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991.
空间方向关系形式化描述模型研究 总被引:12,自引:1,他引:12
空间方向关系形式化描述模型是空间关系研究的难点和重点,目前尚无完善的模型出现,因此进行其模型的研究意义重大。首先论述运用平面目标Voronoi图描述方向关系在理论上的可行性;然后详细阐述基于Voronoi图的空间方向关系形式化描述模型建立;为了验证模型的正确性,给出几个典型的算例;最后指出模型的优、缺点。 相似文献
992.
Stephen Dale Holness 《地球表面变化过程与地形》2003,28(4):337-347
Active sorted circles are quantitatively described for the first time for the maritime Subantarctic. Increasing altitude and hence increasing frost penetration are associated with systematic increases in pattern spacing, cell width, height of the fine centre relative to the border, and depth of sorting (but not the width of coarse margins). These results imply consistent dimensional scaling of circle parameters. It is argued, on the basis of the altitudinal trends in pattern morphology, the dimensional scaling of forms, and the morphology of the patterns, that differential frost heave in association with convection cells is responsible for circle formation. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
993.
Calculated Phase Relations in High-Pressure Metapelites in the System NKFMASH (Na2O-K2O-FeO-MgO-Al2O3-SiO2-H2O) 总被引:6,自引:0,他引:6
Using an internally consistent thermodynamic dataset and updatedmodels of activitycomposition relation for solid solutions,petrogenetic grids in the system NKFMASH (Na2OK2OFeOMgOAl2O3SiO2H2O)and the subsystems NKMASH and NKFASH have been calculated withthe software THERMOCALC 3.1 in the PT range 536kbar and 400810°C, involving garnet, chloritoid,biotite, carpholite, talc, chlorite, kyanite/sillimanite, staurolite,phengite, paragonite, albite, glaucophane, jadeite, with quartz/coesiteand H2O in excess. These grids, together with calculated AFMcompatibility diagrams and PT pseudosections, are shownto be powerful tools for delineating the phase equilibria andPT conditions of Na-bearing pelitic assemblages for avariety of bulk compositions from high-P terranes around theworld. These calculated equilibria are in good agreement withpetrological studies. Moreover, contours of the calculated phengiteSi isopleths in PT pseudosections for different bulkcompositions confirm that phengite barometry is highly dependenton mineral assemblage. KEY WORDS: phase relations; HP metapelite; NKFMASH; THERMOCALC; phengite geobarometry 相似文献
994.
Micro and macroscopic models of rock fracture 总被引:8,自引:0,他引:8
Donald L. Turcotte William I. Newman Robert Shcherbakov 《Geophysical Journal International》2003,152(3):718-728
995.
Laboratory simulation of water-resources conservation by means of the layout of a series of ponds along a streambank 总被引:1,自引:0,他引:1
The purpose of this research is to describe a water-storage method that is more reliable than reservoirs, and to study the
efficacy of interception and storage of surface runoff in ponds. In this method, a series of ponds is laid out along a streambank
so that interception of surface runoff can be increased and more water can be stored in the wet season for use in the dry
season. The simulated results show that the structure of a pond, vegetation and the extent of land development, topographic
slope, and the degree to which a pond penetrates an aquifer affect the efficacy of interception and storage of surface runoff
in ponds.
Received, May 1996 Revised, July 1997, March 1998 Accepted, October 1997 相似文献
996.
