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Anisotropic negative thermal expansion behavior of as-smelted Ti-rich Ti-Ni alloys with different Ni contents

机译:具有不同Ni含量的富含Ti-Ni合金的各向异性负热膨胀行为

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Ti-Ni alloys have been found to exhibit unique negative thermal expansion (NTE) performance, namely, contracting upon heating, which is thought to result from the reversible martensitic phase transformation behavior. In Ti-Ni alloys, the high-temperature phase, i.e., austenite (A), has the CsCl structure, while the low-temperature phase, martensite (M), has the monoclinic structure. The parameters of austenite and martensite are as follows: ao=0.3015 nm, V_A=0.02741 nm~3 and a=0.2889 nm, b=0.4120 nm, c=0.4622 nm, β=96.8° and V_M=0.05463 nm~3 [1]. Clearly, the volume of the low-temperature phase is almost twice that of the high-temperature phase. Mavoori et al. [2] reported that Ti-Ni alloys have NTE behavior and the coefficient of thermal expansion (CTE) of uniaxially strained Ti-Ni alloys is up to -200×10~(-6) K~(-1). Uchil et al. [3] studied the thermal expansion in various phases of Ti-Ni alloys using TMA and DSC. Nevertheless, there is still a lack of deep and comprehensive understanding of the NTE behavior of Ti-Ni alloys.
机译:Ti-Ni合金已发现在加热时,这被认为从可逆马氏体相变行为导致表现出独特的负热膨胀(NTE)的性能,即,收缩。在Ti-Ni合金,高温相,即奥氏体(A),具有氯化铯结构,而低温相,马氏体(M),具有单斜晶结构。的奥氏体和参数马氏体如下:AO = 0.3015纳米,V_A = 0.02741纳米〜3且a = 0.2889纳米,B = 0.4120纳米,C = 0.4622纳米,β= 96.8°和V_M = 0.05463纳米〜3 [1 ]。显然,低温相的体积几乎是高温相的两倍。 Mavoori等。 [2]报道Ti-Ni合金具有NTE行为和热膨胀系数(CTE)的系数单轴应变Ti-Ni合金的是至多-200×10〜(-6)K〜(-1)。 Uchil等。 [3]研究了使用TMA和DSC Ti-Ni合金的各个阶段的热膨胀。尽管如此,仍然有欠缺的Ti-Ni合金的NTE行为的深刻和全面的了解。

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