激波对斜孔超声速气膜冷却的影响

本文采用数值模拟的方法,研究了激波对斜孔情况下超声速气膜冷却的影响。其中主流马赫数为2.44,冷却流马赫数分别考虑1.2, 1.5和1.8三种情况,研究了温度场分布规律及平均冷却效率变化情况。结果发现:在本文计算工况范围中,三种冷却流马赫数工况下平均气膜冷却效率较接近;存在激波入射的情况下的平均气膜冷却效率整体要低于无激波入射工况,并且冷却效率呈现出先急剧下降后又逐渐增大、整体趋势为下降的锯齿状现象。     

激波对超音速平板发汗冷却的影响

本文分析了激波影响下,不同激波强度,冷却气体和注入率对发汗冷却效果的影响。马赫数3的超音速主流遇到流道内的楔形激波发生器产生斜激波入射到多孔平板表面。楔块楔角φ分别为0°、4°、8°、12°模拟不同的入射激波强度,冷却介质分别为空气、甲烷与氢气。计算结果表明,激波使多孔区域出口表面静压上升,冷却流体流出受阻而破坏冷却效果,且冷却效率随激波强度增强而下降,随冷却气体分子量增大,冷却效率下降幅度减小;但在激波强度较强时,激波在多孔表面形成逆压梯度,迫使冷却流体流向入射点上游区域而使该区域冷却效果得到恢复。提高冷却剂注入率可以减弱激波对冷却效率的破坏作用,但使壁面温度不均匀性增加。     

冷却流分段注入对超声速气膜冷却的影响

针对超声速气膜冷却中常有激波入射破坏冷却效果的现象,本文在冷却流质量流量一定的条件下研究了5种不同入口高度组合的冷却流分段注入结构,并与冷却流单个注入的情况对比,分析了激波入射情况下冷却流分段注入对超声速气膜冷却的影响。研究结果表明:在激波入射时,对于分段注入只有部分冷却流经历了激波的局部强化掺混作用,因此分段注入与单个注入相比可以提升气膜冷却效果。通过平均气膜冷却效率、最低气膜冷却效率、气膜覆盖率等冷却性能参数的比较,在本文研究的5种冷却流分段注入结构中,结构2的气膜冷却效果最好。     

非定常激波对气膜冷却影响的数值模拟

利用数值计算的方法研究了非定常激波对下游涡轮叶片表面气膜冷却的影响.冷却气流在激波和尾迹经过的过程中,发生了上扬和重新被压制回壁面的现象.考察了壁面上特定点在有气膜和无气膜情况下的换热量.通过计算发现,有气膜时的换热量有不同程度的下降,而且换热量随时间变化的趋势也发生了很大的变化.气膜的覆盖减小了主流场对壁面换热量的影响.     

变截面主流加速对超音速气膜冷却的影响

本文对扩张通道和直通道中的超音速气膜冷却进行了数值模拟,分析了主流加速和不加速两种情况下超音速气膜冷却的差异.计算结果表明,在主流加速的情况下,超音速气膜冷却的效果要好于相同进口条件下主流不加速的情况,并且这种差异越到下游越明显.同时,在本文计算的工况范围中,无论主流加速还是不加速,增大主流进口马赫数或者减少冷却流进口马赫数都使气膜冷却效率下降,而壁面静压则由主流气体决定.     

不同主流进口湍流度下的超音速气膜冷却

本文通过数值模拟的方法计算并分析主流进口湍流度、冷却流进口高度和进口马赫数对超音速气膜冷却的影响。计算结果表明,主流进口湍流度对超音速气膜冷却有较大影响,增大主流进口湍流度会减弱超音速气膜冷却效率,同时还表明,增大冷却流进口高度以及进口马赫数,能减弱主流湍流度对超音速气膜冷却的影响。     

超声速气膜冷却中激波抑制的研究

针对激波破坏超声速气膜冷却的机理,本文提出了一种壁面开孔的结构,数值研究结果表明：一方面,壁面开孔的结构能使激波作用的区域壁面附近的压力分布较均匀,从而使近壁区的马赫数分布比不开孔的壁面要高,有利于超声速气膜冷却。同时在激波的作用下,冷却气体可以通过开孔壁面的孔进入槽道内,而在槽内的下游再从孔里流出,保护下游的壁面,这...     

