首页> 外文期刊>Combustion and Flame >Simultaneous measurements of velocity and CH distributions. Part 1: jet flames in co-flow
【24h】

Simultaneous measurements of velocity and CH distributions. Part 1: jet flames in co-flow

机译:同时测量速度和CH分布。第1部分:并流喷射火焰

获取原文
获取原文并翻译 | 示例
       

摘要

Velocity field and CH distribution are measured simultaneously using particle-image velocimetry (PIV) and planar laser-induced fluorescence (PLIF) of CH in piloted, turbulent, jet flames in coflow. The CH distribution is found to correspond well with the location of the stoichiometric velocity, U_s, both instantaneously and on average. In addition, the CH distribution is observed to align with high-strain rate regions; however, significantly higher values of the maximum strain rates, compared to the mean value, are frequently observed. The residence time in the flame surface as represented by CH, τ_F, remains nearly constant with axial distance downstream and is found to scale as τ_F ~ d/U_b, where d and U_b are nozzle exit diameter and bulk nozzle-exit velocity, respectively. The mean value of the compressive principal strain rate is observed to decrease along the axial direction and shows a good correlation to a S ~ (x/d)~(-0.7) relation for a wide range of jet Reynolds numbers. Finally, the two-dimensional dilatation is not seen to be a good marker of the flame position, unlike the case for premixed flames.
机译:速度场和CH分布是使用粒子图像测速仪(PIV)和平面激光诱导的CH气流在顺流中的湍流射流火焰中同时测量的,并同时测量CH的分布。发现CH分布在瞬时和平均上都与化学计量速度U_s的位置很好地对应。另外,观察到CH分布与高应变率区域一致。然而,经常观察到最大应变率的平均值比平均值高得多。以CH表示的在火焰表面的停留时间τ_F,在下游轴向距离上几乎保持恒定,并且发现其比例为τ_F〜d / U_b,其中d和U_b分别是喷嘴出口直径和总体喷嘴出口速度。在大范围的雷诺数射流中,压缩主应变率的平均值沿轴向方向减小,并且与S〜(x / d)〜(-0.7)关系具有良好的相关性。最后,与预混火焰不同,二维膨胀不能看作是火焰位置的良好标志。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号