The UMIST-N Near-Wall Treatment Applied to Periodic Channel Flow
The UMIST-N Near-Wall Treatment Applied to Periodic Channel Flow
The UMIST-N Near-Wall Treatment Applied to Periodic Channel Flow
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CHAPTER 5. RESULTS 68<br />
a nominal Reτ of 180.<br />
5.1 Steady <strong>Flow</strong> Results<br />
Although the principal goal of this work is <strong>to</strong> test the performance of the<br />
<strong>UMIST</strong>-N method in periodic flow, the steady flow case offers a simpler test<br />
case in which <strong>to</strong> verify the code.<br />
Steady channel flow results for the k-ε and k-ω models are widely available.<br />
<strong>The</strong> <strong>UMIST</strong>-N approach with the standard k-ε model was applied <strong>to</strong> channel<br />
flow using the TEAM code by Gant during the early development of <strong>UMIST</strong>-<br />
N [21]. <strong>The</strong> application of the <strong>UMIST</strong>-N approach with a k-ω model <strong>to</strong><br />
steady channel flow is new.<br />
All the model configurations shown in Table 5.1 were applied <strong>to</strong> steady chan-<br />
nel flow and the results are presented here. Figures 5.1 & 5.2 show U + and<br />
k + (respectively) plotted against y/δ. Figures 5.3 & 5.4 show a better view<br />
of near-wall values plotted against y + on logarithmic scales. <strong>The</strong> results are<br />
compared the analytical profiles from Chapter 3 and <strong>to</strong> the data of Kim et<br />
al. [30], who employed the same Reτ.<br />
<strong>The</strong> pressure gradient driving the flow was chosen <strong>to</strong> produce a nominal Reτ<br />
of 180. By applying the definition of Reτ (Equation 3.25), a value of Uτ was<br />
obtained that was used in nondimensionalisation. From Equations 3.23 &<br />
3.19, a corresponding<br />
∂〈P 〉<br />
∂x<br />
was specified. This ∂〈P 〉<br />
∂x<br />
was allowed <strong>to</strong> drive the<br />
flow, with the actual calculated flow rate being a function of the turbulence<br />
model used.