全文获取类型
收费全文 | 140篇 |
免费 | 43篇 |
国内免费 | 101篇 |
专业分类
测绘学 | 7篇 |
大气科学 | 119篇 |
地球物理 | 22篇 |
地质学 | 74篇 |
海洋学 | 25篇 |
天文学 | 9篇 |
综合类 | 14篇 |
自然地理 | 14篇 |
出版年
2023年 | 3篇 |
2022年 | 5篇 |
2021年 | 6篇 |
2020年 | 1篇 |
2019年 | 11篇 |
2018年 | 4篇 |
2017年 | 2篇 |
2016年 | 8篇 |
2015年 | 6篇 |
2014年 | 14篇 |
2013年 | 17篇 |
2012年 | 11篇 |
2011年 | 15篇 |
2010年 | 7篇 |
2009年 | 11篇 |
2008年 | 10篇 |
2007年 | 15篇 |
2006年 | 26篇 |
2005年 | 13篇 |
2004年 | 16篇 |
2003年 | 7篇 |
2002年 | 10篇 |
2001年 | 4篇 |
2000年 | 12篇 |
1999年 | 5篇 |
1998年 | 7篇 |
1997年 | 4篇 |
1996年 | 5篇 |
1995年 | 5篇 |
1994年 | 6篇 |
1993年 | 3篇 |
1992年 | 4篇 |
1991年 | 3篇 |
1990年 | 1篇 |
1989年 | 2篇 |
1985年 | 3篇 |
1980年 | 1篇 |
1977年 | 1篇 |
排序方式: 共有284条查询结果,搜索用时 31 毫秒
61.
Takashi Setoh Shiro Imawaki Alexander Ostrovskii Shin-Ichiro Umatani 《Journal of Oceanography》1999,55(3):385-394
Interdecadal variations of El Niño/Southern Oscillation (ENSO) signals and annual cycles appearing in the sea surface temperature (SST) and zonal wind in the equatorial Pacific during 1950–1997 are studied by wavelet, empirical orthogonal function (EOF) and singular value decomposition (SVD) analyses. The typical timescale of ENSO is estimated to be about 40 months before the late 1970s and 48–52 months after that; the timescale increased by about 10 months. The spatial pattern of the ENSO signal appearing in SST also changed in the 1970s; before that, the area of strong signal spread over the extratropical regions, while it is confined near the equator after that. The center of the strongest signal shifted from the central and eastern equatorial Pacific to the South American coast at that time. These SST fluctuations near the equator are associated with fluctuations of zonal wiond, whose spatial pattern also shifted considerably eastward at that time. In the eastern equatorial Pacific, amplitudes of annual cycles of SST are weak in El Niño years and strong in La Niña years. This relation is not clear, however, in the 1980s and 1990s. 相似文献
62.
An extended variable-grid global ocean circulation model and its preliminary results of the equatorial Pacific circulation 总被引:2,自引:0,他引:2
1IntroductionThetropicalPacificOceanplaysanimpor-tantroleintheclimatevariabilitiessuchasElNi-no-SouthernOscillation(ENSO)phenomenon(Chao,1993).ManystudieshavefoundthatthetropicalPacificvariabilitiescanhavesignifi-cantinfluenceontheoceancirculationintheseasadjacenttoChina(Yu,1985;Chaoetal.,1996;Wangetal.,2002).TheseaareaadjacenttoChinaischaracterizedbyitscomplextopog-raphyandnumerousnarrowstraits,andthusre-quiresafinegridtoresolve.Tostudytheinter-actionbetweenthetropicalPacificandChinas… 相似文献
63.
多波束水体数据是多波束系统获取的最原始数据,记录了波束从发射到接收整个过程全部的反向散射强度信息,可以为目标识别、水下栖息环境探测等提供重要的数据支撑。目前,针对多波束水体强度时间序列所表现的波形信息的处理及研究仍处于起步阶段,另外水体波形数据易受噪声影响,且存在明显的入射角效应问题,对此,本文提出了一种基于分区异构的多波束水体波形拟合算法。首先,根据不同波束入射角范围的水体波形特性,将水体数据划分为3个区域;然后利用不同函数(中央波束区域—双指数函数、漫反射区域—广义高斯与线性函数叠加、边缘波束区域—高斯与多项式叠加)分别对不同分区的反向散射强度波形进行拟合。采用台湾海峡的多波束水体数据进行验证,结果表明:不同分区拟合相关系数及拟合优度均达到0.95以上,相比简单函数拟合,均方根误差由3.39 dB降到1.5 dB以下,达到了较好的拟合效果,可为多波束水体目标识别和海底分类提供参考。 相似文献
64.
