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首页> 外文期刊>Journal of Non-Crystalline Solids: A Journal Devoted to Oxide, Halide, Chalcogenide and Metallic Glasses, Amorphous Semiconductors, Non-Crystalline Films, Glass-Ceramics and Glassy Composites >Investigation of the free volume change of Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 bulk metallic glass using the cyclic thermal dilatation test
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Investigation of the free volume change of Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 bulk metallic glass using the cyclic thermal dilatation test

机译:利用循环热膨胀试验研究Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2大块金属玻璃的自由体积变化

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In heating process, the free volume of bulk metallic glass (BMG) changes with temperature. This change, however, is too small to be directly investigated by thermal dilatation (DIL) test. In cyclic heating, the free volume change results in a difference between the thermal expansion during heating and reheating processes, i.e., Δ(δV(T)/V _0), which can be obtained by the cyclic DIL test. In this paper, the sample diameter and pre-annealing effect on the free volume change of Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 BMG are investigated by the Δ(δV(T)/V _0) and ΔδV/ ~(V0?), where ΔδV/ ~(V0?) is the average value of Δ(δV(T)/V _0) in the low temperature range and represents the total free volume released in the cyclic DIL test. The as-cast samples with a smaller diameter have a larger ΔδV/ ~(V0?). After pre-annealing below the glass transition temperature for 2 hours, a peak that is attributed to the free volume generation in glass transition process occurs in the Δ(δV(T,t _a)/V _0) curve and becomes sharper as the pre-annealing time t a is prolonged. ΔδV(ta)/ ~(V0?) is fitted by a stretched exponential relaxation function with a characteristic relaxation time τ of 14194 ± 2808 s and a Kohlrausch exponent β kww of 0.34 ± 0.04. The β _(kww) of Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 BMG is markedly lower than that of Pd- and Zr-based BMGs, and deserves a further investigation.
机译:在加热过程中,大块金属玻璃(BMG)的自由体积随温度变化。但是,此更改太小,无法通过热膨胀(DIL)测试直接进行调查。在循环加热中,自由体积变化导致加热和再加热过程中的热膨胀之间的差,即Δ(δV(T)/ V_0),这可以通过循环DIL测试获得。本文通过Δ(δV)研究了Fe_(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 BMG的试样直径和预退火对自由体积变化的影响(T)/ V _0)和ΔδV/〜(V0?),其中ΔδV/〜(V0?)是低温范围内Δ(δV(T)/ V _0)的平均值,代表总的自由体积在循环DIL测试中发布。较小直径的铸态样品具有较大的ΔδV/((V 0))。在低于玻璃化转变温度的条件下进行了2小时的预退火后,在Δ(δV(T,t _a)/ V _0)曲线中出现了一个归因于玻璃化转变过程中自由体积生成的峰,该峰变得更尖锐。 -退火时间ta被延长。 ΔδV(ta)/〜(V0α)由拉伸的指数弛豫函数拟合,其特征弛豫时间τ为14194±2808 s,Kohlrausch指数βkww为0.34±0.04。 Fe _(41)Co _7Cr _(15)Mo _(14)C _(15)B _6Y _2 BMG的β_(kww)明显低于基于Pd和Zr的BMG,并且值得进一步研究调查。

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