推进技术
推進技術
추진기술
JOURNAL OF PROPULSION TECHNOLOGY
2015年
4期
595-600
,共6页
刘焜%余永刚%赵娜%王珊珊
劉焜%餘永剛%趙娜%王珊珊
류혼%여영강%조나%왕산산
撞击式喷嘴%雾化%液滴%小尺度空间%周向分布
撞擊式噴嘴%霧化%液滴%小呎度空間%週嚮分佈
당격식분취%무화%액적%소척도공간%주향분포
Impinging nozzle%Spray%Droplet%Small scale space%Circumferential distributions
为了研究小推力液体火箭发动机燃烧室的喷雾燃烧特性,设计了小尺度模拟燃烧室和对撞射流喷嘴,利用多普勒相位粒子动态分析仪(PDA),观测了对撞射流在小尺度空间内的喷雾,重点观测了喷雾压力对于雾化特性参数的影响。实验结果表明:测量截面与喷嘴的距离越远,液滴平均直径越大,轴向速度越小;测量点到中心轴的距离越远,液滴轴向速度越小,径向速度波动越大;喷雾压力越大,液滴平均直径越小,轴向速度越大。由于受到壁面的影响,径向速度的周向分布在不同的喷雾压力下和测量点位置上的差异不明显;模拟燃烧室内液滴平均直径大于大气环境下的液滴平均直径,两者差值随着喷雾向下游发展而增大;模拟燃烧室对于液滴轴向速度影响较小,而对于液滴径向速度影响较明显。
為瞭研究小推力液體火箭髮動機燃燒室的噴霧燃燒特性,設計瞭小呎度模擬燃燒室和對撞射流噴嘴,利用多普勒相位粒子動態分析儀(PDA),觀測瞭對撞射流在小呎度空間內的噴霧,重點觀測瞭噴霧壓力對于霧化特性參數的影響。實驗結果錶明:測量截麵與噴嘴的距離越遠,液滴平均直徑越大,軸嚮速度越小;測量點到中心軸的距離越遠,液滴軸嚮速度越小,徑嚮速度波動越大;噴霧壓力越大,液滴平均直徑越小,軸嚮速度越大。由于受到壁麵的影響,徑嚮速度的週嚮分佈在不同的噴霧壓力下和測量點位置上的差異不明顯;模擬燃燒室內液滴平均直徑大于大氣環境下的液滴平均直徑,兩者差值隨著噴霧嚮下遊髮展而增大;模擬燃燒室對于液滴軸嚮速度影響較小,而對于液滴徑嚮速度影響較明顯。
위료연구소추력액체화전발동궤연소실적분무연소특성,설계료소척도모의연소실화대당사류분취,이용다보륵상위입자동태분석의(PDA),관측료대당사류재소척도공간내적분무,중점관측료분무압력대우무화특성삼수적영향。실험결과표명:측량절면여분취적거리월원,액적평균직경월대,축향속도월소;측량점도중심축적거리월원,액적축향속도월소,경향속도파동월대;분무압력월대,액적평균직경월소,축향속도월대。유우수도벽면적영향,경향속도적주향분포재불동적분무압력하화측량점위치상적차이불명현;모의연소실내액적평균직경대우대기배경하적액적평균직경,량자차치수착분무향하유발전이증대;모의연소실대우액적축향속도영향교소,이대우액적경향속도영향교명현。
To investigate the spray characteristic in the combustion chamber of the low thrust liquid rocket engine,the small scale simulation chamber and the impinging nozzle were designed. The impinging spray was ob?served with the PDA system. The effects of the pressure on the spray parameters were analyzed emphatically. The results indicate that,the further away from the nozzle,the larger the mean diameter of the droplets is and the lower the axial velocity is. The further the measuring point from the center axis is,the smaller the axial velocity of the droplets is and the more the fluctuation of the radial velocity is. The greater the nozzle pressure is,the smaller the mean diameter of the droplets is and the higher the axial velocity is. Under the influence of the chamber wall ,the effects of the spray pressure and the measuring point location on the circumferential distributions of the radial ve?locity are not obvious. The mean diameter of the droplets in the simulation chamber is larger than that in atmo?sphere environment,and the difference increases as the spray develops downstream. The simulation chamber af?fects the axial velocity of the droplets slightly,but the radial velocity seriously.