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    拘束对实验室试样中氢致应力分布的影响

    Effect of Constraint on Hydrogen-Induced Stress Distribution in Laboratory Specimens

    • 摘要: 以A508钢的单边缺口弯曲(SENB)和紧凑拉伸(CT)2种典型实验室试样为研究对象,基于传质和传热过程的相似性原理,采用有限元软件ABAQUS进行氢扩散和应力场的耦合分析,模拟研究不同拘束条件(裂纹长度a与试样宽度W的比值,a/W取0.1,0.3,0.5,0.7)下的氢质量分数分布、裂尖区域的氢致应力分布及其变化。结果表明:随着扩散时间延长,SENB试样和CT试样的裂尖处氢质量分数均先增加后趋于稳定,在氢扩散初期,CT试样裂尖处氢质量分数的变化较缓慢,相同拘束下CT试样裂尖处稳定氢质量分数更低;随着a/W增加,裂尖处氢质量分数降低。在氢扩散过程中,SENB试样裂尖处的氢致应力先快速增大后减小再增大最后趋于稳定。在a/W=0.1条件下,CT试样裂尖处的氢致应力先快速增大后减小最终趋于稳定,在a/W≥0.3时则先快速增大后增长停滞再继续增大最终趋于稳定。在氢扩散完成后,在a/W=0.1时SENB试样中的氢致应力在裂尖处集中;随着a/W的增加,氢致应力逐渐变得均匀。在a/W=0.1时CT试样中的氢致应力未在裂尖处集中且未趋于均匀分布,当a/W≥3时则均在裂尖处集中。

       

      Abstract: By taking two typical laboratory specimens of A508 steel, namely single-sided notch bending (SENB) and compact tensile (CT), as the research objects, on the basis of the similarity principle of mass transfer and heat transfer processes, the coupling analysis of hydrogen diffusion and stress field was conducted by the finite element software ABAQUS, and the hydrogen mass fraction distribution, and the hydrogen-induced stress distribution and variation in the crack tip area under different restraint conditions (the ratio of crack length a to specimen width W, a/W was 0.1, 0.3, 0.5, 0.7) were studied by simulation. The results show that with the extension of diffusion time, the hydrogen mass fraction at the crack tip of both the SENB specimen and the CT specimen increased first and then tended to stabilize. In the early stage of hydrogen diffusion, the hydrogen mass fraction at the crack tip of the CT specimen changed slowly, and the stable hydrogen mass fraction at the crack tip of the CT specimen was lower under the same constraint condition. With the increase of a/W, the hydrogen mass fraction at the crack tip decreased. During hydrogen diffusion, the hydrogen-induced stress at the crack tip of the SENB specimen initially increased rapidly, then decreased, and subsequently increased again before stabilizing. Under a/W=0.1, the hydrogen-induced stress at the crack tip of the CT specimen initially increased rapidly, then decreased, and finally was stabilized. Under a/W≥0.3, the hydrogen-induced stress at the crack tip initially increased rapidly, followed by a plateau, then continued to increase, and eventually was stabilized. After hydrogen diffusion was complete, the hydrogen-induced stress in the SENB specimen was concentrated at the crack tip under a/W=0.1. As the constraint increased, the hydrogen-induced stress distribution became more uniform. The hydrogen-induced stress of the CT specimen was not concentrated at the crack tip and did not tend to be uniform under a/W=0.1, while concentrated at the crack tip under a/W≥3.

       

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