首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   256篇
  免费   50篇
  国内免费   48篇
测绘学   61篇
大气科学   124篇
地球物理   93篇
地质学   13篇
海洋学   10篇
天文学   1篇
综合类   10篇
自然地理   42篇
  2023年   3篇
  2022年   6篇
  2021年   12篇
  2020年   10篇
  2019年   16篇
  2018年   12篇
  2017年   14篇
  2016年   13篇
  2015年   11篇
  2014年   17篇
  2013年   20篇
  2012年   4篇
  2011年   12篇
  2010年   11篇
  2009年   23篇
  2008年   40篇
  2007年   18篇
  2006年   20篇
  2005年   18篇
  2004年   16篇
  2003年   12篇
  2002年   5篇
  2001年   8篇
  2000年   7篇
  1999年   6篇
  1998年   4篇
  1997年   4篇
  1996年   3篇
  1995年   5篇
  1994年   1篇
  1993年   1篇
  1992年   1篇
  1988年   1篇
排序方式: 共有354条查询结果,搜索用时 31 毫秒
31.
An urban canopy model is incorporated into the Nanjing University Regional Boundary Layer Model. Temperature simulated by the urban canopy model is in better agreement with the observation, especially in the night time, than that simulated by the traditional slab model. The coupled model is used to study the effects of building morphology on urban boundary layer and meteorological environment by changing urban area, building height, and building density.It is found that when the urban area is expanded, the urban boundary layer heat flux, thermal turbulence, and the turbulent momentum flux and kinetic energy all increase or enhance, causing the surface air temperature to rise up. The stability of urban atmospheric stratification is affected to different extent at different times of the day.When the building height goes up, the aerodynamic roughness height, zero plane displacement height of urban area, and ratio of building height to street width all increase. Therefore, the increase in building height results in the decrease of the surface heat flux, urban surface temperature, mean wind speed, and turbulent kinetic energy in daytime. While at night, as more heat storage is released by higher buildings, thermal turbulence is more active and surface heat flux increases, leading to a higher urban temperature.As the building density increases, the aerodynamic roughness height of urban area decreases, and the effect of urban canopy on radiation strengthens. The increase of building density results in the decrease in urban surface heat flux, momentum flux, and air temperature, the increase in mean wind speed, and the weakening of turbulence in the daytime. While at night, the urban temperature increases due to the release of more heat storage.  相似文献   
32.
一种单层城市冠层模式的建立及数值试验研究   总被引:3,自引:1,他引:2  
本文在引进先进的城市地表能量平衡方案 (Town Energy Balance, 简称TEB) 的基础上建立了一个单层城市冠层模式, 并对南京市典型居民区1 km2范围内的局地尺度地表能量平衡各分量进行离线模拟, 将模拟结果与同期观测值作了比对, 发现: TEB方案对城市地表能量平衡各分量的模拟效果良好, 而该方案的模拟性能受建筑物表面材料反照率取值的影响较大。在离线研究的基础上, 本文又将TEB方案成功耦合到南京大学区域边界层模式 (NJU-RBLM) 中, 作为该模式的地表能量平衡参数化方案之一, 分别选取该边界层模式中原有的地表能量平衡参数化方案SVAT (Soil-Vegetation-Atmosphere-Transfer model) 和新引入的TEB方案对冬夏两季不同个例进行模拟, 以常规近地面气温观测资料和Landsat卫星观测的地表反照率资料对模拟结果进行比较, 结果表明: TEB方案对原大气边界层模式的模拟效果有明显改善, 对近地面热力场的改善效果尤为明显, 可以很好地模拟出城市冠层中的“陷阱效应”。  相似文献   
33.
Profiles of wind and turbulence over an urban area evolve with fetch in response to surface characteristics. Sodar measurements, taken on 22 April 2002 during the Salford Experiment in the UK (Salfex), are here related to upstream terrain. A logarithmic layer up to z = 65m was observed in all half-hour averaged profiles. Above this height the profile showed a different vertical gradient, suggesting a change in surface cover upstream. The drag coefficient varied by a factor of two over only a 20° direction change. Turbulence intensity (σ x ) for each wind component (x) decreased with height, but the ratio suggested an underestimate of σ u compared to previous results. Mean urban and suburban cover fraction within the source area for each height decreased sharply between z = 20 and 50m, increasing slightly above. The near-convergence of cover fractions thus occured for source areas of minimum length ≈ 2,200 m. In comparison, the mean length scale of heterogeneity L P was calculated from surface cover data to be 1,284 m, and the corresponding mean blending height h b was 175 m. Finally, the mean streamline angle, α, was negative and the magnitude decreased with height. An exponential fit to α for z ≤ 65m gave an e-folding height scale of 159 m. A simple relationship between this height scale and L P was assumed, giving L P ≈ 1,080 m, which is in reasonable agreement with the estimate from surface cover type. The results suggest that more emphasis is required on modelling and measuring surface-layer flow over heterogeneous urban canopies.  相似文献   
34.
