Features of Arc Surfacing Process in a Longitudinal Magnetic Field

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The electrode wire melting coefficient (αm) is determined for the submerged arc surfacing and welding in a longitudinal magnetic field (LMF) under reverse and direct polarities with ferromagnetic and paramagnetic (non-magnetic) wires. The maximum gain in the wire melting coefficient is achieved in the magnetostatic field assisted surfacing and welding. The effect reduces with the LMF frequency increasing to 4-6 Hz and virtually does not change with the further increase to 50 Hz. The electrode wire melting coefficient is shown to increase depending on magnetic properties.It has been established that the penetration depth of the parent metal reduces at the 50 Hz LMF surfacing when the longitudinal induction exceeds 65 mT.The constant and alternating LMFs reduce the speed of in-bath liquid metal flows, which results in the reduced parent metal penetration efficiency at surfacing.

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313-318

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October 2014

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© 2014 Trans Tech Publications Ltd. All Rights Reserved

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[1] A.D. Razmyshlyaev. Magnetic control of weld formation at arc welding, Mariupol, (2000).

Google Scholar

[2] V.P. Chernysh, V.D. Kuznetsov, A.N. Briskman, G.M. Shelenkov. Welding with electromagnetic stirring, Kiev, (1983).

Google Scholar

[3] J. C. Villafuerte, H. W. Kerr. Electromagnetic stirring and grain refinement in stainless steel GTA welds / Welding journal. – 69 (1990). – No. 1. – pp.1-13.

Google Scholar

[4] M. Malinovski-Brodnicka, G. den Ouden, W. J. P. Vink. Effect of electromagnetic Stirring on GTA welds in austenitic stainless steel / Welding journal. – 69 (1990). – No. 2. – pp.52-59.

Google Scholar

[5] A.M. Boldyrev, V.A. Birzhev, A.V. Chernykh. Improving the electrode wire melting productivity at welding in a longitudinal magnetic field / Welding production. – 1989. – No. 4. – 18-19.

DOI: 10.1080/09507119809447812

Google Scholar

[6] A. M. Boldyrev, V.A. Birzhev, A.V. Chernykh. The penetration depth control in arc welding and surfacing with alternating longitudinal magnetic field / Welding production. – 1993. – No. 6. – pp.30-31.

Google Scholar

[7] Y.H. Kang, S.J. Na. Characteristics of welding and arc signal in narrow groove gas metal arc welding using elecromagnetic arc oscillation / Welding Journal. – 82 (2003). – No. 5. – pp.93-99.

DOI: 10.1016/b978-008044066-8/50004-5

Google Scholar

[8] A. D. Razmyshlyaev, M. V. Mironova. Magnetic control of formation of rollers and welds at arc surfacing and weldingl, Mariupol, (2009).

Google Scholar

[9] Chinakhov D.A. Study of thermal cycle and cooling rate of steel 30ХГСА single-pass weld joints / Applied Mechanics and Materials. – Vols. 52-54. – 2011. – pp.442-447.

DOI: 10.4028/www.scientific.net/amm.52-54.442

Google Scholar

[10] V. D. Kuznetsov, I. V. Malinkin, V. V. Syrovatka. Behaviors of the arc and transfer of electrode metal on welding process in a longitudinal magnetic field / Welding production. – 1972. – No. 4. – pp.3-4.

Google Scholar

[11] B. N. Selyanenkov, V. A. Blinkov, U. V. Kazakov. About weld formation in a longitudinal magnetic field in argon arc welding / Welding production. – 1975. – No. 11. – pp.5-7.

Google Scholar

[12] M. L. Lin, T. W. Eagar. Influence of arc pressure on weld pool geometry / Welding Journal. – 64 (1985). – No. 6. – pp.163-169.

Google Scholar

[13] Z. Cao, Z. Yang, X. L. Chen. Three-Dimensional Simulation of Transient GMA Weld Pool with Free Surface / Welding Journal. – 83 (2004). – No. 6. – 169-176.

Google Scholar