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2.1 Measurement design<br />
– 2.3 –<br />
The flow measurement is aimed at collecting detailed data of the three-dimensional<br />
velocity fields around the cylinder, from which a close investigation can be made to<br />
characterize the alteration of the flow around the cylinder. A series of measurements shall<br />
be performed around the cylinder in an equilibrium scour-depth under a clear-water scour<br />
regime. An equilibrium scour-depth is defined as the depth of scour hole in front of the<br />
cylinder that has no longer changed appreciably under a continuous (steady) flow. A<br />
clear-water scour regime prevails when the scouring process is due solely to the<br />
interaction of the flow with the obstruction (the cylinder) and that the sediment transport<br />
does not exist in the approach flow. A live-bed scour prevails otherwise.<br />
The ADVP shall be used to obtain the vertical distributions of the instantaneous threedimensional<br />
velocities. The measurements are to be performed at stations distributed<br />
along vertical planes around the cylinder, outside and inside the scour hole. The hydraulic<br />
parameters of the experiment are selected according to certain criteria relating to the<br />
scouring mechanism and the available laboratory facilities and instrumentation. In terms<br />
of the scouring process, the flow has to maintain a clear-water scour and result in a<br />
maximum scour depth for the given sediment and cylinder diameter. This can be<br />
achieved with flows having a velocity close to but less than the sediment entrainment<br />
velocity. From the instrument point of view, the scour-hole depth shall be small to keep<br />
the entire flow depth in the range of the instrument measuring capability.<br />
Given in the following sections are the detailed aspects of the measurements, from the<br />
setup to the results of the measurements.<br />
2.2 Experimental setup<br />
2.2.1 Laboratory channel<br />
The experiments were conducted in a 29 [m] long and 2.45 [m] wide rectangular<br />
erodible-bed channel. This wide channel allows for flows with sufficiently large aspect<br />
ratio in terms of the flow depth and cylinder diameter. Large ratios of channel width, B,<br />
to cylinder diameter, Dp, guarantee that the flow around the cylinder is a manifestation of<br />
the interaction between the approaching flow and the cylinder. In the present work, this<br />
ratio is B D p = 16, being sufficiently higher than the generally agreed minimum ratio of<br />
B D p > 8. The large ratios of the channel width to the flow depth, h ∞ , ensure the<br />
approaching flow to be a quasi two-dimensional one where the side wall does not<br />
influence the flow. In the present work, the ratio is B h = 13.6; this is higher than the<br />
minimum value usually taken as the criterion, B h > 7. The general view of the channel<br />
is shown in Fig. 2.1 and its principal elements are presented in the following paragraphs.