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FLOW AROUND A CYLINDER - istiarto

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5.1 Introduction<br />

– 5.2 –<br />

The numerical model presented in the preceding chapter (Chapter 4) shall be used to<br />

simulate flow around a cylinder. Two cases of flow around a cylinder were considered,<br />

namely flat channel bed and scoured channel bed. The first case was the object of<br />

experimental and numerical investigations of the previous study (Yulistiyanto, 1997),<br />

whereas the second case was experimentally investigated in the present study (see<br />

Chapters 2 and 3). In both studies, the experimental investigations were performed by 3D<br />

instantaneous velocity measurements using an acoustic Doppler profiler. The<br />

experimental data thus obtained allow detailed comparisons of the simulation results to<br />

be performed, not only for the velocity fields but also for the turbulence quantities. In the<br />

previous numerical work (Yulistiyanto, 1997), a 2D model was used thus restricting the<br />

comparison to the depth-averaged velocity fields. Nevertheless, the result of this 2D<br />

model was promising and encouraged the 3D model development.<br />

The model has various constants, such as those in the k-� transport equations (c � , c 1 , c 2 ,<br />

� k , and � � ) and the ones of the logarithmic velocity law (� and k s ). In the present model,<br />

the k-� model constants (see Table 4.1 in Chapter 4) and the Karman constant (� = 0.4)<br />

are invariant and are applied to all flow conditions. The equivalent roughness of the wall,<br />

k s , characterizes the roughness of the physical solid boundaries (the channel wall, the<br />

cylinder, and especially the channel bed). It is the only “physical link” of the model to the<br />

roughness characteristics of solid boundaries. In order to obtain the correct model-value<br />

of k s , a calibration had to be performed. Using a uniform flow condition (with neither the<br />

cylinder nor the scour hole), various k s -values were tested to obtain the best match<br />

between the computed and measured flow fields. In the calibration run, adjustment of the<br />

uniform flow depth (which will be the approaching flow depth) was also accordingly<br />

needed.<br />

Before performing the simulation of flow around a cylinder, which is a highly complex<br />

3D flow, a series of test runs were carried out for the simple uniform flow case. The test<br />

runs were aimed at investigating the basic performance of the model and verifying some<br />

computational techniques adopted in the model. This simple well-known flow condition<br />

was the best tool to serve this purpose. The experimental data for the comparison were<br />

taken from the same preceding work (Yulistiyanto, 1997).<br />

The computer code of the model is written in FORTRAN-77. All simulation runs were<br />

executed on a personal computer. The computational CPU time of the simulation run is<br />

typically 70 to 100 hours.

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