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   253篇
  免费   9篇
  国内免费   1篇
测绘学   5篇
大气科学   12篇
地球物理   157篇
地质学   49篇
海洋学   3篇
天文学   28篇
自然地理   9篇
  2020年   5篇
  2019年   3篇
  2018年   4篇
  2017年   5篇
  2016年   12篇
  2015年   11篇
  2014年   15篇
  2013年   14篇
  2012年   10篇
  2011年   7篇
  2010年   12篇
  2009年   5篇
  2008年   5篇
  2007年   4篇
  2006年   3篇
  2005年   6篇
  2004年   3篇
  2003年   3篇
  2000年   4篇
  1996年   3篇
  1995年   3篇
  1994年   3篇
  1993年   4篇
  1990年   3篇
  1989年   3篇
  1988年   4篇
  1987年   9篇
  1985年   4篇
  1984年   5篇
  1983年   4篇
  1982年   5篇
  1981年   5篇
  1980年   3篇
  1979年   4篇
  1978年   5篇
  1977年   6篇
  1975年   8篇
  1974年   3篇
  1973年   5篇
  1972年   4篇
  1971年   3篇
  1970年   3篇
  1969年   2篇
  1967年   2篇
  1966年   3篇
  1964年   4篇
  1962年   2篇
  1960年   3篇
  1958年   3篇
  1957年   3篇
排序方式: 共有263条查询结果,搜索用时 15 毫秒
71.
72.
Summary Seismic microzoning of Prague was performed using geological data and seismic response (ground shaking) computations. The Prague territory was covered by a square grid, each square 250 m×250 m being characterized by a simplified geological cross-section from the Earth's surface to the bedrock boundary. The data were obtained from detailed engineering-geological maps 1:5000. The geological cross-sections were transformed into a set of layered models, specified by the thicknesses of individual layers and corresponding compressional and shear-wave velocities, densities and parameters of the causal absorption. The seismic responses were computed by the matrix method. The main amplitude and frequency characteristics of the responses are demonstrated in the form of microzoning maps. The maps do not depend on the specific type of seismic excitation. They make it possible to predict the relative amplification of P and S waves, with respect to the bedrock outcrop, all over the city.  相似文献   
73.
Summary The amplitude-distance curves of P waves, valid for the region of Central Asia, were derived in the distance range between 13° and 36° using observations of a network of eight Caucasian seismic stations. The curves are characterized by an anomalous increase of amplitudes between 13° and 20° followed by a large decrease of amplitudes in the distance range between 20° and 35°. Both the increase and decrease of amplitudes are interrupted by several local maxima. A comparison of the present amplitude curves with those derived for the regions of South-Eastern Europe and Asia Minor enabled us to correlate the individual local maxima of amplitude curves and to investigate the variation of their position due to the lateral inhomogeneity of the upper mantle structure in Eurasia.A. Tskhakaya deceased in 1970.  相似文献   
74.
75.
76.
Summary With the aid of the selected spherical model the conditions of generation of a stationary magnetic dipole field in a fluid electrically conducting spherical region, bounded by an outer unconducting region, are derived. It is assumed that there exist turbulent motions in the conducting medium, as well as differential rotation. The induction MHD equation is solved under appropriate boundary conditions. It was found that a stationary dipole field may only be generated at a certain positive value of the coefficient G which characterizes the geometric and physical parameters of the conducting region. If this coefficient is zero, the amplitudes of the magnetic fields decrease exponentially with time.  相似文献   
77.
The elastic constants of sixteen garnet specimens of wide variety in chemical composition are accurately determined by means of the rectangular parallelpiped resonance method. The dependence of the elastic properties on chemical composition is analyzed using the present data and those for seven garnets investigated by other authors. The property Xi of a garnet solid solution i is given by a linear addition law in terms of the mole fraction nij of component j; Xi = ΣnijXj where the Xj's are the properties of the end-members j (j = pyrope, almandine, spessartine, grossular and andradite). The Xj's are determined for density ρ, bulk modulus K, and shear moduli Cs = (C11 ? C12)/2 and C44. No systematic deviation is observed from the linear addition law for the elastic moduli nor for other quantities such as the elastic wave velocities. The extrapolated elastic moduli (Mbar) of the end-members are:
  相似文献   
78.
79.
80.
AlmandinePyropeSpessartineGrossularAndradite
K1.779 ± 0.0081.730 ± 0.0091.742 ± 0.0091.691 ± 0.0081.379 ± 0.017
Cs0.981 ± 0.0040.925 ± 0.0040.964 ± 0.0041.106 ± 0.0040.979 ± 0.007
C440.958 ± 0.0050.919 ± 0.0050.937 ± 0.0051.017 ± 0.0060.827 ± 0.010
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