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The microstructure of 40Cr steel sample and its surface is ultra-fined through salt-bath cyclic quenching and high frequency hardening, then the superplasticity is studied under isothermal superplastic compressive deformation condition. The experimental results indicate that the stress-strain curves are shown to take place obvious superplastic flow characteristic at the temperature of 750-770℃ and at the initial strain rate of (1.7-5.0)×10-4 s-1. Its strain rate sensitivity is 0.30-0.38, the steady superplastic flow stress is 60-70MPa, the superplastic flow activation energy is 198-217kJ/mol, and it is close to α-Fe grain boundary self-diffusion activation energy. The super-plastic compressive constitute equations of this steel are correspondingly set up. Due to the finer microstructure of high frequency hardening, it appears bigger strain rate sensitivity value, smaller the steady superplastic flow stress and the superplastic flow activation energy, so it has better superplastic deformation capabili
The microstructure of 40Cr steel sample and its surface is ultra-fined through salt-bath cyclic quenching and high frequency hardening, then the superplasticity is studied under isothermal superplastic compressive deformation condition. The experimental results that that stress-strain curves are shown to take place obvious superplastic flow characteristic at the temperature of 750-770 ° C and at the initial strain rate of (1.7-5.0) × 10-4 s-1. Its strain rate sensitivity is 0.30-0.38, the steady superplastic flow stress is 60- 70 MPa, the superplastic flow activation energy is 198-217 kJ / mol, and it is close to α-Fe grain boundary self-diffusion activation energy. The super-plastic compressive constitutes equations of this steel are correspondingly set up. of high frequency hardening, it shows bigger strain rate sensitivity value, smaller the steady superplastic flow stress and the superplastic flow activation energy, so it has better superplastic d eformation capabili