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91.
Fridman  A.M.  Khoruzhii  O.V. 《Space Science Reviews》2003,105(1-2):1-284
The review contains the important achievements in dynamics of the galactic disks. Among them there are I. New structures discovered recently: • giant vortices (including giant anticyclone in the Solar vicinity); • slow bar; • inner oscillating structure within spiral arms similar that of enveloped soliton; • chaotic streamlines in the velocity field of the gaseous disk of a real galaxy. II. New collective phenomina discovered recently: • new overreflection instability initiating ‘mini-spiral’ in the innermost central parsec of Galaxy; • large-scale convection caused by nonlinear interaction of density wave with disk gas; • non-kolmogorovian spectrum of weak turbulence corresponding to the observed one in the • Solar vicinity. III. New methods worked out recently: • reconstruction of full three-dimensional vector field of gas velocity from the observed line-of- • sight velocity field; • observational test for verification of the wave-nature of the spiral arms; • observational test to distinguish two types of vertical motions: warp and z-motions in the • density wave; • derivation of correct system of two-dimensional dynamical equations from the initial three- • dimensional one. This revised version was published online in June 2006 with corrections to the Cover Date.  相似文献   
92.
飞船返回舱俯仰振荡的动态稳定性研究   总被引:10,自引:3,他引:10  
本文研究了以平衡攻角为中心作单自由度俯仰振荡的飞船返回舱 ,其动态稳定形态随来流M∞ 的变化。设θ(t)是由平衡攻角起算的俯仰振荡角 ,Cm 是作用在飞船返回舱上的气动俯仰力矩系数 ,Cμ(θ, θ)· θ是机械阻尼力矩 (自由飞行时为零 ,实验时要计入其影响 ) ,文中给出飞船返回舱在平衡攻角处的俯仰振荡动态稳定性判据 ,并证明λ =λ(M∞) = Cm θ0+Cμ(0 ,0 ) 1 - Cm ¨θ0 是决定动稳定形态的重要参数。如果随M∞ 的变化 ,λ(M∞)由λ<0经过λ =0变化到λ>0 ,则飞船返回舱将由稳定的点吸引子形态 (即稳定在平衡攻角状态 )演化为周期吸引子形态 (即作周期振荡 )。对应于λ(M∞) =0的马赫数就是飞船返回舱的俯仰运动出现Hopf分叉的临界马赫数Mcr 。本文首先分析了飞船返回舱所受动态气动俯仰力矩的依赖状态变量 ,然后应用非线性动力学理论对飞船返回舱的俯仰运动进行了定性理论分析 ;最后耦合求解俯仰振荡方程和非定常Navier Stokes方程 ,数值模拟了飞船返回舱俯仰振荡随来流马赫数变化的Hopf分叉过程 ,验证了分析结论  相似文献   
93.
地面入射的大功率高频无线电波(泵波)和电离层等离子体之间的参数相互作用,能够引起静电波的激发,在一定条件下,产生不稳定性.本文用PIC静电粒子模拟方法,研究泵波与赤道电离层E区等离子体的相互作用.研究结果表明,泵波能够控制双流不稳定性的发生,在不同条件下,泵波对双流不稳定性起着稳定与不稳作用,模拟结果定性地与理论研究结果相符合,这为我们对不规则体产生的地面人工控制提供了依据.  相似文献   
94.
This paper is devoted to the study of propagation of disturbances caused by interplanetary shocks (IPS) through the Earth’s magnetosphere. Using simultaneous observations of various fast forward shocks by different satellites in the solar wind, magnetosheath and magnetosphere from 1995 till 2002, we traced the interplanetary shocks into the Earth’s magnetosphere, we calculated the velocity of their propagation into the Earth’s magnetosphere and analyzed fronts of the disturbances. From the onset of disturbances at different satellites in the magnetosphere we obtained speed values ranging from 500 to 1300 km/s in the direction along the IP shock normal, that is in a general agreement with results of previous numerical MHD simulations. The paper discusses in detail a sequence of two events on November 9th, 2002. For the two cases we estimated the propagation speed of the IP shock caused disturbance between the dayside and nightside magnetosphere to be 590 km/s and 714–741 km/s, respectively. We partially attributed this increase to higher Alfven speed in the outer magnetosphere due to the compression of the magnetosphere as a consequence of the first event, and partially to the faster and stronger driving interplanetary shock. High-time resolution GOES magnetic field data revealed a complex structure of the compressional wave fronts at the dayside geosynchronous orbit during these events, with initial very steep parts (10 s). We discuss a few possible mechanisms of such steep front formation in the paper.  相似文献   
95.
