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841.
从理论上分析了共面近地圆轨道上的航天器的远程双主动交会的问题.根据轨道动力学基本原理,导出各种情况下特征速度的解析解,为航天器变轨时的燃料消耗分析提供了依据.进一步探讨了航天器轨道转移过程中的时间策略,以保证在不同轨道上运行的航天器在同一时刻、同一空间位置交会.上述理论分析的仿真计算结果表明,双主动交会总特征速度和过程耗时都低于主被动交会情形,单星的燃料消耗大大降低,对大范围快速变轨,优势更加明显. 相似文献
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843.
惯导系统初始对准一般采用卡尔曼滤波器对初始姿态误差角进行估计,而在设计卡尔曼滤波器之前通常要对系统进行可观测性分析,确定卡尔曼滤波器的效果。捷联惯导系统的卡尔曼滤波模型在传递对准时,为线性时变系统,而线性时变系统的可观测性分析比较困难。文中采用一种依据系统矩阵的奇异值确定状态可观测度的方法对基于“速度+姿态”快速传递对准的卡尔曼滤波模型进行可观测性分析,结果表明该方法可直接简单地实现系统状态的可观测度分析。 相似文献
844.
随着激光陀螺技术的发展,旋转调制式激光陀螺惯性导航系统逐渐成为舰载主惯导系统,舰载机、舰载武器系统需要旋转调制式激光惯导系统提供的姿态、速度和位置信息进行对准,即主子惯导的传递对准。由于旋转调制式系统中的姿态、速度和位置具有随旋转的短周期波动问题,势必会影响对准时间较短的子惯导对准精度。为了保证传递对准的快速性,一般采用速度匹配方法。定量分析了主子惯导传递对准过程中主惯导速度误差短周期波动对子惯导系统对准精度的影响,首先进行了数字仿真,之后利用双轴激光陀螺惯导、纯捷联光纤陀螺惯导数据进行了半实物仿真,验证了主惯导速度误差的一次项系数与子惯导初始对准水平姿态误差呈线性关系,二次项系数与子惯导初始对准航向误差呈线性关系。 相似文献
845.
设计了抖动偏频激光陀螺捷联惯导系统的动基座传递对准方案,并进行了仿真计算及海上试验验证。激光陀螺捷联惯导系统采用该传递对准方案在试验船上完成了数十次海上传递对准试验,结果表明,该传递对准方案具有如下优点:在传递对准过程中,不专门要求载体作加速或S型机动运动;抗载体扰动运动的能力强;对准精度高。 相似文献
846.
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848.
Three-dimensional numerical computations are conducted to investigate the effects of the blowing ratio and corrugation geometry on the adiabatic film cooling effectiveness as well as the heat transfer coefficient over a transverse corrugated surface. It is noticeable that the adiabatic wall temperature on the wavy valley of the transverse corrugated surface is relatively lower than that on the wavy peak. Surface corrugation has a relatively obvious influence on the laterally-averaged adiabatic film cooling effectiveness in the region where the effusion film layer is developed, but has little influence in the front region. Compared to a flat surface, the transverse corrugated sur-face produces a smaller adiabatic film cooling effectiveness and a higher heat transfer coefficient ratio. The effusion cooling difference between the flat and corrugated surfaces behaves more obvi-ously under a small aspect ratio of the wavy corrugation. 相似文献
849.
Numerical predictions of three-dimensional flow and heat transfer are performed for a two-pass square channel with 45° staggered ribs in non-orthogonally mode-rotation using the second moment closure model. At Reynolds number of 25,000, the rotation numbers studied were 0,0.24, 0.35 and 1.00. The density ratios were 0.13, 0.23 and 0.50. The results show that at high buoyancy parameter and high rotation number with a low density ratio, the flow in the first passage is governed by the secondary flow induced by the rotation whereas the secondary flow induced by the skewed ribs was almost distorted. As a result the heat transfer rate is enhanced on both co-trailing and co-leading sides compared to low and medium rotation number. In contrast, for the second passage, the rotation slightly reduces the heat transfer rate on co-leading side at high rotation number with a low density ratio and degrades it significantly on both co-trailing and co-leading sides at high buoyancy parameter compared to the stationary, low and medium rotation numbers. The numerical results are in fair agreement with available experimental data in the bend region and the second passage, while in the first passage were overestimated at low and medium rotation numbers. 相似文献
850.
The heat transfer in a novel smooth wedge-shaped cooling channel with lateral ejection of turbine blade trailing edge is experimentally investigated in both non-rotating and rotating cases. Beside the conventional inlet at the bottom of the channel, an extra coolant injection from 8 lateral non-equant holes is introduced to improve the overall heat transfer. The total mass flow rate ratio (lateral mass flow rate/total mass flow rate) varies from 0 to 1.0. The major inlet Reynolds number and rotation number respectively vary from 10000 to 20000 and from 0 to 1.16. Experimental results show that the lateral inlet decreases local bulk temperature and increases local heat transfer at the middle and the top of the static channel. In rotating cases, the lateral inlet notably improves the heat transfer at the high-radius half channel and compensates the negative effects induced by the rotation. Both intensity and uniformity of heat transfer inside the channel are enhanced while flow resistance decreases with proper mass flow rate ratio of coolant from two inlets. The most satisfactory total mass flow rate ratio is around 2/3. This new structural style of cooling channel has huge potential and provides new direction of heat transfer of turbine blade trailing edge. 相似文献