本文从冀中坳陷束鹿凹陷潜山顶面不整合接触类型及分布规律、结构特征及输导类型出发,精细刻画了不整合面之下半风化岩石层的垂向岩溶分带特征。在此基础上对典型剖面烃源岩热演化、油气运移进行模拟,建立了研究区潜山油气的运聚模式。结果表明,束鹿凹陷潜山顶面不整合包括4种接触类型、5种结构模式,具有3种输导类型,其中斜坡区和洼槽区西部以侧向型为主,斜坡区局部构造高点与洼中隆为侧向+圈闭型,凸起区以侧向+垂向型为主。不整合面之下半风化岩石孔缝洞体系发育,垂向上可划分为表层岩溶带、垂直渗流带以及三个水平潜流带,具有多期岩溶旋回特征。潜山顶部发育的垂直渗流带是油气沿不整合面运移的主力输导层,而内幕发育的多期水平潜流带是油气向内幕运移的潜在通道。深、浅部烃源岩热演化的差异以及与薄层砾岩是否接触导致了斜坡区与洼中隆潜山油气充注的差异,形成了斜坡区晚期薄层砾岩高效中转、不整合侧向运移、水平潜流带向内幕输导、顺向断层向上输导、反向断层圈闭成藏的油气运聚模式。 相似文献
65.
Zonal distribution of the erosion-landslide and soil micromorphological features in purple hilly region 总被引:3,自引:0,他引:3
HEYurong LIAOChaolin XUPei ZHANGBaohua 《山地科学学报》2005,2(1):42-49
In the purple hilly region, erosions and landslides are all serious, and it is of great scientific value and practical significance to study their formation mechanism and distribution features there.In this paper, soil micromorphological methods and techniques were used to study the erosion zonal distribution in the region. The results indicated: (1)According to erosion process, the spacial distribution zones of the erosions and landslides in the purple hilly region with different solums were divided into scouring erosion zone, transport-diffusion zone, rocks and soil turbulence zone and sediment-bury zone; (2) The soil micromorphologic taxonomic feature identifying different erosion-landslide zone were found by studying the soil micromorphology of erosive zone in purple hilly region; (3) As for the erosion-landslide formation in the region, besides the external factors, the internal factors were found more important and favorable for landslide formation through the studies on the micormorphologieal features of slide soil. 相似文献
66.
V.V. Makarov L.S. Ksendzenko V.M. Sapelkina A.A. Opanasyuk N.A. Opanasyuk E.N. Jashkova 《世界地质(英文版)》2006,9(2)
Rock mass failure on the high depth near the underground openings often has zonal character. The mechanism of this phenomenon consists in the periodical character of stresses in surrounding rock mass and developing of tensile macrocracks at the places (zones) of maximum tangentional stresses. Mathematical model of the high stressed rock mass is developed on the base of the defect media mechanics and nonequilibrium thermodynamics principals. The correspondence between the experimental research of faulted zonal structures near the high depths openings and mathematical model calculation is achieved. Relationships between the width of cracking zones and rock mass strength property have been determined. 相似文献
67.
68.
The net influx of the circumpolar water on the western (approximately along 10°E) and eastern (approximately 115°E) boundaries
of the Indian Ocean, adopting the method of Montgomery and Stroup is computed on bivariate distribution of potential thermosteric
anomaly and salinity to identify the characteristics of the flux. The zonal flux at both the boundaries indicates an alternate
strong easterly and westerly flow between 36°S and 45°S, south of which the flow is mainly easterly but weak up to 56°S. At
the western boundary the easterly flow is 146 Sv and westerly is 98.07 Sv, while at the eastern boundary (115°E) the corresponding
fluxes are 123.46 Sv and 27.20 Sv respectively, indicating a net outflux of 48.33 Sv. This water should have been accounted
by the melting of ice and influx of the Equatorial Pacific Ocean Water. 相似文献
69.
