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81.
135~130 Ma: 大别山第二次“去根”时间? 总被引:1,自引:0,他引:1
大别杂岩主要由早白垩世侵入岩和三叠纪变质岩组成。它的四周是四条区域性韧性剪切带:郯城—庐江断裂,商城—麻城断裂,襄樊—广济断裂和晓天—磨子潭断裂。其中,晓天—磨子潭断裂和襄樊—广济断裂在早白垩世具有相反的走滑剪切方向:北侧的边界断裂(晓天—磨子潭断裂)是一个左行剪切断裂,而南侧的边界断裂(襄樊—广济断裂)是一个右行剪切断裂。在大别杂岩内部,早白垩世低角度剪切面理的倾伏向以SE向或NW向为主。这些晚期剪切面理上的拉伸线理的倾伏向同样为SE或NW向。大别杂岩总体具有朝SE向挤出和顶部相对朝NW向剪切的构造特征。这些表明晚中生代是该杂岩演化的重要阶段。该杂岩的边界断裂和内部构造特征指示其晚期抬升是沿造山带方向(SE—NW)以低角度方式进行的。这一过程直接导致高压-超高压变质岩和同构造岩浆岩被抬升至近地表。同时,年代学研究表明:大别杂岩(扬子板块东北缘地壳)在晚侏罗世—早白垩世经历大规模混合岩化的时间为145~135 Ma,同造山岩浆作用的时间为145~135 Ma,后造山火山-岩浆活动的时间为135~120 Ma。因此,该杂岩中三叠纪高压-超高压变质岩所记录的早白垩世抬升过程不是印支事件的后续,而是燕山期陆内造山及随后发生的伸展过程有关。尽管这一陆内造山事件的起始时间至今仍不确定,但大别山未变形岩体(130~120 Ma)的年代学研究结果和我们新测得的同构造伟晶岩脉的锆石U-Pb年龄(130 Ma)为早白垩地壳变形提供了良好的上限制约。这样,大别山经历了三叠纪碰撞造山和伸展,晚侏罗世—早白垩世陆内造山-伸展二次过程。 相似文献
82.
笔者探讨了断裂在油气聚集中的作用,它是制约塔中隆起及北围斜区油气分布规律的关键因素。基于地震资料断裂解析,塔中隆起及北围斜区断裂体系主要由北西—南东延伸的压扭性断裂带与北东—南西延伸的走滑断裂构成。断裂体系主要形成于中晚加里东中期,此后经历了晚加里东、晚海西和喜山期的继承性活动与改造。中加里东中期构造是该区构造的主要定型期,断裂不仅控制了构造带发育,也是风化壳岩溶储层、礁滩相储层、热液溶蚀碳酸盐岩储层形成关键因素。断裂带后期活动为油气运聚提供了通道,北北东断裂是油气由北部坳陷向隆起长距离运聚的主要通道。断裂带的复杂性造就了研究区油气具有沿断裂带分布,成藏模式多样,差异富集特征。 相似文献
83.
金川超镁铁质岩体矿物化学特征及矿物地质温度计、压力计研究 总被引:4,自引:0,他引:4
根据金川超镁铁质岩体主要造岩矿物和副矿物的共生组合关系及各种矿物的化学成分特点;选用5种较成熟、使用较方便的矿物地质温度计、压力计(主要是辉石温压计和角闪石压力计),对岩体形成的温、压条件进行了估算,其结果为:成岩温度为1000~1300℃(上限可到1400~1500℃),成岩压力约为5×10 ̄8~11×10 ̄8pa。金川超镁铁质岩体的主要岩石类型为尖晶石二辉橄榄岩,这一岩石类型在复杂体系相关系图中的稳定区域大致处于5×l0 ̄8~15×10 ̄8pa的范围,这与矿物温压计估算的成岩温压条件是一致的。 相似文献
84.
5.12汶川大地震龙门山地区发育地震高位滑坡,通常发生在10~11度的极震区,这种灾害难预测,发生速度快,容易造成惨重的生命和财产损失。本文通过在龙池乡川主坪的实地调查,对典型地震抛射滑坡形成的抛射堆积体进行剖析,探究地震加速度受地形放大效应的影响效应及崩塌被抛射的运动程式。 相似文献
85.
