2009
DOI: 10.1016/j.jmatprotec.2008.11.036
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Characteristics of alternate supply of shielding gases in aluminum GMA welding

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Cited by 35 publications
(45 citation statements)
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“…The Marangoni number for argon is in line with those presented elsewhere [26]. Considering the forces evaluated, it can be inferred that the flow vectors are opposite in direction to that of argon as stated by Kang et al [2]. It was calculated that helium produced a greater plasma shear stress, buoyancy force and Marangoni convection, whereas argon produced a greater arc force and Lorentz force.…”
Section: Resultssupporting
confidence: 86%
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“…The Marangoni number for argon is in line with those presented elsewhere [26]. Considering the forces evaluated, it can be inferred that the flow vectors are opposite in direction to that of argon as stated by Kang et al [2]. It was calculated that helium produced a greater plasma shear stress, buoyancy force and Marangoni convection, whereas argon produced a greater arc force and Lorentz force.…”
Section: Resultssupporting
confidence: 86%
“…This can be attributed to the fact that during the alternating shielding gas process the arc is continually being re-established when each gas is present, whereas when using GTAW-P the power source is simply changing the magnitude of the current supply. As can be seen, the alternating shielding gas transient pressure measurements are considerably different to Figure 2(a) produced by Kang et al [2]. Firstly, the alternating frequency of 2 Hz meant each gas was only supplied for 0.25 seconds before changing to the other gas, thus the entire time either gas is supplied is within the arc initiation pressure impulse and did not have sufficient time to reach steady-state.…”
Section: Resultsmentioning
confidence: 76%
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