全文获取类型
收费全文 | 277篇 |
免费 | 6篇 |
国内免费 | 3篇 |
专业分类
测绘学 | 3篇 |
地球物理 | 177篇 |
地质学 | 72篇 |
海洋学 | 2篇 |
天文学 | 23篇 |
自然地理 | 9篇 |
出版年
2021年 | 4篇 |
2017年 | 8篇 |
2016年 | 6篇 |
2014年 | 4篇 |
2013年 | 11篇 |
2012年 | 8篇 |
2011年 | 9篇 |
2009年 | 11篇 |
2008年 | 10篇 |
2006年 | 5篇 |
2005年 | 4篇 |
2004年 | 4篇 |
2002年 | 4篇 |
2001年 | 3篇 |
2000年 | 6篇 |
1999年 | 6篇 |
1997年 | 7篇 |
1996年 | 6篇 |
1995年 | 4篇 |
1992年 | 3篇 |
1991年 | 5篇 |
1988年 | 6篇 |
1987年 | 2篇 |
1986年 | 8篇 |
1985年 | 7篇 |
1984年 | 6篇 |
1983年 | 4篇 |
1982年 | 10篇 |
1981年 | 5篇 |
1980年 | 4篇 |
1979年 | 5篇 |
1978年 | 2篇 |
1977年 | 6篇 |
1976年 | 5篇 |
1975年 | 6篇 |
1974年 | 3篇 |
1973年 | 7篇 |
1972年 | 3篇 |
1971年 | 6篇 |
1970年 | 4篇 |
1969年 | 4篇 |
1968年 | 3篇 |
1967年 | 2篇 |
1966年 | 5篇 |
1964年 | 3篇 |
1963年 | 3篇 |
1962年 | 6篇 |
1961年 | 2篇 |
1960年 | 5篇 |
1957年 | 2篇 |
排序方式: 共有286条查询结果,搜索用时 0 毫秒
281.
282.
Физическое объяснение частотного уравнения волн Лява для двухслойной среды, покрывающей полупространство, с точки зрения интерференции пространственныхSH-волн дало возможность определить параметры эквивалентной среды с одним слоем, покрывающим долупространство. Под эквивалентностью здесь подразумевается совпадение кривой дисперсии волн Лява. Оказывается, что за исключением нескольких весьма простых случаев двухслсйную среду обобщенно нельзя заменить эквивалентной однослойной моделью таким образом, чтобы как слой, так и полупространство были однородными. Полупространство эквивалентной модели в общих случаях, учитывая наличие пространственныхSH-волн, обладает дисперсионными свойствами и является анизотропным. С помощью принципа эквивалентности частотное увавнение волн Лява в двухслойной среде были установлены дальнейшие волны, сушествуюшие не во всем частотном спектре. Существование и число этих ветвей зависит от отношения мощностьй слоев и от порядкового номера обертона волн Лява. 相似文献
283.
Karel Diviš Viktor Höschl Stanislav Hrách Reviewer M. Pick 《Studia Geophysica et Geodaetica》1981,25(1):14-23
Summary The results of pressure tests of gravimeters Worden No. 961, CG-2 Nos 174 G, 323 and 374 in a pressure chamber are presented. Apart from deriving the barometric correction, the authors have also studied accompanying phenomena, which occur during pressure tests of gravimeters — the barometric after-effect and hysteresis. The processing of the results in two ways differing in the method of eliminating the drift of the gravimeter, yields nearly identical results. The hysteresis was investigated for atmospheric pressures of 720±150 Torr (1 Torr=0.133322 kPa), a rate of change of 30 Torr/min and a temperature of 22°C. The barometric after-effect was investigated in greater detail for the CG-2 gravimeter No. 174 G at a pressure difference of 225 Torr, rate of change of 30, 15 and 7.5 Torr/min and a gravimeter heating temperature of 35 °C. It was also found that the barometric correction can be determined, using the method given, with sufficient accuracy. As a result of the existence of hysteresis, however, the derived results must be applied carefully in field gravity measurements with some gravimeters. 相似文献
284.
Karel Klíma Libuše Ruprechtová Reviewer V. Červený 《Studia Geophysica et Geodaetica》1981,25(3):224-230
Summary The fault plane solution determined by means of a computer algorithm, correlating the radiation pattern with the distribution of observations, was investigated from the point of view of its reliability. The maximum of the correlation function R corresponds to the optimum solution found by the computer. If the families of nodal lines fitting the decreased correlation function R —dR retain the character of the optimum solution even whendR increases, we assume that the solution has been determined with a sufficient accuracy. 相似文献
285.