This study provides new structural data that show that the Adaminaby Group is part of the Narooma accretionary complex and has been overprinted by HT/LP metamorphism associated with Middle Devonian Moruya Suite intrusions. The grade of metamorphism based on Kübler Indices is the same in the Wagonga and Adaminaby Groups at Batemans Bay inferring that these rocks were involved in the same accretionary event. White micas in slates of the Adaminaby Group record apparent K–Ar ages of 384.6 ± 7.9 Ma and 395.8 ± 8.1 Ma. These ages are believed to represent the age of Middle to Upper Devonian Buckenbowra Granodiorite. Kübler Index values indicate lower epizonal (greenschist facies) metamorphic conditions and are not influenced by heating in metamorphic aureoles of the plutons. All b cell lattice parameter values are characteristic of intermediate pressure facies conditions although they are lower in the metamorphic aureole of the Buckenbowra Granodiorite than in the country rock, defining two areas with dissimilar baric conditions. East of the Buckenbowra Granodiorite, b cell lattice parameter values outside the contact aureole (x = 9.033 Å; n = 8) indicate P = 4 kb, and assuming a temperature of 300°C, infer a depth of burial of approximately 15 km for these rocks with a geothermal gradient of 20°C/km. In the metamorphic aureole of the Buckenbowra Granodiorite, b cell lattice parameter values (x = 9.021 Å; n = 41) indicate P = 3.1 kb inferring exhumation of the Adaminaby Group rocks to a depth of approximately 11 km prior to intrusion. A geothermal gradient of 36°C/km operated in the aureole during intrusion. An extensional back-arc environment prevailed in the Adaminaby Group during the Middle to Upper Devonian. 相似文献
86.
Edge loaded annular foundations have been analysed assuming the soil pressure at the contact to be non-uniform using the lower bound approach of Limit Analysis. Variable fixity at the edges has been allowed and the foundation slab is made to follow the Square yield criterion. Results presented in the form of curves can be readily used to obtain the locations of the yield hinge circles for the given slab and the corresponding collapse load. © 1997 John Wiley & Sons, Ltd. 相似文献
87.
水口山矿田矿床定位模式及找矿远景区评价 总被引:4,自引:1,他引:4
文章从水口山矿田所处大地构造背景及矿田构造岩浆作用分析入手,阐明了矿田内两大成岩成矿系列:Ⅰ与燕山中期中酸性侵入类有关的中温热液接触交代(夕卡岩)型铅锌铜银硫矿床,Ⅱ与燕山晚期英安质次火山-火山岩有关的浅成低温热液铅锌金银矿床.讨论了两者间的时空关系,分析了控矿因素,总结了矿床定位模式,并结合地物化遥资料进行了矿田内找矿远景区的评价. 相似文献
88.
In this paper we describe the transport of pollution in groundwater in the neighbourhood of a well in a uniform background flow. We compute the rate at which contaminated particles reach the well as a function of the place of the source of pollution. The motion of a particle in a dispersive flow is seen as a random walk process. The Fokker-Planck equation for the random motion of a particle is transformed using the complex potential for the advective flow field. The resulting equation is solved asymptotically after a stretching transformation. Finally, the analytical solution is compared with results from Monte Carlo simulations with the random walk model. The method can be extended to arbitrary flow fields. Then by a numerical coordinate transformation the analytical results can still be employed. 相似文献
89.
Propagation of fractures, especially those emanating from wellbores and closed natural fractures, often involves Mode I and Mode II, and at times Mode III, posing significant challenges to its numerical simulation. When an embedded inclined fracture is subjected to compression, the fracture edge is constrained by the surrounding materials so that its true propagation pattern cannot be simulated by 2D models. In this article, a virtual multidimensional internal bond (VMIB) model is presented to simulate three‐dimensional (3D) fracture propagation. The VMIB model bridges the processes of macro fracture and micro bond rupture. The macro 3D constitutive relation in VMIB is derived from the 1D bond in the micro scale and is implemented in a 3D finite element method. To represent the contact and friction between fracture surfaces, a 3D element partition method is employed. The model is applied to simulate fracture propagation and coalescence in typical laboratory experiments and is used to analyze the propagation of an embedded fracture. Simulation results for single and multiple fractures illustrate 3D features of the tensile and compressive fracture propagation, especially the propagation of a Mode III fracture. The results match well with the experimental observation, suggesting that the presented method can capture the main features of 3D fracture propagation and coalescence. Moreover, by developing an algorithm for applying pressure on the fracture surfaces, propagation of a natural fracture is also simulated. The result illustrates an interesting and important phenomenon of Mode III fracture propagation, namely the fracture front segmentation. Copyright © 2012 John Wiley & Sons, Ltd. 相似文献
90.