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681.
We present the results of a cross-correlation analysis made on the basis of Spearman’s rank correlation method. The quantities
to correlate are daily values of the fluence of energetic electrons at a geosynchronous orbit, intensities of ground and interplanetary
ultra-low-frequency (ULF) oscillations in the Pc5 range, and parameters of the solar wind. The period under analysis is the
23rd cycle of solar activity, 1996–2006. Daily (from 6 h to 18 h of LT) magnetic data at two diametrically opposite observatories
of the Intermagnet network are taken as ground-based measurements. The fluxes of electrons with energies higher than 2 MeV
were measured by the geosynchronous GOES satellites. The data of magnetometers and plasma instruments installed on ACE and WIND spacecraft were used for analysis of the solar wind parameters and of the oscillations of the interplanetary magnetic field
(IMF). Some results elucidating the role played by interplanetary ULF waves in the processes of generation of magneospheric
oscillations and acceleration of energetic electrons are obtained. Among them are (i) high and stable correlation of ground
ULF oscillations with waves in the solar wind; (ii) closer link of mean daily amplitudes of both interplanetary and ground
oscillations with ‘tomorrow’ values of the solar wind velocity than with current values; and (iii) correlation of the intensity
of ULF waves in the solar wind, normalized to the IMF magnitude, with fluxes of relativistic electrons in the magnetosphere. 相似文献
682.
V. L. Varsegov 《Russian Aeronautics (Iz VUZ)》2010,53(2):212-220
An integral method is proposed for calculating a jet propagating from the turbofan engine thrust reverser and interacting
with a stream formed as a result of the after-landing aircraft run. The calculation results for the PS-90 engine are presented.
The calculation data obtained show that the mathematical model developed adequately describes a qualitative pattern of main
parameter variation in the sector jet propagating in a stream. 相似文献
683.
The application of the optimized dispersion relation preserving scheme (DRP-scheme) in combination with the explicit optimized
two-layer Runge-Kutta scheme is presented to solve a system of one-dimensional and quasi-one-dimensional Euler equations using
as an example the solution of four test problems, namely, discontinuity disintegration in a tube (Sod’s problem); transfer
of the lowamplitude Gaussian pulse; acoustic wave propagation through the transonic nozzle; acoustic wave-shock interaction.
Also given are the comparison of the calculation results using different schemes: DRP, CABARET, CE-SE and the standard Lax-Wendroff
schemes as well as the solutions obtained with the use of software packages. 相似文献
684.
Based on the results of plasma and magnetic measurements at three different points of the heliosphere and telescopic observations
of the Sun from these points we study simultaneously high-speed streams (HSS) of the solar wind (SW) near the Earths’s orbit
and coronal holes (CH) that have generated them. The data from spacecraft STEREO-A, STEREO-B, ACE, and SOHO are used together with ground-based observations from March 2007 to May 2008. In this period there existed HSS whose sources
represented CH of various polarity, geometry, and location relative to the heliographic and heliomagnetic equators. Dependence
of SW parameters on mutual positions of spacecraft with respect to CH and heliospheric current sheet, and also on heliolatitude
and geometry of the CH is revealed. A difference of more than 5° in locations of spacecraft with respect to the heliospheric
current sheet in November 2007 allowed us to discover a heliolatitude velocity gradient of the SW streams between the STEREO-A and STEREO-B spacecraft. On the average this gradient at that time was equal to 20 km/s per degree. Substantial variations in SW streams
associated with variations of the HSS SW sources during a few hours or days were also observed. This variability makes it
difficult to use the data of spacecraft STEREO-B for sufficiently accurate prediction of SW properties in the near-Earth space by the method of simple advanced ti me shift
due to heliolongitude difference between a spacecraft and the Earth even in solar activity minimum. 相似文献
685.
O. Alexandrova C. H. K. Chen L. Sorriso-Valvo T. S. Horbury S. D. Bale 《Space Science Reviews》2013,178(2-4):101-139
Solar wind is probably the best laboratory to study turbulence in astrophysical plasmas. In addition to the presence of magnetic field, the differences with neutral fluid isotropic turbulence are: (i) weakness of collisional dissipation and (ii) presence of several characteristic space and time scales. In this paper we discuss observational properties of solar wind turbulence in a large range from the MHD to the electron scales. At MHD scales, within the inertial range, turbulence cascade of magnetic fluctuations develops mostly in the plane perpendicular to the mean field, with the Kolmogorov scaling $k_{\perp}^{-5/3}$ for the perpendicular cascade and $k_{\|}^{-2}$ for the parallel one. Solar wind turbulence is compressible in nature: density fluctuations at MHD scales have the Kolmogorov spectrum. Velocity fluctuations do not follow magnetic field ones: their spectrum is a power-law with a ?3/2 spectral index. Probability distribution functions of different plasma parameters are not Gaussian, indicating presence of intermittency. At the moment there is no global model taking into account all these observed properties of the inertial range. At ion scales, turbulent spectra have a break, compressibility increases and the density fluctuation spectrum has a local flattening. Around ion scales, magnetic spectra are variable and ion instabilities occur as a function of the local plasma parameters. Between ion and electron scales, a small scale turbulent cascade seems to be established. It is characterized by a well defined power-law spectrum in magnetic and density fluctuations with a spectral index close to ?2.8. Approaching electron scales, the fluctuations are no more self-similar: an exponential cut-off is usually observed (for time intervals without quasi-parallel whistlers) indicating an onset of dissipation. The small scale inertial range between ion and electron scales and the electron dissipation range can be together described by $\sim k_{\perp}^{-\alpha}\exp(-k_{\perp}\ell_{d})$ , with α?8/3 and the dissipation scale ? d close to the electron Larmor radius ? d ?ρ e . The nature of this small scale cascade and a possible dissipation mechanism are still under debate. 相似文献
686.
