Effect of nano-Y2O3 addition on the creep behavior of an as-cast near-α titanium alloy

2021 ◽  
pp. 111249
Author(s):  
Zhuangzhuang Zheng ◽  
Fantao Kong ◽  
Yuyong Chen ◽  
Xiaopeng Wang
Metals ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 837
Author(s):  
Zhuangzhuang Zheng ◽  
Yuyong Chen ◽  
Fantao Kong ◽  
Xiaopeng Wang ◽  
Yucheng Yu

The hot deformation behavior and hot rolling based on the hot processing map of a nano-Y2O3 addition near-α titanium alloy were investigated. The isothermal compression tests were conducted at various deformation temperatures (950⁠–1070 °C) and strain rates (0.001–1 s−1), up to a true strain of 1.2. The flow stress was strongly dependent on deformation temperature and strain rate, decreasing with increased temperature and decreased strain rate. The average activation energy was 657.8 kJ/mol and 405.9 kJ/mol in (α + β) and β region, respectively. The high activation energy and peak stress were contributed to the Y2O3 particles and refractory elements comparing with other alloys and composites. The deformation mechanisms in the (α + β) region were dynamic recovery and spheroidization of α phase, while the β phase field was mainly controlled by the dynamic recrystallization and dynamic recovery of β grains. Moreover, the constitutive equation based on Norton–Hoff equation and hot processing map were also obtained. Through the optimal processing window determined by the hot processing map at true strains of 0.2, 0.4 and 0.6, the alloy sheet with multi-pass hot rolling (1050 °C/0.03–1 s−1) was received directly from the as-cast alloy. The ultimate tensile strength and yield strength of the alloy sheet were 1168 MPa and 1091 MPa at room temperature, and 642 MPa and 535 MPa at 650 °C, respectively, which performs some advantages in current research.


Author(s):  
S. P. Pomytkin ◽  
◽  
K. А. Gukasjan ◽  

In the framework of the hardening hypothesis, the creep behavior of a titanium alloy at room temperature is modeled at stepwise stress change both increasing and decreasing load. Methods for the identification of material constants and functions included in constitutive equations of the hardening theories are considered in detail. The prospects for the computational-experimental method proposed by Rybakina for determination of material constants in some versions of the hardening theory are noted. The results of the creep modeling of titanium alloy confirm the existing theoretical possibilities and limitations of the hardening hypothesis fully.


2010 ◽  
Vol 26 (6) ◽  
pp. 564-571 ◽  
Author(s):  
Zhiyong Chen ◽  
Jinwei Li ◽  
Jie Liu ◽  
Qingjiang Wang ◽  
Jianrong Liu ◽  
...  

2019 ◽  
Vol 761 ◽  
pp. 137977 ◽  
Author(s):  
Jianhui Yang ◽  
Shulong Xiao ◽  
Chen Yuyong ◽  
Lijuan Xu ◽  
Xiaopeng Wang ◽  
...  

Metals ◽  
2020 ◽  
Vol 10 (9) ◽  
pp. 1190
Author(s):  
Weixin Yu ◽  
Shusen Hou ◽  
Zhijun Yang ◽  
Jinyong Zhang ◽  
Shaoting Lang

The creep behavior of a near α TA31 titanium alloy under different compressive pressures has been studied by long-time (up to 500 h) compression tests at room temperature. The experimental results show that several thresholds of the compressive pressure were found to exist in the compression process of the TA31 alloy. When the compressive stress is lower than 0.80Rp0.2, there is no creep. There is a steady-state creep stage at the compressive stresses between 0.85Rp0.2 and 0.93Rp0.2, in which the strain rate is approximately a constant value. When the compressive stress reaches a threshold stress between 0.93Rp0.2 and 0.95Rp0.2, the sample enters the accelerating creep stage directly. The creep model of TA31 alloy has been built by using the regression method, from which the creep strain rate of TA31 titanium alloy in the steady-state creep stage under different compressive stress levels can be calculated. The mean difference between the calculated and the experimental value is 2.54%, indicating the creep model can efficiently predict the creep behavior of TA31 alloy.


2008 ◽  
Vol 59 (6) ◽  
pp. 591-594 ◽  
Author(s):  
H MISHRA ◽  
D SATYANARAYANA ◽  
T NANDY ◽  
P SAGAR

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