Experimental investigation on aero-heating of rudder shaft within laminar/turbulent hypersonic boundary layers

The aero-heating of the rudder shaft region of a hypersonic vehicle is very harsh, as the peak heat flux in this region can be even higher than that at the stagnation point. Therefore, studying the aero-heating of the rudder shaft is of great significance for designing the thermal protection system of the hypersonic vehicle. In the wind tunnel test of the aero-heating effect, we find that with the increase of the angle of attack of the lifting body model, the increasement of the heat flux of the rudder shaft is larger under laminar flow conditions than that under turbulent flow conditions. To understand this, we design a wind tunnel experiment to study the effect of laminar/turbulent hypersonic boundary layers on the heat flux of the rudder shaft under the same wind tunnel freestream conditions. The experiment is carried out in the ?2 m shock tunnel(FD-14 A) affiliated to the China Aerodynamics Research and Development Center(CARDC). The laminar boundary layer on the model is triggered to a turbulent one by using vortex generators, which are 2 mm-high diamonds. The aero-heating of the rudder shaft(with the rudder) and the protuberance(without the rudder) are studied in both hypersonic laminar and turbulent boundary layers under the same freestream condition. The nominal Mach numbers are 10 and 12, and the unit Reynolds numbers are2.4 × 10~6 m~(-1) and 2.1 × 10~6 m-1. The angle of attack of the model is 20°, and the deflection angle of the rudder and the protuberance is 10°. The heat flux on the model surface is measured by thin film heat flux sensors, and the heat flux distribution along the center line of the lifting body model suggests that forced transition is achieved in the upstream of the rudder. The test results of the rudder shaft and the protuberance show that the heat flux of the rudder shaft is lower in the turbulent flow than that in the laminar flow, but the heat flux of the protuberance is the other way around,i.e., lower in the laminar flow than in the turbulent flow. The wind tunnel test results is also validated by numerical simulations. Our analysis suggests that this phenomenon is due to the difference of boundary layer velocities caused by different thickness of boundary layer between laminar and turbulent flows, as well as the restricted flow within the rudder gap. When the turbulent boundary layer is more than three times thicker than that of the laminar boundary layer, the heat flux of the rudder shaft under the laminar flow condition is higher than that under the turbulent flow condition. Discovery of this phenomenon has great importance for guiding the design of the thermal protection system for the rudder shaft of hypersonic vehicles.     

Robust adaptive compensation control for unmanned autonomous helicopter with input saturation and actuator faults

This paper studies a robust adaptive compensation Fault Tolerant Control(FTC) for the medium-scale Unmanned Autonomous Helicopter(UAH) in the presence of external disturbances,actuator faults and input saturation.To improve the disturbance rejection capacity of the UAH system in actuator healthy case, an adaptive control method is adopted to cope with the external disturbances and a nominal controller is proposed to stabilize the system.Meanwhile, compensation control inputs are designed to reduce the negative effects derived from actuator faults and input saturation.Based on the backstepping control and inner-outer loop control technologies, a robust adaptive FTC scheme is developed to guarantee the tracking errors convergence.Under the presented FTC controller, the uniform ultimate boundedness of all closed-loop signals is ensured via Lyapunov stability analysis.Simulation results demonstrate the effectiveness of the proposed control algorithm.     

主流湍流度对涡轮导叶吸力面W型气膜孔冷却效率影响的实验研究

为了获得亚声速涡轮导叶吸力面不同位置处单排W型气膜孔的气膜冷却特性,在短周期跨声速风洞中实验研究了吹风比、主流湍流度对W型气膜孔冷却效率的影响。两列单排气膜孔分别布置在吸力面16%和21%相对弧长处,实验进口雷诺数范围为3.0×10⁵~9.0×10⁵,吹风比范围是0.5~2.0,叶栅出口等熵马赫数为0.8,高低湍流度分别为14.7% 和1.3%。实验结果表明：低湍流度时孔排1和孔排2下游的气膜冷却效率都随吹风比的增大先增大后减小,最佳吹风比分别为BR=1.2和BR=0.8。由于孔排1和孔排2所处位置的主流边界层状态不同,导致湍流度对于气膜冷却效率有不同的影响。对于孔排1,大吹风比时高湍流度使冷气核心向壁面移动,提高了气膜冷却效率;而小吹风比时,湍流度对冷却效率的影响随雷诺数升高而减弱。对于孔排2,大吹风比时高湍流度提高了孔附近区域的冷却效率,同时加快了冷却效率沿流向下降的速度,而在小吹风比时高湍流度显著降低了孔排下游气膜冷却效率。     

封严篦齿特征参数对其密封性能影响的数值分析

利用软件CFX对直通型篦齿的内部流动进行模拟,研究了直通型篦齿齿距、转速对其泄漏量的影响.计算结果表明:篦齿泄漏量随齿距的增大而减少,篦齿转速对篦齿泄漏量的影响很小.另外,本文提出一种变齿距直通型篦齿,研究变齿距对篦齿泄漏量的影响,并对变齿距齿形所处位置对泄漏量的影响进行研究.     

