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| 1 | 基于气体射流的气液两相流动减阻特性显示文摘为了明确射流表面减阻特性,基于气液两相流动原理,建立具有射流功能的气液两相流动减阻计算模型,采用数值计算方法,通过RNG k-ε湍流模型对射流表面不同射流方向角、以及不同气体射流速度情况下的流场进行数值模拟及实验验证,分析气体射流对壁面黏性阻力、减阻率及流场的影响,研究气体射流的气液两相的减阻特性。结果表明:气体射流表面能够减小壁面黏性阻力,具有较好的减阻效果;四种射流方向角下,射流表面减阻率均在气体射流速度为5m/s时达到极大值,并且当射流方向角在xoz平面为-30°时,减阻率最大,为7.18%;数值模拟的减阻率效果略高于实验结果;气体射流的气液两相流动对壁面边界层进行了有效控制,减小了壁面的黏性剪应力和雷诺应力,导致壁面的黏性阻力减小,使得射流表面具有减阻性能。 | 谷云庆 牟介刚 代东顺 郑水华 蒋兰芳 吴登昊 | 2015 | 推进技术2015，36，11： | 5 |
| 2 | Middle or low water pressure direct spiral double helix converging nozzle structure optimization and flow field analysis显示文摘In order to solve the problem of using middle or low water pressure to form fine water mist,a new nozzle is proposed in fire rescue robot.Existing water mist nozzles are basically used for high pressure and in large size,complex structure and poor low pressure atomization effect in comparison with requirement of snake-like fire rescue robots.On the basis of comprehensive typical spray nozzles,a direct spiral double helix converging nozzle(DSDHCN) is proposed,which has the advantages of small volume,light weight,simple structure,and convenient installation.To make the spray nozzle have good performance,and meet the requirements of more efficient fire extinguishing,a numerical study is carried out to analyze the internal and external full flow field of nozzle.A gas-liquid two-phase flow is applied to simulate the external full flow field of nozzle with VOF model in fluent software.The simulation results show the real situation of water flow out of the atomization nozzle and the water jet trajectory.Some simulations about middle or low water pressure direct spiral double helix converging optimized nozzle have been done in 30 bar pressure.The simulation results show that the optimized nozzle structure not only makes the spray droplets have a good cone angle,but also have a sufficient axial velocity,which proves the structure rationality of the proposed optimized nozzle. | 蒋林 Wu Ruolin Zhao Hui Mei Peng Zhang Qiang Zhu Jiangyang Xiao Jun Lei Bin | 2015 | High Technology Letters2015，21，3： | 0 |
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