红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2015年
3期
879-883
,共5页
李胜勇%王晓宇%王江安%宗思光%刘涛
李勝勇%王曉宇%王江安%宗思光%劉濤
리성용%왕효우%왕강안%종사광%류도
环境压强%空泡%脉动特性%声波%频谱
環境壓彊%空泡%脈動特性%聲波%頻譜
배경압강%공포%맥동특성%성파%빈보
ambient pressure%bubble%oscillation properties%sound waves%spectrum
环境压强是影响空泡脉动的一个重要因素。为了研究环境压强对激光空泡声波特性的影响,采用理想液体中单空泡运动的理论模型,对不同环境压强下液体中空泡运动过程进行了数值模拟,并通过充气泵精确调节高压水箱内的气压,采用高速照相机、高频测量水听器,得到了在不同压强条件下,空泡脉动特性的序列图像和声谱图,根据实验数据研究了不同环境压强下液体中激光诱导产生的空泡脉动规律与声波特性。结果表明:环境压强的改变影响了空泡生存周期和脉动的剧烈程度,但对声波的强度和声谱分布没有影响。辐射的频率集中在0~50 kHz范围内,所辐射的声波能量主要集中在0~20 kHz频段范围,并在2 kHz与8 kHz有两个明显的频率峰值。
環境壓彊是影響空泡脈動的一箇重要因素。為瞭研究環境壓彊對激光空泡聲波特性的影響,採用理想液體中單空泡運動的理論模型,對不同環境壓彊下液體中空泡運動過程進行瞭數值模擬,併通過充氣泵精確調節高壓水箱內的氣壓,採用高速照相機、高頻測量水聽器,得到瞭在不同壓彊條件下,空泡脈動特性的序列圖像和聲譜圖,根據實驗數據研究瞭不同環境壓彊下液體中激光誘導產生的空泡脈動規律與聲波特性。結果錶明:環境壓彊的改變影響瞭空泡生存週期和脈動的劇烈程度,但對聲波的彊度和聲譜分佈沒有影響。輻射的頻率集中在0~50 kHz範圍內,所輻射的聲波能量主要集中在0~20 kHz頻段範圍,併在2 kHz與8 kHz有兩箇明顯的頻率峰值。
배경압강시영향공포맥동적일개중요인소。위료연구배경압강대격광공포성파특성적영향,채용이상액체중단공포운동적이론모형,대불동배경압강하액체중공포운동과정진행료수치모의,병통과충기빙정학조절고압수상내적기압,채용고속조상궤、고빈측량수은기,득도료재불동압강조건하,공포맥동특성적서렬도상화성보도,근거실험수거연구료불동배경압강하액체중격광유도산생적공포맥동규률여성파특성。결과표명:배경압강적개변영향료공포생존주기화맥동적극렬정도,단대성파적강도화성보분포몰유영향。복사적빈솔집중재0~50 kHz범위내,소복사적성파능량주요집중재0~20 kHz빈단범위,병재2 kHz여8 kHz유량개명현적빈솔봉치。
The ambient pressure is one of the basic factors determining cavitation. In order to investigate the influence of ambient pressure on properties of laser-induced cavitation bubble collapse sound waves, besides analysing the influence of ambient pressure on properties of laser-induced cavitation bubble oscillation, the experimental investigation of the laser-induced cavitation bubble callapse in liquids with different ambient pressure was done with high-speed video, the cavity sound waves generated by the cavitation bubble was detected with the high-frequency hydrophone. The pressure inside the tank was accurately controlled by an air pump. The results show that the ambient pressure has obvious influence on the bubble oscillation, but has no influence on sound intensity and spectrum. The radiation frequency range is 0- 50 kHz, the radiation sound wave energy is 0- 20 kHz, and have two obvious frequency peak value at 2 kHz and 8 kHz.