2007
DOI: 10.1504/ijcsm.2007.016531
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On the implementation of the κ-ε turbulence model in incompressible flow solvers based on a finite element discretisation

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Cited by 115 publications
(106 citation statements)
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“…The choice of fixed bubble pivot volumes and fixed class widths offers the advantage of expressing the discretized transport equation (20) in terms of class holdups α i instead of the number probability density, f i = α i υ i ∆υ i (see (1)). Doing so enforces only mass conservation, however the bubble number density may not be conservative.…”
Section: Implementation Of Pbementioning
confidence: 99%
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“…The choice of fixed bubble pivot volumes and fixed class widths offers the advantage of expressing the discretized transport equation (20) in terms of class holdups α i instead of the number probability density, f i = α i υ i ∆υ i (see (1)). Doing so enforces only mass conservation, however the bubble number density may not be conservative.…”
Section: Implementation Of Pbementioning
confidence: 99%
“…Regarding the arising inconsistency we subscribe to the argument of [5], who reported that the difference in the predicted values of interfacial area and Sauter mean bubble diameter obtained with only mass conservation and obtained with mass and bubble number conservation was less than 1%. Multiplying equation (20) with υ i ∆υ i results in conservative source and sink terms, since the overall gas-holdup cannot be changed due to coalescence or breakup procedures 1 . Additionally, any sink (source) term of a given rate associated to a particular breakup or coalescence procedure induces a source (sink) term with the same rate but in a different class.…”
Section: Implementation Of Pbementioning
confidence: 99%
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