Viliam Vatrt 《Studia Geophysica et Geodaetica》1996,40(2):119-124
Summary It has been proved that orbital elements of perturbing bodies should be taken into account when 10–10 accuracy is required for zero-frequency tidal distortion in the second zonal Stokes parameter of the geopotential. A solution at the 10–15 level of magnitude has been presented. The zero-frequency tidal distortion in the fourth zonal Stokes parameter has been derived as 1·3×10–10 if the secular Love number is unity. It should be reflected in the geopotential models respecting the 10–10 level of magnitude. 相似文献
70.
安徽铜陵冬瓜山矿床矿石硫化物环带及地质意义 总被引:1,自引:1,他引:0
安徽冬瓜山矿床是铜陵矿集区内一个重要的大型铜(金)矿床,颇受关注,成因认识分歧较大。矿床内块状硫化物矿石中普遍发育以黄铁矿为核部、黄铜矿为中间带、磁黄铁矿为边部带的硫化物环带。这些环带核部黄铁矿多呈自形-半自形晶,黄铜矿呈他形晶围绕黄铁矿沉淀,磁黄铁矿呈他形分布在黄铜矿外围,内带常被外带硫化物溶蚀交代。硫同位素分析结果显示,环带中硫化物矿物的硫同位素(δ34S=1.6‰~5.1‰)具有岩浆硫源特征,同时从核部黄铁矿到中间带黄铜矿,再到边部磁黄铁矿δ34S值逐渐降低。以上特征表明环带从内到外硫化物之间并非平衡共生关系,而是黄铁矿、黄铜矿和磁黄铁矿先后依次晶出。硫化物环带核部粗粒黄铁矿(粒径大于1.5cm)的Co、Ni含量分别为292×10-6~1504×10-6和32.7×10-6~39.9×10-6,Co/Ni=7.32~46.0(平均26.7),与海底火山喷流沉积型黄铁矿的Co、Ni特征基本一致。核部黄铁矿由颗粒中心向边缘,Fe/S原子比值、Mo和Co含量先逐渐升高,再逐渐降低,而Cu、Zn等成矿元素主要富集于颗粒边缘,并向边缘有逐渐升高趋势。与此同时,细粒黄铁矿(粒径小于0.5cm)中的Cu、Zn等元素的含量明显高于粗粒黄铁矿。环带中三种硫化物矿物的REE配分曲线和微量元素蛛网图极为相似,相对富集LREE、Rb、Th等元素,而亏损Nb、Ta、Zr、Hf、Sr、Ba和HREE等元素,由环带核部到边部δEu逐渐减小,与矿区石英二长闪长(玢)岩表现出较高的相似性。以上特征综合分析表明,冬瓜山铜(金)矿床中硫化物环带经历了以下形成过程:石炭纪海底喷流沉积作用在矿区形成沉积黄铁矿,到燕山期,在区内强烈的构造-岩浆活动作用下,致使早期沉积的黄铁矿首先发生变质重结晶作用,形成粒状黄铁矿,随后岩浆热液对其进行叠加改造,并在岩浆热液作用下相继围绕粒状黄铁矿增生,依次沉淀出热液型黄铁矿、黄铜矿和磁黄铁矿,最终形成硫化物环带。这一认识,结合硫化物环带中元素及硫同位素特征进一步表明冬瓜山铜(金)矿床的形成先后经历了古生代海底喷流沉积成矿作用和燕山期岩浆热液成矿作用,矿床中的成矿物质(特别是Cu、Zn等成矿元素)主要来源于燕山期岩浆热液,但石炭系海底喷流沉积作用也提供了部分物质(例如,Fe、S、Mo、Co和Ni等)。此外,环带中微量元素的变化特征表明,随着硫化物环带的形成,成矿热液系统的温度、硫逸度和氧逸度逐渐降低和(或)p H值升高。 相似文献