全文获取类型
收费全文 | 3937篇 |
免费 | 879篇 |
国内免费 | 983篇 |
专业分类
测绘学 | 318篇 |
大气科学 | 273篇 |
地球物理 | 1914篇 |
地质学 | 2505篇 |
海洋学 | 247篇 |
天文学 | 36篇 |
综合类 | 240篇 |
自然地理 | 266篇 |
出版年
2024年 | 13篇 |
2023年 | 47篇 |
2022年 | 124篇 |
2021年 | 162篇 |
2020年 | 148篇 |
2019年 | 206篇 |
2018年 | 176篇 |
2017年 | 149篇 |
2016年 | 186篇 |
2015年 | 241篇 |
2014年 | 278篇 |
2013年 | 260篇 |
2012年 | 270篇 |
2011年 | 260篇 |
2010年 | 254篇 |
2009年 | 312篇 |
2008年 | 283篇 |
2007年 | 305篇 |
2006年 | 296篇 |
2005年 | 253篇 |
2004年 | 273篇 |
2003年 | 209篇 |
2002年 | 170篇 |
2001年 | 146篇 |
2000年 | 133篇 |
1999年 | 113篇 |
1998年 | 84篇 |
1997年 | 100篇 |
1996年 | 71篇 |
1995年 | 52篇 |
1994年 | 38篇 |
1993年 | 47篇 |
1992年 | 23篇 |
1991年 | 19篇 |
1990年 | 23篇 |
1989年 | 27篇 |
1988年 | 21篇 |
1987年 | 7篇 |
1986年 | 5篇 |
1985年 | 4篇 |
1984年 | 1篇 |
1980年 | 1篇 |
1979年 | 2篇 |
1978年 | 2篇 |
1976年 | 1篇 |
1973年 | 2篇 |
1971年 | 2篇 |
排序方式: 共有5799条查询结果,搜索用时 31 毫秒
121.
“平面图形演化方法”是利用无量刚的异常信息量来反映震前异常空间分布及其随时间的演化,从而预报发震时间和地点的一种方法,这种方法μ值等值线图法,μ值异常平面图法组成,它是通过绘制不同的时间上述二种平面图,通过分析水位,水化异常于震前在时间上,空间上的演化规律,寻找μ值异常集中区或高值区,异常丛集图像分布区,条带图像分布带及条带交叉图像地区,并考虑异常分布图像与活动构造带和地震带的关系,从而对强震发生 相似文献
122.
震级—频度关系的非线性特征 总被引:1,自引:0,他引:1
在假设地震断裂系统具有分形特征前提下,推导出非线性震级-频度关系公式:LogN=a+b△M-C/△M,作为示例,用此公式对一些实际观测资料进行了最小二乘拟合,效果明显好于线性公式。 相似文献
123.
叙述了浅层地下水资源评价中几个常用参数(给水度、降雨入渗补给系数和潜水蒸发系数)的测定和估计方法,并结合实例进行剖析.通过分析,得到几点新的认识:(1)给水度值同注水的方式有关,在实际情况中,由于农田表层土壤疏松,且有作物影响,因而其最大值会出现在地表附近;(2)用抽水试验法测定给水度,其值因孔而异;(3)降雨入渗补给系数与土壤结构和给水度的关系密切,一般随着埋深的增加,该系数随之减小;(4)不同季节和不同作物,潜水蒸发系数不同,表现在计算公式上的参数也不相同. 相似文献
124.
M. Cocco J. Pacheco S. K. Singh F. Courboulex 《Geophysical Journal International》1997,131(1):135-145
An analysis of the Zihuatanejo, Mexico, earthquake of 1994 December 10 ( M = 6.6), based on teleseismic and near-source data, shows that it was a normal-faulting, intermediate-depth ( H = 50 ± 5 km) event. It was located about 30 km inland, within the subducted Cocos plate. The preferred fault plane has an azimuth of 130°, a dip of 79° and a rake of −86°. The rupture consisted of two subevents which were separated in time by about 2 s, with the second subevent occurring downdip of the first. The measured stress drop was relatively high, requiring a Δσ of about a kilobar to explain the high-frequency level of the near-source spectra. A rough estimate of the thickness of the seismogenic part of the oceanic lithosphere below Zihuatanejo, based on the depth and the rupture extent of this event, is 40 km.
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event. 相似文献
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event. 相似文献
125.
张晓云 《华北地质矿产杂志》1996,11(2):245-251
辛安泉是北方第二大泉,泉域面积13000km^2。根据环境水文地质条件,将拉域划分为四个子系统。采用饮用水卫生标准和污染起始值对系统内地下水水质进行评价,并对其污染成因进行了分析。 相似文献
126.
地下采矿是地面塌陷失决条件,自然重力及其他外界触发因素是其发展动因,地面塌陷受覆岩时代及岩性,采空区尺寸大小,煤层倾角,煤层厚度及开采深度,重复采动,水文条件变化,地形地势和松散盖层的影响。 相似文献
127.
根据矿田内岩矿地质波谱与TM图象亮度的线性相关关系,论述了多宝山铜矿田内矿床的地面波谱特征,地空相关模型及TM数据的地空相关分析方法,在此基础上讨论了其在铜矿预测中的应用效果。 相似文献
128.
129.
We present an overview of our recent results on utilizing small earthquakes in the earthquake engineering practice. Site-specific ground motion time-histories of large earthquakes can be successfully simulated using recordings of small earthquakes which are often referred to as 'empirical Green's functions' in seismology. Another important practical problem is whether and how these observations can be used in seismic risk studies which are based on empirical attenuation relations for ground motion parameters. We study a possibility of extrapolating attenuation relations for small earthquakes, to larger magnitudes using the data from the Garner Valley downhole array in Southern California. Finally we introduce efficient ground motion processing techniques in frequency- and time-domains and apply them to site response estimation. 相似文献
130.
The seismic ground motion of a test area in the eastern district of Naples is computed with a hybrid technique based on the mode summation and the finite difference methods. This technique allows us the realistic modelling of source and propagation effects, including local soil conditions. In the modelling, we consider the 1980 Irpinia earthquake, a good example of strong shaking for the area of Naples, which is located about 90 km from the epicenter.The detailed geological setting is reconstructed from a large number of drillings. The sub-soil is mainly formed by alluvial (ash, stratified sand and peat) and pyroclastic materials overlying a pyroclastic rock (yellow neapolitan tuff), representing the neapolitan bedrock. The detailed information available on mechanical properties of the sub-soil and its geometry warrants the application of the sophisticated hybrid technique.As expected, the sedimentary cover causes an increase of the signal's amplitudes and duration. If thin peat layers are present, the amplification effects are reduced, and the peak ground accelerations are similar to those observed for the bedrock model. This can be explained by the backscattering of wave energy at such layers, that tend to seismically decouple the upper from the lower part of the structure.For SH-waves, the influence of the variations of the S-wave velocities on the spectral amplification is studied, by considering locally measured velocities and values determined from near-by down-hole measurements. The comparison between the computed spectral amplifications confirms the key role of an accurate determination of the seismic velocities of the different layers.The comparison performed between a realistic 2-D seismic response and a standard 1-D response, based on the vertical propagation of waves in a plane layered structure, shows considerable difference, from which it is evident that serious caution must be taken in the modelling of expected ground motion at a specific site. 相似文献