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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 4. NUMERICAL IMPLEMENTATION 58<br />

source. 6 Since τw contains a 〈U〉 P term, the SP source is used:<br />

SP = S ′ P − C1/4 µ k 1/2<br />

p<br />

U + p<br />

(4.19)<br />

where S ′ P is the value of SP before the log-law term is added (containing only<br />

the time-dependence term).<br />

Also, AS is modified <strong>to</strong> cut the link <strong>to</strong> the wall and prevent a second (in-<br />

accurate) accounting of τw via the normal functioning of the x-momentum<br />

equation. <strong>The</strong> modified terms are<br />

AS = 0<br />

AP = AN (4.20)<br />

This modification is common <strong>to</strong> all wall function treatments on 〈U〉, k, ε,<br />

and ω.<br />

Average production and dissipation of k in the near-wall cell ( <br />

Pk p and<br />

(ε) p ) are calculated from Equations 2.45 and 2.46. In descretised form, these<br />

become<br />

Substituting Equation 4.18,<br />

<br />

〈U〉P<br />

Pk = τw<br />

p<br />

yp<br />

<br />

(kp)<br />

(ε) p = ρCµ<br />

2<br />

〈U〉P <br />

<br />

Pk p<br />

τw<br />

yp<br />

ρC1/4 µ k<br />

= 1/2<br />

p (〈U〉 P ) 2<br />

U +<br />

P<br />

(ε) p = C 3/4<br />

µ k 3/2<br />

· yp<br />

U +<br />

P<br />

yp<br />

<br />

(4.21)<br />

(4.22)<br />

(4.23)<br />

(4.24)<br />

6 In general, one would integrate τw with respect <strong>to</strong> the surface area over which it acts<br />

before applying the result as a source <strong>to</strong> the x-momentum equation. In channel flow<br />

geometry, τw acts over a surface of unit area.

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