The Navier‐Stokes equation and the species continuity equation have been solved numerically in a boundary fitted coordinate system comprising the geometry of a single strand bare tundish. The solution of the species continuity equation predicts the time evolution of the concentration of a tracer at the outlet of the tundish. The numerical prediction of the tracer concentration has been made with nine different turbulence models and has been compared with the experimental observation for the tundish. It has been found that the prediction from the standard k‐ε model, the k‐ε Chen‐Kim (ck) and the standard k‐ε with Yap correction (k‐ε Yap), matches well with that of the experiment compared to the other turbulence models as far as gross quantities like the mean residence time and the ratio of mixed to dead volume are concerned. It has been found that the initial transient development of the tracer concentration is best predicted by the low Reynolds number Lam‐Bremhorst model (LB model) and then by the k‐ε RNG model, while these two models under predict the mean residence time as well as the ratio of mixed to dead volume. The Chen‐Kim low Reynolds number (CK low Re) model (with and without Yap correction) as well as the constant effective viscosity model over predict the mixing parameters, i.e. the mean residence time and the ratio of mixed to dead volume. Taking the solution of the k‐ε model as a starting guess for the large eddy simulation (LES), a solution for the LES could be arrived after adopting a local refinement of the cells twice so that the near wall y+ could be set lower than 1. Such a refined grid gave a time‐independent solution for the LES which was used to solve the species continuity equation. The LES solution slightly over predicted the mean residence time but could predict fairly well the mixed volume. However, the LES could not predict both the peaks in the tracer concentration like the k‐ε, RNG and the Lam‐Bremhorst model. An analysis of the tracer concentration on the bottom plane of the tundish could help to understand the presence of plug and mixed flow in it.
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1 December 2003
Research Article|
December 01 2003
Mixing in a tundish and a choice of turbulence model for its prediction Available to Purchase
Pradeep K. Jha;
Pradeep K. Jha
Department of Mechanical Engineering, Indian Institute of Technology, Kharagpur, India
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Rajeev Ranjan;
Rajeev Ranjan
Department of Mechanical Engineering, Indian Institute of Technology, Kharagpur, India
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Swasti S. Mondal;
Swasti S. Mondal
Department of Mechanical Engineering, Indian Institute of Technology, Kharagpur, India
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Sukanta K. Dash
Sukanta K. Dash
Department of Mechanical Engineering, Indian Institute of Technology, Kharagpur, India
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Publisher: Emerald Publishing
Online ISSN: 1758-6585
Print ISSN: 0961-5539
© MCB UP Limited
2003
International Journal of Numerical Methods for Heat & Fluid Flow (2003) 13 (8): 964–996.
Citation
Jha PK, Ranjan R, Mondal SS, Dash SK (2003), "Mixing in a tundish and a choice of turbulence model for its prediction". International Journal of Numerical Methods for Heat & Fluid Flow, Vol. 13 No. 8 pp. 964–996, doi: https://doi.org/10.1108/09615530310501920
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