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夏碧珠, 崔长文, 李强. 等离子喷涂层片形成过程流体动力学模拟[J]. 焊接学报, 2012, (2): 85-89.
引用本文: 夏碧珠, 崔长文, 李强. 等离子喷涂层片形成过程流体动力学模拟[J]. 焊接学报, 2012, (2): 85-89.
XIA Bizhu, CUI Changwen, LI Qiang. Computational fluid dynamics simulation of splat formation process in plasma spraying[J]. TRANSACTIONS OF THE CHINA WELDING INSTITUTION, 2012, (2): 85-89.
Citation: XIA Bizhu, CUI Changwen, LI Qiang. Computational fluid dynamics simulation of splat formation process in plasma spraying[J]. TRANSACTIONS OF THE CHINA WELDING INSTITUTION, 2012, (2): 85-89.

等离子喷涂层片形成过程流体动力学模拟

Computational fluid dynamics simulation of splat formation process in plasma spraying

  • 摘要: 建立了等离子喷涂层片形成过程的流动、传热和凝固耦合的三维数学模型,基于计算流体力学软件Fluent,运用有限体积法(FVM)离散控制方程,流体体积跟踪法(VOF)追踪熔滴自由表面,模拟了镍熔滴撞击基底表面形成层片的流体动力学过程,并对结果可视化输出.结果表明,撞击开始时刻,压力在撞击点出现最大值,熔滴内部压力场呈"蘑菇云"状,撞击压力分布从撞击点向熔滴上部递减;熔滴撞击后沿径向铺展,速度矢量场出现两个对称漩涡,在基底导热和熔体流动传热综合作用下,铺展熔滴内部温度场呈"驼峰"状分布;熔滴铺展速度最大值滞后最大撞击压力0.03μs出现.

     

    Abstract: A 3D computational model of the splat formation process was established to simulate the flow,heat transfer and solidification of a Ni droplet impacting on the surface of mild steel substrate with the computational fluid dynamics(CFD) software Fluent.The governing equations were discretized according to typical finite volume method(FVM).A volume of fluid(VOF) tracking algorithm was used to track the droplet free surface.Meanwhile,the simulated results were visualized.The results indicated that the maximum pressure was found at the impact point at the beginning of impact.The pressure distribution inside the deformed droplet during the spreading which came from the impacting was in the shape of a mushroom cloud,and the impact pressure decreased from the impact point to the top side of the droplet.The fluid spreaded radially outward during flattening which was accompanied by impact,consequently two symmetrical vortices appeared in the velocity vector field.Correspondingly,the temperature distribution in the deformed droplet exhibits'camel-hump'shape associated with the combined interaction of the substrate conductivity and convective heat transfer of the melt droplet.The occurrence time of the maximum spreading velocity raised from the impacting delay of 0.03 μs compared with that of the maximum impact pressure.

     

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