2020
DOI: 10.1016/j.actamat.2019.11.055
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Dislocation-induced breakthrough of strength and ductility trade-off in a non-equiatomic high-entropy alloy

Abstract: In conventional metallic materials, strength and ductility are mutually exclusive, referred to as strengthductility trade-off. Here, we demonstrate an approach to improve the strength and ductility simultaneously by introducing micro-banding and the accumulation of a high density of dislocations in single-phase high-entropy alloys (HEAs). We prepare two compositions (Cr 10 Mn 50 Fe 20 Co 10 Ni 10 and Cr 10 Mn 10 Fe 60 Co 10 Ni 10 ) with distinctive different stacking fault energies (SFEs) as experimental mater… Show more

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Cited by 105 publications
(6 citation statements)
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“…Although the directionally solidified EHEA has a high content of hard, low-ductility B2 phase (~41 vol%) (15,22,23), it nonetheless exhibits a large uniform elongation of ~50%. Its elongation is comparable to that of widely studied, high-ductility, fully homogenized face-centered cubic high-entropy alloys (HEAs) (24)(25)(26)(27). The resulting strength-ductility combination, and especially the uniform ductility, in the directionally solidified EHEA outperforms that of any other as-cast eutectic and neareutectic HEAs (14,15,19,20,22,23,(28)(29)(30)(31)(32)(33) (Fig.…”
mentioning
confidence: 59%
“…Although the directionally solidified EHEA has a high content of hard, low-ductility B2 phase (~41 vol%) (15,22,23), it nonetheless exhibits a large uniform elongation of ~50%. Its elongation is comparable to that of widely studied, high-ductility, fully homogenized face-centered cubic high-entropy alloys (HEAs) (24)(25)(26)(27). The resulting strength-ductility combination, and especially the uniform ductility, in the directionally solidified EHEA outperforms that of any other as-cast eutectic and neareutectic HEAs (14,15,19,20,22,23,(28)(29)(30)(31)(32)(33) (Fig.…”
mentioning
confidence: 59%
“…A large number of dislocations in crystals are entangled with each other, which results in the obstruction of the mutual movement of materials and the improvement of the yield strength of materials. Bailey–Hirsch can be used to express the corresponding dislocation strengthening σ dis = M α G b ρ 1 / 2 where M is the Taylor factor of ≈3.06 [ 64 ] ; α is the material constant of the FCC metal (≈0.2 [ 65 ] ); G is the shear modulus of the CoFeNiMn system HEA (81 GPa) [ 66 ] ; and b is the Burgers vector (for FCC structure alloys, b = ( 2 / 2 ) a , where a is the lattice constant (based on the data in Table 4)); The dislocation density can be estimated by the following equation [ 67 ] ρ = 2 3 ε/ ( D b ) where ε is the lattice strain, D is the grain size, ρ is the dislocation density, b is the Burgers vector, and for the FCC structure, b = ( 2 /2) a , where a is the lattice parameter. The values of the various parameters mentioned previously, and the calculated values of dislocation density and lattice stress are summarized in Table 4.…”
Section: Resultsmentioning
confidence: 99%
“…where a is the lattice constant (based on the data in Table 4)); The dislocation density can be estimated by the following equation [67] ρ…”
Section: Strengthening Mechanismsmentioning
confidence: 99%
“…Carefully tuning these parameters enables control over the ductility. Point defects, dislocations and other microstructure effects will also affect the ductility of the system [33][34][35][36][37][38], but are out of the scope of this work.…”
Section: Discussionmentioning
confidence: 99%