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Effect of acoustic field parameters on arc acoustic binding during ultrasonic wave-assisted arc welding
Institution:1. Shanghai Key Laboratory of Materials Laser Processing and Modification, School of Materials Science and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, 200240, PR China;2. Shanghai Electric Nuclear Power Equipment Co. Ltd., Shanghai, 201306, PR China;1. College of Materials Science and Engineering, Chongqing University, Chongqing, 400030, China;2. The School of Robot Engineering and Mechanical - Electrical Engineering, Chongqing University of Arts and Sciences, Yongchuan, 402168, China;1. Tianjin Key Laboratory of Advanced Joining Technology, Tianjin University, Tianjin, 300354, China;2. School of Materials Science and Engineering, Tianjin University, Tianjin, 300354, China;1. State Key Laboratory of Advanced Welding and Joining, Harbin Institute of Technology, Harbin 150001, China;2. Shandong Provincial Key Laboratory of Special Welding Technology, Harbin Institute of Technology at Weihai, Weihai 264209, China;1. School of Mechanical Engineering and Automation, Beihang University, Beijing 100191, China;2. Beijing Xinfeng Aerospace Equipments Co. Ltd., Beijing 100854, China;3. Capital Aerospace Machinery Co. Ltd., Beijing 100706, China;4. Shanghai Aerospace Equipments Manufacturer Co., Ltd., Shanghai 200245, China;5. Beijing Hangxing Machinery Co. Ltd., Beijing 100013, China
Abstract:As a newly developed arc welding method, power ultrasound has been successfully introduced into arc and weld pool during ultrasonic wave-assisted arc welding process. The advanced process for molten metals can be realized by utilizing additional ultrasonic field. Under the action of the acoustic wave, the plasma arc as weld heat source is regulated and its characteristics make an obvious change. Compared with the conventional arc, the ultrasonic wave-assisted arc plasma is bound significantly and becomes brighter. To reveal the dependence of the acoustic binding force on acoustic field parameters, a two-dimensional acoustic field model for ultrasonic wave-assisted arc welding device is established. The influences of the radiator height, the central pore radius, the radiator radius, and curvature radius or depth of concave radiator surface are discussed using the boundary element method. Then the authors analyze the resonant mode by this relationship curve between acoustic radiation power and radiator height. Furthermore, the best acoustic binding ability is obtained by optimizing the geometric parameters of acoustic radiator. In addition, three concave radiator surfaces including spherical cap surface, paraboloid of revolution, and rotating single curved surface are investigated systematically. Finally, both the calculation and experiment suggest that, to obtain the best acoustic binding ability, the ultrasonic wave-assisted arc welding setup should be operated under the first resonant mode using a radiator with a spherical cap surface, a small central pore, a large section radius and an appropriate curvature radius.
Keywords:Radiator parameters  Boundary element analysis  Acoustic binding  Ultrasonic wave-assisted arc
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