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Determining plane strain fracture toughness and the J-Integral for solid materials using stress field modified miniature specimens

机译:使用应力场修正的微型样本确定固体材料的平面应变断裂韧性和J积分

摘要

A method of determining the mechanical behavior of solid materials by using stress field modified miniature specimens. The method is an improvement in the method of determining mechanical behavior information from specimens only so large as to have at least a volume or smallest dimension sufficient to satisfy continuum behavior in all directions. Mechanical behavior of the material is determined from the measurements taken during the loading of the specimen resulting in the formation of cracks and/or the further propagation of cracks in the miniature specimen. The specimens include construction features for applying additional stress field modifying loads upon the specimens during the test. These additional loads result in a desired stress state in the specimen which could not be achieved otherwise. A particular example is the introduction of a transverse tensile load during a bend test to increase the transverse stress field to achieve plane strain conditions in a thin specimen. The methods are useful in determining plane strain fracture toughness, dynamic plane-strain crack initiation and arrest fracture toughness, the J-Integral for the material, and the fracture mode transition behavior when the specimen thickness and volume is smaller than previously thought necessary.
机译:一种通过使用应力场修饰的微型样本确定固体材料力学性能的方法。该方法是对仅从样本确定机械行为信息的方法的一种改进,该样本如此之大以至于至少具有足以满足所有方向上的连续性行为的体积或最小尺寸。材料的机械性能由样品加载过程中获得的测量值确定,这些测量结果导致在微型样品中形成裂纹和/或进一步扩展裂纹。样品具有在测试过程中向样品施加额外应力场修正载荷的构造特征。这些额外的负载会在样品中产生所需的应力状态,否则该应力状态将无法实现。一个特殊的例子是在弯曲试验中引入横向拉伸载荷,以增加横向应力场,从而在薄样品中达到平面应变条件。该方法可用于确定平面应变断裂韧性,动态平面应变裂纹萌生和滞后断裂韧性,材料的J积分以及当样品厚度和体积小于先前认为必要的断裂模式转变行为。

著录项

  • 公开/公告号US4895027A

    专利类型

  • 公开/公告日1990-01-23

    原文格式PDF

  • 申请/专利权人 BATTELLE DEVELOPMENT CORPORATION;

    申请/专利号US19880145830

  • 发明设计人 MICHAEL P. MANAHAN SR.;

    申请日1988-01-19

  • 分类号G01N3/08;

  • 国家 US

  • 入库时间 2022-08-22 06:08:04

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