Mechanism of the Fe3(B, C) and Fe23(C, B)6 solid-state transformation in the hypoeutectic region of the Fe-C-B system. (15th October 2016)

• Record Type: Journal Article
• Authors: Lentz, Jonathan; Röttger, Arne; Theisen, Werner
• Is Part Of: Acta materialia. Volume 119(2016)
• Page Start: 80
• Page End: 91
• Publication Date: 2016-10-15
• Subjects: Fe-C-B -- Ternary alloys -- Boron -- Steel -- Solid state phase transformation; Materials -- Periodicals; Materials science -- Periodicals; Materials -- Mechanical properties -- Periodicals; Metallurgy -- Periodicals; Chemistry, Inorganic -- Periodicals; 620.112
• DOI: 10.1016/j.actamat.2016.08.009
• Languages: English
• ISSNs: 1359-6454

Abstract

Abstract: This study investigates the microstructural mechanisms involved in the solid-state transformation of the Fe3 (B, C) → Fe23 (C, B)6 phases in the hypoeutectic region of the iron-carbon-boron (Fe-C-B) system. We analyzed the influence of different initial microstructural characteristics on the Fe3 (B, C) → Fe23 (C, B)6 transformation with regards to the matrix phase, matrix C content, B/(C + B) ratio, and agglomeration of the parental Fe3 (B, C) phase. We performed thermodynamic calculations using the CALPHAD method, validated by laboratory melts with varying B/(B + C) ratios. These laboratory melts were then microstructurally characterized by means of X-ray diffraction (XRD), scanning electron microscopy (SEM), electron backscatter diffraction (EBSD), and wavelength-dispersive X-ray spectroscopy (WDS). We particularly focused on solid-state transformation of borides and carboborides of type M3 (C, B) and M23 (C, B)6 in the hypoeutectic region of the ternary system Fe-C-B, investigated via both in situ and ex situ XRD measurements. It was found that the solid-state transformations are influenced by enriched B inside the eutectic structure, a result of solidification. This increased B content is not reduced in solid state due to the kinetic limitations of B and C inside the hard-phase structure. Thus phase stability is subject to local equilibria depending on the local C and B concentration of the hard-phase structure. In this process the Fe23 (C, B)6 phase also forms a shell-like structure surrounding the Fe3 (B, C) and Fe2 B phases. Graphical abstract: