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激励器结构对三电极等离子体高能合成射流流场及其冲量特性的影响 被引量:1
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作者 张宇 罗振兵 +2 位作者 李海鹏 王林 夏智勋 《空气动力学学报》 CSCD 北大核心 2016年第6期783-789,共7页
等离子体激励器以其结构简单、响应速度快、环境适应性强等优势,已成为主动流动控制技术和流体力学研究的前沿与热点。相比于传统两电极激励器,三电极等离子体高能合成射流激励器具有更高的能量效率,形成射流冲量更大,有望成为新型快响... 等离子体激励器以其结构简单、响应速度快、环境适应性强等优势,已成为主动流动控制技术和流体力学研究的前沿与热点。相比于传统两电极激励器,三电极等离子体高能合成射流激励器具有更高的能量效率,形成射流冲量更大,有望成为新型快响应直接力产生装置。为揭示激励器结构对射流流场和冲量特性的影响规律,进而优化激励器结构参数,利用电参数测量装置、高速阴影系统及自主设计的单丝扭摆式微冲量测量系统对不同射流孔径、腔体体积和电极间距的三电极激励器放电特性、射流流场及其冲量进行了实验研究。为对比激励器在不同工况条件下的工作特性,定义无量纲能量沉积ε和无量纲射流冲量I*,并分析了激励器结构参数对ε和I*的影响。结果表明对于给定无量纲能量沉积ε,激励器存在最优射流孔径;激励器无量纲能量沉积ε和无量纲射流冲量I*随腔体体积增加而减小,随激励器电极间距增加而增加;射流强度及其流场影响区域随腔体体积增加而减小,随激励器电极间距增加而增加。对比不同腔体体积和电极间距工况条件下I*随ε的变化可知,为设计具有较好射流冲量水平的激励器,在相同无量纲能量沉积ε条件下,应尽量增大激励器无量纲射流冲量I*。当设计激励器无量纲能量沉积ε小于初始工况时,应增大初始工况激励器腔体体积使无量纲能量沉积ε降低至设计值;当设计激励器无量纲能量沉积ε大于初始工况时,应增大初始工况激励器电极间距使无量纲能量沉积ε增加至设计值,使设计激励器具有较好的射流冲量水平。 展开更多
关键词 等离子体合成射流 高速阴影 单丝扭摆 结构参数 主动流动控制 能量沉积 射流冲量 射流流场
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起动射流出口形状对其推力特性影响研究
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作者 王鑫 高磊 《应用物理》 CAS 2019年第4期197-206,共10页
本文采用数值模拟方法研究起动射流推进器出口形状对其产生的推力与冲量的影响。将圆管和圆孔喷管入口直径与出口直径的比值Dr (定义Dr为直径比)作为变量,通过改变直径比的值来表征起动射流出口形状的差异。研究发现,在射流过程中,由于... 本文采用数值模拟方法研究起动射流推进器出口形状对其产生的推力与冲量的影响。将圆管和圆孔喷管入口直径与出口直径的比值Dr (定义Dr为直径比)作为变量,通过改变直径比的值来表征起动射流出口形状的差异。研究发现,在射流过程中,由于圆孔喷管出口形状对射流具有收缩作用,其出口一直有持续的过压效应发生,而圆管喷管只有在射流起始加速阶段会有较强的过压产生,因此圆孔喷管能向尾迹中产生更大的冲量Ih,并获得更大的推力FT。而且起动射流的冲量Ih及推进冲量FT随着直径比Dr的增大而增大,直到直径比达到临界值2.5时,Ih和FT几乎不再增长。 展开更多
关键词 起动 射流推力与冲量 直径比
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Laser Doppler Measurements of Twin Impinging Jets Aligned with a Crossflow
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作者 Jorge M.M. Barata Pedro S.D. Carvalho +3 位作者 Femando M.S.P. Neves1, Andr6 R.R. Silva1, Diana F.C. VieiraI andDiamantino F.G. Duro Andre R.R. Silva Diana F.C. Vieira Diamantino F.G. Durao 《Journal of Physical Science and Application》 2014年第7期403-411,共9页
This paper presents a detailed analysis of the complex flow beneath two impinging jets aligned with a low-velocity crossflow which is relevant for the future F-35 VSTOL configuration, and provides a quantitative pictu... This paper presents a detailed analysis of the complex flow beneath two impinging jets aligned with a low-velocity crossflow which is relevant for the future F-35 VSTOL configuration, and provides a quantitative picture of the main features of interest for impingement type of flows. The experiments were carried out for a Reynolds number based on the jet exit conditions of Rej = 4.3 × 10^4, an impingement height of 20.1 jet diameters and for a velocity ratio between the jet exit and the crossflow VR = V/Uo of 22.5. The rear jet is located at S = 6 D downstream of the first jet. The results show a large penetration of the first (upstream)jet that is deflected by the crossflow and impinges on the ground, giving rise to a ground vortex due to the collision of the radial wall and the crossflow that wraps around the impinging point like a scarf. The rear jet (located downstream) it is not so affected by the crossflow in terms of deflection, but due to the downstream wall jet that flows radially from the impinging point of the first jet it does not reach the ground. The results indicate a new flow pattern not yet reported so far, that for a VSTOL aircraft operating in ground vicinity with front wind or small forward movement may result in enhanced under pressures in the aft part of the aircraft causing a suction down force and a change of the pitching moment towards the ground. 展开更多
关键词 VSTOL ground vortex TURBULENCE complex flows.