High-accuracy large-eddy simulations of neutral atmospheric surface-layer flow over a gapped plant canopy strip have been performed. Subgrid-scale (SGS) motions are parameterized by the Sagaut mixed length SGS model, with a modification to compute the SGS characteristic length self-adaptively. Shaw’s plant canopy model, taking the vertical variation of leaf area density into account, is applied to study the response of the atmospheric surface layer to the gapped dense forest strip. Differences in the region far away from the gap and in the middle of the gap are investigated, according to the instantaneous velocity magnitude, the zero-plane displacement, the potential temperature and the streamlines. The large-scale vortex structure, in the form of a roll vortex, is revealed in the region far away from the gap. The nonuniform spatial distribution of plants appears to cause the formation of the coherent structure. The roll vortex starts in the wake of the canopy, and results in strong fluctuations throughout the entire canopy region. Wind sweeps and ejections in the plant canopy are also attributed to the large vortex structure.  相似文献   
35.
Modelling the transfer of heat, water vapour, and CO2 between the biosphere and the atmosphere is made difficult by the complex two-way interaction between leaves and their immediate microclimate. When simulating scalar sources and sinks inside canopies on seasonal, inter-annual, or forest development time scales, the so-called well-mixed assumption (WMA) of mean concentration (i.e. vertically constant inside the canopy but dynamically evolving in time) is often employed. The WMA eliminates the need to model how vegetation alters its immediate microclimate, which necessitates formulations that utilize turbulent transport theories. Here, two inter-related questions pertinent to the WMA for modelling scalar sources, sinks, and fluxes at seasonal to inter-annual time scales are explored: (1) if the WMA is to be replaced so as to resolve this two-way interaction, how detailed must the turbulent transport model be? And (2) what are the added predictive skills gained by resolving the two-way interaction vis-à-vis other uncertainties such as seasonal variations in physiological parameters. These two questions are addressed by simulating multi-year mean scalar concentration and eddy-covariance scalar flux measurements collected in a Loblolly pine (P. taeda L.) plantation near Durham, North Carolina, U.S.A. using turbulent transport models ranging from K-theory (or first-order closure) to third-order closure schemes. The multi-layer model calculations with these closure schemes were contrasted with model calculations employing the WMA. These comparisons suggested that (i) among the three scalars, sensible heat flux predictions are most biased with respect to eddy-covariance measurements when using the WMA, (ii) first-order closure schemes are sufficient to reproduce the seasonal to inter-annual variations in scalar fluxes provided the canonical length scale of turbulence is properly specified, (iii) second-order closure models best agree with measured mean scalar concentration (and temperature) profiles inside the canopy as well as scalar fluxes above the canopy, (iv) there are no clear gains in predictive skills when using third-order closure schemes over their second-order closure counterparts. At inter-annual time scales, biases in modelled scalar fluxes incurred by using the WMA exceed those incurred when correcting for the seasonal amplitude in the maximum carboxylation capacity (V cmax, 25) provided its mean value is unbiased. The role of local thermal stratification inside the canopy and possible computational simplifications in decoupling scalar transfer from the generation of the flow statistics are also discussed.
“The tree, tilting its leaves to capture bullets of light; inhaling, exhaling; its many thousand stomata breathing, creating the air”. Ruth Stone, 2002, In the Next Galaxy
  相似文献   
36.
Large-Eddy Simulation of Flows over Random Urban-like Obstacles   总被引:2,自引:2,他引:0  
Further to our previous large-eddy simulation (LES) of flow over a staggered array of uniform cubes, a simulation of flow over random urban-like obstacles is presented. To gain a deeper insight into the effects of randomness in the obstacle topology, the current results, e.g. spatially-averaged mean velocity, Reynolds stresses, turbulence kinetic energy and dispersive stresses, are compared with our previous LES data and direct numerical simulation data of flow over uniform cubes. Significantly different features in the turbulence statistics are observed within and immediately above the canopy, although there are some similarities in the spatially-averaged statistics. It is also found that the relatively high pressures on the tallest buildings generate contributions to the total surface drag that are far in excess of their proportionate frontal area within the array. Details of the turbulence characteristics (like the stress anisotropy) are compared with those in regular roughness arrays and attempts to find some generality in the turbulence statistics within the canopy region are discussed.  相似文献   
37.
