Abstract:The magnetostriction-induced ultrasonic cavitation flow was numerically simulated by using “Singhal full cavitation model” and the dynamic mesh technique. The computational results show that cavitation occurs at the local flow field proximity to the specimen and the specimen is subjected to impact of impulse pressure due to high frequency vibration of specimen. Pressure and vapor volume fraction (VVF) are annularly distributed around the center on the specimen, which vary periodically with vibration. Bubbles collapse after twice oscillation on the center region of specimen, which results in intense impulse pressure that can reach about 5MPa. Impulse pressure forms on the interval annular zones and alternately occurs on the adjacent annular zones with vibration cycle. Acoustic pressure quickly attenuates with ultrasonic propagation in the ultrasonic cavitation flow field. The considerable fluctuation of pressure occurs within the distance of 20mm to the end of ultrasonic solid horn. The impulse pressure is promoted on the central region of specimen as the vibration amplitude is increased from 25μm to 30μm. When the vibration amplitude is further increased to 35μm, the effect of cavitation is further enhanced, but the impulse pressure is diminished on the central region of specimen.
[1] Dular M, Bachert B, Stoffel B, et al. Relationship between cavitation structures and cavitation damage[J]. Wear, 2004, 257: 1176-1184.
[2] 朱建元. 船舶柴油机[M]. 北京: 人民交通出版社, 2004.
[3] Leighton T G. The Acoustic Bubble[M]. London: Academic Press, 1997.
[4] Mørch K A. Erosion[M]. London: Academic Press, 1979.
[5] 夏冬生, 张会臣, 张信伟. 基于CFD的柴油机气缸套冷却水空化特性数值分析[J]. 内燃机学报, 2010, 28(4): 368-373.
XIA Dong-sheng, ZHANG Hui-chen, ZHANG Xin-wei. Numerical simulation of cooling-water cavitation of diesel engine cylinder liner by CFD[J]. Transactions of CSICE, 2010, 28(4): 368-373.
[6] 夏冬生, 张会臣, 于彦. 柴油机气缸套冷却水空化流的三维数值模拟[J]. 机械工程学报, 2011, 47(22): 167-173.
XIA Dong-sheng, ZHANG Hui-chen, YU Yan. 3D numerical simulation of cooling-water cavitation flow of cylinder liner for a diesel engine[J]. Chinese Journal of Mechanical Engineering, 2011, 47(22): 167-173.
[7] Ahmed S M. Investigation of the temperature effects on induced impact pressure[J]. Wear, 1998, 218(1): 119-127.
[8] 葛晗, 秦力, 蒋亮, 等. 表面形貌与空化噪声的相关性研究[J]. 润滑与密封, 2010, 35(4): 10-13.
GE Han, QIN Li, JIANG Liang, et al. Correlation studies on surface roughness and cavitation noise[J]. Lubrication Engineering, 2010, 35(4): 10-13.
[9] 邵志文, 乐启炽, 崔建忠. 镁合金熔体中超声空化泡行为的数值模拟[J]. 东北大学学报, 2010, 31(7): 962-965.
SHAO Zhi-wen, LE Qi-chi, CUI Jian-zhong. Numerical simulation of ultrasound-induced cavitation bubbling behavior in magnesium alloy melt[J]. Journal of Northeastern University , 2010, 31(7): 962-965.
[10] Burdin F, Tsochatzidis N A, Guiraud P, et al. Characterisation of the acoustic cavitation cloud by two laser techniques[J]. Ultrasonics Sonochemistry, 1999. 6: 43-51.
[11] Singhal A K, Athavale M M, Li H Y, et al. Mathematical basis and validation of full cavitation model[J]. Journal of Fluid Engineering, 2002, 124(3): 617-624.
[12] Tan L, Cao S L, Wang Y M, et al. Numerical simulation of cavitation in a centrifugal pump at low flow rate[J]. Chinese Physics Letters, 2012, 29(1): 014702.
[13] Tan L, Zhu B S, Cao S L, et al. Cavitation flow simulation for a centrifugal pump at a low flow rate[J]. Chinese Science Bulletin, 2013, 58(8): 949-952.
[14] Menter F R. Two-equation eddy-viscosity turbulence models for engineering applications[J]. AIAA Journal, 1994, 32(8): 1598-1605.
[15] Fluent Inc. Fluent 6.3 user’s guide [M]. Labnon,New Hampshire. Fluent inc., 2006.