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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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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 urn 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-sin~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,通过X射线实验测量样品在径向,轴向和环向方向上的表面残余应力分布,该分布是距渗碳表面距离的函数。淬火样品的表壳深度约为0.8毫米。 Cr-Ka辐射对Fe-211的衍射被用来最小化碳含量梯度对20-sin〜2ψ非线性的影响,因为在sin〜2ψ= 0时有效的x射线穿透深度约为5.8 urn。通过电解抛光逐渐除去硬化的外壳层。在从渗碳表面到内部的抛光表面上重复进行X射线应力测量。在渗碳表面未观察到ψ裂。发现20sin〜2ψ图与碳含量成反比例从低角度向高角度移动。硬化壳层中的残余应力为压缩应力。在0.2mm和0.3mm的深度处,空心圆和外周表面上的最大压缩残余应力分别为约-559和-544MPa。另一方面,未观察到拉伸残余应力。硬化壳层中的Fe-211衍射峰在半最大强度处的全宽比试样内部的宽。富碳层的马氏体相变导致衍射峰变宽。因此渗碳试样的内部发生弹性变形,以平衡表面压缩残余应力的存在。

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