Karel Hron Peter Filzmoser Patrice de Caritat Eva Fišerová Alžběta Gardlo 《Mathematical Geosciences》2017,49(6):797-814
The log ratio methodology converts compositional data, such as concentrations of chemical elements in a rock, from their original Aitchison geometry to interpretable real orthonormal coordinates, thereby allowing meaningful statistical processing and visualization. However, it must be taken into account that the original concentrations can be flawed by detection limit or imprecision problems that can severely affect the resulting coordinates. This paper aims to construct such orthonormal log ratio coordinates, called weighted pivot coordinates, that capture the relevant relative information about an original component and treat the redundant information in a controlled manner. Theoretical developments are supported by a thorough simulation study. Weighted pivot coordinates are then applied to the geochemical mapping of catchment outlet sediments from the National Geochemical Survey of Australia illustrating their advantage over possible alternatives. 相似文献
286.
Jérémie Soldner Pavla Štípská Karel Schulmann Chao Yuan Robert Anczkiewicz Yingde Jiang Marta Koziarska Le Zhang Yunying Zhang Xinyu Wang 《Journal of Metamorphic Geology》2023,41(1):59-96
High-pressure (HP) granulites form either in the domain of the subducted plate during continental collision or in supra-subduction systems where the thermally softened upper plate is shortened and thickened. Such a discrepancy in tectonic setting can be evaluated by metamorphic pressure–temperature–time-deformation (P–T–t–D) paths. In the current study, P–T–t–D paths of Early Palaeozoic HP granulite facies rocks, in the form of metabasic lenses enclosed in migmatitic metapelite, from the Dunhuang block, NW China, are investigated in order to constrain the nature of the HP rocks and shed light on the geodynamic evolution of a modern hot orogenic system in an active margin setting. The rocks show a polyphase evolution characterized by (1) relics of horizontal or gently dipping fabric (S1) preserved in cores of granulite lenses and in garnet porphyroblasts, (2) a N-S trending sub-vertical fabric (S2) preserved in low-strain domains and (3) upright folds (F3) associated with a ubiquitous steep E-W striking axial planar foliation (S3). Garnet in the granulites preserves relics of a prograde mineral assemblage M1a equilibrated at ~11.5 kbar and ~770–780°C, whereas the matrix granulite assemblage (M1b) from the S1 fabric attained peak pressure at ~13.5 kbar and ~850°C. The granulites were overprinted at ~8–11 kbar and ~850–900°C during crustal melting (M2) followed by partial re-equilibration (M3) at ~8 kbar and ~625°C. A garnet Lu–Hf age of 421.6 ± 1.2 Ma dates metamorphism M1, while a garnet Sm–Nd age of 385.3 ± 4.0 Ma reflects M3 cooling of the granulites. The mineral assemblage, M1, of the host migmatitic metapelite formed at ~9–12.5 kbar and ~760–810°C, partial melting and migmatization (M2) occurred at ~7 kbar and ~760°C and re-equilibration (M3) at ~5–6 kbar and ~675°C. A garnet Lu–Hf age of 409.7 ± 2.3 Ma dates thermal climax (M2) and a garnet Sm–Nd age of 356 ± 11 Ma constrains M3 for the migmatitic metapelites. The timing of this late phase is also bracketed by an emplacement age of syntectonic granite dated at c. 360 Ma. Decoupling of M1 and M2 P–T evolutions between the mafic granulites and migmatitic metapelites indicates their different positions in the crustal column, while the shared pressure–temperature (P–T) evolution M3 suggests formation of a mélange-like association during the late stages of orogeny. The high-pressure event D1-M1 is interpreted as a result of Late Silurian–Early Devonian moderate crustal thickening of a thermally softened and thinned pre-orogenic crust. The high-temperature (HT) re-equilibration D2-M2 is interpreted as a result of Mid-Devonian shortening of the previously thickened crust, possibly due to ‘Andean-type’ underthrusting. The D3-M3 event reflects Late Devonian supra-subduction shortening and continuous erosion of the sub-crustal lithosphere. This tectono-metamorphic sequence of events is explained by polyphased Andean-type deformation of a ‘Cascadia-type’ active margin, which corresponds to a supra-subduction tectonic switching paradigm. 相似文献