From experiments to eulerian two-fluid
gas-liquid models for turbulent
bubbly flows
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In spite of the progress
achieved in the adaptation of the CFD codes to bubbly flows modelling, some
important difficulties subsist; in particular the ability to predict phase
distribution remains limited by the inadequate modelling of the turbulence and
of the interfacial forces. At the same time, number of experimental researches
has been achieved during the two last decades and we have now number of databases
concerning basic bubbly flows configurations. These experimental studies have
greatly enhanced our understanding of two-phase flow mechanisms. The analysis
of experimental results show that the presence of the dispersed phase alters
considerably the liquid turbulence structure. With regard to turbulence
modelling, the experimental results suggest that we have to go up to turbulence
closure level so that we may take into account the effect of the bubbles on the
redistribution mechanism. In order to attain this objective, second order
turbulence modelling is required.
On the other hand the turbulence is proved to have in important effect
on the phase distribution phenomenon. Two important questions are thus preamble
to the elaboration of efficient prediction tools applied to gas-liquid systems
especially when transfer problems are considered. The first question is related
to the predetermination of the turbulence structure of the continuous phase as
it is altered by the dispersed phase and the second concerns the prediction of
the void fraction and bubble¹s size distributions. In the two-fluid modelling
to be presented, we precisely attempt to improve the prediction of two-phase
bubbly flows by laying emphasis on two aspects of the interfacial interactions
:
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First,
we develop a turbulence model adapted to bubbly flows in order to describe
accurately the Reynolds stress tensor in each phase. In this model, the
Reynolds stress tensor of the continuous phase is split into two parts, a
turbulent dissipative part produced by the gradient of mean velocity and by the
bubbles wakes, and a pseudo-turbulent non-dissipative part induced by the
bubbles displacements, each part is predetermined by a transport equation.
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Second,
we take into account the turbulent correlations issued from added mass in the
expression of the force exerted by the liquid on the bubbles: this turbulent
contribution, which is customary ignored, is proving to be important in the
phase distribution phenomena especially in bubbly flows under micro-gravity
condition;
The application of the
eulerian-eulerian two-fluid modelling allows an accurate representation of the
turbulence and of the void fraction in number of basic bubbly flows (grid,
uniform shear, 2D thin shear bubbly flows and wall bubbly flows) with moderate
void fractions (up to 15%). In this presentation the most prominent steps of
the modelling will be presented, and the results will be commented in order to
specify the basic requirements in the elaboration of general CFD codes applied to
Gas-liquid bubbly flows.