TY - JOUR
T1 - Phase evolution of highly immiscible alloys under shear deformation
T2 - Kinetic pathways, steady states, and the lever-rule
AU - Ashkenazy, Yinon
AU - Pant, Nirab
AU - Zhou, Jian
AU - Bellon, Pascal
AU - Averback, Robert S.
N1 - Publisher Copyright:
© 2017 Acta Materialia Inc.
PY - 2017/10/15
Y1 - 2017/10/15
N2 - Phase evolution of dilute, highly immiscible, Cu alloys (Cu-Nb, Cu-V, and Cu-Ta) during low-temperature severe plastic deformation was investigated using large-scale molecular dynamics simulations. At low solute concentrations, each system maintained a FCC structure in steady state, but as the concentration was increased above a saturation limit (0.3 at.% for Ta, 1 at.% for Nb and 5 at.% for V), the system became two-phase, comprising co-existing FCC and amorphous phases. Unlike Cu-Nb and Cu-V, the amorphous phase in the Cu-Ta system showed strong solute partitioning. Increasing the solute concentration above a second phase boundary (8 at.% V, 9 at.% Nb, and 24 at.% Ta) led to complete amorphization. Throughout the two-phase region, the compositions of the FCC and amorphous phases remained nearly constant, thus following the lever rule. Initiating the systems either as a FCC homogeneous alloy, or with a BCC sphere embedded in a Cu matrix, had no effect on the steady state microstructure, implying uniqueness of the steady state under low-temperature shear deformation. Lastly, chemical order and phase partitioning in the amorphous Cu-Ta system under low-temperature shear is found remarkably similar to that in the equilibrium structure above the melting temperature.
AB - Phase evolution of dilute, highly immiscible, Cu alloys (Cu-Nb, Cu-V, and Cu-Ta) during low-temperature severe plastic deformation was investigated using large-scale molecular dynamics simulations. At low solute concentrations, each system maintained a FCC structure in steady state, but as the concentration was increased above a saturation limit (0.3 at.% for Ta, 1 at.% for Nb and 5 at.% for V), the system became two-phase, comprising co-existing FCC and amorphous phases. Unlike Cu-Nb and Cu-V, the amorphous phase in the Cu-Ta system showed strong solute partitioning. Increasing the solute concentration above a second phase boundary (8 at.% V, 9 at.% Nb, and 24 at.% Ta) led to complete amorphization. Throughout the two-phase region, the compositions of the FCC and amorphous phases remained nearly constant, thus following the lever rule. Initiating the systems either as a FCC homogeneous alloy, or with a BCC sphere embedded in a Cu matrix, had no effect on the steady state microstructure, implying uniqueness of the steady state under low-temperature shear deformation. Lastly, chemical order and phase partitioning in the amorphous Cu-Ta system under low-temperature shear is found remarkably similar to that in the equilibrium structure above the melting temperature.
KW - Amorphous alloy
KW - Dynamic steady state
KW - Mechanical alloying
KW - Severe plastic deformation
KW - Simulation
UR - http://www.scopus.com/inward/record.url?scp=85028400033&partnerID=8YFLogxK
U2 - 10.1016/j.actamat.2017.08.014
DO - 10.1016/j.actamat.2017.08.014
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:85028400033
SN - 1359-6454
VL - 139
SP - 205
EP - 214
JO - Acta Materialia
JF - Acta Materialia
ER -