首页> 外文会议>International ASTM/ESIS Symposium on Fatigue and Fracture >Prediction of the Shape of the K_J Ductile-to-Brittle Transition Temperature Curve for Ferritic Pressure Vessel Steels Using the Material's Resistance to Crack Extension K_J versus △a Curve
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Prediction of the Shape of the K_J Ductile-to-Brittle Transition Temperature Curve for Ferritic Pressure Vessel Steels Using the Material's Resistance to Crack Extension K_J versus △a Curve

机译:使用材料对裂纹延伸抗裂纹抗裂纹抗裂缝钢的k_j韧性到脆性转变温度曲线形状的预测与曲线相反

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Fracture toughness (K_(J(cleavage))) measurements made within the ductile-to-brittle transition region for ferritic pressure vessel steels are not always described by the shape of the Master Curve currently given in ASTM Standard E 1921. The objective of this paper is to show how the shape of the transition toughness curve may be related to the shape of the material's resistance to crack extension curve (K_(JR)) once the crack tip starts to blunt and ductile crack extension precedes cleavage failure. Using an empirical relationship between the mean ductile crack extension (Aa) prior to the onset of cleavage failure and temperature (△a=λ exp(ΦT)), then the relationship between K_J and T may simply be given by K_J=K_A+α[λ exp(ΦT)]~β, where K_A, a, and p are simply the coefficients to an offset power law to K_J versus △a data given by K_(JR)=K_A+α(△a)~β. For specimens of different sizes, a reference temperature T_K may be defined for a given reference level of Aa or equivalent K_J. Unique curves may be defined for materials with differing crack extension resistance curves through plots of K_J versus (T-T_(△a(ref))) or (T-T_(K(ref))). The generalized form of the transition curve may be given by K_J=K_A+α{△a(ref) exp[Φ(T-T△a(ref))]}~β or K_J=K_A+(K_((ref))-K_A){exp[Φ(T-T_(K(ref)))]}~β. Experimentally, Φ has been estimated as approximately 0.08 for nuclear pressure vessel materials such as A533B/A508. Using a specific situation wherein the value of K_A=30 MPa m, K(ref)=100 MPam, and β=0.25 then, for a B=25-mm specimen, within experimental scatter this provides an almost exact match to the Master Curve given by K_J=30+70 exp[0.019( T- T_(K100))]. The predictions of transition curve shape using the material's resistance to crack extension curve are believed to be complementary to the Master Curve method, and may describe the shape of the transition curve when there is ductile crack extension prior to cleavage failure. Further work is recommended to investigate the relationship between the predicted ductile-to-brittle transition curve and the Master Curve for probabilities of cleavage failure post-initiation.
机译:在铁素体压容器钢的延性到脆性转变区域内的裂缝韧性(K_(j(j(j(j(j(j(j(j(j(j(j)))不始终通过ASTM标准E1921中当前给出的主曲线的形状来描述。这个目标纸张是为了展示转变韧性曲线的形状如何与材料的抗性延伸曲线(K_(JR))的形状有关(K_(JR))一旦裂纹尖端开始钝而延性裂纹延伸之前裂解衰竭。在切割失效和温度开始之前使用平均延展性裂缝延伸(AA)之间的经验关系(△A=λpex(φt)),然后通过k_j = k_a +α表示K_J和T之间的关系[λpex(φt)]〜β,其中k_a,a和p只是偏移电力法的系数与k_j相反,由k_(jr)= k_a +α(△a)〜β给出的数据。对于不同尺寸的标本,可以为AA或等效K_J的给定参考电平定义参考温度T_K。可以为具有不同裂缝延伸电阻曲线的材料来定义独特的曲线,通过k_j的图与(t-t_(△a(ref)))或(t-t_(k(ref))))。过渡曲线的广义形式可以由K_J = K_A +α{α(REF)EXP [φ(TT≥A(REF))]}〜β或k_j = k_a +(k_(ref)) - k_a ){exp [φ(t-t_(k(ref)))]}〜β。实验上,φ已经估计为核压容器材料(如A533B / A508)约0.08。使用特定情况,其中k_a = 30mpa m,k(ref)= 100mpam,β= 0.25然后,对于b = 25mm标本,在实验散射内,这提供了与主曲线几乎完全匹配由K_J = 30 + 70 exp给出[0.019(T-T_(K100))]。据信使用材料对裂缝延伸曲线的抗裂纹延伸曲线的过渡曲线形状的预测与主曲线方法互补,并且当在切割失败之前存在延展性裂缝延伸时,可以描述过渡曲线的形状。建议进一步的工作来研究预测的延性到脆性过渡曲线与发酵后切割衰竭概率的主曲线之间的关系。

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