Acta Metallurgica Sinica (English Letters) ›› 2021, Vol. 34 ›› Issue (11): 1511-1526.DOI: 10.1007/s40195-021-01260-y
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Hai-Feng Zhang1, Hai-Le Yan1(), Feng Fang2, Nan Jia1()
Received:
2021-02-25
Revised:
2021-04-06
Accepted:
2021-04-19
Online:
2021-06-10
Published:
2021-06-10
Contact:
Hai-Le Yan,Nan Jia
About author:
Nan Jia, jian@atm.neu.edu.cnHai-Feng Zhang, Hai-Le Yan, Feng Fang, Nan Jia. Orientation-Dependent Mechanical Responses and Plastic Deformation Mechanisms of FeMnCoCrNi High-entropy Alloy: A Molecular Dynamics Study[J]. Acta Metallurgica Sinica (English Letters), 2021, 34(11): 1511-1526.
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Orientation | X | Y | Z |
---|---|---|---|
Cube | [100] | [010] | [001] |
Rotated-cube | [001] | $[1\overline{1} 0]$ | $[110]$ |
Copper | $[11\overline{2} ]$ | $[\overline{1} 10]$ | [111] |
Brass-R | $[11\overline{1} ]$ | $[\overline{1} 10]$ | [112] |
\ | $[1\overline{5} 3]$ | $[30\overline{1} ]$ | [123] |
Table 1 Initial orientations of the different single crystals
Orientation | X | Y | Z |
---|---|---|---|
Cube | [100] | [010] | [001] |
Rotated-cube | [001] | $[1\overline{1} 0]$ | $[110]$ |
Copper | $[11\overline{2} ]$ | $[\overline{1} 10]$ | [111] |
Brass-R | $[11\overline{1} ]$ | $[\overline{1} 10]$ | [112] |
\ | $[1\overline{5} 3]$ | $[30\overline{1} ]$ | [123] |
Fig. 1 Stress-strain curves of the FeMnCoCrNi single crystals with different initial orientations at 300 K and a strain rate of 108/s under uniaxial tension
Fig. 2 Stress-strain curve of the FeMnCoCrNi single crystal with the [001] orientation. The inverse pole figure shows the initial orientation of the crystal. ‘a’-‘h’ are some key points at different deformation stages. a1-h1 are microstructures corresponding to ‘a’-‘h.’ In (a1)-(h1), ● and ● represent fcc and hcp structures, respectively. a2-h2 are dislocation line distributions corresponding to ‘a’-‘h.’ In (a2)-(h2), ? perfect, ? Shockley, ? stair-rod, ? Hirth, ? Frack, and ? other
Fig. 3 Stress-strain curve of the FeMnCoCrNi single crystal with the [110] orientation. The inverse pole figure shows the initial orientation of the crystal. ‘a’-‘h’ are some key points at different deformation stages. a1-h1 are microstructures corresponding to ‘a’-‘h.’ a2-h2 are dislocation line distributions corresponding to ‘a’-‘h’
Fig. 4 Stress-strain curve of the FeMnCoCrNi single crystal with the [111] orientation. The inverse pole figure shows the initial orientation of the crystal. ‘a’-‘f’ are some key points at different deformation stages. a1-f1 are microstructures corresponding to ‘a’-‘f.’ a2-f2 are dislocation line distributions corresponding to ‘a’-‘f’
Fig. 5 Stress-strain curve of the FeMnCoCrNi single crystal with the [112] orientation. The inverse pole figure shows the initial orientation of the crystal. ‘a’-‘g’ are some key points at different deformation stages. a1-g1 are microstructures corresponding to ‘a’-‘g.’ a2-g2 are dislocation line distributions corresponding to ‘a’-‘g’
Fig. 6 Stress-strain curve of the FeMnCoCrNi single crystal with the [123] orientation. The inverse pole figure shows the initial orientation of the crystal. ‘a’-‘g’ are some key points at different deformation stages. a1-g1 are microstructures corresponding to ‘a’-‘g.’ a2-g2 are dislocation line distributions corresponding to ‘a’-‘g’
Fig. 8 Volume fraction evolution of stacking faults, twin boundaries and hcp-martensite in the FeMnCoCrNi single crystals with different initial orientations. SF stacking fault; TWB twining boundary; HCP hcp-martensite
Fig. 10 Atomic structure and corresponding dislocation line distribution in FeMnCoCrNi, Fe50Ni50, and Cu single crystals with different initial orientations at a tensile strain of 0.5
Fig. 11 Volume fraction evolution of stacking faults, twin boundaries, and hcp-martensite in the FeMnCoCrNi, Fe50Ni50, and Cu single crystals with different initial orientations. SF stacking fault; TWB twining boundary; HCP hcp-martensite
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