于淼, 姜根山, 姜羽, 杨延锋, 孔倩. 声波诱导湍流的实验研究与模拟计算[J]. 动力工程学报, 2021, 41(6): 481-488. DOI: 10.19805/j.cnki.jcspe.2021.06.008
引用本文: 于淼, 姜根山, 姜羽, 杨延锋, 孔倩. 声波诱导湍流的实验研究与模拟计算[J]. 动力工程学报, 2021, 41(6): 481-488. DOI: 10.19805/j.cnki.jcspe.2021.06.008
YU Miao, JIANG Genshan, JIANG Yu, YANG Yanfeng, KONG Qian. Experimental Study and Numerical Simulation on Acoustic Wave Induced Turbulence[J]. Journal of Chinese Society of Power Engineering, 2021, 41(6): 481-488. DOI: 10.19805/j.cnki.jcspe.2021.06.008
Citation: YU Miao, JIANG Genshan, JIANG Yu, YANG Yanfeng, KONG Qian. Experimental Study and Numerical Simulation on Acoustic Wave Induced Turbulence[J]. Journal of Chinese Society of Power Engineering, 2021, 41(6): 481-488. DOI: 10.19805/j.cnki.jcspe.2021.06.008

声波诱导湍流的实验研究与模拟计算

Experimental Study and Numerical Simulation on Acoustic Wave Induced Turbulence

  • 摘要: 为了研究声波特性对流体流动的影响,搭建了声波与流体流动的实验平台,研究了调制声波频率和声压级等因素对流速的影响。利用Comsol软件对声场与流场进行数值计算,分析了流速实验值与计算值之间的相对误差。结果表明:声压级<125 dB时,声波不论与流体同向还是逆向对流速均无影响;当声压级在125~<132 dB,且声波与流体同向时,随着声压级的增大,流速脉动幅值变化减弱,强化了流体层流状态;当声压级在132~155 dB时,随着声压级的增大,流速脉动幅值增大,声压级达到153 dB左右时,流速脉动幅值产生爆发性增长从而引发湍流激变。声波与流体逆向时,当声压级在125~<145 dB,随着声压级的增大,流体脉动幅值先增大后变化缓慢;当声压级在145~155 dB时,随着声压级的增大,流体脉动幅值增大,在相同声压级条件下,随着声波频率的增大,流速脉动幅值变化缓慢;声波与流体同向时,声波频率对流体流速基本无影响;声波与流体逆向时流速脉动幅度的增长率要比声波与流体同向时低。

     

    Abstract: In order to study the influence of acoustic wave characteristics on fluid flow, an experimental platform was built based on which, the research for factors affecting on flow velocity such as acoustic wave frequency, sound pressure level(SPL), etc. In addition, sound and flow fields were numerically calculated via the Comsol software, and the errors between the experimental results and the calculated data were analyzed accordingly. Results show that when SPL is less than 125 dB, the flow velocity is not affected by the sound wave either in the same or opposite direction; when SPL lies in 125-<132 dB and the acoustic wave is in the same direction with fluid, the variation of the fluid velocity pulsation amplitude is weakened and the laminar flow state is strengthened with the increase of SPL; when SPL is 132-155 dB, the fluid velocity pulsation amplitude increases with the increase of SPL, and it would have an explosive increment and lead to turbulence shock when SPL reaches about 153 dB. Moreover, when the acoustic wave is in the opposite direction with fluid, the fluid velocity pulsation amplitude firstly increases and then changes slowly with the increase of SPL which lies in 125-<145 dB; when SPL is 145-155 dB, the fluid velocity pulsation amplitude also increases with SPL rising;, the fluid velocity pulsation amplitude has a slow variation with the increase of the sound wave frequency under the same SPL. The sound wave frequency has no effects on fluid velocity when the acoustic wave is in the same direction with fluid, and the growth rate of the fluid velocity pulsation amplitude is higher than that when the acoustic wave is opposite to the fluid.

     

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