南京理工大学学报(自然科学版)
南京理工大學學報(自然科學版)
남경리공대학학보(자연과학판)
JOURNAL OF NANJING UNIVERSITY OF SCIENCE AND TECHNOLOGY
2014年
2期
228-233
,共6页
张焕好%陈志华%姜孝海%黄振贵
張煥好%陳誌華%薑孝海%黃振貴
장환호%진지화%강효해%황진귀
射流%剪切层%气动声学%大涡模拟%涡合并
射流%剪切層%氣動聲學%大渦模擬%渦閤併
사류%전절층%기동성학%대와모의%와합병
jet flow%shear layers%aeroacoustics%large-eddy simulation%vortex pairing
为了探讨亚声速射流气动声场中的主要噪声源以及声波产生机理,基于大涡模拟方法与高精度加权本质无振荡混合格式,对亚声速脉冲射流初始流场的发展过程进行了数值模拟,并根据得到的动力学流场对气动声场进行了直接计算。数值结果描述了射流剪切层在Kelvin-Helmholtz不稳定作用下失稳卷起小涡序列以及相邻小涡间相互旋转合并现象,并发现脉冲射流场的主要声源包括由前导压缩波形成的脉动噪声源、涡合并形成的四极子声源以及涡核内因涡卷起、变形与破碎所形成的湍流混合噪声源。其中,脉动噪声源最强,而涡合并所产生的四极子声源在整个声场中占主导地位。
為瞭探討亞聲速射流氣動聲場中的主要譟聲源以及聲波產生機理,基于大渦模擬方法與高精度加權本質無振盪混閤格式,對亞聲速脈遲射流初始流場的髮展過程進行瞭數值模擬,併根據得到的動力學流場對氣動聲場進行瞭直接計算。數值結果描述瞭射流剪切層在Kelvin-Helmholtz不穩定作用下失穩捲起小渦序列以及相鄰小渦間相互鏇轉閤併現象,併髮現脈遲射流場的主要聲源包括由前導壓縮波形成的脈動譟聲源、渦閤併形成的四極子聲源以及渦覈內因渦捲起、變形與破碎所形成的湍流混閤譟聲源。其中,脈動譟聲源最彊,而渦閤併所產生的四極子聲源在整箇聲場中佔主導地位。
위료탐토아성속사류기동성장중적주요조성원이급성파산생궤리,기우대와모의방법여고정도가권본질무진탕혼합격식,대아성속맥충사류초시류장적발전과정진행료수치모의,병근거득도적동역학류장대기동성장진행료직접계산。수치결과묘술료사류전절층재Kelvin-Helmholtz불은정작용하실은권기소와서렬이급상린소와간상호선전합병현상,병발현맥충사류장적주요성원포괄유전도압축파형성적맥동조성원、와합병형성적사겁자성원이급와핵내인와권기、변형여파쇄소형성적단류혼합조성원。기중,맥동조성원최강,이와합병소산생적사겁자성원재정개성장중점주도지위。
To discuss the main sources of aeroacoustic field and generation mechanism of acoustic waves,the process of initial flow field development in a subsonic pulse jet is simulated by using the large-eddy simulation and the high-order hybrid-weight essentially non-oscillatory scheme, and the corresponding aeroacoustic field is calculated directly based on the obtained dynamics flow. The numerical results reveal the phenomena of the vortexlets rolled up due to the Kelvin-Helmholtz instability of jet shear layer and the pairing process of neighbor vortices. Calculation results also reveal that the main acoustic sources of the pulse jet include the pulse acoustic source generated by precursor compressible waves, the quadrupole source generated by the vortex pairing and the turbulent blend acoustic sources caused by rolling up,deforming and breakup of the vortexlets within the main vortex ring. The pulse acoustic source is the strongest and the quadrupole source dominates the whole acoustic field.