弹道与气动力技术

圆锥前体大攻角绕流的数值计算与分析

  • 王中一 ,
  • 郑博睿 ,
  • 高超 ,
  • 方洪 ,
  • 熊俊涛 ,
  • 刘锋 ,
  • 罗时钧
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  • 1 西北工业大学翼型/叶栅空气动力学国防科技重点实验室,西安 710072
    2 北京临近空间飞行器系统工程研究所,北京 100076
    3 美国加州大学尔湾分校,美国加州尔湾 92697-3975

王中一(1991-),男,山东聊城人,硕士研究生,研究方向:粒子成像测速。

收稿日期: 2012-09-03

  网络出版日期: 2025-05-26

基金资助

高等学校博士学科点专项科研基金(SPFDP-200806990003);西北工业大学基础研究基金(JC201103)

Numerical Computation and Analysis of Flow over A Conical Forebody at High Angle-of-attack

  • WANG Zhongyi ,
  • ZHENG Borui ,
  • GAO Chao ,
  • FANG Hong ,
  • XIONG Juntao ,
  • LIU Feng ,
  • LUO Shijun
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  • 1 Key Laboratory of National Defense Science and Technology of Airfoil, the Cascade Aerodynamic Design and Research,Northwestern Polytechnical University, Xi'an 710072, China
    2 Beijing Institute of Nearspace Vehicles System Engineering, Beijing 100076, China
    3 University of California, Irvine, CA 92697-3975, USA

Received date: 2012-09-03

  Online published: 2025-05-26

摘要

采用层流模型、Gammatheta转捩模型和SST湍流模型对半顶角10°的圆锥前体进行大攻角绕流的数值模拟,以探究其流动特性。给出了30m/s,不同攻角下流场的总压系数、速度矢量和涡量云图。研究发现,采用Gammatheta转换模型可较好的模拟转捩流动;攻角大于10°时出现主涡,每个主涡都有一个总压系数最小值和无量纲的轴向涡量绝对最大值,它们均位于涡核处,量值随风速和攻角而变化。

本文引用格式

王中一 , 郑博睿 , 高超 , 方洪 , 熊俊涛 , 刘锋 , 罗时钧 . 圆锥前体大攻角绕流的数值计算与分析[J]. 弹箭与制导学报, 2013 , 33(3) : 123 -125,152 . DOI: 10.15892/j.cnki.djzdxb.2013.03.044

Abstract

High angle-of-attack flow over a 20° conical forebody was computed with laminar model, Gamma theta transition model and turbulence model to study the flow characteristics. The contour of computed total pressure coefficient, velocity vector and axial vorticity distributions over the cross-flow plane at 30m/s and different angle-of-attack were plotted here for study. Through the comparison of experimental data with numerical solution, we can get that gamma theta transition model is proper to model flows mainly in transitional region. For angleof-attack greater than 10°, the port and starboard primary vortex occur. Each of them has a minimum value of total pressure coefficient and a maximum absolute value of non-dimensional axial vorticity in the vortex core. Both of them vary with the angle-of-attack and the wind velocity in some regular patterns.

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