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211.
着重介绍了目前变质作用P-T─t轨迹研究在变质作用温压确定、变质作用不同阶段时间标定、变质作用动态演化过程的组构标志、变质作用演化热模拟以及变质作用P─T─t轨迹与大地构造环境之间关系等方面所存在的若干问题。  相似文献   
212.
塔里木盆地北部油气运移二维二相数值模拟分析   总被引:3,自引:0,他引:3       下载免费PDF全文
范土芝  刘鹏生 《地球科学》1995,20(3):322-327
油气运移和聚集过程实际上是油(气)水饱和度知疏导层的变化过程,盆地中油(气)二相流动问题的研究就是对这一过程的定量描述,本项研究是在前人工作基础上,考察压实作用造成骨架变形来推导新的二维二相流动方程,它容描述异常压力演化与二相流动于一式,在模拟方法上采用有限分析的数值方法,这应用于新疆塔里木盆地北部地区,展示了该区异常压力、含水饱和度弥散状扩散效应以及流速场在地质历史时期动态模拟演化特征;指出了该  相似文献   
213.
盆地地史模拟述评   总被引:9,自引:0,他引:9  
论述了盆地地史模拟的一般研究方法,认为回剥法是现今重建盆地沉积史与构造史最精确的方法详细讨论了地坟实校正、不整合处理和构造沉隆分析等主要数学模型及其适用范围;并在介绍地史模拟研究历史和研究现状的基础上,指出了地史模拟的发展方向。  相似文献   
214.
华南滨海断裂带地震危险性的数学模拟   总被引:5,自引:1,他引:5  
华南滨海断裂带是南海北部规模巨大的活动断裂,其地震危险性的确定将为地震几地震工程提供地质背景依据,应用二维有限元分析和正交设计法反演南海北部及其今近地区的构造应力场,探讨可能发震的危险地段。研究结果表明,滨海断裂带的某些地段,尤其是滨海断裂带被NW向断裂切割的部位有一定的地震危险性。南海北部地区最主要的地震威胁来自巴士系断裂带和珠江口盆地南缘的NWW向断裂带,对华南滨海断理解带潜在的地震危险性不宜  相似文献   
215.
印度与欧亚大陆碰撞构造变形数值分析   总被引:8,自引:0,他引:8  
陈开平  马瑾 《地震地质》1995,17(3):277-284
在全面考虑了大陆构造变形三重非线性特征的基础上,用动态有限元法研究了藏东对印度与欧亚大陆碰撞作用的大变形响应。数值模拟结果显示了明显的纵向收缩变形,变形主轴多具有顺时针转动的趋势,但横向位移在总体上并不显著。其最大值正位于红河和鲜水河断裂之间,这一结果论证了印度板块对欧亚大陆的碰撞可能是川滇菱形块体向南东运动的动力来源。红河、鲜水河、昆仑及阿尔金活断层在碰撞作用下发生了顺时针的旋转变形;而且,计算结果模拟出了红河断裂由左旋变为右旋,另3条断裂始终左旋的运动特征  相似文献   
216.
下击暴流的数值模拟研究   总被引:10,自引:3,他引:10  
许焕斌  魏绍远 《气象学报》1995,53(2):168-176
下击暴流是危害飞行安全的一种重要天气现象,特别是尺度为1—4km的微下击暴流。为了了解下击暴流的发展过程,以及大气环境条件和云-降水微物理结构对下击暴流发生演变的影响,利用我们设计发展的非静力全弹性中尺度-γ模式,以一次发生了下击暴流的大气的温、湿、风实测资料为算例进行了数值模拟研究。计算结果给出了下击暴流发生发展的过程,以及在发展过程中各种物理量的变化,得出一些大气环境条件及水凝物粒子微结构对下击暴流发展的影响机理,有助于台站预报员掌握这种天气现象的出现和演变。  相似文献   
217.