湍流度对单排圆孔及后扩孔气膜冷却的影响

通过传热-传质类比法研究了湍流度对单排圆柱孔及后扩孔气膜冷却效率的影响.计算结果表明,小吹风比M=0.5时,圆柱孔与后扩孔的壁面冷却效率相当,湍流度趋向于在整个下游区域使冷却效果恶化;大吹风比M=2时,后扩孔产生的壁面气膜冷却效率的提高明显,而湍流度的提高强化了冷却剂向壁面的扩散,削弱了冷却气膜脱离壁面的现象,趋向于在整个下游区域提升冷却效率.     

带肋通道和气膜冷却交互下的绝热和耦合传热研究

燃气轮机透平叶片冷却中,内部肋片扰流对气膜冷却效果有显著影响,当边界条件为金属壁面绝热和金属壁面耦合时,冷却效率会有不同的表现。本文采用数值计算方法,分别计算绝热边界和耦合边界条件下,气膜孔进口与内部冷却扰流肋片不同相对位置条件下的绝热气膜冷却效率和耦合条件下的整体冷却效率进行计算。结果表明当气膜进口位于肋后扰流区时,绝热气膜冷却效率较差。绝热边界和耦合边界条件下流场相似,气膜孔与肋片相对位置对于气膜孔下游整体冷却效率的影响与绝热条件相似。     

涡轮叶栅前缘槽缝气膜冷却的数值模拟

应用FINE/TURBO软件包,求解三维雷诺平均N-S方程,对叶片前缘有两列冷却槽缝的气膜冷却流场进行了数值模拟,获得了不同吹风比下叶片表面静压分布与极限流线.在计算结果与实验数据良好符合的基础上,详细分析了槽缝冷却三维定常流场结构与槽缝附近的流动细节.研究结果表明,槽缝冷却对前缘压力分布影响较大,且在压力面引起较大的分离流动,不利于冷却.     

涡轮静叶尾缘开槽冷却特性的数值研究

本文用三维数值模拟的方法,对某具有尾缘开槽冷却的涡轮静叶栅进行了详细的气热耦合计算与分析,研究了具有尾缘开槽冷却形式的涡轮静叶片的冷却特性,并结合叶片表面温度分布和静压分布对比分析了叶片在不同吹风比下该冷却方式对流场气动性能的影响。气热耦合计算结果表明:此种尾缘开槽的冷却形式可以对叶片尾缘高温区起到有效的冷却效果,同时使主流通道的气动喉口向上游迁移,在冷却槽口区域引起主流的压力波动。     

涡轮叶片端壁槽缝气与离散气膜孔冷却特性实验研究

真实发动机涡轮叶片端壁为曲面造型,并且其冷却受槽缝气、泄漏流和离散气膜冷却多种冷却气叠加影响,同时又受到主流二次流影响,因此呈现复杂冷却特性。为研究接近真实发动机涡轮叶片端壁构型和工况下的气膜冷却特性,本文采用高速风洞(主流雷诺数为37万)及压敏漆(PSP)技术,研究了槽缝气、泄漏流以及离散气膜对曲面端壁的气膜冷却效率的影响,并针对不同冷气流量比对端壁气膜冷效的影响规律进行了对比分析。结果表明:端壁表面气膜冷效随着槽缝气流量比增大而增大,当流量比增大到1.71%时,槽缝气膜几乎可以覆盖整个端壁表面;与槽缝气相比,端壁表面的离散气膜冷气覆盖范围较为有限,端壁压力面侧下游区域气膜覆盖较差;在喉部之前,随着流量比增大,离散气膜冷效呈现下降趋势;在喉部之后,随着流量比从1.3%增大到1.9%,离散气膜冷效呈现上升趋势;与仅有离散气膜相比,包含槽缝气、泄漏流、离散气膜的全气膜覆盖更为均匀,全气膜冷效的叠加使得端壁冷效相比仅有离散气膜时整体提高了93.4%。     

