2004
DOI: 10.1179/136217104225021814
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Three-dimensional turbulent weld pool convection in gas metal arc welding process

Abstract: A three-dimensional model has been developed to study turbulent fluid flow and heat transfer in a gas metal arc weld pool. The phase change process during melting and solidification is modelled using the enthalpy-porosity technique. Mass and energy transports by droplet transfer are considered through a thermal analysis of the electrode. The droplet heat addition into the molten pool is considered to be in the form of a volumetric heat source distributed in an imaginary cylindrical cavity within the weld pool … Show more

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Cited by 17 publications
(15 citation statements)
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“…For a typical GTA weld pool in low carbon steel with U s = 150 mm/s and r eff = 2.0 mm, d v = 1.0 9 10 À5 m. Evidently, very small elements are in demand within the melt pool necessitating a large number of total elements in the solution domain. However, independent studies with regard to heat transfer and fluid flow analyses in welding [18,20,21] suggest little influence of very fine mesh in the melt pool on the prediction of overall temperature and velocity fields. The minimum element size, therefore, is kept as 3.5 9 10 À5 m in the present work.…”
Section: Computational Aspectsmentioning
confidence: 97%
See 1 more Smart Citation
“…For a typical GTA weld pool in low carbon steel with U s = 150 mm/s and r eff = 2.0 mm, d v = 1.0 9 10 À5 m. Evidently, very small elements are in demand within the melt pool necessitating a large number of total elements in the solution domain. However, independent studies with regard to heat transfer and fluid flow analyses in welding [18,20,21] suggest little influence of very fine mesh in the melt pool on the prediction of overall temperature and velocity fields. The minimum element size, therefore, is kept as 3.5 9 10 À5 m in the present work.…”
Section: Computational Aspectsmentioning
confidence: 97%
“…[13][14][15][16] Alternately, the researchers used the k-e based turbulence equation to compute the turbulent kinetic energy and its influence on convective flow in the weld pool, which not only increased computational time and complexity but also added uncertainty in calculations as the k-e based turbulence equation required additional empirical parameters. [17][18][19][20][21] The fact that a certain amount of uncertainty will ever prevail in the computed temperature and velocity fields in the weld pool is, nevertheless, axiomatic. A recourse, therefore, is to develop a relatively simple heat transfer and fluid flow model with a trade-off between the complex thermophysical phenomena in a real weld pool and the extent of the same that can be accounted for with the minimum number of uncertain model input parameters.…”
Section: Introductionmentioning
confidence: 99%
“…where q is heat flux (Ref 25), g is the arc efficiency, U w is the welding speed, I is the welding current, r b is the heat distribution parameter, r is the distance between the specific location and the heat source, r is the Stefan-Boltzmann constant, h c is the convective heat transfer coefficient, and T 0 is the ambient temperature. At the y = 0 and symmetric surface:…”
Section: Mathematical Modelmentioning
confidence: 99%
“…The second approach, such as the one presented in the present paper, uses analytical models to simulate the heat source and material supply: arc plasma phenomena are not explicitly modelled. Over the years, the simplified Goldak approach and the laminar flow analysis in the weld pool have tended to be replaced by more physically coupled models including a Gaussian surface heat flux and turbulent flows without any enhanced viscosity [9,10,11,12]. However the modelling of turbulent flows has only been proposed in steady conditions, for a coordinate system moving with the heat source.…”
Section: Introductionmentioning
confidence: 99%
“…Unfocused and moderate power laser is used here as an auxiliary heat source, the role of which is essentially to enlarge the welding pool. In addition a third volumetric heat source is implemented to model the heat supply associated with the impingement of molten droplets into the fusion zone [10,14,15,16]. Moreover, for the mass input of these molten droplets, a source term is added to the right hand side of the mass conservation equation for certain liquid finite elements in the fusion zone [25].…”
Section: Introductionmentioning
confidence: 99%