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DFT investigation of carbon-expanded α phase with different alloying element

  • T. Y. Song
  • , R. L. Liu*
  • , L. Z. Li
  • , C. X. Bian
  • , M. F. Yan
  • *Corresponding author for this work
  • College of Materials Science and Chemical Engineering, Harbin Engineering University
  • Harbin Institute of Technology

Research output: Contribution to journalArticlepeer-review

Abstract

The structures of carbon-expanded α phase (αC) phase were modeled with nominal molecular formula of Fe13-xCr3NixCy (x = 0, 1, y = 0,1,2,3,4) based on body-centered cubic α-Fe and calculated by first-principles calculation using density functional theory (DFT). The results show that Fe13Cr3Cy (y = 0,1,2,3,4) structures with less than 11.11 at% carbon (y = 2) can be easily formed and exist stable. The Young's moduli of stable Fe13Cr3, Fe13Cr3C, and Fe13Cr3C2 are 227.08 GPa, 209.71 GPa and 189.19 GPa, respectively. The theoretical hardness of stable Fe13Cr3Cy (y = 1, 2) are obviously improved and can be up to 8.26 GPa. As for Fe12Cr3NiCy (y = 0,1,2), Young’ s moduli of Fe12Cr3Ni, Fe12Cr3NiC, and Fe12Cr3NiC2 are 155.82 GPa, 258.24 GPa and 207.44 GPa, respectively. The hardness of Fe12Cr3NiCy (y = 1,2) can be as high as 17.88 GPa. Ni element can stabilize the structures of Fe13Cr3Cy (y = 1,2) and improve their theoretical hardnesses. The toughness of Fe13Cr3Cy (y = 1,2) structures are shown in ductility based on Pugh's ratio criterion, while the Fe12Cr3NiCy (y = 1,2) structures are shown in brittleness. Electronic structure calculation shown that there are mixture bonding of metal bonding, covalent bonding, and ionic bonding in Fe13-xCr3NixCy (x = 0,1, y = 1,2) structures, which should account for the high hardness of the structure for αC phase.

Original languageEnglish
Article number111199
JournalVacuum
Volume202
DOIs
StatePublished - Aug 2022
Externally publishedYes

Keywords

  • Carbon-expanded α phase
  • Electronic structure
  • First-principles calculation
  • Low-temperature carburizing
  • Mechanical property

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