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不同应力场中压痕应变法的数值模拟
其他题名Numerical simulation of indentation-strain method under different residual stress fields
孟宪陆
学位类型硕士
导师陈怀宁
2007-06-04
学位授予单位中国科学院金属研究所
学位授予地点金属研究所
学位专业材料加工工程
关键词压痕应变法 数值模拟 双向残余应力 应变增量 动载 静载
摘要压痕应变法是一种新型的无损残余应力测试方法,具有使用方便、应用广泛、测量精度高等优点,正在受到越来越多的重视。本文针对压痕应变法实际应用中遇到的不同应力场中塑性区的大小、压痕周围不同方向及不同位置的应变增量分布规律以及动载压痕与静载压痕特征的异同等问题,采用有限元模拟计算的手段进行了研究。研究发现: 1)单向应力场中,当应力数值从最大压缩变化到最大拉伸时,沿受力方向的塑性区尺寸逐渐减小而垂直受力方向的尺寸逐渐增大。在双向应力场中,塑性区的变化规律比较复杂,但最大尺寸均小于单向拉伸的情况。在研究不同应力场作用下压入载荷撤离前后塑性区的变化时发现,由卸载回弹造成的塑性区尺寸变化不明显。 2)在压痕周围的弹性区中,距压痕中心位置越近,应变增量数值越大,也就越容易获得精确的测量结果。压痕制造过程中的定位偏心引起的对应变增量数值的干扰与应变测量范围(应变栅长度)有关,当偏心量为0.1mm时,栅长在0.5-0.9mm范围内的最大测量误差为10.6%,该误差随测量范围的增大而减小。在所有应力场中,卸载回弹对应变增量与残余应变间的关系几乎没有影响。 3)在单向应力场中,在与主方向x轴夹角成62度的分界线两侧,应变增量与有效应变(外加应变与材料屈服点对应应变之比)之间关系曲线的特征不同,该关系曲线随与x轴夹角的变化而变化。当应变增量取值范围为距压痕中心4~5mm时,应变增量与正有效应变间均满足二次曲线关系,而应变增量与负有效应变间的对应关系在分界线两侧可用线性函数和二次函数分别描述。当应变增量取值范围变为距压痕中心3~4mm时,基本规律保持不变,但在与x轴夹角小于45度时,应变增量与正有效应变间的二次曲线关系可以直接用线性关系取代,这些直线的斜率和与x轴的夹角之间满足二次函数关系。等轴双向应力场中,应变增量在所有方向上的分布规律是完全相同的。在任意双向应力场中,主应力方向上的应变增量受该方向应力和垂直该方向应力的综合影响,如果把乘以泊松比的垂直方向应变值叠加到主应变上,则得到的规律与单向应力场的相同。 4)在外加应力场与压头载荷恒定的情况下,压痕深度、压痕周围的塑性区尺寸以及应变增量的绝对值都随试板材料屈服强度的增加而逐渐减小。 5)在外加应力场相同的情况下,与压痕深度大体相当的静载压痕相比,动载压痕的塑性区尺寸变化不大,但其周围应变增量要小一些。 关键字:压痕应变法,数值模拟,双向残余应力,应变增量,动载,静载
其他摘要Indentation-strain method is a new non-destructive method used for residual stress measurement with some virtues, such as convenience, wide application, highly precision, ect. This method has got more and more attention. In order to solve some existing problems, for example, the size of plastic zone under different biaxial residual stresses, the regularities of distribution of strain increment around indentation in different directions and different zone, the difference between dynamic and static indention, a finite element analysis was conducted. The beneficial results obtained in the paper are as follows: 1) Under axial stress, it has been found that the size of plastic zone decreases in the direction parallel to maximum principle stress and increases in the direction normal to maximum principle stress, when the residual stress changed from maximum compress stress to maximum tensile stress. Under biaxial stress, the shape of plastic zone is rather complicated, but the maximum size of plastic zone is less than that in axial stress at all time. The change of plastic zone size was not significant before and after unloaded under any stress field. 2) The change of relation between strain increment and residual strain was not significant before and after unloaded under any stress field. In elastic zone around indentation, strain increment increased when the measure zone get near to the center of indentation. And the residual stress obtained get more exactly under this situation. The change of strain increment caused by eccentric indentation has relation to the size of measured zone (the length of gage lines). The maximal error is 10.6% when the eccentricity of indentation was 0.1mm and gage lines’ length is 0.5-0.9mm. And the error decreased with the increase of measuring zone’s area. 3) The relation between strain increment and effective strain (named the ratio of external strain to the strain when material yield) was different when the inclination with x axial is larger or smaller than 62o. And the relation was changed with this inclination. When the strain increment was measured in the zone where the distance from the center of indentation is 4~5mm, it varied with tensile effective strain corresponding to a square function, and varied with compressive effective strain corresponding to a linear law and square function respectively when the inclination with x axial is larger or smaller than 62o. When the strain increment was measured in the zone where the distance from the center of indentation is 3~4mm, the basic relation between the strain increment and effective strain was unchanged. But when the inclination with x axial is smaller than 45o, the square function which was used to describe the relation of the strain increment and tensile strain can be replaced by linear law. And the slop of the linear law varied with the inclination corresponding to a square function. Under equal biaxial stress field, the regularities of distribution of strain increment in all directions were the same. In any biaxial stress field, strain increment in the direction parallel to maximum principle stress was affected by the stress in this direction and normal to this direction. If plus the product of Poisson’s ratio and the strain in the direction normal to maximum principle stress to the strain in the direction parallel to maximum principle stress, then the relation was the same with that in axial stress field. 4) When the stress field and load are constant, indentation depth, size of plastic zone and the absolute value of strain increment will decrease with the raising of yield strength. 5) Compared with the situation of static indention with the same penetration depth and stress field applied, the size of dynamic indentation plastic zone changed a little, but the strain increment of dynamic indentation was smaller. Key words: indentation-strain method, FEM, biaxial residual stress, strain increments, static load indentation,dynamic load indentation
页数75
语种中文
文献类型学位论文
条目标识符http://ir.imr.ac.cn/handle/321006/17089
专题中国科学院金属研究所
推荐引用方式
GB/T 7714
孟宪陆. 不同应力场中压痕应变法的数值模拟[D]. 金属研究所. 中国科学院金属研究所,2007.
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