Effect of the incident shock wave interacting with transversal jet flow on the mixing and combustion

The interaction between an incident shock wave and a transverse jet flow for mixing and combustion in a supersonic airstream was investigated experimentally and numerically. NO planar laser induced fluorescence (NO-PLIF) and particle imaging velocimetry (PIV) for non-reactive flows and three-dimensional reactive/non-reactive numerical simulations were conducted to examine the effect of the incident shock wave on the three-dimensional flow structure and mixing mechanism between the airstream and the injected gas downstream of the injection slot. Results of NO-PLIF measurement and numerical simulation showed that, in the case without the incident shock wave, injected gas is seldom seen in the recirculation zone just downstream of the injection slot, while the injected gas with higher concentration is almost uniformly distributed in the recirculation zone when the incident shock wave is introduced downstream of the injection slot. Moreover, it was shown by the numerical simulations that the profiles of the local equivalence ratio is in the combustible range due to the enhanced entrainment of the airstream when the incident shock wave is introduced downstream of the injection slot. A large-scale recirculation in the direction parallel to the wall is generated by the three-dimensional flow effects, which enhances the mixing and extends the residence time in the recirculation zone in the case with incident shock wave downstream of the injection slot, the recirculation flow being confirmed successfully by PIV measurements as well. The results of three-dimensional reactive numerical simulations were in good agreement with the experimental flame-holding characteristics at a lower total temperature, which showed that flame-holding can be attained only when the incident shock wave was introduced downstream of the injection slot, confirming that the formation of three-dimensional and large-scale recirculation flow downstream of the injection slot enlarges the recirculation zone and enhances the mixing to produce the conditions for robust flame-holding.     

对运动斜激波绕射波纹壁面的研究

使用计算流体动力学的方法,对经典的运动激波绕射现象做数值模拟,研究了一类复杂激波反射问题一入射的运动斜激波绕射现象.给出一组运动斜激波绕射波纹壁面的非定常过程的模拟结果。计算结果显示出由运动斜激波绕射诱导的多波干扰产生的复杂流场结构。     

Application of the wavenumber jump condition to the normal and oblique interaction of a plane acoustic wave and a plane shock

A kinematic approach is considered whereby the wavenumber jump conditions in conjunction with the appropriate dispersion relations is applied to the investigation of the normal and oblique interaction of a plane acoustic wave with a plane shock wave. For the normal interaction of an acoustic wave with a stationary plane shock a logarithmic shift in the wave spectra is obtained. For the normal interaction with a moving shock front it is shown that for shock Mach numbers above a critical value, the frequency of the transmitted wave becomes negative. This results in the fact that the crests of the transmitted signal arrive at a fixed observer in a reverse order to their generation. Finally, the oblique interaction of an acoustic wave with a stationary shock is considered. The “Snell's Law” for the transmitted wave is derived and two special angles of incidence are identified. The first is a no-refraction angle: i.e., the transmitted wave angle is the same as the incident wave angle. The second is a critical angle such that for incident angles greater than this critical angle there is no transmitted wave. A necessary and sufficient condition for the existence of a transmitted wave is derived in terms of the speed of sound and Mach number of the fluid and the frequency and tangential wavenumber component of the incident wave.The dynamics aspects of the interaction concerning the determination of the frequency independent transmission coefficients and shock displacements are determined for the simple case of the normal interaction with a moving shock as an illustration.     

