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Residual Stress Distribution in Hardened Case Layer of Cr-Mo Steel after Carburizing and Quenching

机译:渗碳淬火后Cr-Mo钢硬化壳层的残余应力分布

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摘要

The hollow circular cylinder specimen of Cr-Mo steel with 0.20 mass% C was carburized in carrier gas and quenched in oil bath.After quenching, the surface residual stress distributions in the radial, axial and hoop directions of the specimen were measured experimentally by x-ray as a function of the distance from the carburized surface.The case depth of the quenched specimen was about 0.8 mm.Diffraction from Fe-211 by Cr-Ka radiation was used to minimize the effect of carbon content gradient on the nonlinearity of 20-sin~2ψ, because effective x-ray penetration depth was about 5.8 μm at sin~2ψ=0.The hardened case layer was gradually removed by electrolytic polishing.X-ray stress measurement was repeated on the polished surface from the carburized surface to the interior.The ψ-splitting was not observed on the carburized surface.The 20-in~2ψ diagrams were found to shift from low to high angles in inverse proportion to carbon content.The residual stresses in the hardened case layer were compressive.The maximum compressive residual stresses on the hollow circle and periphery surfaces were about -559 and -544 MPa at the depth of 0.2 and 0.3 mm, respectively.On the other hand, the tensile residual stress was not observed.The full widths at half-maximum intensity of Fe-211 diffraction peaks in the hardened case layer were wider than that of the interior of the specimen.Martensitic transformation of the carbon-rich layer leaded to the broadening of diffraction peaks.Therefore the interior of carburized specimen were deformed elastically to balance the existence of the surface compressive residual stresses.
机译:将C含量为0.20%的Cr-Mo钢制空心圆柱试样在载气中渗碳并在油浴中淬火,淬火后,用x进行实验测量试样的径向,轴向和环向的表面残余应力分布。射线与渗碳表面距离的函数。淬火试样的表面深度约为0.8 mm。使用Cr-Ka辐射从Fe-211进行衍射,以最小化碳含量梯度对20%非线性的影响-sin〜2ψ,因为在sin〜2ψ= 0时有效x射线穿透深度约为5.8μm。通过电解抛光逐渐去除硬化的表层,并从渗碳表面到抛光后的表面重复进行x射线应力测量在渗碳表面未观察到ψ分裂。发现20 in〜2ψ图与碳含量成反比例从低角度转变为高角度。硬化的表层中的残余应力为c在0.2mm和0.3mm的深度处,空心圆和外围表面上的最大压缩残余应力分别约为-559和-544 MPa,但未观察到拉伸残余应力。硬化壳层中Fe-211衍射峰的半峰最大强度比试样内部宽,富碳层的马氏体相变导致衍射峰变宽,因此渗碳试样内部变形弹性地平衡表面压缩残余应力的存在。

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