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32.
THE ANALYSIS ON THE STATISTICAL CHARACTER OF QUIKSCAT SCATTEROMETER WINDS AND STRONG WIND FREQUENCY USING REMOTE SENSOR DATA FROM QUIKSCAT 总被引:1,自引:1,他引:1
1 INTRODUCTION Most of the conventional sea surface wind data are measurements from ships, buoys and islands, with coverage and spatial resolution far below the requirements of research and application. At present, due to limited understanding of physical processes and efficient exploitation of data, numerical prediction models have not been used as they should be, although routine procedures are able to give sea surface wind fields at the intervals of 6 hours. With the development of sp… 相似文献
33.
本文对1985年至1994年监测的强酸雨资料进行研究和分析,并与一般酸雨进行对比。结果表明,本地的一般酸雨出现较为频繁;强酸雨出现增多;四季中强酸雨频率各不相同,秋季最高,夏季最低;强酸雨的酸沉降量正在逐年增加;强酸雨的电导率较高,电导率和pH间呈现高度显著的负相关;强酸雨的降水量一般较小,并与pH间显现非常显著的正相关;强酸雨中各离子浓度均高于一般酸雨。 相似文献
34.
AnalysisandstudyofthelargeearthquakeriskinYanqingHuailaibasinCHANGQUANLIU(刘昌铨)SHIXUJIA(嘉世旭)MINGJUNLIU(刘明军)CHANGFALI(李长发... 相似文献
35.
四川地区强震发生条件的综合分析 总被引:2,自引:0,他引:2
根据发震断层的时代,发震构造的应力和几何结构条件,对四川地区的强震发生条件进行了综合分析,结果表明,四川地区孕育和发生强震的断层主要晚更新世以来,特别是全新世以来活动的断裂;强震多发生在主压力方向与断层交角成30°~60°之间的最危险滑动角值范围,走滑断层的斜列状结构,断裂的交叉结构,断裂的枢纽结构,断裂上的弯曲,转折部位以及断裂带上的横向隆起,拗陷及其交接部位都是发震构造的结构特征,有利于强震的 相似文献
36.
山西省平陆地区位于山西地震带南端,为了分析该地区未来的长期强需求潜势,本较系统地分析当地的破坏性地震及1500年以来的有地震地震资料,并进一步应用中国在陆特征的地震轮回模式及其复发时间概率模型估算法当前特征地震轮回的平均时间间隔,以及从1995年起未来百年内复发强震的概率,结果表明:未来100年来该地区复发强震的危险性很高,未来50年内复发强震的危险性也不能排除。 相似文献
37.
唐山地震的超晚期强余震估计 总被引:1,自引:0,他引:1
根据华北历史地震的重复性和免疫性,认为在唐山周围85km,200年内,对6级地震具有一定的免疫性;在研究了唐山地震序列自身的衰减规律后,认为在今后几十几强余震的最大活动水平为5级,发生6级以上土地震的可能性很小。 相似文献
38.
阐述了如何利用地下水宏观异常作强烈地震的临震预报,详细叙述了利用地下水宏观异常预报地震三要素的方法。 相似文献
39.
中强地震前油井动态异常机理研究 总被引:1,自引:0,他引:1
在分析油井映震特征的基础上,着重对油井动态异常的形成机理进行了研究。认为:映震灵敏井孔的空间分布主要受应力易于集中的构造条件的控制,特别是断层的又汇处、转折端和断裂带,这是与其他流体观测项目的相同之处;在本研究中,首次提出了油井动态前兆异常形成的三种力学过程,即岩土力学过程、水动力学过程和气体动力学过程以及油井特有的二种”放大”作用(变径和气体膨胀)的观点;解释了油井动态震前多为正异常的力学机制。 相似文献
40.
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