全文获取类型
收费全文 | 2369篇 |
免费 | 413篇 |
国内免费 | 466篇 |
专业分类
测绘学 | 810篇 |
大气科学 | 213篇 |
地球物理 | 669篇 |
地质学 | 881篇 |
海洋学 | 164篇 |
天文学 | 37篇 |
综合类 | 280篇 |
自然地理 | 194篇 |
出版年
2024年 | 22篇 |
2023年 | 34篇 |
2022年 | 76篇 |
2021年 | 81篇 |
2020年 | 114篇 |
2019年 | 124篇 |
2018年 | 110篇 |
2017年 | 137篇 |
2016年 | 149篇 |
2015年 | 178篇 |
2014年 | 128篇 |
2013年 | 177篇 |
2012年 | 152篇 |
2011年 | 157篇 |
2010年 | 131篇 |
2009年 | 154篇 |
2008年 | 149篇 |
2007年 | 160篇 |
2006年 | 153篇 |
2005年 | 106篇 |
2004年 | 100篇 |
2003年 | 95篇 |
2002年 | 71篇 |
2001年 | 82篇 |
2000年 | 65篇 |
1999年 | 54篇 |
1998年 | 46篇 |
1997年 | 40篇 |
1996年 | 34篇 |
1995年 | 32篇 |
1994年 | 32篇 |
1993年 | 20篇 |
1992年 | 12篇 |
1991年 | 13篇 |
1990年 | 16篇 |
1989年 | 12篇 |
1988年 | 7篇 |
1987年 | 7篇 |
1986年 | 5篇 |
1985年 | 2篇 |
1984年 | 2篇 |
1983年 | 1篇 |
1982年 | 2篇 |
1979年 | 4篇 |
1978年 | 1篇 |
1954年 | 1篇 |
排序方式: 共有3248条查询结果,搜索用时 15 毫秒
91.
A laboratory experiment to monitor the contact state of a fault by transmission waves 总被引:1,自引:0,他引:1
We performed a series of laboratory experiments in which elastic waves were transmitted across a simulated fault. Two types of experiments were carried out: (1) Normal Stress Holding Test (NSHT): normal stress was kept constant for about 3 h without shear stress and transmission waves were observed. (2) Shear Stress Increasing Test (SSIT): shear stress was gradually increased until a stick-slip event occurred. Transmission waves were continuously observed throughout the process of stress accumulation. We focused on the change in transmission waves during the application of shear stress and especially during precursory slips.It was found in NSHT that the amplitude of transmission waves linearly increased with the logarithm of stationary contact time. The increase amounted to a few percent after about 3 h. Creep at asperity contacts is responsible for this phenomenon. From a theoretical consideration, it was concluded that the real contact area increased with the logarithm of stationary contact time.We observed in SSIT a significant increase in wave amplitude with shear stress application. This phenomenon cannot be attributed to the time effect observed in NSHT. Instead, it can be explained by the mechanism of “junction growth” proposed by Tabor. Junction growth yields an increase in real contact area. It is required for junction growth to occur that the material in contact is already plastic under a purely normal loading condition. A computer simulation confirmed that this requirement was satisfied in our experiments. We also found that the rate at which the amplitude increased was slightly reduced prior to a stick-slip event. The onset time of the reduction well coincides with the onset of precursory slip. The cause of the reduction is attributed to the reset of stationary contact time due to displacement. This interpretation is supported by the result of NSHT. Taking the time of stationary contact in SSIT into account, we may expect the change in wave amplitude to be, at most, only a few percent. The observed slight reduction in increasing rate is, in this sense, reasonable. The static stiffness of the fault also decreases with precursory slip. It was also found that low frequency waves are a better indicator of precursory slip than high frequency waves. This might suggest that low frequency waves with longer wavelength are a better indicator of average behavior of faults. The problem, however, merits a further investigation. The shifts in phase were also found to be a good indicator of the change in contact state of the fault. The changes in both amplitude and phase of transmission waves are unifyingly understood through the theory of transmission coefficient presented by Pyrak-Nolte et al. Rough surfaces have a tendency to give larger stick-slips than smooth surfaces. The amount of precursory slip is larger for rough surfaces than for smooth surfaces. Although it was confirmed by a computer simulation that rough surfaces have larger contact diameters than smooth surfaces, the rigorous relationship between the surface roughness (contact diameter) and the amount of precursory slips was not established. 相似文献
92.
探槽选址直接决定了古地震研究的质量,且理想探槽位置具有稀缺性。在收集82篇国内外走滑断裂古地震研究论文的基础上,分析了长序列古地震探槽选址和同震位移探槽选址的构造地貌共性特征。长序列古地震探槽一般布设在断塞塘、拉分盆地、小型湖盆、闸门脊汇水一侧及比较平缓的冲洪积扇或大型冲洪积扇末端等地貌位置。这些地貌位置的共同特征是位于连续的、较高沉积速率的沉积环境,且通常富集14C测年物质。在探槽选址的过程中,不仅要对现今沉积环境,也要对其古地理环境进行评价。然而以发掘古地震同震位移为目的的探槽选址则不同,成功的研究点往往较频繁发生侵蚀和下切事件,其中冲沟是最常见的地貌标志。探槽布设以垂直和平行探槽为主,采取逐次掘进或相间平行排列的方式开挖。由于理想探槽位置的稀缺性,所以在这些优质的探槽点一定要开展长期详细地深入研究,最大限度获得古地震事件的长序列,同时也要注意新技术和新方法的应用。 相似文献
93.
