TY - JOUR
T1 - High strain rate compression behavior of a heavily stabilized beta titanium alloy
T2 - Kink deformation and adiabatic shearing
AU - Zheng, Youping
AU - Zeng, Weidong
AU - Wang, Yubo
AU - Zhou, Dadi
AU - Gao, Xiongxiong
N1 - Publisher Copyright:
© 2017 Elsevier B.V.
PY - 2017
Y1 - 2017
N2 - High strain rate compression deformations at 5 × 103s−1 of Ti-35V-15Cr-0.3Si-0.1C beta titanium alloy were conducted at variant temperatures from 20 °C to 800 °C on split-Hopkinson pressure bar system. It is found that the dynamic stress-strain curves at such a high strain rate contain hardening stages and softening stages. Different stages suggest different deformation mechanisms. In the hardening stages, kink deformation is uncommonly observed. The formation of kink bands is found to be responsible for the hardening effect. Adiabatic shearing began with the stress drops in the softening stages. From then on, the deformations localized in narrow regions, where adiabatic shearing bands (ASBs) formed at last. Dynamic recrystallization (DRX) occurred in the ASBs. The ultra-fine recrystallization grains with grain size of 0.28 μm, 0.35 μm, and 4.5 μm are observed in the ASBs formed at 400 °C, 600 °C and 800 °C respectively. It is really hard so far to measure the true shear strains and the true temperatures in the ASBs. In order to estimate the true shear strains in the ASBs, an original method basing on the definition of shear strain is proposed in this paper. Then a modified equation using the true shear strain rather than the empirical factor is employed to estimate the true temperatures in the ASBs. On such a base, the DRX in present ASBs is well explained in kinetics via the rotational dynamic recrystallization (RDR) mechanism.
AB - High strain rate compression deformations at 5 × 103s−1 of Ti-35V-15Cr-0.3Si-0.1C beta titanium alloy were conducted at variant temperatures from 20 °C to 800 °C on split-Hopkinson pressure bar system. It is found that the dynamic stress-strain curves at such a high strain rate contain hardening stages and softening stages. Different stages suggest different deformation mechanisms. In the hardening stages, kink deformation is uncommonly observed. The formation of kink bands is found to be responsible for the hardening effect. Adiabatic shearing began with the stress drops in the softening stages. From then on, the deformations localized in narrow regions, where adiabatic shearing bands (ASBs) formed at last. Dynamic recrystallization (DRX) occurred in the ASBs. The ultra-fine recrystallization grains with grain size of 0.28 μm, 0.35 μm, and 4.5 μm are observed in the ASBs formed at 400 °C, 600 °C and 800 °C respectively. It is really hard so far to measure the true shear strains and the true temperatures in the ASBs. In order to estimate the true shear strains in the ASBs, an original method basing on the definition of shear strain is proposed in this paper. Then a modified equation using the true shear strain rather than the empirical factor is employed to estimate the true temperatures in the ASBs. On such a base, the DRX in present ASBs is well explained in kinetics via the rotational dynamic recrystallization (RDR) mechanism.
KW - Adiabatic shearing
KW - High strain rate
KW - Kink deformation
KW - Rotational dynamic recrystallization
UR - http://www.scopus.com/inward/record.url?scp=85014489161&partnerID=8YFLogxK
U2 - 10.1016/j.jallcom.2017.02.284
DO - 10.1016/j.jallcom.2017.02.284
M3 - 文章
AN - SCOPUS:85014489161
SN - 0925-8388
VL - 708
SP - 84
EP - 92
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
ER -