Scaling effects on combustion modes in a single-side expansion kerosene-fueled scramjet combustor

The combustion modes in two different scramjet combustors with the mass flow rates of 1.8 kg/s and 3.6 kg/s are experimentally investigated to explore the scaling effects on supersonic combustion with a Mach number 2.0 inflow. It is found that the scramjet combustor with a larger scale can broaden the flame rich blowout limit. As the Equivalence Ratio (ER) increases, the combustion in the small-scale combustor maintains in the cavity-stabilized mode, and the flamebase moves downstream along the cavity shear layer; however, the combustion in the large-scale combustor gradually transfers from the cavity-stabilized mode to the jet-wake-stabilized mode. The differences in the cavity residence time, the ignition delay time and the Damkohler number caused by different scales of the scramjet combustor are likely to account for the scaling effects on the combustion modes.     

Large eddy simulation based studies of jet–cavity interactions in a supersonic flow

Interactions of a cavity flameholder with an upstream injected jet in a Ma 2.52 supersonic flow are investigated numerically. A hybrid RANS/LES (Reynolds-Averaged Navier–Stokes/Large Eddy Simulation) method acting as wall-modeled LES is adopted, for which the recycling/rescaling method is introduced to treat the unsteady turbulent inflow. Patterns of the fluid entrainment into the cavity and escape from the cavity are identified using a scalar-tracing method. It is found that the jet–cavity interactions remarkably enhanced the mass exchange between the fluids in and out of the cavity, resulting in reduced residence time of the cavity fluids. Increasing the distance between the fuel injection and the cavity leading edge tends to attenuate the jet–cavity interactions, leading to weaker mass exchange. Raising the injection pressure appears to enhance the jet–cavity interactions, resulting in a shorter residence time of the cavity fluids. Moreover, the mass decay processes for the fuel and air within the cavity are basically the same while the entrainment processes for the fuel and air into the cavity seem quite different.     

氢原子频标腔伺服的研究

描述了氢原子频标腔伺服系统和其对时域的影响 ,并通过测试说明了该方法的可行性。     

极小型氢频标磁控管微波腔的仿真设计

用Ansoft HFSS仿真软件建立了极小型氢频标磁控管微波腔的几种模型结构,在给定腔体尺寸下,仿真了不同电极间距的空型和磁控管型微波腔谐振频率和品质因数,得出极小型氢频标磁控管微波腔的设计参数,并对实际设计中影响磁控管微波腔谐振频率的因素给出了建议。     

激波对凹腔火焰稳定器流场影响

为揭示激波对超声速流中凹腔流场的影响规律,在超声速流中利用长9 mm,坡度为23°的斜坡产生激波。组合利用高速摄影仪和纹影仪,采用碘钨灯、连续激光和脉冲激光作为光源,摄像曝光时间分别为1 m s,8 us,8 ns,获得了斜坡激波入射在单个凹腔中部、中后部和后部,以及激波入射在不同构型凹腔相同位置的流场纹影图像。结果表明,凹腔自由剪切层在受到激波撞击后,在入射点前会发生弯曲而偏向主流,在入射点后加速发展和破碎;激波入射点靠近前沿则引起凹腔前沿激波的增强,靠近凹腔后沿导致再附激波减弱。     

基于跨声速高压涡轮凹槽叶顶间隙模型的大涡模拟研究

为研究跨声速高压涡轮叶顶间隙非定常流动特性及流场结构,基于跨声速高压涡轮凹槽叶顶间隙的几何特征,建立了可行的简化数值模型,并通过大涡模拟对叶顶凹槽间隙内部的非定常流动进行了数值计算,探讨了凹槽叶顶几何参数对流动稳定性和气动性能的影响.研究结果表明,当跨声速泄漏流动流经凹槽叶顶时,在凹槽入口处形成激波,同时凹槽前分离泡发...     

圆柱体落水过程多相流体动力特性数值分析

针对圆柱体大角度落水过程多相流动问题,采用VOF多相流模型和重叠网格技术分析了低弗劳德数条件下圆柱体落水过程空泡演化、水动力特性以及尺度效应的影响。结果表明:不同直径的圆柱体落水空泡均发生拉断闭合,且空泡闭合时间随弗劳德数增加而线性增大。除落水抨击和空泡闭合阶段外,升力系数在空泡闭合前的平均增长率比空泡闭合后快。阻力系数从落水撞击至空泡闭合阶段变化一致,但是在空泡闭合后出现分化现象。     

凹腔几何构型和来流马赫数对部分覆盖型凹腔流动的影响

为了研究覆盖板长度、凹腔深度、凹腔长深比和来流马赫数对部分覆盖型凹腔流场的影响,采用二维耦合隐式N-S方程和标准k-ε湍流模型,对部分覆盖型凹腔的流场进行了数值仿真。发现覆盖板长度对自由来流没有明显影响;长深比是影响不同深度凹腔的覆盖区质量交换的主要因素;覆盖区质量交换随着长深比增大而减少;来流马赫数增加,凹腔覆盖区的质量交换下降;与大长深比凹腔相比,小长深比凹腔的覆盖区质量交换受长深比和来流马赫数影响更加明显。     

液体碳氢燃料超燃冲压发动机支板凹槽稳焰技术试验

液态碳氢燃料点火、稳焰技术是超燃冲压发动机的关键技术之一,是发动机获得推力性能的先决条件。采用直连试验手段,对支板凹槽组合稳焰技术进行了研究,比较了不同燃料喷注方式和不同支板凹槽组合方式对点火、稳定燃烧的影响。结果表明支板喷射与支板凹槽组合稳焰的燃烧组织方式,可以实现在低飞行马赫数范围（Ma0=4～5）液体碳氢燃料的可靠点火与稳定燃烧,并获得较好的燃烧性能。     

Numerical investigation on cavity structure of solid-fuel scramjet combustor

The influences of miscellaneous combustor structures for solid fuel scramjet combustion on the performance are investigated, including a detailed interaction analysis between shocks/waves and combustion. Hydroxyl-terminated polybutadiene is chosen as the solid fuel with the non-premixed equilibrium probability density function combustion model. The results show combustion enhancement when structure of combustor is modified. The radical emphasis is to examine the sensitivity of the properties due to variations on the length-to-depth ratio of cavity, aft wall angle, and offset ratio. It is noted that there is an appropriate structure of cavity (L/D=4, θ=45°, and D_d/D_u=1.25–1.5) regarding the combustion efficiency, total pressure loss and specific impulse. The observation of function for combustor components provides instructional insight into the design considerations for a combustor of a solid-fuel scramjet.