Numerical approach to new tangential slot effect on film cooling effectiveness over asymmetrical turbine blade

The focus of this numerical study is to conceive a new basic film cooling configuration in order to increase film cooling effectiveness, especially at the leading edge zone between the injection holes where cooling is mostly needed. The new configuration, resulting from the tangential slot configuration and especially adapted to the leading edge of an asymmetrical blade, is compared to the uniform slot configuration. Three alternatives geometries were proposed and numerically tested to find the configuration that provides the best film cooling effectiveness. The simulation is conducted at a fixed density ratio of 1.0 and a blowing ratio of 0.7. A new parameter, Rc, is defined to measure the rate of blade coverage by the film cooling. The outcomes of the numerical results indicate that the three proposed configurations allow better thermal protection because of their higher film cooling coverage. At suction side, the new configurations provide a better film cooling coverage than the baseline case. The minimal improvement is at approximately 34%, with a light superiority of case 1. At pressure side, the use of the tangential slot is especially interesting for the allowed minimum adiabatic effectiveness values between 0.3 and 0.5.     

Three-dimensional reactive shock bifurcations

We model interactions of a premixed flame with incident and reflected shocks in a rectangular shock tube using three-dimensional (3D) reactive Navier–Stokes numerical simulations. Shock-flame interactions occur in the presence of boundary layers that cause the reflected shock to bifurcate and form a reactive shock bifurcation (RSB), which contains a flame in the recirculation zone behind the oblique shock. The recirculation zone acts as a flame holder thus attaching the flame to the shock in the vicinity of the wall, and providing a mechanism for a detonationless supersonic flame spread. The accelerated burning induced by an RSB, and Mach stems that may result from RSB–RSB interactions, promote hot-spot formation, and eventually accelerate deflagration-to-detonation transition. Schlieren-type images generated from the simulation results show that the 3D structure of an RSB may not always be easily recognized in experiments if the RSB is attached to the surface of the observation window. The main 3D effect observed in the simulations is caused by the presence of the second no-slip wall in a 3D rectangular channel. Two RSBs that form at adjacent walls interact with each other and produce an oblique Mach stem between two oblique shocks. The oblique Mach stems then interacts with a central Mach stem that forms near symmetry plane, and this interaction creates a hot-spot that leads to a detonation initiation.     

凝聚介质中斜激波的反射

结合数值模拟和理论分析,研究凝聚介质中斜激波反射.采用龙格-库塔控制体积间断有限元方法,数值求解"刚性气体"状态方程形式下的欧拉方程组;理论分析凝聚介质中斜激波反射模式;运用激波极曲线理论,给出典型激波强度下正规反射向非正规反射过渡的临界角及波后状态.比较数值模拟结果和激波极曲线理论分析结果,得到典型弱、强斜激波的反射图像.     

斜激波与轴对称边界层干扰的数值模拟

使用两方程Menter-SST模型,对来流Mach数为3时的斜激波与轴对称边界层的相互干扰现象进行了数值模拟与定性、定量分析。研究了斜楔激波发生器楔角和来流单位Reynolds数变化对干扰区流动的影响,总结了参数变化引起的流动分离变化规律;此外,还计算了与三维计算中心对称面上的入射激波等效的二维情形,并将三维结果与二维情形进行对比,对比结果显示中心对称面上的壁面压力系数、分离涡尺寸、涡量分布等与相应的二维情形存在明显差异。     

等离子体气动激励控制激波的机理研究

针对等离子体气动激励控制激波的热效应机理和电离效应机理的争议,分别采用热阻塞模型和离子声波模型,理论推导出了不同机理前提下电弧等离子体对尖劈斜激波的影响规律.对于热效应机理,激波变化规律是激波起始点前移、形状不弯曲以及角度减小;对于电离效应机理,激波变化规律是激波起始点仍维持在尖劈前缘点处、形状分为两段发生弯曲以及起始段的角度增大.针对该对立的理论推导结果,进行了电弧等离子体控制尖劈斜激波的超声速风洞实验研究,实验观察到尖劈斜激波起始点前移4 mm,激波角度减小8.6%,激波形状未发生弯曲.以热效应机理为前提推导出的理论结果与该实验结果相符,从而验证了等离子体气动激励控制激波是热效应机理在起主要作用. 关键词： 等离子体气动激励 激波 热效应 电离效应