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
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
CHAPTER 3. CHANNEL FLOW 41<br />
profile is<br />
k + =<br />
1<br />
Reτ 2<br />
0.07 + 0.05<br />
∗<br />
1600<br />
y + <br />
2<br />
∗ exp − y+<br />
<br />
7<br />
<br />
+4.5 1 − exp − y+<br />
+ −1 <br />
4y<br />
+ 1<br />
20 Reτ<br />
<br />
+ 2 <br />
y<br />
∗ 1 − exp −<br />
3<br />
Figure 3.4 shows this profile for k + plotted against DNS results.<br />
(3.41)<br />
Table 3.1 offers qualitative descriptions of the contributions of the various<br />
terms in Equation 3.41. <strong>The</strong> final term ensures that k + = 0 at the wall, but<br />
the shape of the profile in the very near-wall region does not closely match<br />
DNS data. An analysis of the near-wall behaviour of turbulence quantities<br />
will follow.<br />
Table 3.1: Qualitative behaviour of terms in Equation 3.41<br />
<br />
Reτ<br />
1600<br />
<br />
0.07 + 0.05<br />
<br />
4.5 1 − exp<br />
<br />
∗ (y + ) 2 <br />
∗ exp − y+<br />
<br />
7<br />
<br />
4y + −1<br />
+ 1<br />
− y+<br />
20<br />
<br />
1 − exp −<br />
y +<br />
3<br />
Reτ<br />
2 <br />
3.4.4 Empirical Profile for u 2 +<br />
<strong>The</strong> following formula for 〈u2 〉 +<br />
k +<br />
fits the peak value of k +<br />
helps <strong>to</strong> roughly capture the curve<br />
at high Reynolds numbers<br />
forces a value of zero at the wall<br />
was adapted from a profile fitted by Alexan-<br />
der Davroux and Dominique Laurence at Electricité de France.