横向声波扰动下的乙醇燃烧火焰结构和振荡特性

Flame structure and oscillation characteristics of ethanol pool flame under transverse acoustic force

  • 摘要: 为研究声波灭火的机理,分析声波对非封闭火焰的具体控制行为,对3、4和5 cm直径油池火焰在30 ~ 90 Hz声波作用下的火焰形态及燃烧特征进行了分析。对火焰图像的分析发现,横向声波加剧了涡旋的不稳定运动,声强迫下的火焰形态可归结为间歇截断、偏转和稳定燃烧三种状态。火焰几何尺寸的数值分析表明:间歇截断和偏转状态下的火焰表面高度扭曲皱褶,具有更高的分形维数。对火焰面积、高度和宽度的频域信号分析表明:在间歇截断状态下火焰信号极不稳定,频域峰值集中在0 ~ 10 Hz之间,声频率在火焰宽度信号的频域分布中始终突出。基于火焰倾角和Richardson数的关系提出了Ri数在声波作用下的形式,Richardson数分析表明:在50 ~70 Hz之间,火焰对声波频率的响应尤为显著,声频高于或低于该段频率时对火焰的影响存在边际效应,间歇截断和偏转状态的临界Ria−1数(声波作用下的火焰Richardson数的倒数)分别为10.32和2.92。

     

    Abstract: Clean and efficient fire extinguishing technology has been a hot research topic in fire science. The research of acoustic extinguishing technology originates from the discovery that the different acoustic modes of combustion noise can lead to an unstable oscillation of the flame and local flame extinction. Recently, acoustic extinguishing technology has gradually entered the research field of scholars because it is clean and exhibits no secondary pollution. To study the fire extinguishing mechanism and analyze the specific control behavior of the acoustic wave on an unclosed flame, the flame shapes and the combustion characteristics of the pool flame with 3, 4, and 5 cm diameters under a 30–90 Hz acoustic force were analyzed. The experimental system includes a high-speed camera, signal generator, power amplifier, loudspeaker, and acoustic signal analysis device. The flame image analysis shows that the transverse sound wave intensifies the unsteady flow of the vortex, and the flame shape under an acoustic force could be divided into three types of state: intermittent, deflective, and stable. The numerical analysis of the flame geometry shows that the flame surface is highly twisted and wrinkled under the intermittent and deflective states with a higher fractal dimension. The frequency-domain signal analysis of the flame area, height, and width shows that the flame signal is very unstable in the intermittent state, and the peak frequency domain is concentrated in the range of 0–10 Hz. The acoustic frequency is always prominent in the frequency distribution of the flame width signal. Based on the relationship between the flame inclination angle and Richardson number, the form of the latter under the action of the acoustic wave was proposed. In the 50–70 Hz range, the response of the flame to the acoustic frequency was particularly considerable, and there may be a marginal effect when the acoustic frequency is higher or lower than the said range. The critical Ria−1 of the intermittent and deflective states are 10.32 and 2.92, respectively.

     

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