Creep microstructures and creep behaviors of pure molybdenum sheet at 0.7 Tm |
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Affiliation: | 1. Korea Institute of Industrial Technology, Incheon 406-840, Republic of Korea;2. Material Science and Engineering, Inha University, Incheon 402-751, Republic of Korea;1. School of Materials Science and Engineering, Xi''an University of Technology, Xi''an 710048, PR China;2. Northwest Institute for Non-ferrous Metal Research, Xi''an 710016, PR China;3. State key laboratory for Mechanical Behavior of Materials, Xi''an Jiaotong University, Xi''an 710049, PR China;1. Karlsruhe Institute of Technology, Institute for Applied Materials, 76344 Eggenstein-Leopoldshafen, Germany;2. PLANSEE SE, 6600 Reutte, Austria;1. School of Mechanical Engineering and Automation, Beihang University, Beijing 100191, PR China;2. School of Aeronautical Manufacturing Engineering, Nanchang Hangkong University, Nanchang 330063, PR China |
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Abstract: | The creep behavior of high purity molybdenum (99.995 wt.%) is investigated at temperatures of 1600 to 2000 °C (0.61–0.77 Tm) by direct ohmic heating. The stress and temperature dependency of creep strain and rupture time are described through optical microstructure observations. Under low load and low temperature conditions, coarse secondary recrystallized grains caused by dynamic recrystallization are observed far from the crack tip. In contrast, under high load and high temperature conditions, coarse secondary recrystallized grains are only fully formed near the crack tip, while coarse secondary recrystallized grains and small primary recrystallized grains coexisted further away from the tip. The recrystallized grain size of the Mo-B sheet is smaller than that of the Mo-A sheet, and small primary and large secondary recrystallized grains are mixed throughout whole specimens of the Mo-B sheet. Mo-A sheet shows elongated ductile fracture, but Mo-B sheet shows irregular brittle fracture under the same conditions. The steady-state creep strain rate at 1800 °C is found to be 7.34 × 10− 6, 2.83 × 10− 5 and 1.53 × 10− 4 s− 1 under a constant stress of 5, 10 and 20 MPa, respectively. The stress exponent is estimated to be 3.85–3.98 and the strain activation energy for steady state creep is 362–413 kJ/mol. |
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