Douglas Stow Allen Hope William Boynton Stuart Phinn Donald Walker Nancy Auerbach 《Geomorphology》1998,21(3-4)
The spatial variability and co-variability of two different types of remote sensing derivatives that portray vegetation and geomorphic patterns are analyzed in the context of estimating regional-scale CO2 flux from land surfaces in the arctic tundra. For a study area encompassing the Kuparuk River watershed of the North Slope of Alaska, we compare satellite-derived maps of the normalized difference vegetation index (NDVI) generated at two different spatial resolutions to a map of vegetation types derived by image classification of data from the Landsat multispectral scanner (MSS). Mean values of NDVI for each cover type stratum are unique (with the exception of moist acidic tundra and shrubland types). Based on analysis of semi-variograms generated for SPOT-NDVI data, most of the vegetation cover and landform features of this arctic tundra landscape have spatial dimensions of less than 1 km. Thaw lakes on the coastal plain and glacial depositional landforms, such as moraines in the foothills, seem to be the largest features, with vegetation units having dimensions no larger than 700 m. Frequency distributions of NDVI and vegetation types extracted for sampling transects flown by an aircraft sensing CO2 flux, relative to distributions for the entire Kuparuk River watershed, suggest a slight sampling bias towards greater cover of mesic wet sedge tundra and thaw lakes and associated lower NDVI values. The regional pattern of NDVI for the North Slope of Alaska corresponds primarily to differences between the two major physiographic provinces of this region. 相似文献
997.
Recurrence relations have been derived for truncation error coefficients of the extended Stokes' function and its partial
derivatives required in the computation of the disturbing gravity vector at any elevation above the earth's surface. The corresponding
formulae, the example of values of the truncation error coefficients for H=30.1 km and ψ0=30∘ and the estimations of truncation error are given in this article.
Received: 26 January 1996 / Accepted: 11 June 1997 相似文献
998.
Katja Henjes 《Boundary-Layer Meteorology》1998,88(2):161-180
The inertial dissipation technique has been successfully employed for many years to measure the wind stress, especially over the open ocean. This method is based on Kolmogorov's theoretical prediction of universality in the inertial wavenumber range. The theory was developed under the assumption of locally isotropic turbulence, and the dissipation technique has been criticized as lacking justification in a boundary-layer shear flow. In this paper, Kolmogorov's theory is explicitly applied to the anisotropic conditions prevailing in the atmosphere. It is shown that the inertial dissipation method relies on the homogeneity and isotropy of the spectrum ii(k) for k in the inertial range. This is a weaker condition than Kolmogorov's assumption of isotropy of the correlation function Bij(r). In high-Reynolds-number shear flows, isotropy of ii(k) is realized to a good approximation, whereas isotropy of Bij(r) is not. Some consequences for the experimental implementation are discussed; in particular, sampling times (block lengths) not exceeding the order of the eddy life time are recommended in the calculation of spectra. 相似文献
999.
1000.
Kusuma G. Rao 《Boundary-Layer Meteorology》2004,111(2):247-273
For the first time, the exchange coefficient of heat CH has been estimated from eddy correlation of velocity and virtual temperature fluctuations using sonic anemometer measurements made at low wind speeds over the monsoon land atJodhpur (26°18' N, 73°04' E), a semi arid station. It shows strong dependence on wind speed, increasing rapidly with decreasing wind speed, and scales according to a power law CH = 0.025U10
-0.7 (where U10 is the mean wind speed at 10-m height). A similar but more rapid increase in the drag coefficient CDhas already been reported in an earlier study. Low winds (<4 m s-1) are associated with both near neutral and strong unstable situations. It is noted that CH increases with increasing instability. The present observations best describe a low wind convective regime as revealed in the scaling behaviour of drag, sensible heat flux and the non-dimensional temperature gradient. Neutral drag and heat cofficients,corrected using Monin–Obukhov (M–O) theory, show a more uniform behaviour at low wind speeds in convective conditions, when compared with the observed coefficients discussed in a coming paper.At low wind convective conditions, M-O theory is unable to capture the observed linear dependence of drag on wind speed, unlike during forced convections. The non-dimensional shear inferred from the present data shows noticeable deviations from Businger's formulation, a forced convection similarity. Heat flux is insensitive to drag associated with weak winds superposed on true free convection. With heat flux as the primary variable, definition of new velocity scales leads to a new drag parameterization scheme at low wind speeds during convective conditionsdiscussed in a coming paper. 相似文献