4.5 Article

Modelling the creation and destruction of columnar and equiaxed zones during solidification and melting in multi-pass welding of steel

期刊

COMPUTATIONAL MATERIALS SCIENCE
卷 97, 期 -, 页码 285-294

出版社

ELSEVIER SCIENCE BV
DOI: 10.1016/j.commatsci.2014.09.022

关键词

Computer simulation; Dendritic growth; Columnar and equiaxed grains; Columnar to equiaxed transition; Remelting in welding

资金

  1. European Commission [NMP3-SL-2009-229108]

向作者/读者索取更多资源

The authors present a novel meso-scale (mm-cm) numerical model of multi-pass welding of stainless steel based on the front tracking formulation. During a typical multi-pass notched butt weld, multiple cycles of melting and solidification occur throughout the weld pool, where previously solidified equiaxed zones are destroyed by melting and subsequently resolidify in columnar form. These thermal cycles result from the thermal effects of the current deposition of liquid filler metal being superimposed onto those of the previous pass. The advancement of the liquidus isotherm is employed to characterize melting, while both columnar and equiaxed dendritic growth in the undercooled melt are considered in the model of solidification. Columnar solidification is simulated using a front tracking method where computational markers are employed to explicitly define the advancing columnar front. Competing equiaxed solidification is modelled using a volume averaging approach. During the first and second welding passes of a case study, the weld pool solidifies as purely columnar. This is due to the high thermal gradient present in the weld pool, which results in a very small region of undercooled liquid ahead of the columnar front and subsequently low levels of equiaxed grain nucleation/growth. Towards the end of the third and final pass the equiaxed grains have sufficient dwell time in the undercooled liquid to form a coherent network and present a physical barrier to the advancing columnar front. A Columnar to Equiaxed Transition (CET) occurs and the remainder of the weld pool solidifies in a fully equiaxed microstructure. The results are compared with Hunt's analytical model of CET and the agreement is reasonably good. The occurrence of CET throughout the weld pool is directly predicted via this front tracking model without the need to rely on estimated thermal gradients and solidification rates. Further simulations indicate that CET can be promoted, even in early passes, by increasing the grain refiner level and/or by pre-heating the parent metal. (C) 2014 Elsevier B.V. All rights reserved.

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