Hot deformation characteristics and processing map analysis of a new designed nickel-based alloy for 700 °C A-USC power plant
| Autor: | Y.D. Wu, Fusheng Lin, Maicang Zhang, Xishan Xie, Shuangqun Zhao, Jianxin Dong |
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| Rok vydání: | 2016 |
| Předmět: |
010302 applied physics
Materials science Mechanical Engineering Metallurgy Metals and Alloys Nucleation 02 engineering and technology Flow stress Strain rate 021001 nanoscience & nanotechnology Microstructure 01 natural sciences Grain growth Hot working Mechanics of Materials 0103 physical sciences Materials Chemistry Dynamic recrystallization Deformation (engineering) Composite material 0210 nano-technology |
| Zdroj: | Journal of Alloys and Compounds. 656:119-131 |
| ISSN: | 0925-8388 |
| DOI: | 10.1016/j.jallcom.2015.09.219 |
| Popis: | The deformation behavior of the new designed nickel-based alloy for 700 °C advanced ultra-super-critical (A-USC) power plant applications was studied by the isothermal compression tests at temperature range of 1000–1200 °C with strain rates of 0.01–10 s −1 on a Gleeble-1500 thermo-mechanical simulator in order to optimize the hot working parameters and control the microstructure under various deformation conditions. The results show that the flow stress increases with the decreasing temperature and increasing strain rate, and the activation energy of the new alloy is about 474.22 kJ/mol. Then the processing maps were developed on the basis of corrected flow stress data. The flow instability domain lies in the temperature range of 1000–1035 °C and strain rate range of 0.03–10 s −1 . The microstructure in the domain is characterized with inhomogeneous microstructure resulting from flow localization which should be avoided in hot working process. The optimum hot working conditions are obtained in the temperature range of 1125–1200 °C and strain rate range of 0.01–0.3 s −1 , except the grain growth domain with the strain rate and temperature range of 0.01–0.03 s −1 and 1175–1200 °C. Microstructure observations reveal that full dynamic recrystallization (DRX) occurs in the optimum conditions and the origin microstructure has been substituted by fine and equiaxed DRX grains. The nucleation mechanism of DRX in the new alloy is discontinuous dynamic recrystallization (DDRX) as to the existence of original grain boundaries bulging under the low strain rate. However, the dominant nucleation mechanism of DRX at high strain rate has turned into CDRX. |
| Databáze: | OpenAIRE |
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