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Experimental Study of Heat Transfer for a Rotating Cylinder Water Jet Impingement Quenching
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作者 Mozumder Aloke Kumar Mitsutake Yuichi Monde Masanori 《Journal of Energy and Power Engineering》 2013年第3期411-422,共12页
Transient heat transfer has been experimentally investigated for subcooled water jet impingement quenching of a hot rotating stainless steel cylinder. Temperatures beneath the impinged surface were measured during que... Transient heat transfer has been experimentally investigated for subcooled water jet impingement quenching of a hot rotating stainless steel cylinder. Temperatures beneath the impinged surface were measured during quenching and used to estimate surface temperature and surface heat flux by using a developed numerical inverse solution of heat conduction. Heat flux reached its maximum value just after the WF (wetting front) (visible leading edge of boiling region) started moving from stagnation towards the circumferential region. WF moved in a non-uniform manner in angular direction on the hot rotating surface. With the increase of surface velocity, heat flux decreased. Higher surface velocity moved away the produced vapor bubbles and reduced the solid-liquid contact time which made it one-dimensional heat conduction from multi-dimensional, that reduced heat flux. The generated boiling curve from the estimated heat flux showed a reasonable agreement with existing studies. The surface maximum heat flux (maximum value in each cycle) distribution trend with radial position is entirely comparable with the static surface critical heat flux in literature. An explosive to a sheet like flow patterns were observed with the decrease of surface temperature. The flow patterns were followed by the intensity of sound during quenching. 展开更多
关键词 Heat conduction inverse solution jet impingement.
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Synchronal Measurement of Flow Structure and Heat Transfer of Impingement Jet
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作者 Shoichi MATSUDA Naomichi SAJI +2 位作者 Minoru YAGA Masaaki ISHIKAWA Kenyu OYAKAWA 《Journal of Thermal Science》 SCIE EI CAS CSCD 2010年第3期228-233,共6页
This paper will present the characteristics of flow behavior and thermal field of both free and impingement jet issued from a circular orifice nozzle at Re=8900.The flow behavior of a single round jet and impingement ... This paper will present the characteristics of flow behavior and thermal field of both free and impingement jet issued from a circular orifice nozzle at Re=8900.The flow behavior of a single round jet and impingement jet was observed by smoke flow visualization recorded by a high speed camera using 5000 frame per second.Heat transfer coefficient on the impingement surface was measured by means of infrared camera (TVS-8500,Avio) with a two-dimensional array of Indeum-Antimony (In Sb) sensors varying in the separation distance between the nozzle and the target plate.The heat transfer coefficient changes in time and spatial.Therefore,the root mean square distribution of the heat transfer was obtained from the data.As a result,it was confirmed that the longitudinal vortex was observed outside of the ring vortex,and then the longitudinal vortex was penetrated in the jet flow.Moreover,the high value of root mean square of the heat transfer coefficient has spread radially in stripy manner,which is caused as the results of the longitudinal vortexes flowing in the radial direction on the impingement plate. 展开更多
关键词 Impingement jet Forced convection Heat transfer Ring vortex Longitudinal vortex
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