V型尾缘喷管流场特性数值模拟

模拟计算了一系列V型尾缘(Chevron)收敛喷管的详细涡结构(包括流向涡和展向涡)、引射系数、推力损失等性能,并与相关实验结果进行了对比验证。采用有限体积QUC IK格式和标准k-ε湍流模型,结合壁面函数求解雷诺平均的N-S方程。通过模拟计算与实验结果的对比,验证了计算方法的可行性。通过计算得出:V型尾缘喷管齿弯角越大,核心区长度越短,喷管出口下游的流向涡和展向涡的强度和尺度也越大。V型尾缘的齿弯角每增加1°,对应的喷管的堵塞比约增加0.98%,喷管的推力损失约增加1.71%,引射系数约增加3.45%。     

并列双发三维非对称多S弯喷管参数化设计方法

形成了一套基于CFD计算评价的并列双发三维非对称多S弯喷管参数化设计方法,并初步证明了该方法的正确性和可行性.多S弯中心线在Z向偏心度为0时:第一S弯Y向偏心度、长度都最小,第二S弯Y向偏心度、长度都最大,第三S弯Y向偏心度、长度分别介于前两个S弯对应参数之间,各S弯都采用进口缓慢转弯,出口快速转弯的规律,以利于抑制背风侧分离和涡.剖面在各S弯上都采用进口快速收缩缓慢转弯,出口缓慢收缩快速转弯的规律,且宽高比与侧边倾角在进出口变化速率相同,且侧边倾角只分布在第一S弯上,以利于稳定流场和增加隐身性能.合流器采用楔底宽高比约束,其值应不超过0.26.      

变弯度后缘与常规舵面机翼的颤振主动抑制对比

后缘变弯度机翼的气动弹性建模与稳定性分析日益受到关注。为了探究变弯度后缘相比常规偏转舵面机翼颤振主动抑制的方法与特点，以一个小展弦比后缘变弯度机翼为对象，首先建立结构有限元模型，并引入变弯度后缘变形模态和常规舵面偏转模态，采用亚声速偶极子格网法计算非定常气动力；然后使用基于最小状态法的有理函数拟合进行频域到时域模型的转换，建立两种构型机翼的气动弹性模型，并在建模时考虑了变弯度后缘与常规舵面控制带宽的差异；最后利用线性高斯二次型方法设计控制律进行颤振主动抑制，分析对比两种控制方式的特性差异。结果表明：采用变弯度后缘的闭环系统能够将颤振临界速度提高22%，其提升效果优于常规舵面，所需舵面偏转峰值更小。     

Review of atomization mechanism and spray characteristics of a liquid jet in supersonic crossflow

The injection and atomization process of a liquid fuel jet is critical for an ignition start of a scramjet engine. Airwall-mounted crossflow injection strategy is widely used in scramjet combustors, avoiding high total pressure loss and allowing the liquid fuel to rapidly undergo atomization, mixing, and evaporation. In this review, research progress on a liquid jet in supersonic crossflow was evaluated from aspects of atomization mechanism and spray characteristics. When a liquid jet is injected into a supersonic crossflow, primary and secondary breakups occur successively. The surface instability of liquid can significantly affect the breakup process. This review discusses the current understanding of the breakup process and spray characteristics of a liquid jet in supersonic crossflow including the mechanism of atomization and the characteristics of distribution and atomization. The development of windward Rayleigh-Taylor (R-T) unstable waves is the main factor in column breakup. The development of Kelvin-Helmholtz (K-H) unstable waves along the circumferential direction of the jet or droplets is the main factor of surface and droplet breakups. The liquid–gas momentum ratio is the most important factor affecting the penetration depth. The span width of the liquid jet is affected by the windward area. Breakup and coalescence lead to a transformation of the size distribution of droplets from S- or C-shaped to I-shaped, and the velocity distribution of the droplets on the central symmetry plane has a mirrored S-shape. The droplet distribution on the spanwise cross-section retains a structure similar to an “Ω” shape. At last, some promising recommendations have been proposed, namely a theoretical predictive model which can describe the breakup mechanism of a liquid jet, the distribution characteristics and droplets size distribution of a liquid jet under a cavity combustion chamber, especially for enthalpy flows with complex wave structures.