全文获取类型
收费全文 | 70431篇 |
免费 | 24710篇 |
国内免费 | 48599篇 |
专业分类
测绘学 | 7055篇 |
大气科学 | 26182篇 |
地球物理 | 20086篇 |
地质学 | 52702篇 |
海洋学 | 19701篇 |
天文学 | 2158篇 |
综合类 | 8025篇 |
自然地理 | 7831篇 |
出版年
2024年 | 348篇 |
2023年 | 965篇 |
2022年 | 2522篇 |
2021年 | 3163篇 |
2020年 | 3630篇 |
2019年 | 7082篇 |
2018年 | 7261篇 |
2017年 | 6857篇 |
2016年 | 7129篇 |
2015年 | 6470篇 |
2014年 | 6301篇 |
2013年 | 7041篇 |
2012年 | 6850篇 |
2011年 | 6729篇 |
2010年 | 6680篇 |
2009年 | 5936篇 |
2008年 | 5247篇 |
2007年 | 5129篇 |
2006年 | 4478篇 |
2005年 | 4133篇 |
2004年 | 3856篇 |
2003年 | 3456篇 |
2002年 | 3187篇 |
2001年 | 2959篇 |
2000年 | 2697篇 |
1999年 | 2893篇 |
1998年 | 2606篇 |
1997年 | 2590篇 |
1996年 | 2142篇 |
1995年 | 2005篇 |
1994年 | 1779篇 |
1993年 | 1663篇 |
1992年 | 1372篇 |
1991年 | 1079篇 |
1990年 | 938篇 |
1989年 | 799篇 |
1988年 | 698篇 |
1987年 | 494篇 |
1986年 | 421篇 |
1985年 | 312篇 |
1984年 | 346篇 |
1983年 | 217篇 |
1982年 | 237篇 |
1981年 | 173篇 |
1980年 | 128篇 |
1979年 | 129篇 |
1978年 | 55篇 |
1977年 | 51篇 |
1971年 | 53篇 |
1970年 | 44篇 |
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
171.
The pyroxenite xenoliths in the volcanic rocks of Hoh Xil consist of clinopyroxenes and orthopyroxenes. The mineral composition of these pyroxenes is similar to that of mantle xenoliths including peridotite and pyroxenite from China and abroad, and different from that of granulites. The pyroxenes formed at 1101–1400°C (averaging 1250°C) and under 30–60 kb (averaging 46 kb). We deduced that the magma was derived from the mantle at a depth of more than 150 km, which fits in with the geophysical conclusion that the low-velocity layer existed in the mantle under 150 km.
相似文献172.
再论贺兰山南部北西向构造成因 总被引:3,自引:0,他引:3
贺兰山南部分布着多个方向的构造,其中最明显地是一系列的北西向构造,目前这些构造的相互关系以及形成机制还没有得到合理地解释,争论很大;野外构造研究表明,贺兰山南部北西向构造的形成与青铜峡一固原断裂活动有密切的关系,是该断裂由走滑运动向挤压运动转换时的派生构造;从另一角度也说明,在中新生代由青铜峡一固原断裂所限定的地块(卫宁北山)向东运动,而这些北西向构造的形成主要发生在新生代。由于卫宁北山向东运动的动力来源于青藏高原,因此,贺兰山南部北西向构造的形成与青藏高原的演化有密切的联系。所以。作为中国重要地质界限的南北向构造——贺兰山已经被青藏高原的构造活动所叠加。 相似文献
173.
174.
175.
The subtle interactions between the magnetohydrodynamics (MHD) and transverse plasmons are investigated. It is shown that there is a resistive instability by the plasmon's soliton in a current sheet, which eventually turns into an eruptive instability at the magnetic field reconnection. In the case of ion-acoustic turbulence, the high temperature current sheet model must adopt the aromalous conductivity instead of the Coulomb conductivity. The numerical results are consistent with the observations obtained by Hanaoka (1994). Thus the flare caused by X-ray loop coalescence can be basically interpreted by this model of magnetic field reconnection driven by ponderomotive force. 相似文献
176.
