NF-6增压连续式跨声速风洞流场特性与标模试验

NF-6风洞是中国第一座增压连续式跨声速风洞。对NF-6风洞试验段流场特性进行了总结分析,研究结果表明该风洞具有优良的流场品质,总体上达到了设计要求,具备了承担型号和科研试验任务的能力。通过AGARD-B标模试验,进一步完善了NF-6风洞试验段流场品质校测项目,检验了该风洞的测力试验能力。NF-6风洞标模试验结果与国内外风洞试验数据吻合较好,试验精度和风洞平均气流偏角满足国军标要求,表明该风洞具备了测力试验的能力。     

NF-6连续式跨声速风洞马赫数控制方式比较与研究

NF-6风洞通过压缩机静叶角预置进行马赫数粗调,而马赫数精确调节包括压缩机转速调节与试验段下游栅指位置调节两种方式。从调节范围、调节精度、调节速度与安全性4个方面对两种调节方式进行了对比研究。栅指调节在调节范围、调节精度方面具有一定优势,但两种精调方式均能很好地满足指标要求,而利用压缩机转速细调马赫数则具有安全性较好,且系统更简洁等特点。风洞最终选定了利用压缩机转速精调马赫数的控制方式,并确定了马赫数控制的流程。测试结果表明,风洞在全运行范围内马赫数控制精度优于±0．002。     

2.4m跨声速风洞多功能支撑系统试验技术研究

针对型号研制的风洞试验需求,在2.4m跨声速风洞中开展了多功能支撑系统试验技术研究,研制了一套多功能支撑系统。该支撑系统既可实现定侧滑角连续变迎角的试验方式,又可实现定迎角连续变侧滑角的试验方式。在0.6m跨声速风洞开展了引导性试验研究,并在2.4m跨声速风洞中对该支撑系统与传统的支撑方式进行了风洞试验对比。结果表明,多功能支撑与传统支撑方式的风洞试验数据相关性良好,表明该支撑装置的研制是成功的,可应用于型号试验。     

低亚声速和跨声速矩形柱绕流的大涡模拟研究

采用基于非结构网格的有限体/有限元混合格式和大涡模拟的方法求解可压缩Navier-Stokes方程,研究了不同长宽比矩形柱低亚声速和跨声速绕流的流动特性。在雷诺数为22000时,对来流马赫数等于0.1和0.75,截面长宽比分别为1∶1、2∶1、3∶1和4∶1的矩形柱绕流进行了大涡模拟,以研究长宽比和压缩性对矩形柱绕流流场的影响。马赫数为0.1时,Strouhal数随着长宽比的增大先降低再增大然后再降低;长宽比为3∶1和4∶1时会有流动的再附产生;柱体上表面的三维特性在长宽比大时更明显。马赫数为0.75时,Strouhal数随着长宽比的增大逐渐减小;湍流脉动和涡脱落受到抑制;方柱的近尾迹区域,有两种形成机制不同的局部超声速区。     

InvesInvestigation of the Effects of Airfoil-probes on the Aerodynamic Performance of an Axial Compressor

In order to investigate the effects of the airfoil-probes on the aerodynamic performance of an axial compressor,a numerical simulation of 3D flow field is performed in a 1.5-stage axial compressor with airfoil-probes installed at the stator leading-edge(LE).The airfoil-probes have a negative influence on the compressor aerodynamic performance at all operating points.A streamwise vortex is induced by the airfoil-probe along both sides of the blade.At the mid-operating point,the vortex is notable along the pressure side and is relatively small along the suction side(SS).At the near-stall point,the vortex is slightly suppressed in the pressure surface(PS),but becomes remarkable in the suction side.A small local-separation is induced by the interactions between the vortex and the end-wall boundary layer in the corner region near the hub.That the positive pitch angle of the airfoil-probe at 6.5% span is about 15° plays an important role in the vortex evolution near the hub,which causes the fact that the airfoil-probe near the hub has the largest effects among the four airfoil-probes.In order to get a further understanding of the vortex evolution in the stator in the numerical simulation,a flow visualization experiment in a water tunnel is performed.The flow visualization results give a deep insight into the evolution of the vortex induced by the airfoil-probe.     

高负荷跨音压气机叶尖间隙流动的数值分析与比较

利用自行开发的叶轮机三维数值模拟软件对高负荷跨音压气机ATS-2转子进行了带叶尖间隙的三维流动数值模拟,并与实验的结果进行了比较。结果表明,数值模拟得到的流场结构与实验结果一致。对粘性与无粘结果的比较显示,由泄漏流所产生的激波后阻塞区是由激波-漏流干扰所致,粘性的作用将削弱其面积和强度。随叶尖间隙增大,激波后阻塞区的径向和轴向尺度增大,压比、效率和流量下降。      

2.4m跨声速风洞流场性能调试研究

介绍了2.4m跨声速风洞性能调试研究结果,并作了简要分析.研究结果表明,该风洞流场品质全面达到国军标指标,部分达到当今世界先进水平.该研究首次在国内四壁均为斜孔壁的大型跨声速风洞中解决了优化开闭比、加速区分布形式以及特大驻室M数参考点位置确定等一系列技术问题,表明我国大型跨声速风洞流场性能调试研究取得新进展.     

计算跨声速平面叶栅流场的压力方法

以压力和速度分量为原始变量,将不可压流的ＳＩＭＰＬＥ算法应用到可压缩流动,成功求解了具有严重非正交网格及周期性边界条件的跨声速平面叶栅流场,计算结果与实验符合较好。     

新的解跨音速Euler方程的隐式杂交方法

 本文提出一个新的杂交格式,它由Jameson-Turkel LU分解法和Harten TVD（total variation diminishing）格式的修正数值通量耦合而成。LU分解用于Euler方程隐式部分的离散化而Harten的数值通量控制所谓的稳态解残差。精心构造LU算子,可使矩阵算子L和U很容易逐点推进求逆;以Harten的数值通量计算杂交格式右边的通量,这样做在a=1/2的条件下,可保证收敛的稳态解具有二阶精度并能高分辨率地捕获激波。数值实验表明,本文格式对于稳态计算是有生命力的并能保证较高的激波分辨率。     

二维机翼二自由度跨音速颤振分析

 <正> On the assumption that airfoils take small amplitude ha-rmonic oscillating and middle reduced frequency, the two-dimensional, inviscid, small-disturbance nonlinear unsteady transonic flow equation can be split into two parts. One is the nonlinear steady small-disturbance equation, the other is the time-linearized unsteady small-disturbance equation. The steady equation is solved by Carlson code. The unsteady equation is solved by integral method. The standard v-g method is used to solve the flutter eigenvalue equations. A transonic flutter analysis is performed for a NACA 64A006 airfoil with pitching and plunging degrees of freedom.The Mach numbers considered are 0.7, 0.8, and 0.85. The aerodynamic coefficients are obtained by the above method. For each Mach number, the flutter speed and the corresponding flutter reduced frequencies are achieved by varying the airfoil-airmass ratio, plunge-pitch frequency ratio. The results are compared with other computational method and good agreement has been observe