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    the mechanisms of liquid flow over outlet weirs of distillation and
    absorption trays (Wijn, 1999). Rao, Goutami, and Jain (2001) pre-
    sented a method that used the tray efficiency matrix directly in
    simulations. The tray efficiency matrix used in the simulation was
    obtained frompoint efficiencymatrix. They used the direct incorpo-
    ration of efficiencymatrix in the Naphtali Sandholmmethod (1971)
    and reported that their modified method had better convergence
    characteristics than the original Naphtali Sandholm method for
    distillation, absorption and extraction columns. Wang, Li, Wozny,
    and Wang (2003) proposed a model to express the startup behav-
    iors of batch columns starting from an empty cold state. They
    verified their model through experiments on a pilot batch plant
    with a bubble-cap tray column to separate a methanol/water mix-
    ture.
    Due to progresses in computer hardware and software and con-
    sequent increase of the calculation speed, the Computational Fluid
    Dynamics (CFD) modeling technique would be a powerful and
    effective tool for understanding the complex hydrodynamics in
    many industrial processes.Mehta, Chuang, andNandakumar (1998)
    analyzed the liquidphaseflowpatterns ona sieve tray by solving the
    time-averaged governing equations ofmass andmomentumfor the
    liquid phase. In their study, interactions with the vapor phase were
    taken into account using the interphasemomentumtransfer coeffi-
    cients determined fromempirical correlations. The two-phase flow
    behavior on a sieve tray column was studied by Yu, Yan, You, and
    Liu (1999) using a two-dimensional model. They focused on the
    description of the hydrodynamics along the liquid flow path while
    variations in the direction of gas flow along the height of the dis-
    persion were ignored. van Baten and Krishna (2000) developed a
    CFD model for describing the hydrodynamics of sieve trays. They
    modeled the gas and liquid phases in the Eulerian framework as
    two interpenetrating phases. The interphasemomentumexchange
    coefficient was estimated based on the Bennett, Agrawal, and Cook
    (1983) correlation. In their study, several three-dimensional tran-
    sient modelings were carried out for a 0.3m diameter sieve tray
    by varying the gas superficial velocity, the column weir height and
    liquid loads. Their CFD model reflected chaotic tray hydrodynam-
    ics and revealed several liquid circulation patterns, which had true
    three-dimensional characteristics. They reported that the predicted
    clear liquid height obtained from their models was in good agree-
    ment with the Bennett correlation.
    Gesit, Nandakumar, and Chuang (2003) employed the commer-
    cial CFX package to predict the flow patterns and hydraulics of
    a commercial scale 1.22m diameter air–water sieve tray. In their
    investigation, the velocity distributions, clear liquid height, froth
    height, and liquid holdup fraction in froth were predicted for var-
    ious combinations of gas and liquid flow rates. In their model,
    each phase was treated as an interpenetrating continuum hav-
    ing separate transport equations and interaction between the two
    phaseswas considered via an interphasemomentumtransfer. They
    claimed that CFD could be used as a valuable tool in tray design and
    analysis. A CFD model using the commercial CFX code was intro-
    duced by Hoffmann, Ausner, Repke, and Wozny (2005) in order
    to model two and three-phase transient film flow in packed tow-
    ers. An Euler–Euler algorithmformultiphase calculationswith free
    surfaceswas used. Similar to the VOFmethod, averaged phase frac-
    tions inside the finite volume cells and the surface tension was
    implemented in themodel. The turbulencemodelingwas not taken
    into account due to the relatively low range of the Reynolds num-
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