首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   118245篇
  免费   1915篇
  国内免费   1039篇
测绘学   2985篇
大气科学   8712篇
地球物理   24130篇
地质学   40990篇
海洋学   10131篇
天文学   26134篇
综合类   311篇
自然地理   7806篇
  2021年   944篇
  2020年   1122篇
  2019年   1190篇
  2018年   2527篇
  2017年   2379篇
  2016年   3133篇
  2015年   2000篇
  2014年   3106篇
  2013年   6138篇
  2012年   3273篇
  2011年   4610篇
  2010年   3946篇
  2009年   5397篇
  2008年   4955篇
  2007年   4574篇
  2006年   4490篇
  2005年   3697篇
  2004年   3732篇
  2003年   3485篇
  2002年   3275篇
  2001年   2947篇
  2000年   2861篇
  1999年   2397篇
  1998年   2453篇
  1997年   2346篇
  1996年   2012篇
  1995年   1963篇
  1994年   1769篇
  1993年   1606篇
  1992年   1531篇
  1991年   1398篇
  1990年   1599篇
  1989年   1373篇
  1988年   1228篇
  1987年   1510篇
  1986年   1312篇
  1985年   1650篇
  1984年   1844篇
  1983年   1753篇
  1982年   1629篇
  1981年   1511篇
  1980年   1344篇
  1979年   1253篇
  1978年   1318篇
  1977年   1195篇
  1976年   1143篇
  1975年   1073篇
  1974年   1072篇
  1973年   1069篇
  1972年   686篇
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
191.
We investigate, via a two-dimensional (nonplanar) MHD simulation, a situation wherein a bipolar magnetic field embedded in a stratified solar atmosphere (i.e., arch-filament-like structure) undergoes symmetrical shear motion at the footpoints. It was found that the vertical plasma flow velocities grow exponentially leading to a new type of global MHD-instability that could be characterized as a Dynamic Shearing Instability, with a growth rate of about 8{ovV} A a, where {ovV} A is the average Alfvén speed and a –1 is the characteristic length scale. The growth rate grows almost linearly until it reaches the same order of magnitude as the Alfvén speed. Then a nonlinear MHD instability occurs beyond this point. This simulation indicates the following physical consequences: the central loops are pinched by opposing Lorentz forces, and the outer closed loops stretch upward with the vertically-rising mass flow. This instability may apply to arch filament eruptions (AFE) and coronal mass ejections (CMEs).To illustrate the nonlinear dynamical shearing instability, a numerical example is given for three different values of the plasma beta that span several orders of magnitude. The numerical results were analyzed using a linearized asymptotic approach in which an analytical approximate solution for velocity growth is presented. Finally, this theoretical model is applied to describe the arch filament eruption as well as CMEs.  相似文献   
192.
193.
A preliminary numerical analysis of the power spectrum of solar oscillations of the SCLERA group suggests that this curve can be characterized by a Hausdorff-Besicovich dimension close to 3/2 near the present observational resolution (0.03 mHz). We show that this result is not inconsistent with the presence of a component due to non-linear, turbulent-like motions, which, in addition to linear oscillation modes, is shaping the observed spectral distribution.On leave of absence from Institut d'Astrophysique, Cointe-Ougrée, Belgium.  相似文献   
194.
195.
196.
197.
198.
The secular variation of the thermal structure of the Martian atmosphere during the dissipation phase of the 1971 dust storm is examined, using temperatures obtained by the infrared spectroscopy investigation on Mariner 9. For the latitude range ?20° to ?30°, the mean temperature at the 2mbar level is found to decrease from approximately 220 K in mid-December 1971 to about 190 K by June 1972 while for the 0.3mbar level a decrease from 203 K to 160 K is observed. Over the same period, the amplitude of the diurnal temperature wave also decreased. Assuming a simplified radiative heating model, the dust optical depth is found to decrease approximately exponentially with an e-folding time of about 60 days at both the 0.3 and 2mbar levels. Stokes-Cunningham settling alone cannot account for this behavior. Sedimentation models which include both gravitational settling and vertical mixing are developed in an effort to explain the time evolution of the dust. Within the framework of a model which assumes an effective vertical diffusivity K independent of height, a mean dust particle diameter of ~2 μm is inferred. To provide the necessary vertical mixing, K ? 107 cm2sec?1 is required in the lower atmosphere.  相似文献   
199.
200.
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号