全文获取类型
收费全文 | 821篇 |
免费 | 28篇 |
专业分类
测绘学 | 21篇 |
大气科学 | 60篇 |
地球物理 | 197篇 |
地质学 | 296篇 |
海洋学 | 40篇 |
天文学 | 167篇 |
综合类 | 1篇 |
自然地理 | 67篇 |
出版年
2023年 | 7篇 |
2021年 | 12篇 |
2020年 | 17篇 |
2019年 | 24篇 |
2018年 | 17篇 |
2017年 | 28篇 |
2016年 | 36篇 |
2015年 | 29篇 |
2014年 | 22篇 |
2013年 | 37篇 |
2012年 | 29篇 |
2011年 | 33篇 |
2010年 | 20篇 |
2009年 | 44篇 |
2008年 | 25篇 |
2007年 | 29篇 |
2006年 | 33篇 |
2005年 | 27篇 |
2004年 | 22篇 |
2003年 | 16篇 |
2002年 | 19篇 |
2001年 | 10篇 |
2000年 | 8篇 |
1999年 | 14篇 |
1998年 | 8篇 |
1997年 | 14篇 |
1996年 | 7篇 |
1995年 | 19篇 |
1994年 | 22篇 |
1993年 | 8篇 |
1992年 | 8篇 |
1991年 | 15篇 |
1990年 | 10篇 |
1989年 | 9篇 |
1988年 | 6篇 |
1987年 | 8篇 |
1986年 | 8篇 |
1985年 | 6篇 |
1984年 | 13篇 |
1983年 | 15篇 |
1982年 | 10篇 |
1981年 | 7篇 |
1980年 | 13篇 |
1979年 | 6篇 |
1978年 | 5篇 |
1977年 | 12篇 |
1975年 | 7篇 |
1974年 | 6篇 |
1973年 | 13篇 |
1971年 | 6篇 |
排序方式: 共有849条查询结果,搜索用时 609 毫秒
41.
42.
The basic equation of motion to analyse the interaction of a non-linear structure and an irregular soil with the linear unbounded soil is formulated in the time domain. The contribution of the unbounded soil involves convolution integrals of the dynamic-stiffness coefficients in the time domain and the corresponding motions. Alternatively, a flexibility formulation for the contribution of the unbounded soil using the dynamic-flexibility coefficients in the time domain, together with the direct-stiffness method for the structure and the irregular soil can be applied. The dynamic-stiffness or flexibility coefficient in the time domain is calculated as the inverse Fourier transform of the corresponding value in the frequency domain. The dynamic-stiffness coefficient's asymptotic behaviour for high frequencies determines the singular part whose transformation exists only in the sense of a distribution. As the dynamic-flexibility coefficient converges to zero for the frequency approaching infinity, the corresponding coefficient in the time domain is simpler to calculate, as no singular part exists. The salient features of the dynamic-stiffness and flexibility coefficients in the time domain are illustrated using a semi-infinite rod with exponentially increasing area. The dynamic-flexibility coefficients in the time domain are calculated for a rigid circular disc resting on the surface of an elastic halfspace and of a layer built-in at its base. Material damping is also introduced using the three-parameter Kelvin and the Voigt models. 相似文献
43.
The contribution of the (linear) unbounded soil to the basic equation of motion of a non-linear analysis of soil-structure interaction consists of convolution integrals of the displacement-force relationship in the time domain and the history of the interaction forces. The former is calculated using the indirect boundary-element method, which is based on a weighted-residual technique and involves Green's functions. As an example of a non-linear soil-structure-interaction analysis, the partial uplift of the basemat of a structure is examined. As the convolution integrals have to be recalculated for each time step, the computational effort in this rigorous procedure is substantial. A reduction can be achieved by simplifying the Green's function by ‘concentrating’ the region of influence. Alternatively, assuming a specified wave pattern, a coupled system of springs and dashpots with frequency-independent coefficients can be used as an approximation. 相似文献
44.
The effect of urbanization in an arid region: Formation of a perched water table that causes environmental damages 总被引:1,自引:0,他引:1
Construction in a new neighborhood in the israeli town of Dimona, situated in an arid region in the south of the country (150
mm average annual rainfall), resulted in a rise in groundwater levels during the subsequent rainy seasons This caused flooding
of shelter basements, soil sliding, and sagging which permanently damaged walls and buildings The neighborhood had been built
on continental sands and marls blanketed by loess, on a valley slope near a rocky anticlinal dip-slope
Subsurface studies, using piezometer holes and groundwater analyses, revealed the presence of sand lenses alternating with
plastic marls, which act as seasonal aquifers with perched water tables Groundwaters obtain high SO
4
−2
and Cl− corrosivity through contact with these nonflushed marls of the Neogene valley fill (Hazeva Formation)
The reasons for the rising of groundwater were found to be (a) artificial interference with the natural (pre-construction)
drainage system—interception of the hillside runoff by building plots, roads, etc, (b) partial denudation of the loess blanket,
increasing the local infiltration and the build-up of local, perched water tables, and (c) corrosion of concrete and steel
pipelines, as well as foundations, by prolonged contact with corrosive groundwater, resulting in haphazard but massive leakage
Guidelines are proposed for an environmental improvement plan, which would include terracing and planting of the watershed
above town to increase evapotranspiration, lowering of the water table by pumping, and diverting the water to suburban parks
(groves of saltresistant trees), and replacement of steel and cement pipes by a non-corrodable plastic pipe system 相似文献
45.
