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A numerical model for simulating the effect of strain rate on eutectic band thickness
University West, 46132, Trollhättan, Sweden.ORCID iD: 0000-0002-2197-6243
Luleå University of Technology, Department of Engineering Sciences and Mathematics, Mechanics of Solid Materials.ORCID iD: 0000-0002-3514-9441
Luleå University of Technology, Department of Engineering Sciences and Mathematics, Mechanics of Solid Materials.ORCID iD: 0000-0002-7298-020x
Luleå University of Technology, Department of Engineering Sciences and Mathematics, Mechanics of Solid Materials.ORCID iD: 0000-0002-2544-9168
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2020 (English)In: Welding in the World, ISSN 0043-2288, E-ISSN 1878-6669, Vol. 64, no 10, p. 1635-1658Article in journal (Refereed) Published
Abstract [en]

Large tensile strains acting on the solidifying weld metal can cause the formation of eutectic bands along grain boundaries. These eutectic bands can lead to severe liquation in the partially melted zone of a subsequent overlapping weld. This can increase the risk of heat-affected zone liquation cracking. In this paper, we present a solidification model for modeling eutectic bands. The model is based on solute convection in grain boundary liquid films induced by tensile strains. The proposed model was used to study the influence of strain rate on the thickness of eutectic bands in Alloy 718. It was found that when the magnitude of the strain rate is 10 times larger than that of the solidification rate, the calculated eutectic band thickness is about 200 to 500% larger (depending on the solidification rate) as compared to when the strain rate is zero. In the paper, we also discuss how eutectic bands may form from hot cracks.

Place, publisher, year, edition, pages
Springer, 2020. Vol. 64, no 10, p. 1635-1658
Keywords [en]
Macrosegregation, Solidification, Hot cracking, Alloy 718
National Category
Applied Mechanics
Research subject
Solid Mechanics
Identifiers
URN: urn:nbn:se:ltu:diva-76423DOI: 10.1007/s40194-020-00918-yISI: 000540687300001Scopus ID: 2-s2.0-85086930636OAI: oai:DiVA.org:ltu-76423DiVA, id: diva2:1361942
Note

Validerad;2020;Nivå 2;2020-09-21 (johcin)

Available from: 2019-10-17 Created: 2019-10-17 Last updated: 2023-09-05Bibliographically approved
In thesis
1. Modeling and Simulation of Weld Hot Cracking
Open this publication in new window or tab >>Modeling and Simulation of Weld Hot Cracking
2019 (English)Doctoral thesis, comprehensive summary (Other academic)
Abstract [en]

Several alloy systems are susceptible to weld hot cracking. Weld hot cracking occurs by fracture of liquid films, normally grain boundary liquid films, at the late stage of the solidification of the weld. The cracks can be small and therefore difficult to detect by nondestructive test methods. If hot cracks are not repaired, they can act as sites for initiation of fatigue and stress corrosion cracking, which in turn can lead to catastrophic failure in critical applications such as aerospace engines and nuclear power plants. Therefore, it is of highest importance to design weld processes so that hot cracking can be avoided. Here, numerical simulation can be a powerful tool for optimizing weld speed, heat input, weld path geometry, weld path sequences, weld fixturing, etc., such that the risk for hot cracking can be minimized. In this thesis, we propose a modeling approach for simulating weld hot cracking in sheet metals with low welding speeds and fully penetrating welds. These conditions are assumed to give rise to isolated grain boundary liquid films (GBLFs) whose crack susceptibility can be analyzed using one-dimensional models. The work is divided into four journal papers. The three first papers treat hot cracking that occurs in the fusion zone of the weld while the last paper treats hot cracking in the partially melted zone of the weld. The main content of the four papers are summarized below. In paper A, a pore-based crack criterion for hot cracking has been developed. This criterion states that cracking occurs in a GBLF if the liquid pressure in the film goes below a fracture pressure. The fracture pressure is determined from a pore model as the liquid pressure that is required to balance the surface tension of an axisymmetric pore in a liquid film located between two parallel plates at a given critical pore radius. The fracture pressure depends on the surface tension, the spacing between the parallel plates and the gas concentration in the liquid. In order to evaluate the above pore-based crack criterion in a GBLF the liquid pressure in the film most be known. In paper B, a one-dimensional GBLF pressure model for a columnar dendritic microstructure has been developed. This model is based on a combination of Poiseuille parallel plate flow and Darcy porous flow. Flow induced by mechanical straining of the GBLF is accounted for by a macroscopic mechanical strain field that is localized to the GBLF by a temperature dependent length scale. In paper C, a computational welding mechanics model for a Varestraint test is developed. The model is used to calibrate the crack criterion in paper A and the pressure model in paper B. It is then used to test the crack criterion in Varestraint tests with different augmented strains. Calculated crack locations, orientations, and widths are shown to correlate well to the experimental Varestraint tests. vii Finally, in paper D, a segregation model for predicting the thickness of eutectic bands has been developed. The thickness of eutectic bands affects the degree of liquation in partially melted zone, and therefore is an important factor for hot cracking in this region of the weld.

Place, publisher, year, edition, pages
Luleå: Luleå tekniska universitet, 2019
Series
Doctoral thesis / Luleå University of Technology 1 jan 1997 → …, ISSN 1402-1544
National Category
Manufacturing, Surface and Joining Technology
Research subject
Material Mechanics
Identifiers
urn:nbn:se:ltu:diva-76425 (URN)978-91-7790-476-2 (ISBN)978-91-7790-477-9 (ISBN)
Public defence
2019-12-12, E246, Luleå, 09:00 (English)
Opponent
Supervisors
Available from: 2019-10-17 Created: 2019-10-17 Last updated: 2023-09-05Bibliographically approved

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Draxler, JoarÅkerström, PaulEdberg, JonasLindgren, Lars-Erik

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