{"title":"Integrated thermokinetics and thermomechanics dependent pathways for evolution of cracks in laser additively fabricated tungsten","authors":"Rohit Randhavan , Krishna Kamlesh Verma , K.V. Mani Krishna , Shashank Sharma , Narendra B. Dahotre","doi":"10.1016/j.ijrmhm.2025.107366","DOIUrl":null,"url":null,"abstract":"<div><div>Cracking remains a critical challenge in the Laser Powder Bed Fusion (LPBF) of Tungsten (W) due to its inherent brittleness and the extreme thermal gradients involved in the process. While prior research has explored thermomechanical modeling and experimental observation of cracking in LPBF-processed W, a comprehensive correlation between track-by-track crack evolution and the underlying thermokinetic and thermomechanical phenomena is lacking. This study bridges this gap by integrating thermomechanical simulations with detailed microstructural examinations to systematically characterize crack morphology and behavior in multiscale (single- and multi-track) LPBF experiments. Samples were fabricated using input laser fluences of 10 J/mm<sup>2</sup>, 15 J/mm<sup>2</sup>, and 22.5 J/mm<sup>2</sup> to evaluate the influence of the process parameters (power, beam diameter, and scanning speed) on crack formation. Microstructural analysis revealed input laser fluence-dependent crack densities and morphologies. Samples produced at 10 J/mm<sup>2</sup> exhibited extensive cracking (60–65 mm/mm<sup>2</sup> for single-track, 10–12 mm/mm<sup>2</sup> for multi-track) with transverse cracks and a dense microcrack network. Increasing input laser fluence to 15 J/mm<sup>2</sup> reduced microcrack density, while input laser fluence of 22.5 J/mm<sup>2</sup> resulted in a shift to a single longitudinal crack (14–16 mm/mm<sup>2</sup> for single-track, 3–4 mm/mm<sup>2</sup> for multi-track), similar to welding-induced cracks. Track-by-track analysis of thermokinetic and thermomechanical evolution during multiscale LPBF processing coupled with crack evolution is discussed for these varying process parameters. This integrated approach provides a unique physics-based understanding of crack evolution mechanisms in LPBF-processed W, highlighting the critical role of input laser fluence in managing thermal stresses, dictating crack morphology, and offering a pathway for optimized process control.</div></div>","PeriodicalId":14216,"journal":{"name":"International Journal of Refractory Metals & Hard Materials","volume":"133 ","pages":"Article 107366"},"PeriodicalIF":4.6000,"publicationDate":"2025-08-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Refractory Metals & Hard Materials","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0263436825003312","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Cracking remains a critical challenge in the Laser Powder Bed Fusion (LPBF) of Tungsten (W) due to its inherent brittleness and the extreme thermal gradients involved in the process. While prior research has explored thermomechanical modeling and experimental observation of cracking in LPBF-processed W, a comprehensive correlation between track-by-track crack evolution and the underlying thermokinetic and thermomechanical phenomena is lacking. This study bridges this gap by integrating thermomechanical simulations with detailed microstructural examinations to systematically characterize crack morphology and behavior in multiscale (single- and multi-track) LPBF experiments. Samples were fabricated using input laser fluences of 10 J/mm2, 15 J/mm2, and 22.5 J/mm2 to evaluate the influence of the process parameters (power, beam diameter, and scanning speed) on crack formation. Microstructural analysis revealed input laser fluence-dependent crack densities and morphologies. Samples produced at 10 J/mm2 exhibited extensive cracking (60–65 mm/mm2 for single-track, 10–12 mm/mm2 for multi-track) with transverse cracks and a dense microcrack network. Increasing input laser fluence to 15 J/mm2 reduced microcrack density, while input laser fluence of 22.5 J/mm2 resulted in a shift to a single longitudinal crack (14–16 mm/mm2 for single-track, 3–4 mm/mm2 for multi-track), similar to welding-induced cracks. Track-by-track analysis of thermokinetic and thermomechanical evolution during multiscale LPBF processing coupled with crack evolution is discussed for these varying process parameters. This integrated approach provides a unique physics-based understanding of crack evolution mechanisms in LPBF-processed W, highlighting the critical role of input laser fluence in managing thermal stresses, dictating crack morphology, and offering a pathway for optimized process control.
期刊介绍:
The International Journal of Refractory Metals and Hard Materials (IJRMHM) publishes original research articles concerned with all aspects of refractory metals and hard materials. Refractory metals are defined as metals with melting points higher than 1800 °C. These are tungsten, molybdenum, chromium, tantalum, niobium, hafnium, and rhenium, as well as many compounds and alloys based thereupon. Hard materials that are included in the scope of this journal are defined as materials with hardness values higher than 1000 kg/mm2, primarily intended for applications as manufacturing tools or wear resistant components in mechanical systems. Thus they encompass carbides, nitrides and borides of metals, and related compounds. A special focus of this journal is put on the family of hardmetals, which is also known as cemented tungsten carbide, and cermets which are based on titanium carbide and carbonitrides with or without a metal binder. Ceramics and superhard materials including diamond and cubic boron nitride may also be accepted provided the subject material is presented as hard materials as defined above.