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Gradient Distribution of Martensite Phase in Melt-Spun Ribbons of a Fe-Ni-Ti-Al Alloy

机译:Fe-Ni-Ti-Al合金熔纺薄带中马氏体相的梯度分布

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摘要

Metallographic, X-ray diffraction and magnetometric analysis were used to study the regularities of martensitic transformation in melt-spun ribbons of a Fe – 28 wt. % Ni – 2.1 wt. % Ti – 2 wt. % Al – 0.05 wt. % C alloy. The substantial differences in volume fractions of the martensite phase in local regions of thin melt-spun ribbons of the alloy are related to the size effect of the transformation and structural inhomogeneity of the ribbons. The distribution of austenitic grain size in different local areas of melt-spun ribbons is significantly different. The principal factor for changing the completeness of the martensitic transformation is the size effect of transformation. Difference in the martensite volume fraction in local regions of a ribbon is mainly determined by the different volume fractions of ultrafine-grained (500–1000 nm) and nanosized (80–100 nm and less) initial austenite grains, in which the transformation was slowed down or completely suppressed. Other factors almost do not affect the completeness of the martensitic transformation. The strong stabilizing effect of the reverse α–γ transformation with respect to the subsequent direct γ–α transformation in the melt-spun ribbons is also related to the grain size effect.
机译:用金相,X射线衍射和磁力分析法研究了Fe – 28 wt。的熔纺带中的马氏体转变规律。 Ni含量– 2.1 wt。 %Ti – 2 wt。 Al含量– 0.05 wt。 %C合金。在合金的薄熔纺薄带的局部区域中马氏体相的体积分数的实质差异与薄带的相变的尺寸效应和结构的不均匀性有关。在熔纺带材的不同局部区域中,奥氏体晶粒尺寸的分布差异显着。改变马氏体相变完整性的主要因素是相变的尺寸效应。带状区域马氏体体积分数的差异主要由超细晶粒(500–1000nm)和纳米尺寸(80–100nm及以下)的初始奥氏体晶粒的不同体积分数决定,下降或完全被压制。其他因素几乎不影响马氏体相变的完整性。反向α-γ相变相对于随后的熔纺薄带中直接γ-α相变的强稳定作用也与晶粒尺寸效应有关。

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