全文获取类型
收费全文 | 4654篇 |
免费 | 770篇 |
国内免费 | 1531篇 |
专业分类
测绘学 | 351篇 |
大气科学 | 1381篇 |
地球物理 | 768篇 |
地质学 | 2318篇 |
海洋学 | 684篇 |
天文学 | 512篇 |
综合类 | 299篇 |
自然地理 | 642篇 |
出版年
2024年 | 35篇 |
2023年 | 82篇 |
2022年 | 164篇 |
2021年 | 220篇 |
2020年 | 222篇 |
2019年 | 242篇 |
2018年 | 196篇 |
2017年 | 199篇 |
2016年 | 250篇 |
2015年 | 255篇 |
2014年 | 283篇 |
2013年 | 286篇 |
2012年 | 302篇 |
2011年 | 338篇 |
2010年 | 260篇 |
2009年 | 343篇 |
2008年 | 301篇 |
2007年 | 328篇 |
2006年 | 310篇 |
2005年 | 285篇 |
2004年 | 278篇 |
2003年 | 262篇 |
2002年 | 216篇 |
2001年 | 199篇 |
2000年 | 148篇 |
1999年 | 134篇 |
1998年 | 136篇 |
1997年 | 94篇 |
1996年 | 99篇 |
1995年 | 83篇 |
1994年 | 82篇 |
1993年 | 59篇 |
1992年 | 55篇 |
1991年 | 47篇 |
1990年 | 34篇 |
1989年 | 28篇 |
1988年 | 38篇 |
1987年 | 12篇 |
1986年 | 9篇 |
1985年 | 7篇 |
1984年 | 10篇 |
1983年 | 1篇 |
1982年 | 4篇 |
1981年 | 3篇 |
1980年 | 4篇 |
1979年 | 1篇 |
1978年 | 9篇 |
1976年 | 1篇 |
1973年 | 1篇 |
排序方式: 共有6955条查询结果,搜索用时 15 毫秒
131.
Using the lAP two-level general circulation model,the ice age July climate was simulated through the surface conditions of 18 000 years before present assembled by the CLIMAP Project.Comparing with the present July simulation results,the ice age atmosphere is found to have a substantially lower temperature,precipitation,and cloudiness,higher sea-level pressure,especially in the high latitude land region of the Northern Hemisphere and Antarctica.When the CO2 content is set as the modern value the climatic response is very small,which shows that the problems of CO2 sensitivity should be studied by means of coupled models.It is also pointed out that there are some common characteristics between CO2-induced climatic changes and the ice age surface condition-induced climatic changes,which may give us some insight into how climate responds to external forcings. 相似文献
132.
采用城市化的多项要素指标,系统考察了太原1980-2009年期间城市化的发展对其城市热岛效应的影响关系,发现城市化的发展是导致城市热岛效应形成和加剧的主要原因.认为:①近30年,太原市郊区的增温率为0.51℃/10a,市区的增温率为0.90℃/10a,热岛强度的增温率为0.39℃/10a,热岛效应不断增强;②各类城市发展指数与城市热岛效应都有很好的相关关系;③太原城郊温差和总人口对数呈线性相关关系,其长期变化相关系数为0.81;④太原城郊温差和城市房屋建筑面积对数呈线性关系,其长期变化相关系数为0.85. 相似文献
133.
134.
K. Blümel 《Boundary-Layer Meteorology》1998,86(2):193-232
By means of the algorithm presented here, the temporal course H(t) and the daily mean H¯ of the sensible heat flux H can be estimated from measurements of the thermodynamic surface temperature (as a function of time) and from a one-time-of-day air temperature observation. In addition to these temperatures, one needs estimates for daily mean wind speed, for the roughness lengths of momentum and heat transfer, and for the displacement height. First, a quite general solution of the equation for heat conductance (equation for the vertical profile of potential temperature (z,t)) in the dynamic sublayer will be presented. The undetermined parameters in this solution will be defined with the aid of the above mentioned measurements. The influence of horizontal advection will be taken into account. After that, the sensible heat flux can be evaluated from the temperature difference between surface and air with the well known resistance formulae. In this paper the algorithm is derived for areas with homogeneous surfaces, i.e., with uniform surface temperatures. Finally, the method will be verified by measurements taken during the field campaigns HIBE 89 (Hildesheimer Börde in Germany) and EFEDA 91 (Spain). The root mean square errors (RMSE) for the comparison between measurement and model with regard to the temperature difference of surface and air amount to one or two degrees Kelvin, and the error of H¯ reaches 10 to 25 per cent. The method can be used to determine the sensible heat flux from measurements of surface temperatures by satellites (e.g., METEOSAT), but can also be applied to ground based measurements. For instance, horizontal temperature advection can be estimated from measurements at a single location, especially if more than one near-surface air temperature is available. The procedure can be generalized for larger areas, which consist of various surface types with different surface temperatures. This generalization of the algorithm is in progress and will be addressed in a subsequent paper. It will allow us to improve the estimates for H(t) by means of temperature measurements from, e.g., NOAA/AVHRR or LANDSAT/TM, taking into account the heterogeneity of the area that is contained in one METEOSAT pixel. 相似文献
135.
