以N<sub>2</sub>O为工质的汽蚀文氏管流场仿真

史刚; 梁国柱

以N₂O为工质的汽蚀文氏管流场仿真

史刚,
梁国柱

北京航空航天大学宇航学院, 北京 100191

计量
- 文章访问数: 1747
- HTML浏览量: 126
- PDF量: 460
- 被引次数: 0
出版历程
- 收稿日期: 2011-03-05
- 修回日期: 2011-09-08
- 刊出日期: 2012-02-28

Flow field simulation of N₂O cavitation Venturi

School of Astronautics, Beijing University of Aeronautics and Astronautics, Beijing 100191, China

摘要

摘要: 为得到N₂O在汽蚀文氏管中的汽蚀流场分布,以实际气体状态方程和完全汽穴模型为基础,求解两相混合物流动的控制方程组.针对N₂O的特点,对三种不同工况下文氏管的汽蚀流场分别考虑汽化热和不考虑汽化热进行了仿真,并对两种计算结果进行了对比分析.考虑汽化热计算得到的汽蚀区比不考虑汽化热计算得到的要小,而且汽蚀区及周边温度有明显的变化,计算结果更加真实合理,说明了考虑汽化热计算的必要性和正确性,对汽蚀文氏管的设计有一定的指导作用.
- N₂O /
- 汽蚀文氏管 /
- 流场仿真 /
- 汽化热 /
- 汽蚀区
Abstract: In order to get the distribution of cavitation flow field of N₂O in cavitation Venturi,governing equations of two-phase mixture flow were solved based on state equation for real gas and full cavitation model.According to the special properties of N₂O,numerical simulation was performed on a cavitation Venturi under three experimental states.Two different methods:with and without the influences of latent heat were used respectively and comparison and analysis of two different results were made.The cavitation area calculated by the method considering the influences of latent heat was smaller and obvious change of temperature in and around the cavitation area was found.The results indicate that the necessity and correctness of calculation considering the influences of latent heat,which can be a certain guide for the design of Venturi.
- N₂O /
- cavitation Venturi /
- flow field simulation /
- latent heat /
- cavitation zone

HTML

参考文献(12)

[1]	Dyer J,Doran E,Dunn Z,et al.Modeling feed system flow physics for self-pressurizing propellants.AIAA-2007-5702,2007.
[2]	张小斌,曹潇丽,邱利民,等.液氧文氏管汽蚀特性计算流体力学研究[J].化工学报,2009,60(7):1638-1643. ZHANG Xiaobin,CAO Xiaoli,QIU Limin,et al.CFD study on cavitaion of liquid oxygen in Venturi[J].CIESC Journal,2009,60(7):1638-1643.(in Chinese)
[3]	王智勇,张晓冬,杨会中.文丘里管中空化流场的数值模拟[J].计算机与应用化学,2006,23(10):939-942. WANG Zhiyong,ZHANG Xiaodong,YANG Huizhong.Numerical simulation of cavitation flow field in the Venturi[J].Computers and Applied Chemistry,2006,23(10):939-942.(in Chinese)
[4]	黄建彬.工业气体手册[M].北京:化学工业出版社,2002.
[5]	朱明善,刘颖,林兆庄,等.工程热力学[M].北京:清华大学出版社,1995.
[6]	Span R,Wagner W.Equations of state for technical applications:I simultaneously optimized functional forms for nonpolar and polar fluids[J].International Journal of Thermophysics,2003,24(1):1-39.
[7]	Dabiri S,Sirignano S A,Joseph D D.Cavitation in an orifice flow.AIAA-2007-1118,2007.
[8]	Hosangadi A,Ahuja V.Numerical study of cavitation in cryogenic fluids[J].Journal of Fluids Engineering,2005,127(2):267-281.
[9]	XU Changhai,Heister S D,Collicott S H,et al.Modeling cavitating Venturi flows.AIAA-2002-3699,2002.
[10]	Bunnell R A,Heister S D,Yen C,et al.Cavitating injector flows:validation of numerical models and simulation of pressure atomizers[J].Atomization and Sprays,1999,9(5):445-465.
[11]	Tamaki N,Shimizu M,Nishida K,et al.Effects of cavitation and internal flow on atomization of a liquid jet[J].Atomization and Sprays,1998,8(2):179-197.
[12]	Zhang X B,Qiu L M,Gao Y,et al.Computational fluid dynamic study on cavitation in liquid nitrogen[J].Cryogenics,2008,48(9-10):432-438.