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Materials Data on TiCr2 by Materials Project

TiCr2 is Cubic Laves structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Ti is bonded in a 12-coordinate geometry to four equivalent Ti and twelve equivalent Cr atoms. All Ti–Ti bond lengths are 2.97 Å. All Ti–Cr bond lengths are 2.85 Å. Cr is bonded to six equivalent Ti and six equivalent Cr atoms to form a mixture of edge, corner, and face-sharing CrTi6Cr6 cuboctahedra. All Cr–Cr bond lengths are 2.43 Å.

36 MATERIALS SCIENCE↗

Materials Data on TiCr2 by Materials Project

TiCr2 is Hexagonal Laves structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ti is bonded in a 12-coordinate geometry to four equivalent Ti and twelve Cr atoms. There are three shorter (2.97 Å) and one longer (2.98 Å) Ti–Ti bond lengths. There are three shorter (2.81 Å) and nine longer (2.86 Å) Ti–Cr bond lengths. There are two inequivalent Cr sites. In the first Cr site, Cr is bonded to six equivalent Ti and six equivalent Cr atoms to form a mixture of edge, corner, and face-sharing CrTi6Cr6 cuboctahedra. All Cr–Cr bond lengths are 2.44 Å. In the second Cr site, Cr is bonded to six equivalent Ti and six Cr atoms to form a mixture of edge, corner, and face-sharing CrTi6Cr6 cuboctahedra. There are two shorter (2.39 Å) and two longer (2.49 Å) Cr–Cr bond lengths.

36 MATERIALS SCIENCE↗

Materials Data on TiCr2 by Materials Project

TiCr2 is Hexagonal Laves-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are four inequivalent Ti sites. In the first Ti site, Ti is bonded in a 12-coordinate geometry to four Ti and twelve Cr atoms. There are one shorter (2.96 Å) and three longer (2.97 Å) Ti–Ti bond lengths. There are a spread of Ti–Cr bond distances ranging from 2.83–2.86 Å. In the second Ti site, Ti is bonded in a 12-coordinate geometry to four Ti and twelve Cr atoms. There are three shorter (2.97 Å) and one longer (2.98 Å) Ti–Ti bond lengths. There are three shorter (2.81 Å) and nine longer (2.85 Å) Ti–Cr bond lengths. In the third Ti site, Ti is bonded in a 12-coordinate geometry to four Ti and twelve Cr atoms. The Ti–Ti bond length is 2.96 Å. There are a spread of Ti–Cr bond distances ranging from 2.83–2.86 Å. In the fourth Ti site, Ti is bonded in a 12-coordinate geometry to four Ti and twelve Cr atoms. There are three shorter (2.97 Å) and one longer (2.98 Å) Ti–Ti bond lengths. There are three shorter (2.81 Å) and nine longer (2.85 Å) Ti–Cr bond lengths. There are three inequivalent Cr sites. In the first Cr site, Cr is bonded to six Ti and six Cr atoms to form a mixture of edge, face, and corner-sharing CrTi6Cr6 cuboctahedra. There are two shorter (2.41 Å) and four longer (2.43 Å) Cr–Cr bond lengths. In the second Cr site, Cr is bonded to six Ti and six Cr atoms to form a mixture of edge, face, and corner-sharing CrTi6Cr6 cuboctahedra. There are a spread of Cr–Cr bond distances ranging from 2.38–2.48 Å. In the third Cr site, Cr is bonded to six Ti and six Cr atoms to form a mixture of edge, face, and corner-sharing CrTi6Cr6 cuboctahedra.

36 MATERIALS SCIENCE↗

Design of novel refractory equiatomic multi-principal elemental alloys based on Mo-Nb-Ti system for Gen IV reactor applications

Excellent irradiation damage resistance demonstrated by multi-principal elemental alloys (MPEAs) has sparked significant interest among researchers, prompting exploration into their vast compositional space, to validate their suitability for nuclear applications. A combined approach of thermodynamic and empirical parameters calculations alongside CALPHAD (CALculation of PHAse Diagrams) for phase formation predictions enable high-throughput material selection for sophisticated applications like nuclear, overcoming laborious and time-consuming experiments. Key thermodynamic and empirical parameters for eight novel equiatomic MPEAs, based on seven low thermal neutron cross section refractory elements, for predicting phase formation were calculated, and equilibrium and non-equilibrium simulations in CALPHAD were employed to comprehensively model the systems. Pseudo binary phase diagram simulations showed that Zr, V or equiatomic CrV additions to the base MoNbTi alloy (MoNbTi-Zr, MoNbTi-V and MoNbTi-CrV alloys) favor the formation of isomorphous body-centered cubic (BCC) phase at high temperatures, while Cr, Al, equiatomic ZrV, or equiatomic CrAl additions (MoNbTi-Cr, MoNbTi-Al, MoNbTi-ZrV or MoNbTi-CrAl alloys) limit the solubility of them. Equilibrium CALPHAD simulations at 750 oC were consistent with XRD results on MoNbTi, MoNbTiZr and MoNbTiCr alloys, and partially for others. Notably, elemental segregation observed in the backscattered electron (BSE) scanning electron microscopy (SEM) images of the alloys was accurately simulated through non-equilibrium Scheil solidification calculations in CALPHAD, further verified by experiments. The precipitation of TiCr2 Laves phase in Cr containing MoNbTiCr and MoNbTiCrAl was accurately predicted while discrepancies were noted in MoNbTiCrV. The equilibrium simulations also provided insights into phase compositions at specific temperatures offering a pathway for tailoring the desired microstructure and properties of these systems. Empirical parameters calculations successfully predicted random solid solution in the base MoNbTi alloy, and with an exception in MoNbTiV and MoNbTiAl, predicted intermetallic precipitation in the rest, especially, Laves phase precipitation in Cr containing alloys.

36 - MATERIALS SCIENCE↗