2012
DOI: 10.1016/j.ijheatmasstransfer.2012.03.070
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Mathematical and numerical model of solidification process of pure metals

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Cited by 20 publications
(14 citation statements)
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“…The variational formulation of energy conservation equation is expressed in the following form [15]: (1) is completed by the initial condition t = 0 : T = T o and boundary conditions of Dirichlet and Neumann type: (2) as well as Newton type condition with the heat loss due to convection and radiation [16]: (3) additionally, evaporation and heat flux toward welded element are taken into account within the area of heat source activity [17]: (4) where k is convective coefficient (assumed as k =150 W/ (m 2 o C), is radiation coefficient ( =0.5), is Stefan-Boltzmann constant and q(r,0) is the heat flux towards the top surface of welded workpiece (z=0) in the source activity zone of radius r, T 0 is an ambient temperature (assumed as 20 o C). The distribution of welding heat source power is adopted in mathematical model as a movable, volumetric heat source, having Gaussian power distribution with the linear decrease of energy intensity along material penetration depth [18]: (5) where [7,19,20], assuming solidus temperature T S =1400 o C, liquidus T L =1455 o C and latent heat of fusion H L =260×10 3 J/kg. Mechanical analysis in elastic-plastic range is based on classic equilibrium equations, supplemented by constitutive relations as well as initial and boundary conditions, which are assumed to ensure the external static determination of considered system [21]:…”
Section: Mathematical Modelmentioning
confidence: 99%
“…The variational formulation of energy conservation equation is expressed in the following form [15]: (1) is completed by the initial condition t = 0 : T = T o and boundary conditions of Dirichlet and Neumann type: (2) as well as Newton type condition with the heat loss due to convection and radiation [16]: (3) additionally, evaporation and heat flux toward welded element are taken into account within the area of heat source activity [17]: (4) where k is convective coefficient (assumed as k =150 W/ (m 2 o C), is radiation coefficient ( =0.5), is Stefan-Boltzmann constant and q(r,0) is the heat flux towards the top surface of welded workpiece (z=0) in the source activity zone of radius r, T 0 is an ambient temperature (assumed as 20 o C). The distribution of welding heat source power is adopted in mathematical model as a movable, volumetric heat source, having Gaussian power distribution with the linear decrease of energy intensity along material penetration depth [18]: (5) where [7,19,20], assuming solidus temperature T S =1400 o C, liquidus T L =1455 o C and latent heat of fusion H L =260×10 3 J/kg. Mechanical analysis in elastic-plastic range is based on classic equilibrium equations, supplemented by constitutive relations as well as initial and boundary conditions, which are assumed to ensure the external static determination of considered system [21]:…”
Section: Mathematical Modelmentioning
confidence: 99%
“…Temperature field during material melting and solidification is affected by the latent heat of fusion. Macro models describing solidification process for both pure metals [20][21][22][23] and alloys [24][25][26][27][28] can be found in the literature. Mostly, one domain approach is used with fuzzy solidification front in the model where latent heat is included into effective heat capacity.…”
Section: Thermal Phenomenamentioning
confidence: 99%
“…In the third step the solution of the equation (35) gives the real velocity field u f +1 . The numerical treatment of the equation (4) was discussed in details in [35,36]. The reinitialization of the level set function as well as the calculation of the heat fluxes on the solid and liquid sides of Γ LS were the same as in [36].…”
Section: Numerical Modelmentioning
confidence: 99%