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Control of the Radiation of Screech Tone by Cavity Tone Generated in the Supersonic Jets

Control of the Radiation of Screech Tone by Cavity Tone Generated in the Supersonic Jets
超音速喷气机空腔音对尖叫音辐射的控制
批准号:
09650187
负责人:
UMEDA Yoshikuni
金额:
$2.11万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for Scientific Research (C)
财政年份:
1997
资助国家:
日本
项目状态:
已结题
起止时间:
1997 至 1998

项目摘要

项目成果

相关文献

中文摘要
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英文摘要
In recent years, a supersonic passenger airplane of next generation is developping. The supersonic jets will be used as the thrust of this airplane. However, it is well known that very strong sound waves called screech tone is radiated. This screech tone is generated by the feedback loop consisting of downstream-convecting coherent vortical structures around the jet and upstream-propagating sound waves in the ambient. The radiation of such very intense noise from the supersonic jets will cause the serious noise pollution near the airports as well as the fatigue failure of the airplanes. Therefore, this experimental study was performed to clarify the possibilty of the noise reduction radiated from supersonic jets. The acoustical characteristics of the cavity tone and the screech tone radiated by the jet issuing from a rectangular nozzle with cavity were investigated in the last year. In this year, the acoustical characteristics of the tones radiated by the supersonic jet discharged from … More the circular nozzle with cavity were investigated. From the experimental results, the following things were found : (1) The screech tone whose frequency is higher than that of cavity tone is effectively reduced. (2) The sound pressure level (SPL) of the screech tone radiated from the jets exhausting from the nozzle with cavity becomes lower than that of the screech tone radiated from the free jet discharging from the nozzle without cavity by about 30dB at most. The SPL of the cavity tone is lower than that of the screech tone radiated from the free jet issuing from the nozzle without cavity by about 20dB at most. (3) When the length of the cavity is 1.2 times the nozzle diameter, one of two resonance frequencies, 11.5kHz and 14.0kHz, is appeared. When the frequency of the cavity tone of 11.5kHz is appeared in the pressure ratio range higher than 3.5, the frequency is changed into 14.0kHz abruptly during decreasing of the pressure ratio. The reverse process is not observed. When the cavity tone is produced in the pressure ratio range lower than 3.5, it is observed that the frequency of the cavity tone firstly appeared is not changed during decreasing of the pressure ratio. Less
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会议论文
Y.Umeda and R.Ishii: "Oscillation modes of supersonic multijets" J.Acoustical Soc.America. 101. 3353-3360 (1997)
Y.Umeda 和 R.Ishii:“超音速多喷嘴的振荡模式”J.Acoustical Soc.America。
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Y.Umeda: "Acoustical Characteristics of the noise radiated from supersonic multi-jets" Proc.16th International Cong.on Acoustics and 135th Meeting Acoust.Soc.America(Seattle, Wa.), Vol.4aPAc15. 1967-1968 (1998)
Y.Umeda:“超音速多喷嘴辐射噪声的声学特性”Proc.16th International Cong.on Acoustics and 135th Meeting Acoust.Soc.America(华盛顿州西雅图),Vol.4aPAc15。
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Y.Umeda,R.Ishii: "Acoustical characteristics of the noise radiated from supersonic multi-jets" Proc.16th international congress on Acoustics and 135th Meeting Acoust.Soc.America(Seattle.Wa.). 4aPAc15. 1967-1968 (1998)
Y.Umeda、R.Ishii:“超音速多喷嘴辐射噪声的声学特性”,第 16 届国际声学大会和第 135 届美国声学协会会议(华盛顿州西雅图)。
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Y.Umeda: "Osillation modes of supersonic multijets" J.Acoust.Soc.America. Vol.101. 3353-3360 (1997)
Y.Umeda:“超音速多喷嘴的振荡模式”J.Acoust.Soc.America。
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