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 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.