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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 2. TURBULENCE MODELS 23<br />

way that<br />

<strong>The</strong> difference between ˜ε and ε is defined as ˆε:<br />

From Equations 2.22 and 2.23, it follows that<br />

˜ε| y=0 = 0 (2.22)<br />

ε = ˜ε + ˆε (2.23)<br />

ˆε| y=0 = ε| y=0<br />

(2.24)<br />

<strong>The</strong> equation for νt is modified <strong>to</strong> use ˜ε for convenience. Also, damping<br />

terms exist in the equation for νt and the transport equation for ˜ε. <strong>The</strong>se<br />

damping terms are a function of the turbulent Reynolds number, ˜<br />

Ret. ˜<br />

Ret<br />

is a Reynolds number based on local turbulence quantities (in this case, k<br />

and ˜ε). <strong>The</strong> tilde is a reminder that, for convenience, the turbulent Reynolds<br />

number used in the low-Reynolds-number standard k-ε model uses ˜ε rather<br />

than ε. ˜ Ret is defined as<br />

˜Ret ≡ k2<br />

˜εν<br />

(2.25)<br />

In the low-Reynolds-number version of the standard k-ε model [33], the trans-<br />

port equation of ˜ε is<br />

<br />

D˜ε ν + νt<br />

= ▽ ·<br />

Dt σε<br />

where<br />

<br />

▽ ˜ε + Cε1f1<br />

E = 2ννt<br />

<br />

˜ε<br />

Pk − Cε2f2<br />

k<br />

∂ 2 〈U〉<br />

∂y 2<br />

2<br />

2 ˜ε<br />

+ E (2.26)<br />

k<br />

(2.27)<br />

f1 = 1 (2.28)<br />

−Ret ˜<br />

f2 = 1 − 0.3e 2<br />

(2.29)

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