1987
DOI: 10.13182/nt87-a33990
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A Three-Field Diffusion Model of Three-Phase, Three-Component Flow for the Transient Three-Dimensional Computer Code IVA2/001

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Cited by 22 publications
(3 citation statements)
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“…The first order donor cell discretized mass conservation equation ( It is advisable to compute the geometry coefficients, At this point the method used for computation of the field volumetric fractions in the computer codes IVA2 Kolev (1986, 1987, 1993, and IVA3 Kolev (1991) will be described. The method exploits the point Gauss-Seidel iteration assuming known velocity fields and thermal properties.…”
Section: Discretization Of the Mass Conservation Equationsmentioning
confidence: 99%
“…The first order donor cell discretized mass conservation equation ( It is advisable to compute the geometry coefficients, At this point the method used for computation of the field volumetric fractions in the computer codes IVA2 Kolev (1986, 1987, 1993, and IVA3 Kolev (1991) will be described. The method exploits the point Gauss-Seidel iteration assuming known velocity fields and thermal properties.…”
Section: Discretization Of the Mass Conservation Equationsmentioning
confidence: 99%
“…The so called volume conservation equation (5.188) was already derived in [1] in 1986 and published in [2] in 1987: is the mixture density. It is very useful for designing numerical solution methods.…”
Section: The Volume Conservation Equationmentioning
confidence: 99%
“…It is very useful for designing numerical solution methods. We derive this equation for the transformed system following the same procedure as in Chapter 5 [1,2]. This means we start with the mass conservation for each velocity field, use the chain rule, divide by the field density and add the resulting field equations.…”
Section: The Volume Conservation Equationmentioning
confidence: 99%