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121.
1IntroductionTheavailabilityofnearly9aofhighqual-itysealevelanomaly(SLA)datafromsatellitealtimetersmakesitnowpossibletoestimatethedominantsignalsofvariabilityintheglobalo-ceanmoreaccuratelythanwaspreviouslypos-sible.Moreover,mergingtheT/PandERS-1and2altimeterdatathroughanadvancedglobalobjectiveanalysiscangreatlyimproveoura-bilitytoaccuratelyestimateoceanicvariabili-tycomparedwithusingasinglealtimeter(BoulagerandMenkes,1995).ThealtimeterdatarevealthedominantroleofplanetaryRoss-bywavesinocea…  相似文献   
122.
用国际地球自转服务提供的高精度日长序列ΔLOD(IERS(EOP99C04),和由美国国家环境预报中心(NCEP)对过去的气象资料进行重新分析和计算,提供的轴向大气角动量序列(AAM)来研究大气和带谐潮汐对地球自转变化(ΔLOD)中高频振荡激发的贡献。由Multitaper功率谱分析表明,ΔLOD序列在9.13d(天)、13.63d、13.66d、27.55d周期时呈现出比较强的谱峰,这些谱都在95%的显著性水平以上,有比较强的信噪比。从ΔLOD和AAM之差值序列谱分析结果及地球带谐响应系数k的估计,表明大气不是ΔLOD的高频变化的主要激发源。根据理论潮汐周期可知,有可能存在其它的激发源,如海洋对地球自转变化的激发。这还有待于进一步深入探讨。  相似文献   
123.
张人禾  黄荣辉 《大气科学》1998,22(4):587-599
通过资料分析,研究了发生在热带西太平洋海表面西风或东风应力异常与El Ni?o事件的关系。分析结果表明,对应着El Ni?o事件从发生到消亡的过程,热带西太平洋纬向风应力存在着从西风应力异常到东风应力异常的变化,并且在这个过程中,西风应力异常向东传,东风应力异常紧接其后也向东传。本文还根据观测资料的分析结果建立了理想风应力,并利用简单热带海洋模式,对热带西太平洋纬向风应力异常及其东传在ENSO循环中的作用进行了动力学分析,指出了它们在El Ni?o事件发生和消亡中起着重要的作用。西风应力异常通过激发出海洋中东传的暖Kelvin波及其在大洋东边界反射产生的暖Rossby波、以及西风应力异常本身东传到赤道东太平洋,引起正的海洋混合层扰动厚度异常,导致了El Ni?o事件的发生;而异常东风应力则通过激发出东传的冷Kelvin波及其在大洋东边界反射产生的冷Rossby波、以及东风应力异常本身东传到赤道东太平洋,引起负的海洋混合层扰动厚度异常,导致了El Ni?o事件的消亡。对于热带西太平洋上风应力异常的形式是东部为异常西风应力而其西部为异常东风应力,并且它们同时向东传时,则大洋东部混合层厚度对异常风应力的响应随异常东风和西风应力的强度不同而不同,它们强度的相对大小对El Ni?o的持续时间具有重要的作用。  相似文献   
124.
Ore textures and electron microprobe analyses show that in addition to highly scattered blebs in sphalerite grains,intergrown chalcopyrite also occurs as rods,myrmekites and lamellae aligned along cleavages and twin boundaries of the host sphalerite.The majority of the intergrowths could have been formed by replacement of sphalerite by chalcopyrite,albeit part of them may have resulted from exsolution,Not only copper,but also iron were introduced into the sphalerite by replacive fluids.While the front of the replacing fluid was moving forward through a sulphide orebody,Zn and Pb were dissolved and Cu was precipitated,resulting in zonal refining of the sulphide ores,The remobilized zinc and lead were precipitated at favourable sites with changed physico-chemical conditions .This is a possible mechanism for the formation of copper-poor zinc and lead ores above or lateral to the copper orebodies in some of the massive sulphide deposits reworked and overprinted by late-stage granites and their hydrothermal fluids.  相似文献   
125.
