Heterogeneous precipitation behavior and stacking-fault-mediated deformation in a CoCrNi-based medium-entropy alloy

Abstract Combining high strength and good ductility is highly-desired yet challenging for conventional structural materials. Newly emerging concentrated multi-component alloys with face-centered-cubic structure provide an ultra-ductile matrix, and the precipitation hardening based on these alloys provides a very effective way to achieve a superior strength-ductility combination. Here, we report a high-strength CoCrNi-based medium-entropy alloy hardened by nanoscale L1 2 -(Ni, Co, Cr) 3 (Ti, Al)-type particles with mixing heterogeneous and homogeneous precipitation behaviors. Compared to the single-phase CoCrNi medium-entropy alloy, the yield strength and the tensile strength of the precipitation-strengthened CoCrNi medium-entropy alloy were increased by ∼70% to ∼750 MPa and ∼44% to ∼1.3 GPa, respectively, whereas a good ductility, ∼45%, was still achieved. The underlying deformation micro-mechanisms were systematically investigated using transmission electron microscope. In the single-phase CoCrNi medium-entropy alloy, the deformation mode was dominated by mechanical twinning. In the precipitation-hardened medium-entropy alloy, however, a high density of stacking faults prevailed. We revealed that the absence of mechanical twinning in this low stacking fault energy precipitation-strengthened medium-entropy alloy could relate to the increasing critical twinning stress affected by the channel width of the matrix. We further calculated that the increment of the yield strength was substantially from precipitation strengthening. Our present findings provide not only a fundamental understanding of the deformation micro-mechanism of the precipitation-strengthened CoCrNi medium-entropy alloy but also a useful guidance for the development of precipitation-hardened concentrated multi-component alloys in the future.

[1]  K. An,et al.  A precipitation-hardened high-entropy alloy with outstanding tensile properties , 2016 .

[2]  David B. Williams,et al.  Grain boundary discontinuous precipitation reactions , 1981 .

[3]  J. Silcock,et al.  Strengthening Mechanisms in γ′ Precipitating Alloys , 1970 .

[4]  D. Dye,et al.  The effect of grain size on the twin initiation stress in a TWIP steel , 2015 .

[5]  Bin Liu,et al.  Ductile CoCrFeNiMox high entropy alloys strengthened by hard intermetallic phases , 2016 .

[6]  D. Lloyd,et al.  Yielding behaviour of γ′- precipitation-strengthened Co–Ni–Cr superalloys , 1976 .

[7]  G. Chin,et al.  The interaction of twins with existing substructure and twins in cobalt-iron alloys , 1974 .

[8]  Jian Lu,et al.  Phase stability and tensile properties of Co-free Al0.5CrCuFeNi2 high-entropy alloys , 2014 .

[9]  J. K. Lee,et al.  Deformation twinning in h.c.p. metals and alloys , 1991 .

[10]  Xiaoxia Huang,et al.  Superalloys: Alloying and Performance , 2010 .

[11]  E. George,et al.  Reasons for the superior mechanical properties of medium-entropy CrCoNi compared to high-entropy CrMnFeCoNi , 2017 .

[12]  D. Schryvers,et al.  On the mechanism of twin formation in Fe–Mn–C TWIP steels , 2010 .

[13]  G. Purdy,et al.  Discontinuous precipitation in CuCo alloys , 1981 .

[14]  J. Venables Deformation twinning in face-centred cubic metals , 1961 .

[15]  N. Jones,et al.  High-entropy alloys: a critical assessment of their founding principles and future prospects , 2016 .

[16]  Bernd Gludovatz,et al.  Exceptional damage-tolerance of a medium-entropy alloy CrCoNi at cryogenic temperatures , 2016, Nature Communications.

[17]  Jian Lu,et al.  High-entropy alloy: challenges and prospects , 2016 .

[18]  R. Scattergood,et al.  Effect of stacking fault energy on mechanical behavior of bulk nanocrystalline Cu and Cu alloys , 2011 .

[19]  K. N. Braszczyńska-Malik,et al.  Discontinuous and continuous precipitation in magnesium–aluminium type alloys , 2009 .

