Two Phase Flow, Phase Change and Numerical Modeling 2011
DOI: 10.5772/19699
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Modeling Solidification Phenomena in the Continuous Casting of Carbon Steels

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Cited by 4 publications
(7 citation statements)
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References 29 publications
(22 reference statements)
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“…Therefore, during solidification of carbon steels, there is always a range between solidus and liquidus temperatures in which the solid fraction is in the range from 0 to 1; this physical range inside a solidifying steel body is called mushy zone, and the whole phenomenon is related to micro-segregation. The simple micro-segregation model [32] has been adopted in this work, and the analysis has been described in similar previous studies [24,29,33]. It appears that the larger the carbon content in a steel grade, the larger the mushy zone gets, and central porosity becomes inevitable in the final stages of solidification.…”
Section: Comparison Of Temperature Values Between the Theoretical (Fomentioning
confidence: 98%
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“…Therefore, during solidification of carbon steels, there is always a range between solidus and liquidus temperatures in which the solid fraction is in the range from 0 to 1; this physical range inside a solidifying steel body is called mushy zone, and the whole phenomenon is related to micro-segregation. The simple micro-segregation model [32] has been adopted in this work, and the analysis has been described in similar previous studies [24,29,33]. It appears that the larger the carbon content in a steel grade, the larger the mushy zone gets, and central porosity becomes inevitable in the final stages of solidification.…”
Section: Comparison Of Temperature Values Between the Theoretical (Fomentioning
confidence: 98%
“…The vertical side, MZ, is the boundary from which the main heat flow (cooling) takes place; the horizontal side OZ and the diagonal side OM, with an inclination of π/8, or 22.5°, are considered to be adiabatic to heat flow due to the aforementioned symmetry reasons. This study is part of a series of published works with respect to the numerical solution of the heat transfer equation in 2D (square and rectangular) and 3D domains [24,[27][28][29]. Although the core of the existing program remained intact, due to the nature of the present trigonal domain, the part of the program related to the boundary conditions had to be developed from scratch.…”
Section: Numerical Solutionmentioning
confidence: 99%
“…This specific article is part of a series of published works with respect to the numerical solution of the heat transfer equation in 2D and 3D domains [28][29][30]. The strongly implicit method as practiced by Patankar [23] was applied.…”
Section: Numerical Solutionmentioning
confidence: 99%
“…The Gauss-Seidel algorithm for the iterative solution of the matrix of equations was applied, as it was proven as a very suitable scheme for the solution of the temperature distribution putting into effect the OpenMP instruction set for parallel computation. Over-relaxation was applied for the fastest possible convergence; the over-relaxation parameter used was ω= 1.870, which has exhibited good results for these kinds of studies [28][29][30][31][32]. This specific piece of software was developed in GNU C++, version 4.8.1, supplied by TDM-GCC, and accessed through the open source, cross-platform IDE, Code::Blocks, version 13.12.…”
Section: Numerical Solutionmentioning
confidence: 99%
“…The tests must be performed several times at various T , so the time and cost are high [ 10 , 11 ]. Too high cooling rate and alloying amount may reduce cast steel plasticity and lead to crack formation [ 2 , 11 , 12 ]. Alloying also has an important effect on the ductility of cast steel [ 10 , 13 ].…”
Section: Introductionmentioning
confidence: 99%