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Numerical Simulation of the Behavior of Hydrogen Source in a Novel Welding Process to Reduce Diffusible Hydrogen.

作者信息

Tashiro Shinichi, Mukai Naoki, Inoue Yoshihide, Murphy Anthony B, Suga Tetsuo, Tanaka Manabu

机构信息

Joining and Welding Research Institute, Osaka University, Osaka 5670047, Japan.

Kobe Steel, Ltd., Kanagawa 251-8551, Japan.

出版信息

Materials (Basel). 2020 Apr 1;13(7):1619. doi: 10.3390/ma13071619.

DOI:10.3390/ma13071619
PMID:32244709
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7178352/
Abstract

This study aims to reduce the diffusible hydrogen content in deposited metal during gas metal arc welding (GMAW) and flux-cored arc welding (FCAW) which induces cold cracking. To achieve this, a novel welding torch with a dual gas nozzle has been developed. This special welding torch decreases the hydrogen source gas evaporated from a welding wire by the suction from the inner gas nozzle. In order to improve the suction efficiency of this evaporated gas, precise control of the suction gas flow is indispensable. In this paper, a simplified numerical simulation model of this process has been described. This model can take account of the evaporation of the hydrogen source gas from the wire while simulating the behavior of the shielding gas and the arc. Using this model, the effect of suction nozzle structure and torch operating conditions on suction gas flow pattern and suction efficiency was also investigated to understand the process mechanism. Furthermore, the diffusible hydrogen content in deposited metal was measured by chromatography as a validation step. Results show that some of the shielding gas introduced from a shielding nozzle was drawn inward and also branched into an upward flow that was sucked into the suction nozzle and a downward flow to a base metal. This branching height was defined as the suction limit height, which decisively governed the suction efficiency. As a result, in order to reduce the diffusible hydrogen, it was suggested that the suction limit height should be controlled towards below the wire position, where the evaporation rate of the hydrogen source gas peaks through optimization of the suction nozzle design and the torch operating conditions.

摘要
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/d39389a103fd/materials-13-01619-g017.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/e78373b2a977/materials-13-01619-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/5e90fde9325a/materials-13-01619-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/16a39499e1e2/materials-13-01619-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/50b66d3ba0c3/materials-13-01619-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/c18883a93e9a/materials-13-01619-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/d3bbc073ffc0/materials-13-01619-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/9e2957bf9331/materials-13-01619-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/1204447789de/materials-13-01619-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/3089d1738f25/materials-13-01619-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/3a8cc6e14ad3/materials-13-01619-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/7ed4c4e2c657/materials-13-01619-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/8ceb588b58f9/materials-13-01619-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/54f3a85b9f2a/materials-13-01619-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/660f07f0a767/materials-13-01619-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/436791c88d43/materials-13-01619-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/e4cbacdaa391/materials-13-01619-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/d39389a103fd/materials-13-01619-g017.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/e78373b2a977/materials-13-01619-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/5e90fde9325a/materials-13-01619-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/16a39499e1e2/materials-13-01619-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/50b66d3ba0c3/materials-13-01619-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/c18883a93e9a/materials-13-01619-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/d3bbc073ffc0/materials-13-01619-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/9e2957bf9331/materials-13-01619-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/1204447789de/materials-13-01619-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/3089d1738f25/materials-13-01619-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/3a8cc6e14ad3/materials-13-01619-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/7ed4c4e2c657/materials-13-01619-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/8ceb588b58f9/materials-13-01619-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/54f3a85b9f2a/materials-13-01619-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/660f07f0a767/materials-13-01619-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/436791c88d43/materials-13-01619-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/e4cbacdaa391/materials-13-01619-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/66e0/7178352/d39389a103fd/materials-13-01619-g017.jpg

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