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复合型载荷缺口前端双氢峰的规律和研究
王利
学位类型硕士
导师陈廉
1992
学位授予单位中国科学院金属研究所
学位授予地点中国科学院金属研究所
关键词双氢峰 复合型载荷 缺口前端 开裂方向 Γ_p~(Max)方向 有限元法 Kyky离子探针
摘要本文以21Cr-7Ni-9Mn-0.25N奥氏体不锈钢为材料,利用高压斧热充氢,在KYKY离子探针上,运用自己设计的一种新的直观微区定位方法,对负载的复合型缺口顶端氢浓度的再分布行为进行了系统的研究。结果表明:在不同的K_(II)/K_I比值下,负载的复合型缺口顶端,不论是在开裂方向还是在塑性区尺寸最大方向上,皆有两个氢浓度的富集峰,一个紧靠缺口,另一个位于缺口稍远处。且随着II型分量的增加,远离缺口的氢富集峰都有下降且移向缺口顶端的趋势。I+II复合型缺口顶端也存在两个氢浓度的富集峰。III型分量的加入,使缺口顶端的两个氢浓度富集峰皆有下降,且有使第二个氢峰移向缺口的趋势。钢中原始氢浓度的改变,并不严重影响缺口顶端双氢峰的形成,缺口前端的应力、应变场的变化,才是导致缺口顶端氢浓度再分布的主导因素。为了判别缺口顶端双氢峰的性质,利用ADINA非线性有限元程序,定量计算结果表明:对I+II复合型缺口试样,在开裂方向上,随着II型分量的增大,最大静水应力σ_h~(max)逐渐下降且有移向缺口的趋势,而等效塑性应变ε_(eq)的分布,却是随距缺口距离的增大迅速下降。从缺口顶端氢浓度的测定与应力、应变分布计算对照的理论分析表明:复合型载荷裂端的氢富集峰是位错对氢陷阱作用的结果,而远离裂端的氢浓度富集峰是由三向静水应力引起的。位错和静水应力的交互作用导致缺口顶端形成两个氢的浓度富集峰,且存在以下关系:C_H/C_O = f(θ)/r~(1/2) + exp(-A_O) |R - R_O|) - B_O其中,R_O为最大静水应力σ_h~(max)的位置,A_O和B_O分别为与应变和应力状态及材料性质有关的函数。
其他摘要The distribution of hydrogen near notch tip of austenitic steel 21Cr-7Ni-9Mn-0.25N charging in autoclave under mixed mode loading (I + II and I + III) has been studied with a new method of microregion locating in Ion Microprobe Mass Analyzer (KYKY LT-1A type). It was shown that there were two peaks of hydrogen accumulation, one at notch tip and the other far apart from it, either in cracking direction or in maximum plastic region's(γ_p~(max)), and with the increasing of mode II loading, the peak of hydrogen accumulation of the latter decreased and moved to notch tip. There existed also two peaks of hydrogen accumulation near notch tip under mixed mode I + III loading, with the increasing of mode III component, the two peaks of hydrogen accumulation all decreased and the second hydrogen accumulation peak moving closer to the notch tip. The change of original hydrogen concentration of steel has few effects on the two peaks of hydrogen accumulation near notch tip, Whereas the stress and strain field affect predominantly the formation of the two peaks near notch tip. In order to determine the properties of the two hydrogen accumulation peaks, ADINA non-linear finite element method was used to caculate quantitatively the distribution of hydrostatic stress(σ_h) and eqivalent strain (ε_(eq)) near notch tip, It is shown that with the increasing of distance from the notch tip, σ_h~(max) decrease gradually and move to notch tip. while the (ε_(eq)) decrease griftly. It is revealed by the analysis of comparising hydrogen concentration with stress and strain near notch tip that: The hydrogen accumulation peak at notch tip is caused by trapping effect of dislocation on dissolved hydrogen, while the other one caused by the hydrostatic stress. The interaction between dislocation and hydrostatic stress caused the two hydrogen peaks near notch tip, and the distribution of hydrogen concentration near notch tip is give by: C_H/C_O = f(θ)/r~(1/2) + exp(-A_O) |R - R_O|) - B_O Where, C_0 is hydrogen concentration in absent of stress, A_O, B_O are functions of strain and stress state and material properties.
页数68
语种中文
文献类型学位论文
条目标识符http://ir.imr.ac.cn/handle/321006/17550
专题中国科学院金属研究所
推荐引用方式
GB/T 7714
王利. 复合型载荷缺口前端双氢峰的规律和研究[D]. 中国科学院金属研究所. 中国科学院金属研究所,1992.
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