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Electric welding arc modeling with the three-dimensional solver OpenFOAM: A comparison of different electromagnetic models
Högskolan Väst, Institutionen för ingenjörsvetenskap, Avd för industriell produktion. (Welding PTW)ORCID-id: 0000-0003-2535-8132
Högskolan Väst, Institutionen för ingenjörsvetenskap, Avd för industriell produktion. (Welding PTW)ORCID-id: 0000-0002-7897-621X
Chalmers University of Technology. (Department of Applied Mechanics)
2011 (Engelska)Ingår i: 64 th Annual Assembly and International Conference of International Institute of Welding, 64th IWW: Chennai, 17-22 july, 2011. Working group 212, 2011, s. 212-1189-11-1-212-1189-11-16Konferensbidrag, Publicerat paper (Övrigt vetenskapligt)
Abstract [en]

This study focuses on the modeling of a plasma arc heat source in the context ofelectric arc welding. The model was implemented in the open source CFD softwareOpenFOAM-1.6.x, coupling thermal fluid mechanics in three dimensions with electromagnetics.Different approaches were considered for modeling the electromagneticfields: i) the three-dimensional approach, ii) the two-dimensional axi-symmetric approach,iii) the electric potential formulation, and iv) the magnetic field formulation asdescribed by Ramírez et al. [1]. The underlying assumptions and the differencesbetween these models are detailed. The models i) to iii) reduce to the same quasione-dimensional limit for an axi-symmetric configuration with negligible radial currentdensity, contrary to the formulation iv). The models ii) to iv) cannot represent the samephysics when the radial current density is significant, such as for a short arc or anelectrode with a conical tip. The models i) to iii) were retained for doing numerical simulations.The corresponding solvers were tested against analytic solution for an infiniteelectric rod. Perfect agreement was obtained for all the models tested. The completesolver (thermal fluid coupled with electromagnetics) was tested against experimentalmeasurements for Gas Tungsten Arc Welding (GTAW). The shielding gas was argon,the arc was short (2mm), the electrode tip conical, and the configuration axi-symmetric.Anode and cathode were treated as boundary conditions. The models i) and ii) lead tothe same results, but not the formulation iii). It indeed neglects the radial current densitycomponent, resulting in a poor estimation of the magnetic field, and in turn of thearc velocity. Limitations of the complete solver were investigated changing also the gascomposition, and testing boundary conditions. These conditions, difficult to measureand to estimate a priori, significantly affect the simulation results.

Ort, förlag, år, upplaga, sidor
2011. s. 212-1189-11-1-212-1189-11-16
Nyckelord [en]
electric arc welding, thermal plasma, short arc, electromagnetic model
Nationell ämneskategori
Bearbetnings-, yt- och fogningsteknik
Forskningsämne
TEKNIK; TEKNIK, Fysik
Identifikatorer
URN: urn:nbn:se:hv:diva-3719OAI: oai:DiVA.org:hv-3719DiVA, id: diva2:444158
Konferens
64 th Annual Assembly and International Conference of International Institute of Welding, 64th IWW.Chennai, 17-22 july, 2011
Anmärkning

Publicerat på IWW:s webbplats - krävs lösenord

Tillgänglig från: 2011-09-28 Skapad: 2011-09-28 Senast uppdaterad: 2019-11-21Bibliografiskt granskad

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Choquet, IsabelleJavidi Shirvan, Alireza

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