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Nucleation and early growth during solidification of aluminum-copper alloys.

机译:铝铜合金凝固过程中的形核和早期生长。

摘要

Using a relatively simple experimental setup, thermal history, microstructural evolution, nucleation, and early growth during solidification of aluminum-copper alloys are investigated. In particular, nucleation rates are measured, and contact angles calculated using the classical heterogeneous nucleation theory. Also, growth velocities of the dendrites are measured and compared with those predicted using kinetic models in order to elucidate which model is controlling during recalescence or early growth. Two groups of aluminum alloys with 5.1, 6.6, 15.6, and 30 wt% Cu are studied. One group is uninoculated and the other is grain refined with Ti-B-Al, Ti-B, and Ti-C-Al master alloys. In alloys that exhibit recalescence of primary solid, solidification occurs at a temperature, approximately 0.4 °C or less before the minimum in the curve is reached. Grain refined alloys exhibit dendrites which are equiaxed in morphology and appear as clusters in a matrix of quenched liquid. Uninoculated alloys, however, contain somewhat columnar dendrites. Nucleation rates are composition sensitive and range from 4.8 x 10¹³ m³/s to 1.6 x 10sp¹⁵ m³/s in uninoculated alloys; with an increase in copper content there is an increase in nucleation rate. In grain refined alloys, the same metric measures from 4.4 x 10¹⁶ m³/s to 1.4 x 10¹⁹ m³/s. The calculated contact angles are consistently smaller in the grain refined alloys when compared with their uninoculated counterparts and are rather sensitive to small changes in the measured undercooling. For example, if the undercooling with respect to the liquidus temperature is known to within ± 1°, the calculated contact angle changes by ± 0.8°. Experimental growth rates in grain refined alloys are less than in uninoculated alloys, because the undercoolings during the early stages of growth are less. While growth rate in uninoculated alloys typically range from 2.2 x 10⁻⁴ m/s in the most concentrated alloy to 1.8 x 10⁻³ m/s in the most dilute alloy, the same metric in grain refined alloys ranges from 7.8 x 10⁻⁵ m/s to 1.7 x 10⁻⁴ m/s. Experimental growth rates compare favorably to dendrite growth models of Ivantsov, and Lipton-Glicksman-Kurz. Consequently, during recalescence and/or early growth, the growth velocity of primary solid is controlled by solute diffusion processes and not by interface kinetics.
机译:使用相对简单的实验设置,研究了铝铜合金凝固过程中的热历史,微观组织演变,成核和早期生长。特别地,测量成核速率,并使用经典的异质成核理论计算接触角。同样,测量树枝状晶体的生长速度,并将其与使用动力学模型预测的速度进行比较,以阐明哪个模型在重新发光或早期生长过程中处于控制状态。研究了两组含5.1、6.6、15.6和30 wt%的铝合金的铝合金。一组未接种,另一组使用Ti-B-Al,Ti-B和Ti-C-Al中间合金进行晶粒细化。在表现出一次固体再度凝固的合金中,在达到曲线最小值之前,在约0.4°C或更低的温度下发生固化。晶粒细化的合金显示出枝晶,这些枝晶在形态上是等轴的,并以簇的形式出现在淬火液体的基质中。但是,未接种的合金含有一些柱状树枝状晶体。成核速率对成分敏感,在未接种的合金中,成核速率为4.8 x 10 13m³/ s至1.6 x 10 sp 17m³/ s。随着铜含量的增加,成核速率也增加。在晶粒细化合金中,相同的度量单位为4.4 x 10 15m³/ s至1.4 x 10 15m³/ s。与未接种的合金相比,晶粒细化合金中计算出的接触角始终较小,并且对测得的过冷度的微小变化相当敏感。例如,如果已知相对于液相线温度的过冷度在±1°以内,则计算出的接触角将变化±0.8°。晶粒细化合金的实验生长速率低于未接种合金,因为生长早期的过冷度较小。未接种合金的生长速率通常在最浓合金中为2.2 x10⁻⁴m / s,而在最稀合金中为1.8 x10⁻³m / s,而晶粒细化合金中相同的量度为7.8 x10⁻ ⁵m / s至1.7 x10⁻⁴m / s。实验增长率比Ivantsov和Lipton-Glicksman-Kurz的枝晶生长模型优越。因此,在重新钙化和/或早期生长期间,主要固体的生长速度由溶质扩散过程控制,而不是由界面动力学控制。

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