The formal solutions of displacement field to the problem of elastic wave scattering and diffraction due to an infinitely long rigid cylinder embedded in an infinite elastic medium by an impulsive point source have been obtained in the integral form. The integrals for the reflected and the diffracted waves both in the shadow zone and in the illuminated zone are evaluated asymptotically for the early time motion by the Reisdue-Cagniard method and the Saddle-point-Cagniard method.Numerical results of the diffractedP, S andPS waves at a fixed circum-distance from the surface of the rigid cylinder show noticeably that (1) the energy partition for the diffractedS wave is small in comparison with that for the diffractedP wave, (2) the wave form of the diffractedS wave is broader and more diffused than that of the diffractedP wave, (3) the direction of the radial motions of the diffractedP andS waves varies as a function of the observational point, and (4) the energy partition for the diffractedP wave is much smaller than that for the direct or the reflectedP waves.This paper has been presented at the 46th Annual International Meeting of Society of Exploration Geophysicists in Houston, Texas, Oct. 28, 1976.  相似文献   
218.
Hydrodynamical Modeling Of Oceanic Vortices   总被引:1,自引:0,他引:1  
Mesoscale coherent vortices are numerous in the ocean.Though they possess various structures in temperature and salinity,they are all long-lived, fairly intense and mostly circular. Thephysical variable which best describes the rotation and the density anomaly associated with coherent vortices is potential vorticity. It is diagnostically related to velocity and pressure, when the vortex is stationary. Stationary vortices can be monopolar (circular or elliptical) or multipolar; their stability analysis shows thattransitions between the various stationary shapes are possible when they become unstable. But stable vortices can also undergo unsteady evolutions when perturbed by environmental effects, likelarge-scale shear or strain fields, -effect or topography. Changes in vortex shapes can also result from vortex interactions. such as the pairing, merger or vertical alignment of two vortices, which depend on their relative polarities and depths. Such interactions transfer energy and enstrophy between scales, and are essential in two-dimensional and in geostrophic turbulence. Finally, in relation with the observations, we describe a few mechanisms of vortex generation.  相似文献   
219.
Tectono-thermal modeling of the Yinggehai Basin,South China Sea   总被引:1,自引:0,他引:1  
Based on the observed data, the average value of surface heat flow in the Yinggehai Basin is calculated and it turns out to be 84.1 mW/m2. The thermal evolution of the basin since the Cenozoic era has been attempted by tectono-thermal modeling. Three-phase extension made the basin become hotter and hotter, reaching its climax in paleo-temperature history since 5.2 Ma. And nowadays, the basin is in the heat flow decreasing period. During the Cenozoic era, the basement heat flow remained at 50–70 mW/m2 all the time. This is related to the degree of each extension phase, stretching rate mode and also the limited basin scale. Modeling results also show that, the surface heat flow is controlled mainly by the basement heat flow, and less than 20% comes from radiogenic heat production in the sediments of the basin  相似文献   
220.
Prospects for forecasting climate variability over the tropical Indian Ocean sector, specifically extreme positive events of the Indian Dipole Mode (IDM), with lead times of a season or more are investigated using the NASA Seasonal-to-Interannual Prediction Project (NSIPP) coupled-model system. The coupled system presents biases in its climatology over the Indian Ocean sector, which include (i) warmest sea-surface temperatures (SSTs) occurring in the central equatorial basin rather than on the eastside with the eastern (western) tropical SSTs up to 1 °C too cool (warm), (ii) a too northwest lying InterTropical Convergence Zonal over the ocean in boreal fall, (iii) a thermocline shallower (deeper) than observed west of Sumatra-Java (north of Madagascar), (iv) a delay of about a month in the onset (cessation) of the southwest (southeast) monsoon in the west (east) in boreal spring (fall). These biases affect the effectiveness of the SST-clouds-shortwave radiation negative feedback, the sensitivity of SST to wind-stress perturbations, and the character of equatorial coupled ocean-atmosphere modes. Despite these biases, ensemble hindcasts of the SST anomalies averaged over the eastern and western poles of the IDM for the decade 1993–2002, which included extreme positive events in 1994 and 1997/1998, are encouragingly good at 3-months lead. The onset of the 1997/1998-event is delayed by about a month, though the peak and decay are correctly timed. At 6-months lead-time, the forecast at the eastern pole deteriorates with either positive or negative false alarms generated each boreal fall. The forecast at the western pole remains good.  相似文献   
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