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A transient model is established and solved by finite volume algorithm.
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A solution of the Navier Stokes equations was obtained by applying an implicit finite volume algorithm.
In this paper, the formulation is further enhanced by introducing a novel upwind vertex centred finite volume algorithm with three key novelties.
A vertex centred Jameson Schmidt Turkel (JST) finite volume algorithm was recently introduced by the authors (Aguirre et al., 2014 [1]) in the context of fast solid isothermal dynamics.
A vertex centred Finite Volume algorithm is presented for the numerical simulation of fast transient dynamics problems involving large deformations.
The second-order finite volume algorithm (40) requires numerical fluxes centered on the interface mid-point.
Moreover, many finite volume algorithms do not use the shape function reconstruction.
The high resolution finite volume algorithms are able to solve multidimensional population balance equations avoiding these unwanted phenomena.
The computational problem is solved by finite volume method (FVM) with the SIMPLE algorithm.
A numerical model by finite volume is used for the solution of the physical model.
The direct and the sensitivity problems are solved by finite volume method.
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