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FLOW AROUND A CYLINDER - istiarto

FLOW AROUND A CYLINDER - istiarto

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– 5.8 –<br />

(� 2 � d 50 ) was considered as the one suitable as the model k s -value after evaluating the<br />

model results using several different k s values. This corresponds to k su � � = 118, which<br />

signifies that the channel bed is hydraulically rough.<br />

The calibrated k s and h ∞ were subsequently used as the model values for the test runs<br />

using uniform flow (Sect. 5.4) and also for the simulation of the flow around a cylinder<br />

on a flat channel bed (Sect. 5.5) and in a scoured channel bed (Sect. 5.6).<br />

5.4 Test run using uniform flow condition<br />

5.4.1 Boundary and initial conditions<br />

Having found the k s and h ∞ values for the model, test runs were carried out in which the<br />

basic performance of the model under uniform flow conditions was examined. The<br />

uniform flow condition according to Yulistiyanto measurement data was selected as the<br />

test case. The same quasi 2D flow as in the calibration runs was considered (see Sect.<br />

5.3.1).<br />

Using the calibrated values of k s = 0.22 [mm] and h ∞ = 18.3 [cm], three test runs using<br />

different initial and boundary conditions were performed:<br />

� Test A: the initial flow depth along the channel varies linearly between the inflow<br />

depth, h inflow = 17.3 [cm], and the outflow depth, h outflow = 18.3 [cm]. The initial<br />

conditions for the other variables were taken from the results of the calibration run,<br />

which were linearly adjusted according to the ratio of the local flow-depth. The same<br />

spatial discretisation as used for the calibration run ( 500 �1� 22 ) as shown in Fig.<br />

5.1 was used. This test run is aimed at validating the method of the surface<br />

computation. Given a variable depth along the channel, the model shall find the<br />

uniform depth when it converges to the steady-state condition.<br />

� Test B: uniformly distributed velocity and turbulence parameters were specified at the<br />

inflow boundary. These values were also used as the initial conditions along the entire<br />

domain. The initial flow depth was h = h ∞ = 18.3 [cm] everywhere. The<br />

computational domain covers the entire channel reach (38 [m]), but the number of<br />

cells was kept the same as that of Test A (500 �1� 22 ). The coordinate system was<br />

oriented such that the z-axis was vertical. This is different from that of Test A where<br />

the z-axis was normal to the channel bed. This test run is aimed at verifying the wall<br />

function implementation. Given a uniformly distributed velocity at the upstream<br />

boundary, the model shall produce the logarithmic velocity distribution after a certain<br />

distance away from the entrance. This can be considered as a developing flow<br />

condition.<br />

� Test C: this is a run identical to Test B, except that the surface boundary is not<br />

necessarily updated at every time step (the n-iteration), but only after several time<br />

steps. The pressure convergence criterion in the time-step iteration was set to 10 [Pa]

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