原位观察钢/铝界面铝酸钙夹杂物的聚结

Juntao Ba, Qiuyue Zhou, Ying Ren, Lifeng Zhang
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引用次数: 0

摘要

在本研究中,使用激光共聚焦扫描显微镜现场观察了不同 CaO 含量的 CaO-Al2O3 包裹体在钢/Ar 界面的聚集情况。测量并计算了夹杂物聚集过程中的临界加速距离和吸引力,分析了夹杂物成分和半径对夹杂物聚集的影响。当 16Mn 钢中 CaO-Al2O3 包裹体中的 CaO 含量从 3% 增加到 51% 时,包裹体逐渐从固态变为液态。固态夹杂物和部分液态夹杂物聚集成大的团块,最大直径为 446.2 μm。当包裹体中的 CaO 含量从 3 pct 增加到 26 pct 时,包裹体对之间的临界加速距离从 104.9 μm 减小到 62.1 μm,包裹体对之间的吸引力从 1.0 × 10-16 N~1.0 × 10-13 N 减小到 1.0 × 10-18 N~1.0 × 10-15 N。对于液体包裹体,当包裹体中的 CaO 含量从 38% 增加到 51% 时,临界减速距离从 59.7 μm 增加到 93.6 μm,排斥力从 1.0 × 10-17 N~5.0 × 10-15 N 增加到 1.0 × 10-17 N~1.0 × 10-13 N。计算得出的夹杂物之间的吸引力大于克拉切夫斯基-保诺夫模型计算得出的理论值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

In Situ Observation of Aggregation of Calcium Aluminate Inclusions at Steel/Ar Interface

In Situ Observation of Aggregation of Calcium Aluminate Inclusions at Steel/Ar Interface

In the current study, the aggregation of CaO-Al2O3 inclusions with different CaO contents at the steel/Ar interface was in situ observed using the confocal laser scanning microscope. The critical acceleration distance and attractive force during the inclusion aggregation process were measured and calculated, and effects of inclusion composition and radius on the aggregation of inclusions were analyzed. When the CaO content in CaO-Al2O3 inclusions in 16Mn steels increased from 3 to 51 pct, inclusions gradually changed from solid to liquid. Solid and partial liquid inclusions aggregated to form large clusters with a maximum diameter of 446.2 μm. When the CaO content in inclusions increased from 3 to 26 pct, the critical acceleration distance between inclusion pairs decreased from 104.9 to 62.1 μm, and the attractive force between inclusion pairs decreased from 1.0 × 10−16 N~1.0 × 10−13 N to 1.0 × 10−18 N~1.0 × 10−15 N. As the host inclusion radius increased from 5~15 to 25~35 μm, the critical acceleration distance increased from 104.9 to 166.6 μm. For liquid inclusions, when the CaO content in inclusions increased from 38 to 51 pct, the critical deceleration distance increased from 59.7 to 93.6 μm, and the repulsive force increased from 1.0 × 10−17 N~5.0 × 10−15 N to 1.0 × 10−17 N~1.0 × 10−13 N. The liquid inclusion overcame the repulsive force and aggregated, when the host inclusion radius was larger than 10 μm, and the initial velocity of the guest inclusion was faster than 150 μm/s. The calculated attractive force between inclusions was larger than the theoretical value calculated by Kralchevsky-Paunov model.

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