王瑞珉, 郭亨嘉, 陈燕娜, 等. 关于阻力曲线法测定J1c在低温下如何标定钝化线方程的探讨[J]. 北京工业大学学报, 1984, 10(2): 23-32.
    引用本文: 王瑞珉, 郭亨嘉, 陈燕娜, 等. 关于阻力曲线法测定J1c在低温下如何标定钝化线方程的探讨[J]. 北京工业大学学报, 1984, 10(2): 23-32.
    Wang Rui-men, Guo Heng-jia, Chen Yan-na, et al. On the Evaluation of the Blunting Line Equation at Low Temperatures as Used in the Determination of Ductile Fracture Toughness J1c by J-R Curve[J]. Journal of Beijing University of Technology, 1984, 10(2): 23-32.
    Citation: Wang Rui-men, Guo Heng-jia, Chen Yan-na, et al. On the Evaluation of the Blunting Line Equation at Low Temperatures as Used in the Determination of Ductile Fracture Toughness J1c by J-R Curve[J]. Journal of Beijing University of Technology, 1984, 10(2): 23-32.

    关于阻力曲线法测定J1c在低温下如何标定钝化线方程的探讨

    On the Evaluation of the Blunting Line Equation at Low Temperatures as Used in the Determination of Ductile Fracture Toughness J1c by J-R Curve

    • 摘要: 本文就J积分测试标准GB2038-80所推荐的钝化线公式进行了讨论,在对共所表达的意义予以理论征明的同时,并着重指出了在低温条件下它的不适用性(根据试验证明)。
      研究在低温条件下如何标定钝化线过程中,我们认识到:应在不同低温下具体标定转动因子γ来计算COD,由此确定具体材料试验温度下的J-δ关系,并根据不同材料在钝化阶段的δ-△a关系,以确定饨化阶段的J-△a关系,即得相应低温下的钝化线方程。
      由此得到的钝化线方程,具有J0+βa的形式,它和JR阻力曲线交点所确定的J值,与利用多试件法结合声发射监测技术确定的裂纹尖端全面启裂时的J1c值颇为接近。

       

      Abstract: The blunting line equation recommended in the National Standard (BG 2038-80) for the determination of ductile fracture toughness using J integral techniques is discussed in this paper. In expounding its meaning we discovered that this equation is not appliccable to low temperatures (verified by experiments).Some work has been done to find equations of the blunting line at low temperatures.
      We found that for the calculation of COD at low temperatures, the rotational factor r must be first determined for various low temperatures. Using this r we could determine the relation of J versus δ for the material tested under the specified low temperature. Then according to the specific δ-△a relation in the process of blunting of the tested material, we finally evaluate the J-△a relation, which is the very bluntig line equation we need at the corresponding low temperature.
      The blunting line equation thus obtained has the form of J = a0+β△a. The JQ given by the point of intersection of the J-R regression line and the blunting line well agrees with the J1C value determined by the method of multiple specimens in combination with ultrasonic crack monitoring techniques.

       

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