High frequency temperature measurements were recorded at five heights and surface renewal (SR) analysis was used to estimate sensible heat flux density (H) over 0.1 m tall grass. Traces of the temperature data showed ramp-like structures, and the mean amplitude and duration of these ramps were used to calculate H using structure functions. Data were compared with H values measured with a sonic anemometer. Latent heat flux density (E) was calculated using an energy balance and the results were compared with E computed from the sonic anemometer data. SR analysis provided good estimates of H for data recorded at all heights but the canopy top and at the highest measurement level, which was above the fully adjusted boundary layer. 相似文献
136.
用二维非静力完全弹性的中-γ尺度数值模式模拟了移动性热岛的大气边界层特征。试验中,热岛移速取为4m·s^-1,热岛强度取△θg=60K和30K两种。△θg=60K时,在热岛后方出现了强烈的垂直运动并形成了水平尺度为3-5km的局地环流,最大上升速度100cm·s^-1,出现在低层300-400m高度;△θg=30K时,移动热岛的边界效应比前大为减弱,且不再出现闭合的局地环流。 相似文献
137.
Seasonal variability regarding the nature of precipitation and the activity of cumulus convection during the 1991 Meiyu season of Changjiang-Huaihe River Basin(Jianghuai)has been investigated by calculating apparent heat source/apparent moisture sink and analyzing TBB(cloud-top blackody radiation temperature)data.It is found that three periods of strong ascending motion during the Meiyu season lead to three episodes of heavy rain,and the latent heat due to the precipitation is of the sole heat source of the atmosphere.The nature of precipitation shows distinct seasonal variability,from frontal precipitation of the first episode to the extremely strong convective precipitation of the third episode.TBB field of East Asia may well reflect not only the intensity of convection and rainfall,but also the movement of rain belt and convection belt.In the whole Meiyu season.convection belt mainly stays in Jianghuai.but may shift within the domain of East Asia.Its locating in Jianghuai or not determines the maintenance or break of Meiyu.In the third episode,the narrow convection belt over Jianghuai is mainly caused by southwest monsoon which takes moist and convective atmosphere from tropical ocean. 相似文献
138.
Numerical weather prediction models are increasingly employed for providing meteorological data for urban air quality applications.
Model resolution, physiographic parameters and surface-layer parameterisations need to be adapted to the requirements of the
urban boundary layer. The Lokalmodell of the German Weather Service was triple-nested down to a horizontal grid resolution
of 1.1 km, urbanised physiographic parameters were implemented, and an additional anthropogenic heat source was introduced.
Results of a sensitivity study for a spring dust episode in Helsinki show a clear urbanisation effect of these measures on
temperature, humidity and the partitioning of surface fluxes, leading to an increased Bowen ratio and heat storage and an
urban heat island effect. 相似文献
139.
城市景观格局与热岛效应研究进展 总被引:5,自引:0,他引:5
概述了城市景观格局和城市热岛效应及城市景观格局对城市热岛效应影响等领域的研究现状,探讨了城市景观格局对城市热岛效应的影响作用,并结合城市景观格局研究中的新领域——景观格局优化,提出了解决城市热岛问题的新思路,即通过优化景观格局来达到缓解甚至消除热岛效应。展望了城市景观格局和城市热岛效应研究领域存在的问题和面临的任务。 相似文献
140.
We have performed a one-dimensional and transient radiative heat transfer analysis in order to investigate interaction between atmospheric radiation and convective instability within a nocturnal fog. The radiation element method using the Ray Emission Model (REM2), which is a generalized numerical method, in conjunction with a line-by-line (LBL) method, is employed to attain high spectral resolution calculations for anisotropically scattering fog. The results show that the convective instability has a strong dependence on radiative properties of the fog. For the condition of a 20-m droplet diameter and liquid water content of 0.1 × 10–3 kg m–3;, the temperature profile within the fog becomes S shaped, and a convective instability layer forms in the middle or lower level of the fog. However, for the same water content and a 40-m diameter droplet, no strong convective instability layer forms, whereas for a 10-m diameter droplet a strong convective instability is observed. 相似文献