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首页> 外文期刊>Acta Materialia >MARTENSITIC TRANSITIONS AND MECHANICAL SPECTROSCOPY OF Ni_50.8Ti_49.2 ALLOY CONTAINING HYDROGEN
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MARTENSITIC TRANSITIONS AND MECHANICAL SPECTROSCOPY OF Ni_50.8Ti_49.2 ALLOY CONTAINING HYDROGEN

机译:Ni_50.8Ti_49.2含氢合金的马氏体转变和力学光谱

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Hydrogen additions [n_H = H/(Ni + Ti) = 0.003, 0.008, 0.013, 0.021, 0.029, 0.045 at.] to a Ni_50.8Ti_49.2 alloy produce several effects in the elastic and anelastic properties of the material. At tempera- tures between 100 and 150 K hydrogen atoms act as fixed pinning points for dislocations, as they cancel a newly observed dislocation relaxation. At low H contents (0 < n_H ≤ 0.008) the internal friction peak P_AM (P_RM) associated with austenite./martensite (A → M) or R-phase/martensite (R → M) transitions dramati- cally increases with increasing the H content, while the dip occurring in the Young's modulus (E) vs tem- perature curves becomes gradually wider and shallower. The enhancement of peak P_AM (P_RM) can be accounted for in terms of a mechanism involving the excitation of collective vibration modes (dyadons) of twin boundaries interacting with H or the stress-induced motion of parent/product interfaces. The widening of the dip in the Young's modulus is due to the introduction by H of a two-step transition (A → R → M). With increasing the H content n_H from 0.008 to 0.045 the height of peak P_AM (P_RM) decreases and a higher temperature peak (P_H) appears and progressively grows becoming the only internal friction feature for n_H = 0.045. With increasing H content the thermal hysteresis in the E(T) curves occur- ring over the coexistence region of the A and M (R and M) phases decreases due to the inhibition caused by H of the martensitic transition. Peak P_H is most likely associated with stress-induced motion of H in solid solution within the R-phase or withi
机译:向Ni_50.8Ti_49.2合金中添加氢[n_H = H /(Ni + Ti)= 0.003、0.008、0.013、0.021、0.029、0.045 at。]对材料的弹性和非弹性性质产生多种影响。在100到150 K之间的温度下,氢原子充当位错的固定钉扎点,因为它们消除了新观察到的位错弛豫。在低H含量(0 <n_H≤0.008)下,与奥氏体/马氏体(A→M)或R相/马氏体(R→M)相伴的内摩擦峰P_AM(P_RM)随着H的增加而急剧增加。含量,而杨氏模量(E)对温度曲线的下降逐渐变宽和变浅。峰值P_AM(P_RM)的增强可以通过一种机制来解决,该机制涉及激发与H相互作用的双边界的集体振动模式(激子)或母体/产品界面的应力诱导运动。杨氏模量下降的加宽是由于H引入了两步跃迁(A→R→M)。随着H含量n_H从0.008增加到0.045,峰P_AM(P_RM)的高度减小,并且出现更高的温度峰(P_H)并逐渐增长,成为n_H = 0.045的唯一内部摩擦特征。随着H含量的增加,由于马氏体转变的H所引起的抑制作用,在A和M(R和M)相的共存区域内,E(T)曲线中的热滞现象会降低。 P_H峰值很可能与H相在固溶或H相下的应力诱导运动有关

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