全文获取类型
收费全文 | 12338篇 |
免费 | 2747篇 |
国内免费 | 1380篇 |
专业分类
测绘学 | 303篇 |
大气科学 | 1215篇 |
地球物理 | 8396篇 |
地质学 | 3896篇 |
海洋学 | 682篇 |
天文学 | 11篇 |
综合类 | 576篇 |
自然地理 | 1386篇 |
出版年
2024年 | 29篇 |
2023年 | 113篇 |
2022年 | 317篇 |
2021年 | 393篇 |
2020年 | 457篇 |
2019年 | 565篇 |
2018年 | 432篇 |
2017年 | 436篇 |
2016年 | 369篇 |
2015年 | 465篇 |
2014年 | 647篇 |
2013年 | 685篇 |
2012年 | 718篇 |
2011年 | 763篇 |
2010年 | 613篇 |
2009年 | 718篇 |
2008年 | 740篇 |
2007年 | 902篇 |
2006年 | 903篇 |
2005年 | 776篇 |
2004年 | 727篇 |
2003年 | 660篇 |
2002年 | 531篇 |
2001年 | 404篇 |
2000年 | 459篇 |
1999年 | 400篇 |
1998年 | 370篇 |
1997年 | 299篇 |
1996年 | 343篇 |
1995年 | 287篇 |
1994年 | 258篇 |
1993年 | 212篇 |
1992年 | 133篇 |
1991年 | 76篇 |
1990年 | 56篇 |
1989年 | 55篇 |
1988年 | 48篇 |
1987年 | 34篇 |
1986年 | 24篇 |
1985年 | 11篇 |
1984年 | 4篇 |
1981年 | 4篇 |
1980年 | 2篇 |
1979年 | 18篇 |
1978年 | 1篇 |
1954年 | 8篇 |
排序方式: 共有10000条查询结果,搜索用时 250 毫秒
921.
922.
923.
924.
水环境污染的修复技术 总被引:8,自引:0,他引:8
由于人口增加 ,经济建设发展 ,人民生活水平提高 ,需水量也日益增长。中国水资源紧缺 ,而水污染又加重了水资源危机。水资源及水污染的修复技术的探讨有利于改善人类的生存环境。文中叙述了中国水资源紧缺、地下水超采引起的环境地质灾害 ,提倡节约用水 ,降低万元产值耗水量 ,提高单位水资源的投入产出率 ,开发节水型农业体系。建议以流域为单位 ,实行统一管理调配 ,利用地下水开采所腾出库容 ,拦蓄洪水及将处理后的污水回灌地下 ,以减少灾害 ,增加水资源量。文中还综述了地面水污染、水质富营养化、海水古咸水入侵 ,酸雨影响地下水水质及垃圾堆放场下淋滤液对地下水的污染 ;探讨了用絮凝沉淀、好氧厌氧生物处理工艺、脱氮除磷工艺、膜分离技术及高浓度有机有毒废水等在水污染治理方面的修复技术 ;探讨了对地下水中病原微生物、重金属离子、溶解有机物、硬度、三氮的截、坝、投、抽、排等的修重技术。 相似文献
925.
金属矿地震散射波场的数值模拟研究 总被引:7,自引:0,他引:7
地震方法用于寻找石油、煤田等沉积层控矿床已取得许多成功经验和大量的成果;对于金属矿可依据微扰理论,通过地震波散射响应的强弱推断矿体。模拟实验结果表明,散射波相干性的好坏与杂乱散射体的不均匀性有关;不均匀性越强,产生的散射相干性就越好。 相似文献
926.
兴海6.6级地震灾害调查与损失评估 总被引:3,自引:0,他引:3
2000年9月12日青海省兴海县发生6.6级地震,青海省地震局为本次地震进行了地震灾害调查和损失评估。 相似文献
927.
山东数字遥测地震台网地震监测能力评估 总被引:3,自引:0,他引:3
根据地震仪器的性能对山东数字遥测地震台网的监测能力进行评估,并利用2000年3-10月地震资料进行了检验。其结果为:山东地区12%的面积监测能力为ML≥2.0级,山东中部及渤海、黄河沿海地区监测能力为ML≥2.5级,渤海、黄海近海地区的监测能力为ML≥3.0级。最后指出台网布局的疏密程度、观测条件及台基条件的优劣等是影响台网监控能力的重要因素。 相似文献
928.
