全文获取类型
收费全文 | 32851篇 |
免费 | 5420篇 |
国内免费 | 8400篇 |
专业分类
测绘学 | 4936篇 |
大气科学 | 6178篇 |
地球物理 | 7460篇 |
地质学 | 14411篇 |
海洋学 | 5541篇 |
天文学 | 358篇 |
综合类 | 2468篇 |
自然地理 | 5319篇 |
出版年
2024年 | 238篇 |
2023年 | 618篇 |
2022年 | 1198篇 |
2021年 | 1472篇 |
2020年 | 1630篇 |
2019年 | 1763篇 |
2018年 | 1466篇 |
2017年 | 1726篇 |
2016年 | 1802篇 |
2015年 | 1980篇 |
2014年 | 2128篇 |
2013年 | 2438篇 |
2012年 | 2203篇 |
2011年 | 2245篇 |
2010年 | 1845篇 |
2009年 | 2036篇 |
2008年 | 1994篇 |
2007年 | 2114篇 |
2006年 | 1990篇 |
2005年 | 1728篇 |
2004年 | 1560篇 |
2003年 | 1347篇 |
2002年 | 1253篇 |
2001年 | 1045篇 |
2000年 | 1004篇 |
1999年 | 873篇 |
1998年 | 795篇 |
1997年 | 740篇 |
1996年 | 632篇 |
1995年 | 568篇 |
1994年 | 506篇 |
1993年 | 425篇 |
1992年 | 307篇 |
1991年 | 245篇 |
1990年 | 172篇 |
1989年 | 132篇 |
1988年 | 128篇 |
1987年 | 77篇 |
1986年 | 52篇 |
1985年 | 49篇 |
1984年 | 28篇 |
1983年 | 21篇 |
1982年 | 20篇 |
1981年 | 16篇 |
1980年 | 12篇 |
1979年 | 9篇 |
1978年 | 17篇 |
1977年 | 6篇 |
1976年 | 4篇 |
1954年 | 10篇 |
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
41.
42.
在局地热平衡情况下,将物理量先用韦伯函数展开,然后去掉相应分量的滤波方 法,讨论了简单热带海气耦合模型中不同形式扰动的作用和贡献,结果表明,在热带海气耦合 系统中,大气准定常 Rossby波和海洋 Rossby波对于耦合系统贡献较大,它们决定着耦合系统 与耦合扰动的性质,而大气准定常Kelvin波和海洋Kelvin波对于耦合系统贡献相对较小. 相似文献
43.
Based on the theory of elastic mechanics, and using the typical rupture model of shallow earthquake, the authors considered the shallow earthquake as a plane mechanical problem, which was constructed the corresponding mechanical model. By the stress components' formulas of the semi-infinite model acted by the finite even shearing force, the main stress is deduced. It is clear that the sector on the right of the center section is squeezed zone, where the maximum principal stress points at the "source of stress", and that on the left is tensile zone, where the minimum principal stress points to the "source of stress". 相似文献
44.
Aftershocks have the potential to cause collapse of a structure that has been already damaged by the preceding main shock. Seismic safety of a structure should therefore be ascertained through a damage analysis using the anticipated main shock and few larger-aftershock motions. Simulation of aftershock motions needs characterization of the seismic hazard due to aftershocks, and therefore it will be useful to develop a conditional scaling model that can predict the response spectrum of an anticipated aftershock motion consistent with the design spectrum of the main shock motion anticipated at the same station. In this study an attempt is made to develop a conditional scaling model for the pseudo spectral velocity spectrum via linear regression analysis on the aftershock and main shock recordings for the 1999 Chi–Chi earthquake. It is shown that it may be possible to obtain a simpler and approximate version of the conditional model from an unconditional model. Damage-causing potential of a ground motion also depends on its strong motion duration (SMD) and therefore a conditional scaling model is developed for SMD of the aftershock motion in several narrow frequency-bands. The model is developed for the larger-aftershock motions and it is shown that a reasonable replacement of such a model may be obtainable directly from an unconditional model. Finally, a simple weighted averaging scheme is proposed to obtain the composite SMD from the SMDs for different frequency bands by using the pseudo spectral acceleration spectrum of the motion. 相似文献
45.
Crustal Growth by Magmatic Accretion Constrained by Metamorphic P-T Paths and Thermal Models of the Kohistan Arc, NW Himalayas 总被引:2,自引:0,他引:2
Magmatic accretion is potentially an important mechanism inthe growth of the continental crust and the formation of granulites.In this study, the thermal evolution of a magmatic arc in responseto magmatic accretion is modeled using numerical solutions ofthe one-dimensional heat conduction equation. The initial andboundary conditions used in the model are constrained by geologicalobservations made in the Kohistan area, NW Himalayas. Takingconsideration of the preferred intrusion locations for basalticmagmas, we consider two plausible modes of magmatic accretion:the first involves the repeated intrusion of basalt at mid-crustaldepths (intraplate model), and the second evaluatesthe simultaneous intrusion of basalt and picrite at mid-crustaldepths and the base of the crust respectively (double-platemodel). The results of the double-plate model accountfor both the inferred metamorphic PT paths of the Kohistanmafic granulites and the continental geotherm determined frompeak PT conditions observed for granulite terranes. Thedouble-plate model may be applicable as a key growth processfor the production of thick mafic lower crust in magmatic arcs. KEY WORDS: thermal model; magmatic underplating; PT path; granulite; lower crust 相似文献
46.
47.
