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CREEP BEHAVIOUR OF TYPE 310 STAINLESS STEEL. PART 2: ANALYSIS BASED ON THE STUDY OF TRANSIENTS AFTER STRESS REDUCTION EXPERIMENTS

机译:310型不锈钢的蠕变行为。第2部分:基于压力减少实验后瞬态研究的分析

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Stress-drop experiments during secondary creep in AISI 310 stainless steel were performed at seven stress levels in the range from 70 to 210MPa, at 700°C. Incubation periods were systematically detected following the stress reductions and their duration measured. Recovery kinetics parameters and friction stress (σ_o) data were determined by extrapolation using a physical equation suggested in literature for the process. The friction stress was found to increase linearly with applied stress in the range from 70 to 120MPa and to reach a constant value σ_o≈ 66 MPa from 120 to 210 MPa. The initial friction stress level of the material was also estimated to be about 6 MPa. Secondary creep rates could be expressed by a single power law relation with n ≈ 3.5 in terms of the effective stress (σ - σ_o). Initial creep rates could also be expressed by the same power law relation in the range from 40 to 140 MPa. Assumptions are put forward for the variation of the friction stress in secondary creep stage, in the interval from 250 to 375 MPa, so that secondary creep rate in the whole interval from 70 to 375 MPa can be expressed by: ε_s=4.943x10~(-14).(σ-σ_o)~(3.85). Normalization of the effective stress by the yield stress σ_(0.05) of the material at 700°C, gives the relation: ε_s=5.86x10~(-6).[(σ-σ_o)/σ_(0.05)]~(3.85) This expression is not fully consistent with the universal equation proposed by Evans and Harrison for secondary creep in metallic materials.
机译:AISI 310不锈钢中次蠕变期间的应力下降实验在700℃下以70至210MPa的七个应力水平进行。在应力减少后系统地检测到潜伏期,测量它们的持续时间。通过使用文献中的文献中的外部方程来确定回收动力学参数和摩擦力(Σ_o)数据。发现摩擦应力随施加的应力在70至120MPa的范围内线性增加,并且在120至210MPa中达到恒定值σ_o≈66MPa。还估计材料的初始摩擦力水平约为6MPa。二次蠕变率可以通过在有效应力(σ-Σ_O)方面与N≈3.5的单个电力律关系表示。初始蠕变率也可以通过40至140MPa的相同电力律关系表示。在250至375MPa的间隔中提出了次要蠕变阶段中摩擦应力的变化的假设,使整个间隔的次级蠕变率从70到375MPa表示:ε_s= 4.943x10〜( -14)。(Σ-Σ_o)〜(3.85)。通过700℃的材料的屈服应力σ_(0.05)进行有效应力的标准化,给出了关系:ε_s= 5.86x10〜(-6)。[(Σ-Σ_o)/σ_(0.05)]〜(3.85 )这种表达与埃文斯和哈里森以金属材料中的二次蠕变提出的通用方程完全一致。

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