针对多源地理空间矢量数据多来源、难以集成综合利用这一现状,本文提出了多源地理空间矢量数据关联方法,并以此为基础构建了多源地理空间矢量数据关联的可视与计算查询系统。首先,对多源地理空间矢量数据关联的概念及分类进行了定义。然后,以此为基础,提出了关联关系构建技术:自适应四叉树编码技术、扫描线技术、几何匹配及语义匹配技术。最后,为实现关联关系的直观展示,设计了原型系统。关联技术的提出可建立起多源地理空间矢量数据之间的关联关系,原型系统的构建也为用户综合利用多源地理空间矢量数据提供了平台,提高了数据的利用率及数据查询的效能。 相似文献
94.
完全Q矢量的引入及其诊断分析 总被引:30,自引:14,他引:30
参照准地转Q矢量推导,考虑天气系统发展的主要热力强迫因子-非绝热加热作用,引出考虑非绝热效应的完全Q矢量的概念,并应用于实例分析。结果表明,完全Q矢量能较清楚地揭示暴雨天气系统的演变;考虑了湿过程的完全Q矢量在暴雨的诊断过程中显示了更大的优越性;定性而言,完全Q矢量散度的辐合中心或辐合线、散度场和锋生函数场有助于确定暴雨的落区,暴雨区正好落在低层完全Q矢量散度场辐合中心和锋生函数场正值中心之间;定量而言,低层完全Q矢量散度场辐合中心和锋生函数场正值中心大小对暴雨强度有显著的指示作用。因而在暴雨的诊断和预报过程中完全Q矢量散度和锋生函数是两个重要的参数。 相似文献
95.
Chun Jiang Xueli Wei Xiaofeng Cui Dexiang You Earthquake Administration of Tianjin Municipality Tianjin China Tianjin University of Technology Tianjin China 《地震学报(英文版)》2009,(3):315-320
This paper introduces the method of support vector machine (SVM) into the field of synthetic earthquake pre-diction, which is a non-linear and complex seismogenic system. As an example, we apply this method to predict the largest annual magnitude for the North China area (30°E-42°E, 108°N-125°N) and the capital region (38°E-41.5°E, 114°N-120°N) on the basis of seismicity parameters and observed precursory data. The corresponding prediction rates for the North China area and the capital region are 64.1% and ... 相似文献
96.
Deepti Joshi Andre St-Hilaire Taha B. M. J. Ouarda Anik Daigle Nathalie Thiemonge 《水文科学杂志》2013,58(11):1996-2010
ABSTRACTThis work explores the ability of two methodologies in downscaling hydrological indices characterizing the low flow regime of three salmon rivers in Eastern Canada: Moisie, Romaine and Ouelle. The selected indices describe four aspects of the low flow regime of these rivers: amplitude, frequency, variability and timing. The first methodology (direct downscaling) ascertains a direct link between large-scale atmospheric variables (the predictors) and low flow indices (the predictands). The second (indirect downscaling) involves downscaling precipitation and air temperature (local climate variables) that are introduced into a hydrological model to simulate flows. Synthetic flow time series are subsequently used to calculate the low flow indices. The statistical models used for downscaling low flow hydrological indices and local climate variables are: Sparse Bayesian Learning and Multiple Linear Regression. The results showed that direct downscaling using Sparse Bayesian Learning surpassed the other approaches with respect to goodness of fit and generalization ability.
Editor D. Koutsoyiannis; Associate editor K. Hamed 相似文献
97.
98.
99.
富蕴断裂带位于阿尔泰山南侧,横切阿尔泰山褶皱带南缘及额尔齐斯深断裂,是一条呈北北西向展布的右旋走滑断裂带。沿断裂带发育一系列错断水系、错断冲积扇、挤压脊、走滑拉分盆地等反映右旋走滑活动的典型构造地貌标志。本研究在高分辨率遥感图像和数字高程模型分析的基础上,结合野外实地构造地貌测量,对沿富蕴断裂带发育的系统错断水系特征进行了详细分析研究。研究结果表明,沿富蕴断裂带发育不同级别的错断水系,大致可划分为6级:1931年地震形成的冲沟;90m左右断距的错断水系;150m左右断距的错断水系;500m左右断距的错断水系;1500m左右断距的错断水系;2000m以上断距的错断水系。同时,结合研究区及邻区的第四纪冰川资料讨论了不同级别水系可能形成时间:恰尔沟三级支流可能形成时间为末次冰期Ⅲ阶段末期,约20ka;恰尔沟二级支流可能形成时间为末次冰期Ⅰ阶段末期,约120ka;恰尔沟一级支流可能形成于该地区冰川广泛消融的倒数第2次冰期的Ⅱ阶段末期,约为250ka;恰尔沟、水磨沟、白杨沟、乌铁布拉克河、卡布尔特河等可能形成于倒数第3次冰期Ⅱ阶段末期,约为360ka。最后,我们估算出富蕴断裂带晚第四纪以来的平均右旋走滑速率为1.46~4.99mm/a。 相似文献
100.
临界滑动面搜索一直是边坡稳定性分析中十分重要的课题,由于极限平衡法具有理论简单,易于被工程师掌握的优点,因此,仍在工程应用中占主导地位。剩余推力法是国内学者提出的一种简单实用且有较高精度极限平衡法,已被纳入国家规范。针对目前剩余推力法条间力假设简单,只考虑了力的平衡而忽略力矩平衡的缺点,通过Spencer法迭代构造了严格剩余推力法边坡临界滑动面搜索优化的模型,并结合蚁群算法搜索出了最大的剩余推力相应的临界滑动面。该模型具有精度高,收敛快的特点。最后给出的两个算例与传统的蚁群算法直接搜索安全系数最小得到的结果做了比较,表明了本文方法的正确性。 相似文献