Abstract:Dramatic increases in the depth of weld bead penetration have been demonstrated by welding stainless steel using the gas tungsten arc (GTA) process with activating fluxes consisting of oxides and halides. However, there is no commonly agreed mechanism for the effect of flux on the process. In order to clarify the mechanism, behaviour of the arc and weld pool in the GTA process with activating flux was observed in comparison with a conventional GTA process. A constricted anode root was found in the GTA process … Show more
“…Adding and precisely controlling the quantity of these minor elements in the weld pool in GTA welding process are critical for a satisfactory weld with deep penetration. After decades of development, several methods have been found for the addition of minor elements to the weld pool by adjusting the chemical composition of the raw material, [1][2][3][4][5][6] smearing oxide or halide fluxes on the plate surface (A-TIG) [7][8][9][10][11][12][13][14][15][16][17][18][19][20] or adding active gases to the argon shielding gas. [21][22][23][24][25] Compared with the research on A-TIG, the investigation on the effect of active gaseous addition on the weld shape is limited.…”
“…Adding and precisely controlling the quantity of these minor elements in the weld pool in GTA welding process are critical for a satisfactory weld with deep penetration. After decades of development, several methods have been found for the addition of minor elements to the weld pool by adjusting the chemical composition of the raw material, [1][2][3][4][5][6] smearing oxide or halide fluxes on the plate surface (A-TIG) [7][8][9][10][11][12][13][14][15][16][17][18][19][20] or adding active gases to the argon shielding gas. [21][22][23][24][25] Compared with the research on A-TIG, the investigation on the effect of active gaseous addition on the weld shape is limited.…”
“…Minor elements can be added to the weld pool by adjusting the chemical composition to the base material, [1][2][3][4][5][6] smearing fluxes (halides or oxides) on the plate surface [7][8][9][10][11][12][13][14][15][16][17][18][19] or using active gaseous addition to the argon shielding gas. [20][21][22] The intentional or unintentional addition of a small amount of minor elements to the base material significantly changes the weld penetration.…”
In order to investigate the effect of oxygen additions on the weld shape in gas tungsten arc welding, bead-on-plate specimens were made of SUS304 stainless steel using O 2 -Ar mixed shielding gas with oxygen additions from 1 000 to 10 000 ppm. The weld bead cross-sections and the weld surface oxide layer were observed by optical microscopy after welding. The oxygen content in the weld metal was measured using an Oxygen/Nitrogen Analyzer. The weld depth/width ratio increases substantially as a result from the additions of oxygen to the argon shielding gas in the range of 3 000 to 5 000 ppm both for the 10 and 20 L/min shielding gas flow rates. When the oxygen addition contents are below 2 000 ppm or over 6 000 ppm, the weld D/W ratio decreases to approximately 0.2. The oxygen in the weld pool plays an important role as an active element affecting the Marangoni convection mode. The inward Marangoni convection occurs on the liquid pool surface when the oxygen in the weld is over 100 ppm, and hence the D/W ratio increases suddenly. The thicker oxide layer on the weld pool surface is not only a barrier for the oxygen to transfer and become a solute in the weld pool, but also prevents the weld pool from moving freely, and hence changes the weld pool shape.
“…3 (17) . These driving forces depend not only on the physical properties of the anode materials but also the properties of the plasma state (18) . In order to obtain an assessment of the relative significance of these four forces, we have made the calculations for the steady state under the conditions of arc current 150 A and arc gap 5 mm, and with only one of the four forces operating.…”
In order to clarify the formative mechanism of weld penetration in an arc welding process, a numerical model is useful to understand quantitative values of the balances of mass, energy and force in the welding phenomena. In the present paper, the whole region of welding process using a free-burning arc, namely, tungsten cathode, arc plasma and weld pool is treated in a unified numerical model to take into account the close interaction between the arc plasma and the liquid metal. Calculations are made for the time dependent development of the weld pool for the free-burning arc in helium at atmospheric pressure. It is shown that the calculated convective flow in the weld pool is dominated by the surface tension gradient force and the electromagnetic force. It is also shown that different surface tension properties can change the direction of re-circulatory flow in the weld pool and dramatically vary the weld penetration geometry.
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