用时域分析组合模型建立了100万年来60°N6月份太阳辐射量时间序列、宝鸡黄土粒度时间序列、渭南夏季风指数时间序列的动态模型.研究结果表明,时域分析组合模型较好地提取了时间序列的信息,得到的几个显著周期T=133,100,89,41,23,19ka,与地球轨道三要素的变化周期接近.用组合模型拟合实测数据,精度是高的;用其预测未来气候替代性指标时间序列的变化情况,发现未来气候有向干冷方向发展的趋势.时域分析组合模型为研究气候变化趋势提供了一种定量分析、预测的方法. 相似文献
48.
为了探讨琼东南盆地华光凹陷海底天然气水合物稳定带的分布规律,定量研究了静水压力、底水温度、地温梯度和气源组分对水合物稳定带的影响程度。在此基础上,分析了华光凹陷现今甲烷水合物稳定带的厚度分布。最后,综合各因素的历史演化过程,初步探讨了华光凹陷1.05 Ma BP以来天然气水合物稳定带的演化。结果表明:(1)气源组分和海底温度的变化对研究区内水合物稳定带的影响较大;水合物稳定带厚度与海底温度呈良好的线性负相关性。(2)水深超过600 m的海域具备形成天然气水合物的温压条件;超过600 m水深的海域水合物稳定带厚度大部分超过 100 m,其中西北部稳定带的最大厚度超过300 m,是有利的水合物勘探区。(3)华光凹陷1.05 Ma BP以来天然气水合物稳定带厚度经历了快速增厚–窄幅变化–快速减薄和恢复的过程。麻坑群与水合物稳定变化敏感区在空间上具有较好的叠合关系。结合前人的研究成果,推测其形成与天然气水合物的分解释放有关。 相似文献
49.
Compositional Zoning of the Bishop Tuff 总被引:14,自引:0,他引:14
Compositional data for >400 pumice clasts, organized accordingto eruptive sequence, crystal content, and texture, providenew perspectives on eruption and pre-eruptive evolution of the>600 km3 of zoned rhyolitic magma ejected as the Bishop Tuffduring formation of Long Valley caldera. Proportions and compositionsof different pumice types are given for each ignimbrite packageand for the intercalated plinian pumice-fall layers that eruptedsynchronously. Although withdrawal of the zoned magma was lesssystematic than previously realized, the overall sequence displaystrends toward greater proportions of less evolved pumice, morecrystals (0·524 wt %), and higher FeTi-oxide temperatures(714818°C). No significant hiatus took place duringthe 6 day eruption of the Bishop Tuff, nearly all of which issuedfrom an integrated, zoned, unitary reservoir. Shortly beforeeruption, however, the zoned melt-dominant portion of the chamberwas invaded by batches of disparate lower-silica rhyolite magma,poorer in crystals than most of the resident magma but slightlyhotter and richer in Ba, Sr, and Ti. Interaction with residentmagma at the deepest levels tapped promoted growth of Ti-richrims on quartz, Ba-rich rims on sanidine, and entrapment ofnear-rim melt inclusions relatively enriched in Ba and CO2.Varied amounts of mingling, even in higher parts of the chamber,led to the dark gray and swirly crystal-poor pumices sparselypresent in all ash-flow packages. As shown by FeTi-oxide geothermometry,the zoned rhyolitic chamber was hottest where crystal-richest,rendering any model of solidification fronts at the walls orroof unlikely. The main compositional gradient (75195ppm Rb; 0·82·2 ppm Ta; 71154 ppmZr; 0·401·73% FeO*) existed in the melt,prior to crystallization of the phenocryst suite observed, whichincluded zircon as much as 100 kyr older than the eruption.The compositions of crystals, though themselves largely unzoned,generally reflect magma temperature and the bulk compositionalgradient, implying both that few crystals settled or were transportedfar and that the observed crystals contributed little to establishingthat gradient. Upward increases in aqueous gas and dissolvedwater, combined with the adiabatic gradient (for the 5 km depthrange tapped) and the roofward decline in liquidus temperatureof the zoned melt, prevented significant crystallization againstthe roof, consistent with dominance of crystal-poor magma earlyin the eruption and lack of any roof-rind fragments among theBishop ejecta, before or after onset of caldera collapse. Amodel of secular incremental zoning is advanced wherein numerousbatches of crystal-poor melt were released from a mush zone(many kilometers thick) that floored the accumulating rhyoliticmelt-rich body. Each batch rose to its own appropriate levelin the melt-buoyancy gradient, which was self-sustaining againstwholesale convective re-homogenization, while the thick mushzone below buffered it against disruption by the deeper (non-rhyolitic)recharge that augmented the mush zone and thermally sustainedthe whole magma chamber. Crystalmelt fractionation wasthe dominant zoning process, but it took place not principallyin the shallow melt-rich body but mostly in the pluton-scalemush zone before and during batchwise melt extraction. KEY WORDS: Bishop Tuff; ignimbrite; magma zonation; mush model; rhyolite 相似文献
50.
利用ARC/INFO进行三维地形模型的建立、处理和动态模拟 总被引:2,自引:0,他引:2
介绍了利用 ARC/ INFO建立三维地形模型的方法 ,以及利用其新版本的部分新功能处理三维地形模型、进行动态模拟的方法 ,与以往处理三维模型必须借助外部三维图形开发软件包的方法相比 ,具有高速、灵活、可视性强、支持强大分析功能等优点。形成的三维模型可随时与 ARC/ INFO的其它数据模型交换信息 ,与外部进程实时通讯 ,为使用者提供了二维分析工具所不能提供的信息 ,为开发视景仿真系统等与表面分析、立体显示有关的应用系统提供了强有力的支持。 相似文献