[20]  L. Rayleigh On The Instability Of Jets , 1878 .

[21]  Zijiao Zhang,et al.  Dislocation mechanisms and 3D twin architectures generate exceptional strength-ductility-toughness combination in CrCoNi medium-entropy alloy , 2017, Nature Communications.

[22]  J. Cahoon,et al.  The determination of yield strength from hardness measurements , 1971, Metallurgical Transactions.

[23]  W. J. Weber,et al.  Pressure-induced fcc to hcp phase transition in Ni-based high entropy solid solution alloys , 2017 .

[24]  Srikumar Banerjee,et al.  Deformation behaviour of γ″ strengthened inconel 718 , 1988 .

[25]  J. Weertman,et al.  A dislocation model for twinning in f.c.c. metals , 1963 .

[26]  C. Liu,et al.  The origin of negative stacking fault energies and nano-twin formation in face-centered cubic high entropy alloys , 2017 .

[27]  M. Azzaz,et al.  Plastic deformation, extended stacking faults and deformation twinning in single crystalline indium phosphide. 2. S doped InP , 1994 .

[28]  A. Ardell,et al.  Precipitation hardening of Ni-12.19 at.% Al alloy single crystals , 1975 .

[29]  A. Argon,et al.  Creep resistance of CMSX-3 nickel base superalloy single crystals , 1992 .

[30]  R. Reed The Superalloys: Fundamentals and Applications , 2006 .

[31]  A. Heuer,et al.  Nucleation and growth of deformation twins: A perspective based on the double-cross-slip mechanism of deformation twinning , 2002 .

[32]  K. Du,et al.  Deformation mechanisms in a Co-rich nickel based superalloy with different size of γ׳ precipitates , 2015 .

[33]  J. Yeh,et al.  Effect of the aluminium content of AlxCrFe1.5MnNi0.5 high-entropy alloys on the corrosion behaviour in aqueous environments , 2008 .

[34]  L. Höglund,et al.  Thermo-Calc & DICTRA, computational tools for materials science , 2002 .

[35]  Tresa M. Pollock,et al.  Strengthening Mechanisms in Polycrystalline Multimodal Nickel-Base Superalloys , 2009 .

[36]  C. Tasan,et al.  Phase stability of non-equiatomic CoCrFeMnNi high entropy alloys , 2015 .

[37]  G. Eggeler,et al.  Microstructure evolution and critical stress for twinning in the CrMnFeCoNi high-entropy alloy , 2016 .

[38]  Abhik Choudhury,et al.  Phase field modelling of rayleigh instabilities in the solid-state , 2016 .

[39]  R. Ritchie,et al.  A fracture-resistant high-entropy alloy for cryogenic applications , 2014, Science.

[40]  G. Pharr,et al.  Temperature dependence of the mechanical properties of equiatomic solid solution alloys with face-centered cubic crystal structures , 2014 .

[41]  Kyung-Tae Park,et al.  Stacking fault energy and plastic deformation of fully austenitic high manganese steels: Effect of Al addition , 2010 .

[42]  D. Miracle,et al.  A critical review of high entropy alloys and related concepts , 2016 .

[43]  D. A. Hughes,et al.  Microstructural evolution in a non-cell forming metal: AlMg , 1993 .

[44]  H. Van Swygenhoven,et al.  Stacking fault energies and slip in nanocrystalline metals , 2004, Nature materials.

[45]  I. M. Robertson,et al.  Enhancing radiation tolerance by controlling defect mobility and migration pathways in multicomponent single-phase alloys , 2016, Nature Communications.

[46]  C. Tasan,et al.  Metastable high-entropy dual-phase alloys overcome the strength–ductility trade-off , 2016, Nature.

[47]  H. Karnthaler,et al.  On the origin of planar slip in f.c.c. alloys , 1989 .

[48]  John C. Horwath,et al.  Absence of long-range chemical ordering in equimolar FeCoCrNi , 2012 .

[49]  V. Kuokkala,et al.  Dependence of tensile deformation behavior of TWIP steels on stacking fault energy, temperature and strain rate , 2010 .

[50]  J. Venables On dislocation pole models for twinning , 1974 .