N.C. Joshi W. Uddin A.K. Srivastava R. Chandra N. Gopalswamy P.K. Manoharan M.J. Aschwanden D.P. Choudhary R. Jain N.V. Nitta H. Xie S. Yashiro S. Akiyama P. Mäkelä P. Kayshap A.K. Awasthi V.C. Dwivedi K. Mahalakshmi 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2013
687.
N. Gopalswamy H. Xie P. Mäkelä S. Yashiro S. Akiyama W. Uddin A.K. Srivastava N.C. Joshi R. Chandra P.K. Manoharan K. Mahalakshmi V.C. Dwivedi R. Jain A.K. Awasthi N.V. Nitta M.J. Aschwanden D.P. Choudhary 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2013
Employing coronagraphic and EUV observations close to the solar surface made by the Solar Terrestrial Relations Observatory (STEREO) mission, we determined the heliocentric distance of coronal mass ejections (CMEs) at the starting time of associated metric type II bursts. We used the wave diameter and leading edge methods and measured the CME heights for a set of 32 metric type II bursts from solar cycle 24. We minimized the projection effects by making the measurements from a view that is roughly orthogonal to the direction of the ejection. We also chose image frames close to the onset times of the type II bursts, so no extrapolation was necessary. We found that the CMEs were located in the heliocentric distance range from 1.20 to 1.93 solar radii (Rs), with mean and median values of 1.43 and 1.38 Rs, respectively. We conclusively find that the shock formation can occur at heights substantially below 1.5 Rs. In a few cases, the CME height at type II onset was close to 2 Rs. In these cases, the starting frequency of the type II bursts was very low, in the range 25–40 MHz, which confirms that the shock can also form at larger heights. The starting frequencies of metric type II bursts have a weak correlation with the measured CME/shock heights and are consistent with the rapid decline of density with height in the inner corona. 相似文献
688.
F. Vigier A. Le Postollec G. Coussot D. Chaput H. Cottin T. Berger S. Incerti S. Triqueneaux M. Dobrijevic O. Vandenabeele-Trambouze 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2013
Biochips might be suited for planetary exploration. Indeed, they present great potential for the search for biomarkers – molecules that are the sign of past or present life in space – thanks to their size (miniaturized devices) and sensitivity. Their detection principle is based on the recognition of a target molecule by affinity receptors fixed on a solid surface. Consequently, one of the main concerns when developing such a system is the behavior of the biological receptors in a space environment. In this paper, we describe the preparation of an experiment planned to be part of the EXPOSE-R2 mission, which will be conducted on the EXPOSE-R facility, outside the International Space Station (ISS), in order to study the resistance of biochip models to space constraints (especially cosmic radiation and thermal cycling). This experiment overcomes the limits of ground tests which do not reproduce exactly the space parameters. Indeed, contrary to ground experiments where constraints are applied individually and in a limited time, the biochip models on the ISS will be exposed to cumulated constraints during several months. Finally, this ISS experiment is a necessary step towards planetary exploration as it will help assessing whether a biochip can be used for future exploration missions. 相似文献
689.
M. V. Levskii 《Cosmic Research》2011,49(6):521-533
The problem of optimal turn of a spacecraft from an arbitrary initial position to a final specified angular position in a
minimum time is considered and solved. A case is investigated, when the constraint on spacecraft’s angular momentum during
the turn is essential. Based on the quaternion method a solution to the posed problem has been found, and an optimal control
program is constructed taking the constraints on controlling moment into account. The optimal control is found in the class
of regular motions. A condition (calculation expression) is presented for determining the moment to begin braking with the
use of measurements of current motion parameters, which considerably improves the accuracy of putting the spacecraft into
a preset position. For a dynamically symmetrical spacecraft the solution to the problem of optimal control by the spacecraft
spatial turn is presented in analytical form (expressions in elementary functions). An example of mathematical modeling of
the spacecraft motion dynamics under optimal control over reorientation is given. 相似文献
690.