利用二维混合数值模拟研究了有速度驱动、低等离子体β值情况下的磁场重联过程,结果表明磁重联过程可以产生Alfven波,该Alfven波动对重新区中的新生离子作用,使得新生离子经历投掷角散射方程,具有球壳分布特征,部分新生离子得到加速,其获得的最大能量约为4(miVA0^2/2),此加速过程所需的加速时间在100/Ωi量级,是一个极快的加速机制,加速粒子能谱为双幂律谱。  相似文献   
96.
应用钠原子和中性大气分子的质量连续性方程来模拟突发纳层(SSL),垂直风场采用接近实际大气重力波的正弦行波模式,结果较好地反映了SSL的形成过程。SSL的形成时刻在5-15min之间并可持续到30min之后,形成高度大约在90-100km之间,峰宽为0.5-2km之间,这些都与实际观测SSL的特点相符,同时还进一步地研究了当重力波参数(主要指垂直波长和周期)、风速以及常态钠层半宽度发生变化时SSL的变化趋势。  相似文献   
97.
There are a host of factors influencing the excitation of Pc1 geomagnetic pulsations, which are ULF waves in the frequency range between 0.2 and 5 Hz. We have studied carefully the dependence of the pearl-type Pc1 activity at Sodankylä, Finland (L = 5.1) on the plasma density N in front of the magnetosphere, the bulk velocity V of the solar wind, and the intensity B of the IMF. The result is as follows: high values of N and reduced values of V are favorable to appearance of Pc1, whereas the dependence of Pc1 activity on B is practically absent. We also show that the probability of Pc1 occurrence decreases with the interplanetary electric field, and increases with solar wind impact pressure and with the plasma to magnetic pressure ratio “beta”.  相似文献   
98.
The present study examines the role of transverse waves and hydrodynamic instabilities mainly, Richtmyer–Meshkov instability (RMI) and Kelvin–Helmholtz instability (KHI) in detonation structure using two-dimensional high-resolution numerical simulations of Euler equations. To compare the numerical results with those of experiments, Navier–Stokes simulations are also performed by utilizing the effect of diffusion in highly irregular detonations. Results for both moderate and low activation energy mixtures reveal that upon collision of two triple points a pair of forward and backward facing jets is formed. As the jets spread, they undergo Richtmyer–Meshkov instability. The drastic growth of the forward jet found to have profound role in re-acceleration of the detonation wave at the end of a detonation cell cycle. For irregular detonations, the transverse waves found to have substantial role in propagation mechanism of such detonations. In regular detonations, the lead shock ignites all the gases passing through it, hence, the transverse waves and hydrodynamic instabilities do not play crucial role in propagation mechanism of such regular detonations. In comparison with previous numerical simulations present simulation using single-step kinetics shows a distinct keystone-shaped region at the end of the detonation cell.  相似文献   
99.
The Accelerometer Experiment (ACC) onboard Mars Global Surveyor (MGS) measured 1600 density profiles in the upper atmosphere of Mars during aerobraking. These measurements reveal large-scale and small-scale structure in the thermosphere of Mars. Here, the measurements of mass density for 115 orbits (#P0670–P0789) from November 1 to 30, 1998, under spring equinox and medium solar activity conditions (average F10.7 ∼ 137) during phase 2 of the aerobraking in the thermosphere of Mars at different altitudes and longitudes are presented for northern mid-latitude (17–42°N) in the dayside atmosphere using ACC onboard MGS. From these mass densities, the neutral densities of different gases are derived from their mixing ratios. Using these neutral densities, the longitudinal distribution of photoionization rates and photoelectron impact ionization rates are calculated at wavelength range 1–102.57 nm due to EUV and soft X-ray radiation under photochemical controlled region using Analytical Yield Spectrum approach (AYS). These conditions are appropriate for MGS Phase 2 aerobraking period from which the accelerometer data is used. Under the photochemical equilibrium condition, the electron density near the peak varies as the square root of the total peak ionization rate. Using this fact, an attempt is being made to estimate the mean primary and secondary peak electron density by averaging the longitudinal variations of total peak ionization rates in the northern mid-latitude (17–42°N) ionosphere of Mars, as there is no radio science measurement at this latitude region by MGS.  相似文献   
100.
Modulation of whistler waves in a plasma with time-dependant magnetic field perturbations was investigated experimentally. The experiments were performed on large “Krot” device, which was specially designed to study space plasma physics phenomena. It is shown that magnetic field variations on the wave propagation path can lead to splitting of initially continuous whistler wave into the sequence of bursts, whose repetition rate corresponds to magnetic field perturbation period. The frequency inside each burst is changing from its front edge to the back edge. Relative shift of the wave frequency can be as large as the relative magnetic disturbance. Distortion of whistler wave frequency spectrum after its passing through magnetically disturbed areas can be used as a diagnostics for low-frequency magnetic field variations. The applicability of our laboratory results to space plasma is discussed.  相似文献   
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