留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

菱形口射流与超音主流的相互作用

樊怀国 张春晓 何川

樊怀国, 张春晓, 何川. 菱形口射流与超音主流的相互作用[J]. 应用数学和力学, 2005, 26(10): 1209-1215.
引用本文: 樊怀国, 张春晓, 何川. 菱形口射流与超音主流的相互作用[J]. 应用数学和力学, 2005, 26(10): 1209-1215.
FAN Huai-guo, ZHANG Chun-xiao, HE Chuan. Diamond Port Jet Interaction With Supersonic Flow[J]. Applied Mathematics and Mechanics, 2005, 26(10): 1209-1215.
Citation: FAN Huai-guo, ZHANG Chun-xiao, HE Chuan. Diamond Port Jet Interaction With Supersonic Flow[J]. Applied Mathematics and Mechanics, 2005, 26(10): 1209-1215.

菱形口射流与超音主流的相互作用

详细信息
    作者简介:

    樊怀国(1966- ),男,浙江人,讲师,博士(联系人.Tel:+86-23-65112117;Fax:+86-23-65102473;E-mail:hfan@cqu.edu.cn).

  • 中图分类号: O358

Diamond Port Jet Interaction With Supersonic Flow

  • 摘要: 基于在不同射流角(10°, 27.5°, 45°, 90°)和射流总压(0.1 MPa, 0.46 MPa)下,对音速次膨胀射流通过菱形口喷射到马赫5横穿主流的实验及圆形射流器的对比实验,研究了次膨胀射流与超音横穿主流相互作用流场, 实验包括横截面流场的Pitot和锥静压力, 获得横截面马赫数、 压力分布.结果表明近壁面低马赫数半圆区为尾区,尾区附近边界层减薄.脱体激波高度向自由流扩展,激波形状更弯曲, 低马赫数区较大.高射流压力和射流角增加羽流涡度,激波位置较高.90°菱形和圆形喷射器有更强的羽流涡度,但圆形喷射器的低马赫数区较小.前沿渐细的变壁面的斜面物增加羽流涡度,反之,双变壁面的斜面物减弱羽流涡度.通过表面激波形状、中心平面激波及横截面激波模化三维激波形状,激波总压损失用正激波关系式通过马赫数法向分量估计.激波总压损失随射流角和动压比的减小而减小,最大损失发生在90°圆形和菱形喷射器.
  • [1] Weber R,Mckay J.Analysis of ramjet engines using supersonic combustion[R]. Washington DC: National Aeronautics and Space Administration,NASA TN-4386,1958.
    [2] Mccann G J,Bowersox R D W.Experimental investigation of supersonic gaseous injection into a supersonic freestream[J].AIAA J,1996,34(2):317—323. doi: 10.2514/3.13066
    [3] Schetz J A,Billig F S.Penetration of gaseous jets injected into a supersonic stream[J].Journal of Spacecraft,1966,3(11):1658—1665. doi: 10.2514/3.28721
    [4] Chenault L,Beran P,Bowersox R.Second-order Reynolds stress turbulence modeling of three-dimensional oblique supersonic injection[J].AIAA J,1999,37(10):1257—1269. doi: 10.2514/2.594
    [5] Bowersox R D W,Schetz J A.Compressible turbulence measurements in a high-Reynolds-number mixing layer[J].AIAA J,1994,32(4):758—764. doi: 10.2514/3.12050
    [6] Schetz J A,Thomas R H,Billig F S.Mixing of transverse jets and wall jets in supersonic flow[A].In:Kozlov V V,Dovgal A V Eds.Separated Flows and Jets.IUTAM Symposium[C].Berlin:Springer-Verlag,1990,807—837.
    [7] Barber M,Schetz J,Roe L.Normal sonic helium injection through a wedge-shaped orifice into a supersonic flow[J].Propulsion and Power,1997,13(2):257—263. doi: 10.2514/2.5157
    [8] Fan H,Bowersox R.Gaseous injection through diamond orifices at various incidence angles into a hypersonic freestream[A].In:AIAA Ed.39th AIAA Aerospace Sciences Meeting & Exhibit[C].Reston, USA: American Institute of Aeronautics and Astronautics,AIAA Paper 2001-1050,2001.
    [9] Wilson M P,Bowersox R D W,Glawe D D.Experimental investigation of the role of downstream ramps on a supersonic injection plume[J].Journal of Propulsion and Power,1999,15(3):432—439. doi: 10.2514/2.5462
    [10] Mcclinton C.The effects of injection angle on the interaction between sonic secondary jets and a supersonic freestream[R]. Washington DC: National Aeronautics and Space Administration,NASA TN D-6669,1972.
    [11] Volluz R.Handbook of supersonic aerodynamics[R]. Section 20.Wind Tunnel Instrumentation and Operation,Vol 6,Ordnance Aerophysics Lab, NAVORD Rept 1488, Daingerfield, TX 1961.
    [12] White F.Viscous Fluid Flow[M].New York:McGraw-Hill,1991.
  • 加载中
计量
  • 文章访问数:  2632
  • HTML全文浏览量:  113
  • PDF下载量:  753
  • 被引次数: 0
出版历程
  • 收稿日期:  2004-02-23
  • 修回日期:  2005-05-13
  • 刊出日期:  2005-10-15

目录

    /

    返回文章
    返回