冶金法提纯多晶硅退火工艺优化的数学模型分析与试验验证

冶金法制备多晶硅过程中,通过对不同退火温控方案进行数学建模,探求优化的退火理论温度控制函数与曲线。数学模型表明,对硅铸锭直接进行保温,依靠自然热平衡退火,会使内部应力大于产生位错的临界应力;采用加热元件对硅铸锭适当加热保温可减缓降温速率。通过比较,选择较低的退火温度1 236℃和较短的退火时间8.52 ks作为试验退火温控方案。试验验证表明,该退火方案得到的多晶硅铸锭目视裂纹较少,少数载流子寿命与电阻率具有明显优势。     

某平台卫星发射及在轨力学环境测量与分析

为获取航天器准确的发射及在轨力学环境数据,设计了一套具有数据采集、存储和传输功能的星载测量系统。利用该系统对某大型平台卫星发射飞行过程进行了测量,获取了星箭界面及卫星结构典型位置在发射主动段的正弦振动响应、随机振动响应、冲击响应及在轨微振动的环境数据。将测量数据与星箭载荷耦合分析结果、地面力学试验结果进行了详细对比,结果表明:星箭载荷耦合分析的结果在星箭界面处横向相对准确,而纵向在有限频段准确,其他频段及星上分析结果均大于测量结果,即存在极大裕度;地面试验结果大于测量结果,意味着有较大的裁剪设计空间。测量数据对后续卫星模型修正、试验条件设计、相似平台卫星抗力学环境优化、部组件设计等均具有重要的参考价值。     

多旋翼无人机飞行控制自动调参技术

目前,多旋翼无人机控制器设计问题中存在着大量的依靠经验的调参工作。为了使调参简单而又可靠,本文基于控制器参数与控制系统性能响应存在的对应关系,提出了自动调参思想。在满足控制器各项性能指标的前提下,利用粒子群算法(Particle swarm optimization,PSO)提炼出优化目标和约束条件。对被控对象进行建模并搭建非线性模型。然后,利用工程实践方法估算出参数范围,并利用粒子群快速优化特点自动寻找在约束条件下符合性能指标的控制器参数。最后,通过Matlab/Simulink对模型进行仿真验证。仿真结果分析表明,PSD可快速准确地对飞行控制进行自动调参。     

民用无人机的监管与规范探讨

民用无人机（Unmanned aerial vehicle,UAV）市场广阔,但由于监管缺失导致威胁公共安全的事件频发。本文针对无人机监管难的问题,对民用无人机监管进行了研究。从无人机的生命周期入手,提出了应对无人机实施全生命周期监管的理念。从监管机构职能划分、监管措施制定与完善、法律法规制定与持续更新这三个方面对无人机全生命周期监管进行了详细的论述,建议通过理清任务、明确职责、设置目标、规范流程、制定措施、形成法律法规的方式,来构建无人机监管体系。重点论述了无人机监管措施的制定与完善,提出了由政府制定框架和规范、依靠民间力量来执行和完善的监管建议。     

基于非定常面元/黏性涡粒子法的低雷诺数滑流气动干扰

针对太阳能无人机螺旋桨滑流与机翼的气动干扰,考虑了低雷诺数流动下气体黏性和压缩性影响,并根据黎曼边界条件和涡量等效原则建立了能够快速计算分析螺旋桨-机翼气动干扰的非定常面元/黏性涡粒子的混合方法。首先使用有试验数据的风洞模型以及数值模拟技术对混合方法进行验证,在此基础上研究了不同安装位置与工况下螺旋桨与机翼的气动干扰。结果表明:螺旋桨对轴向气流的加速以及滑流诱导的上洗和下洗效应使机翼气动力呈现出增升增阻的现象,机翼升阻比有所下降。较大的弦向间距以及较高的垂直安装位置在减缓机翼升阻比下降的同时也使得螺旋桨拉力有所减小。对于多个螺旋桨的气动干扰,不同的桨叶旋转方向导致机翼气动力不同的变化规律,当旋转方向与机翼翼尖涡反向时,螺旋桨滑流能够抑制翼尖涡的强度,提高机翼气动效率。     

高重合度外啮合齿轮齿根弯曲应力计算方法

针对高重合度外啮合直齿圆柱齿轮副,对其齿根弯曲应力计算方法进行了研究.计算了高重合度齿轮的轮齿变形和刚度,对单个轮齿承受的载荷进行了研究,给出了高重合度齿轮齿间载荷分配率的定义和计算方法.以高重合度齿轮的双齿啮合界点作为计算载荷的加载点,给出了高重合度齿轮齿根过渡曲线30°切线位置危险截面的双齿啮合区界点的齿形系数和应力集中系数计算方法,获得了齿根危险截面弯曲应力的计算公式;采用CL 100齿轮试验机,设计了不同重合度的外啮合齿轮副,测量了其齿根的弯曲应力数值,试验结果表明:在高载荷下主动轮的齿根弯曲应力理论计算误差小于7.85%,从动轮的计算误差小于9.8%;低载荷下主动轮的齿根弯曲应力理论计算误差小于24.1%,从动轮的计算误差小于19%.