引用本文:
【打印本页】   【HTML】 【下载PDF全文】   查看/发表评论  【EndNote】   【RefMan】   【BibTex】
←前一篇|后一篇→ 过刊浏览    高级检索
本文已被:浏览 2829次   下载 1005 本文二维码信息
码上扫一扫!
分享到: 微信 更多
导弹水下发射时喷管的气体流动
王晓宏1, 陈义良1, 李潜2, 刘长江2
1.中国科学技术大学热科学和能源工程系!安徽合肥230026;2.北京空气动力研究所!北京100074
摘要:
针对导弹水下发射时喷管的气体流动问题 ,建立了水下喷管流的简化模型 ,定性地研究水环境的惯性对水下喷管内气体流动造成的阻滞作用。计算显示受阻滞流量ΔQ及受阻滞时间Δt和喷管的喉部面积At 呈幂函数关系 ,固定其他参数仅改变水深 ,ΔQ及Δt和进口处气体的滞止压力p0 与当地水下静压之间的压力差也有幂函数关系。结果表明喷管所处的水下深度越大 ,喷管内气体流动受阻滞状况也就越严重 ,而减小喉部面积At 和适当增加膨胀比Ab/At 以及增加滞止压力p0 ,均有助于改善水环境对喷管喷出气体造成的阻滞状况。
关键词:  潜射导弹  水下点火  喷管气流  数学仿真
DOI:
分类号:V525
基金项目:中国科技大学青年基金 !(KB132 3);留学回国人员基金!(KB132 4)
Nozzle flows of the missile launching under water
Wang Xiao hong1, Chen Yi liang1, Li Qian2, Liu Chang jiang2
1.Dept. of Thermal Science and Energy Engineering, China Univ. of Science and Technology, Hefei 230026,China;2.Beijing Inst.of Aerodynamic Beijing 100074,China
Abstract:
A simple model was proposed to study the flows in the Laval nozzle under water. Numerical simulations show that there are power law relations for the obstruction mass flows Δ Q and the obstruction interval Δ t with the throat area A t of nozzle: Δ Q ∝ A 1.5 t ,Δ t ∝ A 0.5 t , and with the difference between the stagnant pressure p 0 and the local static pressure: Δ Q andΔ t ∝{[ p 0-( p 1+ ρ w gH )]/ ρ w } -0.76 when only changing the depth H . It is reasonable that the obstruction is stronger when increasing the depth H . Nevertheless, the obstruction can be decreased by decreasing the throat area A t, or increasing ratio of exit to throat areas A b/ A t or increasing stagnant pressure p 0.
Key words:  Submarime launched missle  Underwater firing:Nozzle flow  Mathematical Simulation.