全文获取类型
收费全文 | 2183篇 |
免费 | 276篇 |
国内免费 | 327篇 |
专业分类
航空 | 582篇 |
航天技术 | 1012篇 |
综合类 | 89篇 |
航天 | 1103篇 |
出版年
2024年 | 3篇 |
2023年 | 45篇 |
2022年 | 51篇 |
2021年 | 89篇 |
2020年 | 86篇 |
2019年 | 64篇 |
2018年 | 93篇 |
2017年 | 43篇 |
2016年 | 69篇 |
2015年 | 93篇 |
2014年 | 214篇 |
2013年 | 153篇 |
2012年 | 114篇 |
2011年 | 208篇 |
2010年 | 154篇 |
2009年 | 150篇 |
2008年 | 144篇 |
2007年 | 101篇 |
2006年 | 115篇 |
2005年 | 115篇 |
2004年 | 77篇 |
2003年 | 57篇 |
2002年 | 73篇 |
2001年 | 54篇 |
2000年 | 66篇 |
1999年 | 74篇 |
1998年 | 45篇 |
1997年 | 36篇 |
1996年 | 31篇 |
1995年 | 28篇 |
1994年 | 16篇 |
1993年 | 18篇 |
1992年 | 17篇 |
1991年 | 17篇 |
1990年 | 13篇 |
1989年 | 16篇 |
1988年 | 30篇 |
1987年 | 8篇 |
1986年 | 4篇 |
1984年 | 2篇 |
排序方式: 共有2786条查询结果,搜索用时 651 毫秒
991.
Karim Douch Hu Wu Christian Schubert Jürgen Müller Franck Pereira dos Santos 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2018,61(5):1307-1323
The prospects of future satellite gravimetry missions to sustain a continuous and improved observation of the gravitational field have stimulated studies of new concepts of space inertial sensors with potentially improved precision and stability. This is in particular the case for cold-atom interferometry (CAI) gradiometry which is the object of this paper. The performance of a specific CAI gradiometer design is studied here in terms of quality of the recovered gravity field through a closed-loop numerical simulation of the measurement and processing workflow. First we show that mapping the time-variable field on a monthly basis would require a noise level below . The mission scenarios are therefore focused on the static field, like GOCE. Second, the stringent requirement on the angular velocity of a one-arm gradiometer, which must not exceed ?rad/s, leads to two possible modes of operation of the CAI gradiometer: the nadir and the quasi-inertial mode. In the nadir mode, which corresponds to the usual Earth-pointing satellite attitude, only the gradient , along the cross-track direction, is measured. In the quasi-inertial mode, the satellite attitude is approximately constant in the inertial reference frame and the 3 diagonal gradients and are measured. Both modes are successively simulated for a 239?km altitude orbit and the error on the recovered gravity models eventually compared to GOCE solutions. We conclude that for the specific CAI gradiometer design assumed in this paper, only the quasi-inertial mode scenario would be able to significantly outperform GOCE results at the cost of technically challenging requirements on the orbit and attitude control. 相似文献
992.
Victor U.J. Nwankwo Sandip K. Chakrabarti 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2018,61(7):1880-1889
We study the effects of space weather on the ionosphere and low Earth orbit (LEO) satellites’ orbital trajectory in equatorial, low- and mid-latitude (EQL, LLT and MLT) regions during (and around) the notable storms of October/November, 2003. We briefly review space weather effects on the thermosphere and ionosphere to demonstrate that such effects are also latitude-dependent and well established. Following the review we simulate the trend in variation of satellite’s orbital radius (r), mean height (h) and orbit decay rate (ODR) during 15 October–14 November 2003 in EQL, LLT and MLT. Nominal atmospheric drag on LEO satellite is usually enhanced by space weather or solar-induced variations in thermospheric temperature and density profile. To separate nominal orbit decay from solar-induced accelerated orbit decay, we compute and ODR in three regimes viz. (i) excluding solar indices (or effect), where and (ii) with mean value of solar indices for the interval, where and and (iii) with actual daily values of solar indices for the interval ( and ODR). For a typical LEO satellite at h?=?450?km, we show that the total decay in r during the period is about 4.20?km, 3.90?km and 3.20?km in EQL, LLT and MLT respectively; the respective nominal decay () is 0.40?km, 0.34?km and 0.22?km, while solar-induced orbital decay () is about 3.80?km, 3.55?km and 2.95?km. h also varied in like manner. The respective nominal is about 13.5?m/day, 11.2?m/day and 7.2?m/day, while solar-induced is about 124.3?m/day, 116.9?m/day and 97.3?m/day. We also show that severe geomagnetic storms can increase ODR by up to 117% (from daily mean value). However, the extent of space weather effects on LEO Satellite’s trajectory significantly depends on the ballistic co-efficient and orbit of the satellite, and phase of solar cycles, intensity and duration of driving (or influencing) solar event. 相似文献
993.
