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排序方式: 共有893条查询结果,搜索用时 15 毫秒
52.
针对变截面结构产品,提出了一种变截面搭接结构搅拌摩擦焊接方法,通过加装辅助板将整条焊缝焊接方向上补偿为等厚度。焊接采用一次定位焊接+二次定位焊接+正式焊接的工艺方式,一次定位焊为预定位,二次定位焊保证辅助板与试片主体结构之间形成有效连接,正式焊保证形成完整的焊缝。焊缝表面成形良好,超声相控阵检测无超标缺陷。通过对力学性能的分析,变截面搭接结构处焊缝与非搭接处焊缝和常规对接焊缝的力学性能基本相同,平均抗拉强度均达到母材的70%以上,平均延伸率均在5.8%以上。变截面搭接焊缝焊核处晶粒形态为细小的等轴晶,靠近轴肩影响区部分的晶粒尺寸大于靠近焊缝根部的晶粒尺寸,受再结晶影响,焊缝两侧热机影响区处辅助板搭接界面消失。 相似文献
53.
从研究超声速气流中简化液滴(刚性小球)的气动力着手,比较分析使用CFD方法与使用两相流理论中已有的颗粒阻力系数模型得到的简化液滴气动力结果,得出Charles B.Henderson给出的阻力系数经验关系式适用于计算简化液滴在超声速气流中的运动。进一步,对不同直径简化液滴的运动开展工程方法的计算。在来流Ma=2.7的二维平板超声速流场中选取一个截面,作为气相流场,结果显示:(1)简化液滴与主气流存在相对超声速运动,当简化液滴直径dk≤0.12mm时,纵向相对超声速运动区域约为0.15m~0.4m,当dk0.12mm时,作用区域明显增大;(2)以10m/s喷射出的简化液滴,其横向穿透深度与纵向运动距离比约为0.004m/1m~0.021m/1m;(3)以100m/s的速度喷射出的30~120μm直径简化液滴,其横向穿透深度与纵向运动距离比约为0.02m/1m~0.055m/1m,实际过程中,小尺寸简化液滴的汽化很快,其穿透深度很小。 相似文献
54.
在风浪槽中进行水气动量交换实验,测量了不同风速和风区下的波浪及空气湍流流场。测量数据表明水面上风速分布符合对数律,水气界面附近在小范围的动量交换常通量层。阻力系数CD随风速增加线性增长,随波龄增加而减小。这一趋向与理论分析及外海帝测结果一致。对风浪发展过程中波浪和空气湍流谱结构的分析证明了水气运动的耦合关系。 相似文献
55.
单框架控制力矩陀螺(SGCMG)框架伺服系统内部存在的各种干扰会严重影响陀螺的力矩输出精度。为了实现力矩输出的高精度控制,需要对框架伺服系统进行精确动力学建模与控制。通过对作用于航天器上SGCMG的详细动力学分析,建立了框架伺服系统动力学模型,其中考虑了动静不平衡干扰力矩以及摩擦力矩。基于正弦永磁同步电机,利用自抗扰理论设计了框架伺服系统内外环控制器。仿真结果表明,在忽略转子不平衡所引起的高频干扰力矩的前提下,此控制器能对内外环存在的所有建模及未建模干扰进行准确估计和补偿,保证了框架的高精度控制。通过仿真还得到了转子不平衡对框架控制精度的影响量级,将为进一步研究如何抑制不平衡振动提供参考依据。 相似文献
56.
在0.6m×0.6m亚跨超声速风洞中,采用油膜干涉测量技术(OFI)和Preston管方法开展了马赫数0.4~0.8下的平板模型表面摩擦应力测量实验研究。模型头部经过椭圆化处理,避免出现流动分离。实验发现:在亚跨声速条件下,两种方法的测量结果具有很好的一致性;油膜粘性对摩擦应力测量结果影响很小;当来流马赫数或总压发生变化时,摩擦应力系数随来流动压或马赫数与雷诺数的乘积(Ma·Re)的增大而减小。在Ma=0.4和0.6时,观测到一种类似斑纹的干涉图像,基于其特性分析,提出以此作为一种转捩判据的设想;在Ma=0.8时,未观察到类似斑纹,根据油膜图像和数值模拟结果判断,模型头部出现了分离泡,边界层由分离诱导转捩。 相似文献
57.
This paper studies a nonlinear robust control algorithm of the electro-hydraulic load simulator (EHLS). The tracking performance of the EHLS is mainly limited by the actuator's motion disturbance, flow nonlinearity, and friction, etc. The developed controller is developed based on the nonlinear motion loading model. The problems of the actuator's disturbance and flow nonlinearity are considered. To address the friction problem, the friction model of the loading motor is identified experimentally. The friction disturbance is compensated using the obtained friction model. Therefore, this paper considers the main three factors comprehensively. The developed algorithm is easy to apply since the controller can be obtained just with one step back-stepping design. The stability of the developed algorithm is proven via Lyapunov analysis. Both co-simulation and experiments are performed to verify the effectiveness of this method. 相似文献
58.
To overcome the influence of the nonlinear friction on the gimbaled servo-system of an inertial stabilized platforms(ISPs) with DC motor direct-drive, the methods of modeling and compensation of the nonlinear friction are proposed. Firstly, the inapplicability of LuGre model when trying to interpret the backward angular displacement in the prestiction regime is observed experimentally and the reason is deduced theoretically. Then, based on the dynamic model of direct-drive ISPs, a modified LuGre model is proposed to describe the characteristic of the friction in the prestiction regime. Furthermore, the state switch condition of the three friction regimes including presliding, gross sliding and prestiction is presented. Finally, a composite compensation controller including a nonlinear friction observer and a feedforward compensator based on the novel LuGre model is designed to restrain the nonlinear friction and to improve the control precision. Experimental results indicate that compared with those of the conventional proportion–integration–differentiation(PID) control method and the PID plus LuGre model-based friction compensation method, the dwell-time has decreased from 0.2 s to almost 0 s, the position error decreased to 86.7%and the peak-to-peak value of position error decreased to 80% after the novel compensation controller is added. It concludes that the composite compensation controller can greatly improve the control precision of the dynamic sealed ISPs. 相似文献
59.
This paper presents the model of calculating the total friction moment of space gyroscope ball bearings which usually work under ultra-low oscillatory motion and are very sensitive to the friction moment. The aim is to know the proportion of the friction moment caused by each frictional source in the bearing's total friction moment, which is helpful to optimize the bearing design to deduce the friction moment. In the model, the cage dynamic equations considering six degree-of-freedom and the balls dynamic equations considering two degree-of-freedom were solved.The good trends with different loads between the measured friction moments and computational results prove that the model under constant rate was validated. The computational results show that when the speed was set at 5 r/min, the bearing's maximum total friction moment when oscillation occurred was obviously larger than that occurred at a constant rate. At the onset of each oscillatory motion, the proportion of the friction moment caused by cage in the bearing's total friction moment was very high, and it increased with the increasing speed. The analyses of different cage thicknesses and different clearances between cage pocket and ball show that smaller thickness and clearance were preferred. 相似文献
60.