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RESIDUAL STRESS MEASURING METHOD FOR METALLIC MATERIAL

机译:金属材料的残余应力测量方法

摘要

PROBLEM TO BE SOLVED: To provide a method for easily and accurately measuring a residual stress distribution of a metallic material at a metallic structure level in a whole area of a sample even if the sample is relatively large.;SOLUTION: A method for measuring residual stress on a metallic material includes: a step S1 of acquiring a crystal orientation distribution from a backscattered electron diffraction pattern of a metallic material; a step S2 of calculating lattice strain between adjacent lattice points from the crystal orientation distribution; a step S3 of calculating plastic strain from dislocation density indicated by a difference in orientation in the crystal orientation distribution; a step S4 of calculating elastic strain from a difference between the lattice strain and the plastic strain; a step S5 of plastically deforming the metallic material by applying a predetermined load to it, executing steps S1 to S4 again to the plastically-deformed metallic material, and measuring a coordinate displacement on a surface of the plastically-deformed metallic material; and a step S6 of associating a coordinate before the plastic deformation with the coordinate after the plastic deformation on the basis of the coordinate displacement, and obtaining a difference in a residual stress component between before and after the plastic deformation.;COPYRIGHT: (C)2013,JPO&INPIT
机译:解决的问题:提供一种即使在样品相对较大的情况下,也可以容易且准确地测量金属材料在整个样品区域的残余应力分布的方法。在金属材料上的应力包括:步骤S1,从金属材料的反向散射电子衍射图案获取晶体取向分布;步骤S2,根据晶体取向分布计算相邻晶格点之间的晶格应变;步骤S3,从由晶体取向分布中的取向差表示的位错密度计算塑性应变;步骤S4,根据晶格应变与塑性应变之差计算弹性应变。步骤S5,通过对金属材料施加预定的载荷使金属材料塑性变形,再次对塑性变形的金属材料执行步骤S1至S4,并测量塑性变形的金属材料表面上的坐标位移;步骤S6,根据坐标位移,将塑性变形前的坐标与塑性变形后的坐标相关联,求得塑性变形前后的残余应力分量之差。 2013,日本特许厅

著录项

  • 公开/公告号JP2013032991A

    专利类型

  • 公开/公告日2013-02-14

    原文格式PDF

  • 申请/专利权人 NIPPON STEEL & SUMITOMO METAL;

    申请/专利号JP20110169587

  • 发明设计人 SAKURADA EISAKU;

    申请日2011-08-02

  • 分类号G01L1/25;G01N23/203;

  • 国家 JP

  • 入库时间 2022-08-21 17:00:15

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