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不带导流板矩形腔流激振荡的幅值特性
引用本文:李大刚 陈家骅. 不带导流板矩形腔流激振荡的幅值特性[J]. 大连理工大学学报, 1999, 39(3): 440-444
作者姓名:李大刚 陈家骅
作者单位:大连理工大学动力工程系
基金项目:中国船舶总公司军工预研项目
摘    要:通过试验,分析,探讨了流激振荡的幅值特性和耦合振荡特性,发现在小迎角下,腔的驻波振荡占优势,其振荡产声压随迎角的增大而增大迎角下,流体动力振荡占优势,其振荡声压级随迎角的增大而增强,在大迎角下,流体动力振荡与腔的驻波振荡发生耦合共振,其耦合振荡声压级随迎角的增大而减小,耦合振荡的产生有限制条件,即迎角存在下限,流速存在上下限,上限流速随气流迎角的增大而增大。

关 键 词:流激振荡 幅值特性 矩形腔 风洞 导流板

Amplitude property about flow induced oscillation o f cavity without flange plate
LI Da gang, CHEN Jia hua. Amplitude property about flow induced oscillation o f cavity without flange plate[J]. Journal of Dalian University of Technology, 1999, 39(3): 440-444
Authors:LI Da gang   CHEN Jia hua
Abstract:The paper analyses and inquires into the amplitude property about the flow indu ced oscillation of the cavity without the flange plate by experiments. The follo wing results are valuable: (1)At small attack angle, the sound standing wave re sonance is dominant, and the sound pressure increases with increase of the attac k angle. (2)At large attack angle, the coupling oscillation between fluid dyna mic oscillation and sound standing wave resonance is found out and the oscillati on pressure decreases with increase of attack angle. (3)The formation of the co upling oscillation has criteria. The attack angle has a lower limit. And the fl ow speed has a finite range.
Keywords:fluid mechanics  oscillation/flow in duced oscillation  amplitude distribution analysis  fluid dynamic oscillation  s tanding waves
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