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   630篇
  免费   14篇
  国内免费   9篇
测绘学   15篇
大气科学   43篇
地球物理   132篇
地质学   197篇
海洋学   80篇
天文学   117篇
综合类   3篇
自然地理   66篇
  2021年   5篇
  2020年   9篇
  2019年   5篇
  2018年   10篇
  2017年   9篇
  2016年   11篇
  2015年   18篇
  2013年   34篇
  2012年   11篇
  2011年   26篇
  2010年   20篇
  2009年   21篇
  2008年   25篇
  2007年   18篇
  2006年   12篇
  2005年   23篇
  2004年   24篇
  2003年   26篇
  2002年   25篇
  2001年   15篇
  2000年   27篇
  1999年   21篇
  1998年   19篇
  1997年   11篇
  1996年   8篇
  1995年   8篇
  1994年   12篇
  1993年   14篇
  1992年   4篇
  1991年   5篇
  1990年   6篇
  1989年   7篇
  1988年   4篇
  1987年   9篇
  1986年   14篇
  1985年   11篇
  1984年   10篇
  1983年   15篇
  1982年   13篇
  1981年   5篇
  1980年   5篇
  1979年   11篇
  1978年   10篇
  1977年   9篇
  1976年   10篇
  1975年   7篇
  1974年   4篇
  1973年   4篇
  1971年   8篇
  1970年   4篇
排序方式: 共有653条查询结果,搜索用时 31 毫秒
621.
622.
Numerical experiments with steady-state ground water flow models show that spiraling flow lines occur in layered aquifers that have different anisotropic horizontal hydraulic conductivities in adjacent layers. Bundles of such flow lines turning in the same direction can be referred to as ground water whirls. An anisotropic layered block in a field of uniform horizontal flow results in one or more whirls with their axes in the uniform flow direction. The number of whirls depends on the number of interfaces between layers with different anisotropic properties. For flow to a well in an aquifer consisting of two anisotropic layers, with perpendicular major principal directions, whirls are found to occur in quadrants that are bounded by the principal directions of the hydraulic conductivity. The combined effect of flow to a well and a layered anisotropy implies that a single well in a system with a single anisotropic layer within an otherwise isotropic aquifer causes eight whirls. All adjacent whirls rotate in opposite directions.  相似文献   
623.
Willes  A. J.  Robinson  P. A. 《Solar physics》1997,170(2):341-356
Previous comparisons between predicted and observed electric field strengths and volume emissivities in second harmonic type III solar radio emission are improved in two ways. First, the assumption of the head-on approximation in deriving the harmonic emission rate, which is not applicable over the full range of observed type III parameters, is replaced with a more suitable approximation. Secondly, a more realistic functional form for the Langmuir wave spectra is adopted. The revised predicted electric field strengths and volume emissivities are consistent with the observed values.  相似文献   
624.
SPEAR is a new polar cap HF radar facility which is to be deployed on Svalbard. The principal capabilities of SPEAR will include the generation of artificial plasma irregularities, operation as an all-sky HF radar, the excitation of ULF waves, and remote sounding of the magnetosphere. Operation of SPEAR in conjunction with the multitude of other instruments on Svalbard, including the EISCAT Svalbard radar, and the overlap of its extensive field-of-view with that of several of the HF radars in the SuperDARN network, will enable in-depth diagnosis of many geophysical and plasma phenomena associated with the cusp region and the substorm expansion phase. Moreover, its ability to produce artificial radar aurora will provide a means for the other instruments to undertake polar cap plasma physics experiments in a controlled manner. Another potential use of the facility is in field-line tagging experiments, for coordinated ground-satellite experiments. Here the scientific objectives of SPEAR are detailed, along with the proposed technical specifications of the system.  相似文献   
625.
P. A. Robinson 《Solar physics》1996,168(2):357-374
Energy-balance arguments are combined with the stochastic-growth theory of type III radio sources to determine the properties of the source in average dynamical equilibrium with the beam, and the beam's long-term evolution. Purely linear stochastic-growth theory has previously emphasized that the beam evolves to a state close to marginal stability. Small mean residual deviations from marginal stability are present at dynamical equilibrium and these lead to residual energy flows that feed the waves observed in situ and by remote receivers; consequently the beam energy is depleted. Here, dynamical equilibrium beam and wave levels are estimated for the first time and it is found that the main sink of beam-driven Langmuir waves is either via electrostatic decay into product Langmuir and ion-sound waves or via scattering by short-wavelength density fluctuations, depending on the conditions. Improved estimates of energy branching ratios imply that, at 1 AU from the Sun, typically 20% of the beam energy is converted to Langmuir waves that are scattered off low-frequency density fluctuations and then dissipated, with almost all the remaining waves undergoing electrostatic decay, although as little as one-third of the Langmuir waves may decay in atypical circumstances. Of order 10–3 of the beam energy is converted into sound waves, which are mostly dissipated, and of order 10–5 is converted into potentially observable electromagnetic waves. The mean lifetime of the Langmuir waves at 1 AU is 1–40 s, while that of the beam is of order 1000 s. The beam density decreases relative to that of the background as the beam propagates. For most parameters, analysis of energy losses from the beam to the waves shows that the beam velocity decreases at roughly the same rate as the thermal velocity of the background plasma. It is argued from these considerations, and from in situ observations at 1 AU, that these trends imply that only the densest and fastest type III beams will be able to penetrate much past 1 AU from the Sun. This implies a low-frequency cutoff to type III emission at roughly 10 kHz, in good agreement with recent Ulysses remote observations, showing their consistency with in situ measurements.  相似文献   
626.
This paper is concerned with an extension of the classical restricted problem of three bodies in three dimensions. Usually, the satellite is considered to be a point mass. Here, the satellite is assumed to have a simple structure. The equations of motion are obtained and some of their consequences are discussed.  相似文献   
627.
628.
629.
630.
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