Hou-Yuan Lin Chang-Yin Zhao 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2018,61(1):182-188
The rotational state of Envisat is re-estimated using the specular glint times in optical observation data obtained from 2013 to 2015. The model is simplified to a uniaxial symmetric model with the first order variation of its angular momentum subject to a gravity-gradient torque causing precession around the normal of the orbital plane. The sense of Envisat’s rotation can be derived from observational data, and is found to be opposite to the sense of its orbital motion. The rotational period is estimated to be , where t is measured in days from the beginning of 2013. The standard deviation is 0.760?s, making this the best fit obtained for Envisat in the literature to date. The results demonstrate that the angle between the angular momentum vector and the negative normal of the orbital plane librates around a mean value of with an amplitude from about (in 2013) to (in 2015), with the libration period equal to the precession period of the angular momentum, from about 4.8?days (in 2013) to 3.4?days (in 2015). The ratio of the minimum to maximum principal moments of inertia is estimated to be , and the initial longitude of the angular momentum in the orbital coordinate system is . The direction of the rotation axis derived from our results at September 23, 2013, UTC 20:57 is similar to the results obtained from satellite laser ranging data but about closer to the negative normal of the orbital plane. 相似文献
在外场雷达散射截面(RCS)测量中,受随时间变化的环境因素影响,不同时刻测得到的数据其幅度和相位不完全相干,导致直接采用背景矢量相减技术难以有效地抑制背景杂波。建立了测量系统-测试场时变传递函数的参数化模型来表征环境变化对雷达接收回波的影响,并在此基础上提出了一种改进的精确背景抵消处理技术。首先,从现场测量回波数据中提取辅助校准区域数据;然后,利用降噪互相关法和优化相干函数法估计出时变传递函数模型参数,并据此对不同时刻测得的回波数据进行幅度和相位补偿,使得两者完全相干;最后,做精确的背景矢量相减处理。实验结果验证了本文技术和算法的有效性。 相似文献
995.
为研究三电极的电偶腐蚀行为,测量了CF8611/AC531复合材料(CFRP)、7B04-T74铝合金(7B04)和镀锌30CrMnSiA钢(GSB)的极化曲线;开展了搭接件在模拟海洋环境下的全浸试验;设计了圆形三电极,推导了稳态腐蚀场和参数化扫描方程,建立了三电极和搭接件的电偶腐蚀模型。结果表明:稳态腐蚀场中的电势分布符合Laplace方程;电位最高的CFRP为阴极,最低的GSB为阳极,中间的7B04阴/阳极角色会随某一电极面积变化而转变,给出了转变的临界面积比,各电极表面电偶电流服从指数分布,相关系数近于1,拟合精度高;在搭接件中,搭接区电位和电流密度最高,并向两端对称递减,7B04和GSB均为阳极,电流密度分别提高约210倍和328倍,电偶腐蚀效应显著;搭接区7B04板全面腐蚀,厚度损失约1.011%;仿真所得点蚀敏感区宽度范围为3.9~7.6mm,实测所得宽度范围为4.667~8.872mm,二者范围、形状及变化规律吻合较好,表明模型有效、可靠。 相似文献
996.