Numerical analysis of undercut defect mechanism in high speed gas tungsten arc welding

Abstract A computational fluid dynamics model is developed to investigate undercut defect formation in high speed gas tungsten arc welding (GTAW) process. Double-ellipse arc shear stress model and modified double-ellipse arc heat source and arc pressure models are used, which are self-adaptive to weld pool surface evolution. The heat and mass transfer in weld pool and solidified weld bead profile are simulated and the undercut mechanism are discussed. The prematurely solidified periphery part at maximum width of weld pool is the initiation of undercut defect and the inward velocity component at trailing periphery due to teardrop-shaped weld pool profile promotes subsequent undercut formation, which provides an explanation to the high tendency of undercut formation during high current and high speed welding. The undercut morphology is unremarkably influenced by Marangoni force and the capillary pressure hinders undercut formation to some extent. The developed model is validated by comparing undercut morphology and gouging region profile from both simulation and experiment.

[1]  V. Voller,et al.  The modelling of heat, mass and solute transport in solidification systems , 1989 .

[2]  K. Mills,et al.  Equation to estimate the surface tensions of stainless steels , 2005 .

[3]  J. Szekely,et al.  On the calculation of the free surface temperature of gas-tungsten-arc weld pools from first principles: Part I. modeling the welding arc , 1992 .

[4]  M. Ohara,et al.  Study on High Speed Submerged Arc Welding (Report 1) , 1983 .

[5]  Chuansong Wu,et al.  A unified 3D model for an interaction mechanism of the plasma arc, weld pool and keyhole in plasma arc welding , 2015 .

[6]  Akira Matsunawa,et al.  Role of Surface Tension in Fusion Welding (Part 2) : Hydrostatic Effect , 1983 .

[7]  W. Shimada,et al.  A Study on Bead Formation by Low Pressure TIG Arc and Prevention of Under-Cut Bead , 1983 .

[8]  P. Mendez Order of magnitude scaling of complex engineering problems, and its application to high productivity arc welding , 1999 .

[9]  Thomas W. Eagar,et al.  Distribution of the heat and current fluxes in gas tungsten arcs , 1985 .

[10]  Donald Peckner,et al.  Book Review: Handbook of Stainless Steels , 1978 .

[11]  H. Tsai,et al.  Heat transfer and fluid flow in a partially or fully penetrated weld pool in gas tungsten arc welding , 2001 .

[12]  G. Qin,et al.  Investigation of humping defect in high speed gas tungsten arc welding by numerical modelling , 2016 .

[13]  Richard C. Flagan,et al.  The wall shear stress produced by the normal impingement of a jet on a flat surface , 2000, Journal of Fluid Mechanics.

[14]  J. Brackbill,et al.  A continuum method for modeling surface tension , 1992 .

[15]  J. M. Toguri,et al.  The effect of the cathode tip angle on the GTAW arc and weld pool: I. Mathematical model of the arc , 1997 .

[16]  Kenneth C. Mills,et al.  Factors affecting variable weld penetration , 1990 .

[17]  Dave F. Farson,et al.  Understanding Bead Hump Formation in Gas Metal Arc Welding Using a Numerical Simulation , 2007 .

[18]  Thomas W. Eagar,et al.  Penetration and defect formation in high-current arc welding , 2003 .

[19]  Thomas W. Eagar,et al.  Pressures produced by gas tungsten arcs , 1986 .

[20]  H W Sudnik,et al.  RESEARCH INTO FUSION WELDING TECHNOLOGIES BASED ON PHYSICAL-MATHEMATICAL MODELS , 1991 .

[21]  M. Abid,et al.  Effect of different electrode tip angles with tilted torch in stationary gas tungsten arc welding: A 3D simulation , 2013 .