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首页> 外文期刊>Acta Materialia >EFFECT OF HEATING RATE AND GRAIN SIZE ON THE MELTING BEHAVIOR OF THE ALLOY Nb-47 MASS Ti IN PULSE-HEATING EXPERIMENTS
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EFFECT OF HEATING RATE AND GRAIN SIZE ON THE MELTING BEHAVIOR OF THE ALLOY Nb-47 MASS Ti IN PULSE-HEATING EXPERIMENTS

机译:脉冲加热实验中升温速率和晶粒尺寸对Nb-47质量钛合金熔化行为的影响

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摘要

The effect of heating rate and grain size on the melting behavior of Nb-47 mass Ti is measured and modeled. The experimental method uses rapid resistive self heating of wire specimens at rates between ~102 and ~104 K/s and simultaneous measurement of radiance temperature and normal spectral emissivity as functions of time until specimen collapse, typically between 0.4 and 0.9 fraction melted. During heating, a sharp drop in emissivity is observed at a temperature that is independent of heat- ing rate and grain size. This drop is due to surface and grain boundary melting at the alloy solidus tem- perature even though there is very little deflection (limited melting) of the temperature-time curve from the imposed heating rate. Above the solidus temperature, the emissivity remains nearly constant with increas- ing temperature and the temperature vs time curve gradually reaches a sloped plateau over which the major fraction of the specimen melts. As the heating rate and/or grain size is increased, the onset tempera- ture of the sloped plateau approaches the alloy liquidus temperature and the slope of the plateau approaches zero. This interpretation of the shapes of the temperature--time curves is supported by a model that includes diffusion in the solid coupled with a heat balance during the melting process. There is no evi- dence of loss of local equilibrium at the melt front during meltiong in these experiments.
机译:测量并模拟了加热速率和晶粒尺寸对Nb-47质量Ti熔化行为的影响。该实验方法使用金属丝样品的快速电阻自加热,其速率介于〜102和〜104 K / s之间,并同时测量辐射温度和法线光谱发射率,作为样品塌陷的时间的函数,通常在0.4至0.9之间熔化。在加热过程中,在与加热速率和晶粒尺寸无关的温度下观察到发射率急剧下降。该下降是由于合金固相线温度下的表面和晶界熔化造成的,即使温度-时间曲线因施加的加热速率而产生的挠度很小(有限的熔化)。在固相线温度以上,发射率随温度的升高几乎保持恒定,并且温度与时间的关系曲线逐渐达到一个倾斜的平台,在该平台上样品的大部分熔化。随着加热速率和/或晶粒尺寸的增加,倾斜平台的起始温度接近合金液相线温度,而平台的斜率接近零。对温度-时间曲线形状的这种解释得到一个模型的支持,该模型包括固体中的扩散以及熔化过程中的热平衡。在这些实验中,在熔融过程中,没有证据表明熔融前沿的局部平衡损失。

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