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The UMIST-N Near-Wall Treatment Applied to Periodic Channel Flow

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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.

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