等离子喷涂中氧化铝颗粒的模拟与测量

W. H. Zhuang, H.F. Chen, K. Etemadi, D. Benenson
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引用次数: 0

摘要

采用数值模拟和激光多普勒测速技术对等离子喷涂炬(Miller SG-100)进行了研究。给出了在冷空气环境中注入氧化铝颗粒的轴对称湍流氩等离子体射流的实验结果。该数学模型涉及等离子体射流的连续性、动量和能量方程的同时求解,以及等离子体中粒子的动力学和传热。计算采用抛物线和椭圆两种方法进行。紊流效应用k-E模型表示。湍流色散对粒子的影响也包括在内。考虑了等离子体射流与粒子之间的耦合。-在电流为900 a时,将模型确定的等离子体温度与实验结果进行了比较[1]。在距离喷嘴出口小于2cm处,差值小于4%。在更远的距离,模拟得到的等离子体温度比[1]中测量的温度高约3040%。在300 a电流下,将模拟得到的粒子速度与单次和双次注入时的LDV测量结果进行了比较。在距离喷管出口5.2 cm处,粒子速度通过L、DV测量和数值模拟得到峰值离轴分布。由模型确定的粒子速度比轴上LDV测量的粒子速度高20%。抛物线法和椭圆法测定的粒子速度之间的差异在5%以内。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Simulations And Measurements Of Alumina Particles In Plasma Spraying
A plasma spraying torch (Miller SG-100) has been studied by numerical modeling and Laser Doppler Velocimetry (LDV) techniques. Results are presented for axisymmetric turbulent argon plasma jets flowing into a cold air environment with the injection of alumina particles. The mathematical model involves the simultaneous solution of the continuity, momentum and energy equations for the plasma jet, and the dynamics and heat transfer of the particles in the plasma. Calculations are performed using the both parabolic and elliptic approaches. Turbulent effects are represented by the k-E model. The turbulent dispersion effect on the particles is also included. Coupling between the plasma jet and the particles is considered. -At a current of 900 A, plasma temperatures determined by modeling are compared with experimental results [l]. The difference is less than 4% at a distance less than 2 cm from the nozzle exit. At longer distance, plasma temperatures, obtained from modeling are about 3040% higher than those measured in [I] . At a current of 300 A, particle velocities obtained by the simulation are compared to LDV measurements with single and double injection. At a distance of 5.2 cm from the torch nozzle exit, particle velocities show a peak off-axis profile as measured by L,DV and as calculated by numerical modeling. Particle velocities determined from modeling are 20% higher than those measured by LDV at the axis. Differences between particle velocities determined from the parabolic and elliptic approaches are within 5%.
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