After its maturity, El Ni?o usually decays rapidly in the following summer and evolves into a La Ni?a pattern. However, this was not the case for the 2018/19 El Ni?o event. Based on multiple reanalysis data sets, the space-time evolution and triggering mechanism for the unusual second-year warming in late 2019, after the 2018/19 El Ni?o event, are investigated in the tropical Pacific. After a short decaying period associated with the 2018/19 El Ni?o condition, positive sea surface temperature anomalies (SSTAs) re-intensified in the eastern equatorial Pacific in late 2019. Compared with the composite pattern of El Ni?o in the following year, two key differences are evident in the evolution of SSTAs in 2019. First, is the persistence of the surface warming over the central equatorial Pacific in May, and second, is the re-intensification of the positive SSTAs over the eastern equatorial Pacific in September. Observational results suggest that the re-intensification of anomalous westerly winds over the western and central Pacific, induced remotely by an extreme Indian Ocean Dipole (IOD) event, acted as a triggering mechanism for the second-year warming in late 2019. That is, the IOD-related cold SSTAs in the eastern Indian Ocean established and sustained anomalous surface westerly winds over the western equatorial Pacific, which induced downwelling Kelvin waves propagating eastward along the equator. At the same time, the subsurface ocean provided plenty of warm water in the western and central equatorial Pacific. Mixed-layer heat budget analyses further confirm that positive zonal advection, induced by the anomalous westerly winds, and thermocline feedback played important roles in leading to the second-year warming in late 2019. This study provides new insights into the processes responsible for the diversity of El Ni?o evolution, which is important for improving the physical understanding and seasonal prediction of El Ni?o events.  相似文献   
126.
The dynamics of river channel processes were analyzed in the region of complex floodplain-channel branching of the Amur River near Khabarovsk using remote sensing data of the Earth’s surface. Zones of steady accumulation and long-term erosion of the river channel are established within the Khabarovsk water junction over the period of 1964–2004. The main problems related to restoring the Amur River back to its initial channel were distinguished in the course of these works. A map of individual streams formed in the Amur River channel under the influence of large tributaries (the Sungari and Ussuri rivers) was developed. The importance of this map for forecasting the spreading of anthropogenic pollution in the channel of the Amur River is shown using the example of the emergency situation that resulted from the explosion at the chemical plant in the Sungari River basin (Jilin, China; November 2005).  相似文献   
127.
根据1980—2000年ERA-Interim再分析的风场和温度场资料,计算12月与1—2月北半球行星波的EP通量及其散度,并按冬季不同月份分析了平流层整层温度和风场从20世纪80年代到90年代变化的特征及其与行星波活动变化的关系。结果表明,12月高纬度地区中低平流层呈增温趋势;而1—2月温度变化呈冷却趋势。在12月中高纬度中上平流层纬向风明显减速;而在1—2月高纬度中高平流层,随着纬度和高度的增加,纬向风呈明显加速趋势。冬季北半球行星波主要沿低纬度和极地波导两支波导向上传播。但是,12月行星波沿低纬度波导的传播减弱,沿极地波导向平流层整层的传播则明显增强。而1—2月行星波沿低纬度波导的传播明显增强,沿极地波导向平流层的传播则减弱。因此,北半球极区平流层1980—2000年间12月与1—2月波流相互作用的年代际变化形势趋于相反,有必要针对冬季不同月份分开进行讨论。  相似文献   
128.
This paper is a contribution to the Theory of the Artificial Satellite, within the frame of the Lie Transform as canonical perturbation technique (elimination of the short period terms). We consider the perturbation by any zonal harmonic J n (n ≥ 2) of the primary on the satellite, what we call here the complete zonal problem of the artificial satellite. This is quite useful for primaries with symmetry of revolution. We give an analytical formula to compute directly the first order averaged Hamiltonian. The computation is carried out in closed form for all terms, avoiding therefore tedious expansions in the eccentricity or in any anomaly; this feature makes the averaging process, not only valid for all kind of elliptic trajectories but at the same time it yields the averaged Hamiltonian in a very short and compact way. The formula allows us to now skip the averaging process, which means an asymptotic gain of a factor 3n/2 regarding the computational cost of the n th zonal. Our analytical formulae have been widely checked, by comparison on one hand with published works (Brouwer, 1959) (which contained results for particular zonal harmonics, let’s say typically from J 2 to J 8), and on the other hand with the results of 3 symbolic manipulation software, among which the MM (standing for ‘Moon’s series Manipulator’), which has already been used and described in (De Saedeleer B., 2004). Additionally, the first order generator associated with this transformation is given into the same closed form, and has also been validated.  相似文献   
129.
