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<strong>Arab</strong> <strong>Journal</strong> Of <strong>Nuclear</strong> Science And <strong>Applications</strong>, 46(2), (276-286) 2013<br />

was, thus, important to survey over the available turbulence models in terms <strong>of</strong> their criteria <strong>of</strong><br />

applicability, limitations <strong>and</strong> restrictions in order to choose the one that might be appropriate to model<br />

this complex system. Moreover, literature surveys were conducted to explore on what other researcher<br />

have recommended for similar systems. It was found that substantial amount <strong>of</strong> research work have<br />

been done on rod bundle geometry using the st<strong>and</strong>ard k turbulence models over the past few<br />

decades for a recent in-depth review on CFD analysis on rod bundle geometries ( Tzanos 2001 (1) ). In<br />

general, there is a great deal <strong>of</strong> agreement between researchers that the st<strong>and</strong>ard k model may not<br />

be the turbulence model <strong>of</strong> choice in rod bundle geometries. On the other h<strong>and</strong>, most <strong>of</strong> these<br />

researches have considered periodic arrays <strong>of</strong> rods which allowed them to solving the flow in<br />

elementary sections <strong>and</strong> assuming symmetry across the boundaries (Rapley <strong>and</strong> Gosman 1986 (2) ;<br />

Baglietto <strong>and</strong> Ninokata, 2005 (3) ; <strong>and</strong> many others). However, as Chang <strong>and</strong> Tavoularis, 2007 (4) pointed<br />

out, this approach restricts the solution based on the fact that symmetry in geometrical configurations<br />

does not necessarily imply symmetry in the flow. In other words, simulating a full sector may be<br />

required to better capture the essential features <strong>of</strong> the flow field. It was reported the use <strong>of</strong> the shearstress<br />

transport (SST) k <br />

model to perform CFD analysis <strong>of</strong> flow field in a triangular rod bundle<br />

by Toth <strong>and</strong> Aszodi (2008) (5) . Chang <strong>and</strong> Tavoularis, 2005 (6) , on the other h<strong>and</strong>, used the unsteady<br />

Reynolds averaged Navier-Stokes equations supplemented by a st<strong>and</strong>ard Reynolds stress model to<br />

simulate the experimental work <strong>of</strong> Guellouz <strong>and</strong> Tavoularis 2000 (7) a,b <strong>and</strong> reported good agreement.<br />

In this work, we consider the use <strong>of</strong> the shear-stress transport (SST) <br />

Toth <strong>and</strong> Aszodi, 2008 (5) . Moreover, the two approaches to dealing with the near wall region were<br />

considered with the aim that if it is founded that the wall function approach provides reasonable<br />

approximation to the measured inner clad surface temperature, then it might be recommended for<br />

further investigation since it usually requires less computing resources.<br />

2-The Shear-Stress Transport (SST) <br />

k model<br />

281<br />

k model as suggested by<br />

k <strong>and</strong> SST models, which are basically two equation eddy-viscosity models, the<br />

In both the <br />

Reynolds stresses can be calculated from the eddy-viscosity hypothesis introduced by Boussinesq,<br />

(Pope, 2000 (8) ):<br />

2 <br />

<br />

U<br />

uiu j k<br />

ij <br />

t<br />

3 <br />

<br />

x<br />

j<br />

i<br />

U<br />

<br />

x<br />

i<br />

j<br />

<br />

<br />

<br />

<br />

As suggested by Menter, if it is possible to combine the st<strong>and</strong>ard <br />

shows to be relatively accurate if applied to the near wall region with the <br />

accurate in the far field, one may obtain a model that may be used in a variety <strong>of</strong> applications<br />

involving confining walls. This model is called the shear-stress transport <br />

basically the same formulation as the st<strong>and</strong>ard <br />

activate the <br />

region. In addition the definition <strong>of</strong> turbulent viscosity is modified to account for the transport <strong>of</strong> the<br />

turbulent shear stress.<br />

(1)<br />

k model, Wilcox, which<br />

k model which is also<br />

k model. It has<br />

k model but it includes blending function to<br />

k model in the near-wall region or the transformed <br />

k away from the wall<br />

In this model, the turbulent kinetic energy, k, <strong>and</strong> the specific dissipation rate, , may be<br />

obtained from the following transport equations (FLUENT, 2006 (9) ):<br />

k<br />

~<br />

( k)<br />

( kui<br />

) (<br />

k<br />

) Gk<br />

Yk<br />

S k<br />

(2)<br />

t<br />

xi<br />

x<br />

j <br />

x<br />

j

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