Please cite this article in press as: Liao, Y., et al., Application of new closure models for bubble coalescence and breakup to steam–water
vertical pipe flow. Nucl. Eng. Des. (2014), http://dx.doi.org/10.1016/j.nucengdes.2014.02.015
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Nuclear Engineering and Design
jou rn al hom ep age: www.elsevier.com/locate/nucengdes
Application of new closure models for bubble coalescence
and breakup to steam–water vertical pipe flow
Yixiang Liao
∗
, Dirk Lucas, Eckhard Krepper
Helmholtz-Zentrum Dresden-Rossendorf e.V., Institute of Fluid Dynamics, PO Box 510 119, 01314 Dresden, Germany
h i g h l i g h t s
•
New development in closure models for bubble coalescence and breakup.
•
Application of new coalescence and breakup model for condensing steam bubbles.
•
Considerable improvement brought by the new model.
•
General applicability of the new model for air–water and steam–water flows.
•
Uncertainty in inlet liquid sub-cooling affects the results significantly.
a r t i c l e i n f o
Article history:
Received 20 February 2014
Accepted 25 February 2014
Keywords:
Coalescence and breakup
Steam condensation
Bubbly flow
Vertical pipe
a b s t r a c t
New closure models for bubble coalescence and breakup proposed in Liao et al. (2011), Nucl. Eng. Des.
241, 1024, are assessed for the case of condensing steam–water pipe flows. Steady-state CFD calculations
are performed employing the commercial CFD solver ANSYS CFX. Predicted evolution of cross-section
averaged bubble size and gas volume fraction distribution along the pipe is compared with the measure-
ments provided by the TOPFLOW facility (Lucas et al., 2010. CFD4NRS-3, Int. Workshop on Experimental
Validation and Application of CFD and CMFD Codes to Nuclear Reactor Safety Issues, Paper 13.1, 14.16.09,
Washington D.C., USA.). It is shown that for cases with small initial bubble size and low gas volume frac-
tion, bubble coalescence and breakup can be taken to be nearly negligible and the change of bubble size
is primarily due to condensation. Nevertheless, with the increase of initial bubble size or gas volume frac-
tion, bubble coalescence and breakup become more prevalent. Performance of new and standard closure
models of bubble coalescence and breakup is investigated It is shown that both models overestimated
the breakup rate; in particular, the standard model. The numerical results are also found to be dependent
on the inlet liquid temperatures and inter-phase heat transfer models have a significant impact on the
results.
© 2014 Elsevier B.V. All rights reserved.
1. Introduction
The phenomena of gas–liquid flows are omnipresent in our
daily life as well as having being significant in industrial applica-
tions and scientific investigations. With increasing computational
power, computer-aided simulation of computational fluid dynam-
ics (CFD) is increasingly becoming an important analysis tool of
fluid flow phenomena. Furthermore, in recent CFD simulations of
gas–liquid flows, instead of assuming mono-dispersity it is crucial
that the change of local bubble size is adequately predicted. In order
to aptly predict the bubble size distribution, additional closure
∗
Corresponding author. Tel.: +49 3512602389.
E-mail address: y.liao@hzdr.de (Y. Liao).
models are needed in the Eulerian framework for the description of
the interfacial processes that change the bubble size or interfacial
area density such as coalescence and breakup.
Although there has been considerable development of theories
and models, the prediction of bubble coalescence and breakup rates
remains one of the weakest links in the modern CFD simulation of
poly-dispersed bubbly flows (Krepper et al., 2008). Concrete limi-
tations of existing models can be summarized by one issue, that is,
the transferability is limited (Liao and Lucas, 2009a, 2010). Starting
from this point, new models have been presented in our previous
work, which attempts to accommodate all important mechanisms
leading to the coalescence and breakup of bubbles in a turbulent
flow (Liao and Lucas, 2009b; Liao et al., 2011).
The new models of coalescence and breakup have been vali-
dated for air–water vertical pipe flows over a wide range of gas and
http://dx.doi.org/10.1016/j.nucengdes.2014.02.015
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