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1Cr12Ni3Mo2VN

1Cr12Ni3Mo2VN

1Cr12Ni3Mo2VN,

1Cr12Ni3Mo2VN數(shù)據(jù)表下載

1Cr12Ni3Mo2VN化學成分 - GJB 2295A

C Si Mn P S Cr Ni N V
0.08-0.13 ≤0.40 0.50-0.90 ≤0.030 ≤0.025 11.00-12.50 2.00-4.00 0.020-0.040 0.25-0.40

1Cr12Ni3Mo2VN標準規(guī)范

  • GJB 2295A - Specification for stainless steel cold rolled sheet for aviation

1Cr12Ni3Mo2VN機械性能

熱處理 最小值 最大值 近似值 備注
熱處理 最小值 最大值 近似值 備注
熱處理 最小值 最大值 近似值 備注
熱處理 最小值 最大值 近似值 備注
熱處理 最小值 最大值 近似值 備注
熱處理 Type 最小值 最大值 近似值 備注

1Cr12Ni3Mo2VN is a new type of martensitic stainless steel for the last-stage blades of large-capacity nuclear and thermal power turbines. The deformation behavior of this steel was studied by thermal compression experiments that performed on a Gleeble-3500 thermal simulator at a temperature range of 850°C to 1200°C and a strain rate of 0.01s-1 to 20s-1. When the deformation was performed at high temperature and low strain rate, a necklace type of microstructures was observed, the plastic deformation mechanism is grain boundary slip and migration, when at low temperature and lower strain rate, the slip bands were observed, the mechanism is intracrystalline slips, and when at strain rate of 20s-1, twins were observed, the mechanism are slips and twins. The Arrhenius equation was applied to describe the constitutive equation of the flow stress. The accuracy of the equation was verified by using the experimental data and the correlation coefficient R2 = 0.9786, and the equation can provide reasonable data for the design and numerical simulation of the 1Cr12Ni3Mo2VN forging process.


1Cr12Ni3Mo2VN產(chǎn)品形態(tài)