.1 and<br />

Fig. 4.19). The so obtained Excel spreadsheet was exported to a text file for further treatment with<br />

Matlab. A scheme of the performed Matlab treatment 1 is described in the flowchart on Fig. 4.24.<br />

The Matlab treatment combined the automatically acquired levels, the manual readings on the<br />

outer side wall and the manually recorded levels in the straight inlet and outlet reaches. The computation<br />

was performed in two steps. First, the different input files were combines for each individual<br />

test (water respectively bed level). Then first graphics of the obtained raw data were plotted<br />

and analyzed to make sure that the data contained no errors (procedure dh_level1 on Fig. 4.24). In<br />

a second step the pretreated data sets were combined and compared to each other. At this stage<br />

the following plots were computed and printed: water and bed level changes compared to the initial<br />

bed level (Appendix 4 and 5), longitudinal plots (Appendix 8) and cross-section plots<br />

(Appendix 7) containing measured water and bed levels as well as the initial bed level (procedure<br />

(dh_level2 on Fig. 4.24).<br />

4.6.2 Velocity treatment<br />

In order to extract the 3D velocity field in six cross-sections over the whole channel (10°, 25°, 40°,<br />

55°, 70° and 85°), the acquired binary velocity file (see § 4.4.4) needed some treatment.<br />

First, the nine 1D records were extracted from the raw data file (Fig. 4.26) and written to a text<br />

file. The high velocities in tangential direction exceeding the measurement domain (negative sign)<br />

were then corrected to be located in the positive range (see § 4.4.4). Then the time-averaged measured<br />

components (average over 64 velocity profiles) at a given location had to be projected in a<br />

cylindrical coordinate system relative to the bend (tangential, radial and vertical velocities). Assuming<br />

that the measured velocity components are a, b and c (Fig. 4.21), the velocity components in<br />

a point are given with (Fig. 4.25):<br />

v θ<br />

=<br />

a<br />

---------------------------<br />

+ b–<br />

2 ⋅ c<br />

, v<br />

– a + b<br />

, (4.1)<br />

2 ⋅ sinα<br />

r = ----------------- v<br />

a+<br />

b<br />

2 ⋅ sinα<br />

z = -------------------<br />

2 ⋅ cosα<br />

1. The developed Matlab treatment needed about 4400 lines of program code.<br />

page 94 / November 9, 2002<br />

Wall roughness effects on flow and scouring

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