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Visualization of Marangoni Convection in Simulated Weld Pools

机译:模拟焊池中Marangoni对流的可视化

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摘要

A transparent pool of NaNO_3 (10 mm in diameter) was heated with a defocused CO_2 laser beam to simulate Marangoni convection in arc weld pools without a surface-active agent. The flow patterns were revealed clearly by flow vi-sualization with a laser light-cut technique, the surface temperature profiles were measured immediately below the pool surface, and a device for measuring the beam diameter was developed. The observed Marangoni convection was expected to resemble that in welding because the Marangoni number was close to those in welding. Two counterrotating cells were observed in the meridian plane of the pool. The maximum velocity was at the pool surface, the outward surface flow was much faster than the inward return flow and the centers of the cells were near the pool edge. These characteristics suggest Marangoni convection dominates in the pool over gravity-induced convection. Increasing the beam power (from 0.5 to 5.4 W) and reducing the beam diameter (from 5.9 to 1.5 mm) both made Marangoni convection stronger. The latter, however, had a significantly greater effect; the surface flow was so much stronger as to make the return flow penetrate deeper into the pool. The results of physical simulation provided interesting insights for understanding the significant effect of Marangoni convection on the weld pool shape, as will be presented in a follow-up report.
机译:用散焦的CO_2激光束加热透明的NaNO_3熔池(直径为10毫米),以模拟没有表面活性剂的电弧焊熔池中的Marangoni对流。通过使用激光切割技术进行流可视化,可以清楚地显示出流型,在池表面的正下方测量表面温度分布,并开发了一种用于测量束直径的装置。预期观察到的Marangoni对流与焊接中的对流相似,因为Marangoni数接近于焊接中的对流。在水池的子午面上观察到两个反向旋转的细胞。最大速度是在池表面,向外表面的流动要比向内回流快得多,并且细胞的中心在池的边缘附近。这些特征表明,在重力引起的对流中,Marangoni对流在池中占主导地位。增加光束功率(从0.5到5.4 W)和减小光束直径(从5.9到1.5 mm)都使Marangoni对流更强。然而,后者的作用要大得多。地表水的强度要大得多,以至于回流会更深地渗入水池。物理模拟的结果为理解Marangoni对流对焊池形状的重大影响提供了有趣的见解,将在后续报告中介绍。

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