Based on Chen et al. (2006), the scheme of the combination of the pentad-mean zonal height departure nonlinear prediction with the T42L9 model prediction was designed, in which the pentad zonal heights at all the 12-initial-value-input isobar levels from 50 hPa to 1000 hPa except 200, 300, 500, and 700 hPa were derived from nonlinear forecasts of the four levels by means of a good correlation between neighboring levels.Then the above pentad zonal heights at 12 isobar-levels were transformed to the spectrum coefficients of the temperature at each integration step of T42L9 model. At last,the nudging was made. On account of a variety of error accumulation, the pentad zonal components of the monthly height at isobar levels output by T42L9 model were replaced by the corresponding nonlinear results once more when integration was over. Multiple case experiments showed that such combination of two kinds of prediction made an improvement in the wave component as a result of wave-flow nonlinear interaction while reducing the systematical forecast errors. Namely the monthly-mean height anomaly correlation coe cients over the high- and mid-latitudes of the Northern Hemisphere, over the Southern Hemisphere and over the globe increased respectively from 0.249 to 0.347, from 0.286 to 0.387, and from 0.343 to 0.414 (relative changes of 31.5%, 41.0%, and 18.3%).The monthly-mean root-mean-square error (RMSE) of T42L9 model over the three areas was considerably decreased, the relative change over the globe reached 44.2%. The monthly-mean anomaly correlation coefficients of wave 4-9 over the areas were up to 0.392, 0.200, and 0.295, with the relative change of 53.8%, 94.1%,and 61.2%, and correspondingly their RMSEs were decreased respectively with the rate of 8.5%, 6.3%, and 8.1%. At the same time the monthly-mean pattern of parts of cases were presented better.  相似文献   
130.
本文利用NCEP/NCAR月平均再分析资料及中国160个测站月降水资料, 采用经验正交函数分解 (EOF)、相关分析、合成分析等方法, 对青藏高原夏季500 hPa纬向风近59年来的年际、 年代际变化趋势及其与我国降水的关系进行了分析。时空演变特征的分析结果表明: 自1950年以来, 青藏高原夏季500 hPa纬向风总体呈现减弱趋势, 其中在1950年代西风偏弱, 1960年代西风明显偏强, 1970年代至21世纪初西风一直处于偏弱阶段; 纬向风变化趋势的空间分布表现为高原大部分区域上空纬向风呈现减弱趋势, 其减弱趋势由东南向西北递增, 高原西北部及中部地区减弱趋势最为明显; 对高原夏季500 hPa纬向风距平时间序列作EOF分解, 得出第一特征向量的空间分布表现为整体减弱型, 其时间权重系数呈现长期正趋势; 时间系数的11年滑动平均分析表明1950年代后期到1960年代中后期纬向西风整体增强趋势比较明显, 1960年代末到21世纪初为西风减弱阶段, 且期间没有出现明显的上升或下降趋势; 时间系数的突变分析表明纬向风在1967年发生了一次较明显的减弱突变; 时间系数的小波分析表明其具有2~4年的周期, 这一周期成分在1950年代前期和1990年代末至21世纪初这两个时段比较显著。年际、 年代际尺度上高原夏季500 hPa纬向风减弱与我国降水关系的分析均表明: 高原纬向风减弱时长江中下游以北的我国部分地区降水偏少, 以东北和华北表现明显, 长江中下游以南地区降水明显偏多, 降水场与大气环流、 水汽通量散度场都有较好的配置关系。  相似文献   
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