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Published: 31 October 2011
Fig. 6 Temperature isotherms near the weld pool in Barlow's weld. Note that contour “I” has two pools: one under the arc and one in the region behind the arc. This heat source was modeled as a prescribed-temperature region. More
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Published: 01 January 1993
Fig. 2 Schematic showing typical weld pool dynamics of a submerged arc weld More
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Published: 01 January 1993
Fig. 6 Temperature isotherms near the weld pool in Barlow's weld. Note that contour I has two pools: one under the arc and one in the region behind the arc. This heat source was modeled as a prescribed-temperature region. More
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Published: 31 October 2011
Fig. 7 Cross section of weld pool. Source: Ref 14 More
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Published: 31 October 2011
Fig. 7 (a) Experimental weld pool geometry. The vertical line shows the joint of the two plates. (b) Calculated temperature and velocity fields in the weld pool. The contours represent the temperatures in degrees Kelvin, and the vectors represent the liquid velocity. (c) The contours represent More
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Published: 31 October 2011
Fig. 10 Distribution of turbulent variables in the weld pool. (a) Dimensionless viscosity, μ t /μ. (b) Dimensionless thermal conductivity, k t / k . (c) Turbulent kinetic energy, m 2 /s 2 × 10 −4 . (d) Dissipation rate of turbulent kinetic energy, m 2 /s 3 × 10 −4 . Adapted from Ref 15 More
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Published: 31 October 2011
Fig. 12 Typical sequence showing the impinging of droplets, weld pool dynamics, and temperature distribution (side view). Adapted from Ref 83 More
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Published: 31 October 2011
Fig. 5 Typical weld pool/heat source interaction times as a function of heat-source intensity. Materials with a high thermal diffusivity, such as copper or aluminum, would lie near the top of the band, whereas magnesium alloys and steels would lie in the middle. Titanium alloys, with very low More
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Published: 31 October 2011
Fig. 5 Effect of arc jet on depression of weld pool More
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Published: 31 October 2011
Fig. 5 Plot of electron beam weld pool ratio ( d / w ) versus electron beam power density for low-sulfur (20 ppm) and high-sulfur (>120 ppm) type 304L stainless steel. Keyhole formation begins at approximately 2 × 10 3 W/mm 2 . More
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Published: 31 October 2011
Fig. 9 Effect of arc pressure on the weld pool for stationary and traveling welds. (a) v = 0. (b) v > 0, with weak radial pressure gradient, p 1 . (c) v > 0, with strong radial pressure gradient, p B . Source: Ref 13 More
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Published: 31 October 2011
Fig. 12 Schematic showing typical flow pattern in a submerged arc weld pool. Source: Ref 20 More
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Published: 31 October 2011
Fig. 9 Effect of electrode tip geometry and shielding gas composition on weld pool shape for spot-on-plate welds. Welding parameters: current, 150 A; duration, 2 s More
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Published: 31 October 2011
Fig. 1 Typical weld pool-heat source interaction time. Source: Ref 4 More
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Published: 31 October 2011
Fig. 2 Submerged arc weld pool schematic More
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Published: 31 October 2011
Fig. 7 Effect of increase in welding parameters on weld pool form factor. (a) Optimum weld pool dimensions (shallow weld pool, high form factor, acute angle between grains). (b) Undesirable weld pool dimensions (deep weld pool, low form factor, obtuse angle between grains). Source: Ref 6 More
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Published: 01 January 1993
Fig. 17 Silicone rubber replication technique used to evaluate decanted weld pool shape. Source: Ref 21 More
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Published: 01 January 1993
Fig. 3 Typical weld pool-heat source interaction times as function of heat-source intensity. Materials with a high thermal diffusivity, such as copper or aluminum, would lie near the top of this band, whereas steels, nickel alloys, or titanium would lie in the middle. Uranium and ceramics More
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Published: 01 January 1993
Fig. 5 Plot of electron beam weld pool ratio ( d / w ) versus electron beam power density for low-sulfur (20 ppm) and high-sulfur (>120 ppm) type 304L stainless steel. Keyhole formation begins at about 2 × 10 3 W/mm 2 . More
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Published: 01 January 1993
Fig. 9 Effect of arc pressure on the weld pool for stationary and traveling welds. (a) v = 0. (b) v > 0, with weak radial pressure gradient, p 1 . (c) v > 0, with strong radial pressure gradient, p B . Source: Ref 12 More