以首都圈地区现今活动断层上近20年的位移测量资料为依据,用二维线弹性有限元对该区断层的活动特征进行了拟合,并结合有关资料讨论了该区的地震危险性。结果表明:1977-1986年间该区主压应力优势方位与华北较一致,约为N45°-80°E;1986-1990年其主压应力方向向北偏转,约为N5°-60°E;1990年至现在其主压应力又向东偏转,角度大于第一阶段,约为N80°-95°E。该区的张家口-延庆一带近期有发生中强震的可能;丰镇-阳高-大同地区和凉城-古营盘地区应力较高,也应引起注意。 相似文献
177.
本文介绍了对时序垂直角观测值进行谱分析的方法和所得到的结论。使以往对于大气折射影响及其变化规律的定性认识得以定量化。 相似文献
178.
The masers of E-type methanol in orion KL and SGR B2 总被引:2,自引:0,他引:2
Using a simplified model the statistical equilibrium and radiative transfer equations of E-type-CH3OH are solved for Orion KL and SgrB2. According to our calculation results and the observation data taken by Matsakiset al. (1980) and Morimotoet al. (1985a, b), the physical conditions of both sources are estimated. In theJ
2-J
1 E methanol maser region of Orion KL, the density, kinetic temperature, dust temperature, and the fractional abundance are 0.8–2×106 cm–3, 150, 30–90 K, 0.8–8×10–6. In the 4–1-30 E and 5–1-40 E methanol maser region of Sgr B2 the correspondance physical conditions above are 104 cm3, 45, 23 K, and 7×10–7, respectively. 相似文献
179.
180.
This study concludes that the elongation axis (K
1) of the ellipsoid of anisotropic magnetic susceptibility (AMS) is a suitable proxy for flow axis in ashflow tuffs. 153 oriented samples (176 specimens) were studied from 18 sites in the 1.1 Ma Tshirege member of the Bandelier Tuff. These sites are distributed around the Valles caldera at distances of 5–25 km outside of the rim.K
1 axes correlate well with postulated radial flow axes at 13 sites.K
1 also agrees with measured geological flow indicators, mainly imbricated larger clasts, at 7 sites. At 2 of the 5 sites where significant disagreement is seen between theoretical radial flow directions and measuredK
1 axes, theK
1 axes correspond well with geological flow indicators, indicating that the divergence of flow from the predicted radial flow pattern is real. Two major topographic buttresses are suggested as the cause of flow divergence for the Tshirege ash flows: the San Pedro buttress northwest of the caldera, and the San Miguel buttress in the southeast. In situK
1 axes plunge about 7° toward the source at two-thirds of the sites; therefore the plunge ofK
1 is a plausible in situ indicator for thedirection of flow. Multiple flow zones in sections of several meters thickness indicate changes of flow direction that are both rapid and large during ash-flow emplacement. These observations raisre the question of how best to represent mean flow directions in ash-flow sheets: by eigenvector methods, by vector-sum methods, or by modes. A method for measuring imbrication of larger clasts using apparent dips in vertical joints is outlined. Imbrication, determined in this way at one-third of the sites, dips toward the source, i.e., up-flow. The minimum (K
3) axis of the AMS ellipsoid correlates with the flow foliation rather than with the larger clast imbrication. The flow axes of ash flows correspond with theK
1 axes, not with the declination ofK
3 axes as suggested by some authors. Initial dip of the sampled ash flows is not large and does not affect the paleomagnetic remanence direction, which is reversed with a mean ofD=173.5°,I=-38.4°, 95=3.4°N=18. This mean is not different at the 95% confidence level from that of earlier workers. The mean pole, at 098.0°E, 74.8°N,A
95=3.3°,N=18, is about 15° far-sided relative to the expected time-averaged geomagnetic pole, suggesting a history of emplacement too short to adequately average secular variation. 相似文献