3-D S-waveQ structure in Jiashi earthquake region is inverted based on the attenuation of seismic waves recorded from earthquakes in
this region in 1998 by the Research Center of Exploration Geophysics (RCEG), CSB, and a rough configuration of deep crustal
faults in the earthquake region is presented. First, amplitude spectra of S-waves are extracted from 450 carefully-chosen
earthquake records, called observed amplitude spectra. Then, after instrumental and site effect correction, theoretical amplitude
spectra are made to fit observed amplitude spectra with nonlinear damped least-squares method to get the observed travel time
overQ, provided that earthquake sources conform to Brune’s disk dislocation model. Finally, by 3-D ray tracing method, theoretical
travel time overQ is made to fit observed travel time overQ with nonlinear damped least-squares method. In the course of fitting, the velocity model, which is obtained by 3-D travel
time tomography, remains unchanged, while onlyQ model is modified. When fitting came to the given accuracy, the ultimateQ model is obtained. The result shows that an NE-trending lowQ zone exists at the depths of 10–18 km, and an NW-trending lowQ zone exists at the depths of 12–18 km. These roughly coincide with the NE-trending and the NW-trending low velocity zones
revealed by other scientists. The difference is that the lowQ zones have a wider range than the low velocity zones.
Foundation item: Joint Seismological Science Foundation of China (957-07-414) and State Key Basic Research Development and Programming Project
(95-13-02-02).
Contribution No. RCEG200105, Research Center of Exploration Geophysics, China Seismological Bureau. 相似文献
929.
An approach to generate artificial earthquakeaccelerograms on hard soil sites is presented. Eachtime-history of accelerations is considered as arealization of a non-stationary gaussian stochasticprocess, with statistical parameters depending onmagnitude and source-to-site distance. In order tolink the values of these parameters for each groundmotion record with the corresponding magnitude andsource-to-site distance, semi-empirical functionalrelations called generalized attenuationfunctions are determined. The set of realground-motion time histories used to obtain thesefunctions correspond to shocks generated at differentsources and recorded at different sites in thevicinity of the southern coast of Mexico. The resultsshow significant dispersion in the parameters of themodel adopted, which reflect that associated with thereal earthquakes included in the sample employed.The problem of conditional simulation of artificialacceleration time histories for prescribed intensitiesis briefly presented, but its detailed study is leftfor a companion paper. The criteria and modelsproposed are applied to generate two families ofartificial acceleration records for recurrenceintervals of 100 and 200 years at a specific sitelocated in the region under study. The results shownin this article correspond to acceleration timehistories recorded on firm ground for earthquakesgenerated at the subduction zone that runs along thesouthern coast of Mexico, and cannot be generalized tocases of earthquakes generated at other sources orrecorded at other types of local conditions. Thismeans that the methods and functional forms presentedhere are applicable to these other cases, but thevalues of the parameters that characterize thosefunctions may differ from those presented here. 相似文献
930.
Arecibo (18.4 N, 66.7 W) incoherent scatter (IS) observations of electron density N(h) are compared with the International Reference Ionosphere (IRI-95) during midday (10/14 h), for summer, winter and equinox, at solar maximum (1981). The N(h) profiles below the F2 peak, are normalized to the peak density NmF2 of the F region and are then compared with the IRI-95 model using both the standard B0 (old option) and the Gulyaeva-B0 thickness (new option). The thickness parameter B0 is obtained from the observed electron density profiles and compared with those obtained from the IRI-95 using both the options. Our studies indicate that during summer and equinox, in general, the values of electron densities at all the heights given by the IRI model (new option), are generally larger than those obtained from IS measurements. However, during winter, the agreement between the IRI and the observed values is reasonably good in the bottom part of the F2 layer but IRI underestimates electron density at F1 layer heights. The IRI profiles obtained with the old option gives much better results than those generated with the new option. Compared to the observations, the IRI profiles are found to be much thicker using Gulyaeva-B0 option than using standard B0. 相似文献