A. Hotta et al., 3-DIMENSIONAL EVALUATION OF 2-PHASE FLOW IN BWR FUEL BUNDLES BASED ONCOMPRESSIBLE 2 FLUID-ONE PRESSURE AND KAPPA-EPSILON TURBULENCE MODELS, Annals of nuclear energy, 25(7), 1998, pp. 437-463
The three dimensional fluid dynamic code system was developed to simul
ate a comprehensive two-phase flow field in fuel bundles of boiling wa
ter reactors. The system is based on the compressible two fluid-one pr
essure (six equations) model and is designed to be applicable to both
detailed fully three dimensional geometries and porous medium sub-chan
nel type geometries. In the detailed modeling, the turbulence effect i
s considered by the additional four conservation equations of the k-ep
silon turbulence model and the convective terms are formulated by the
modified skewed upwind scheme. The sub-channel type modeling, in contr
ast, is built from coarser meshes. The empirical void drift and turbul
ence mixing models are introduced to replace the k-epsilon turbulence
model and other additional constitutive models such as the local loss
are added to facilitate efficient sub-channel-type calculations. Gener
al problems were investigated regarding numerical methodologies in dis
cretizing a vapor-liquid two-phase flow field based on the two fluid-o
ne pressure model. The performances of several pressure iteration sche
mes were compared in combination with the outer Newton-Raphson iterati
on loop. Among them, the MILUCR scheme is found to be most stable and
efficient. It was also observed that the turbulent effect simulated by
the k-epsilon model enhances the local build-up of vapor. Two sample
calculations, one numerical and the other experimental verification, w
ere performed to prove the performance of the code system. In the firs
t simulation, flow fields of two typical spacer designs were compared
and it was indicated that the vapor acceleration and its winding motio
n can be changed notably by design modifications. In the second simula
tion, a two-phase flow field of the 4x4 heated bundle test section was
evaluated by the detailed model and the resultant macroscopic loss co
efficients were reflected in the subsequent sub-channel type model. Th
e void distribution was compared with the measurement by the X-ray CT
scanner and it was indicated that not only the axial pressure loss, bu
t also the transverse pressure loss, has a significant effect on the p
lanar void distribution in the wake of the spacers. (C) 1997 Elsevier
Science Ltd.