46.
47.
Prof. Dr. Wolf von Engelhardt Günther Graup 《International Journal of Earth Sciences》1984,73(2):447-481
Suevites are impact breccias with a montmorillonitic matrix that contains shocked and unshocked mineral and rock fragments from the crystalline basement, glass inclusions and a small amount of sedimentary clasts. Data are given of the modal composition of fall-out suevites (deposited at isolated points around the crater) and crater suevite (forming a layer below post-impact lake sediments in the crater cavity). Fall-out suevites contain aerodynamically shaped bombs which are absent in crater suevite. Taking into account not only large glass fragments and bombs, but also the finer fractions, the glass content of fall-out and crater suevites amounts to 47 and 29 vol%, respectively. Crystalline clasts in suevites consist of all igneous and metamorphic rock types that constitute the local basement which consists of an upper layer of igneous rocks (mainly granites) and a lower series of gneisses and amphibolite. Based on a collection of 1 200 clasts from 13 suevite occurrences the average crystalline clast population of suevites was determined. Suevites contain on the average 46 % igneous and 54 % metamorphic clasts. In constrast, weakly shocked and unshocked crystalline ejecta of the Ries structure consist of 82 % igneous and 18 % metamorphic rocks. From 138 analyses of crystalline rock samples average compositions of the major rock types were calculated. Comparison of these averages with the average glass composition leads to the conclusion that suevite glasses were formed by shock melting of gneisses in deeper levels of the basement. Suevite matrices consist in most cases of 80 to 90 % montmorillonite, in special cases of celadonite. Chemical analyses are given of some matrices and montmorillonite formulas calculated. It is supposed that montmorillonite was formed by early hydrothermal alteration of rock flour or fine glass particles. In the latter case the original glass content of suevites was higher than at present. Of all ejecta from the Ries crater only crystalline rocks contained in suevites occur in all stages of shock metamorphism up to complete fusion. The overwhelming majority of the ejecta from the sedimentary sequence (about 580 m) show no indications of shock pressures above 10 GPa. The same holds true for crystalline megablocks and breccias around the crater which consist mainly of granites from upper levels of the basement. We assume that the Ries impact can be approximated by a deep-burst model: The projectile penetrated through the sedimentary cover into the basement in such a way that the highest pressures and temperatures developed within the gneiss complex below the upper, predominately granitic layer and that rocks of the sedimentary sequence experienced weak shock compression. Numerical data are given for such a model of the Ries impact on transient crater geometry and volumes of vaporized, melted, shocked and excavated rocks. Fall-out suevites are supposed to have been lifted from the central zone by an expanding plume of vaporized rocks and deposited as fluidized turbulent masses outside the crater whereas the main mass of crater suevite was not removed from the crater cavity. 相似文献
48.
49.
John P. Wolf 《地震工程与结构动力学》1986,14(4):655-673
A non-linear interaction analysis with a (generalized) non-linear structure and a linear unbounded soil is analysed in the time domain, based either on the sub-structure method, which involves global convolution integrals, or on the direct method with local boundary conditions. Alternatively, the hybrid frequency–time-domain method of analysis, which is an iterative scheme, could be used. Approximate local boundary conditions to model the wave propagation towards infinity on the artificial boundary used in the direct method of non-linear soil–structure-interaction analysis to be performed in the time domain are examined. A semi-infinite rod supported elastically, which exhibits the same properties as certain unbounded soils such as dispersion and a cut-off frequency, is used for the investigation. For a transient excitation, the superposition boundary with frequent averaging, the well-known viscous damper and the extrapolation algorithm lead to good accuracy. Moving the artificial boundary further away from the structure (or more precisely, increasing the ratio of the distance of the artificial boundary to the wave length) improves the accuracy. 相似文献
50.
Rifting dynamics at spreading axes is governed by two processes: the large-scale plate divergence and the local magma accumulation in the crust-mantle transition layer. Both evolve simultaneously. A model is developed particularly for the situation in Iceland where a well studied rifting episode occurred in the Krafla volcanic system 1975–1984. Both the divergence and the buoyant rise of magma create tensile deviatoric stress in the axial region, but while divergence generates an altogether extensional stress field, uprising of buoyant melt produces tension only near the axis but compression of the sides. The buoyant rise is driven by the differential pressure gradient in rock and melt. The processes are studied with a two-dimensional finite-element routine. Presently thermal effects are neglected. The model parameters are density difference, size of the buoyant body, externally applied stress field, mechanical properties of rock and melt. Relatively small amounts of divergence and small increases of buoyancy are shown to generate axial tension which can overcome the tensile strength. Axial tension produced by buoyant bodies can even overcome lateral compression. Observed long intervals of quiescence require either large rock strength, quasi-continuous stress relaxation, small buoyant bodies, and/or a compressive deviatoric stress normal to the axis during much of the time between rifting episodes. Buoyant rise and injection of melt must be important in generating compression. 相似文献