Two techniques are analysed to derive mean street width and mean building width from morphological data of real cities: one based on a two-dimensional simplified morphology, and the other based on a three-dimensional regular simplified morphology. For each simplified morphology (two-dimensional and three-dimensional), the sky-view factors (street-to-sky) are computed and compared with the sky-view factors derived from the real morphology for selected districts of three European and two North American cities. The two-dimensional simplified morphology reproduces the real sky-view factors better than the three-dimensional morphology. Since many urban canopy parameterizations represent the city using simplified morphologies, this can be useful information for the derivation of input parameters for urban canopy parameterizations from real morphological data.  相似文献   
38.
多层城市冠层模式的建立及数值试验研究   总被引:4,自引:1,他引:3  
王咏薇  蒋维楣 《气象学报》2009,67(6):1013-1024
为在城市气象数值模拟中更好地体现由城市发展引起的下垫面土地利用改变及人为活动对大气过程的影响,建立了基于建筑物三维分布的多层城市冠层模式,冠层内动力方程组考虑了建筑物冠层拖曳力的作用及雷诺应力的影响,通过引入建筑物宽度、间距以及垂直分布密度指数等建筑物形态特征参数,以更好地体现城市复杂地表对大气温度、湿度及动量方程的影响.同时,该模式分屋顶、4个侧壤及地面分别考虑辐射及能量平衡求解表面温度,计算各表面与大气的通量交换,并考虑辐射阴影效应、冠层内部各个面之间的可视因子、以及与冠层内建筑物密度指数、可视因子等相关的多重反射辐射导致的辐射截陷作用.模式的离线检验结果表明:(1)冠层模式计算风廓线与风洞实验测量数据吻合良好;(2)离线冠层模式能够模拟实际小区的风速、温度垂直廓线,并能够较好地体现小区内气温日变化.冠层模式与区域边界层模式耦合检验结果表明:(1)耦合模拟的近地面(2 m处)气温及地表温度的结果明显优于传统的水泥平板方案,尤其是在夜间,水泥平板方案与实测气温最大偏差4 K左右,耦合模拟方案为1-2 K;(2)耦合模拟方案考虑了建筑物对冠层之上的拖曳力影响以及建筑物形态结构对雷诺应力的影响,风速(10 m处)计算结果与观测值相差约在1 m/s,水泥平板方案偏差3 m/s左右.  相似文献   
39.
北京商务中心区大气环境的数值模拟   总被引:1,自引:0,他引:1  
北京商务中心区(Central Business District,CBD)位于北京市中心的东部,距离故宫博物院约4.5km,占地约4km2,最高建筑物超过300m,建成后会导致局地大气环境改变。采用基于k-ε湍流闭合的城市冠层模式对CBD建成后的大气环境进行模拟,结果表明:主导风向西北风时的大气通风能力稍优于次主导风向西南风,空气动力学粗糙度约5.3m,零平面位移约110.0m;浅色建筑外观、屋顶绿化及高叶面指数植被有助于气温的降低,可缓解夏季热岛效应;交通高峰时段,主要道路尤其是交叉路口的NOx浓度超过国家二级标准。上述研究结果对优化CBD规划设计有重要参考价值。  相似文献   
40.
江海英  柴琳娜  贾坤  刘进  杨世琪  郑杰 《遥感学报》2021,25(4):1025-1036
植被冠层含水量CWC (Canopy Water Content)和植被地上部分含水量VWC (Vegetation Water Content)对于植被健康状况和土壤干旱监测具有重要意义。本文联合PROSAIL辐射传输模型和植被水分指数NDWI(Normalized Difference Water Index),发展了一种简单、通用性较好的低矮植被CWC和VWC反演方法,可实现中、高空间分辨率下的CWC和VWC估算。首先对PROSAIL模型输入参数进行敏感性分析,明确各参数对模型输出反射率的影响机制,以优化PROSAIL模型输入参数设置并生成低矮植被的反射率模拟数据。基于模拟数据,计算了4个植被水分指数NDWI_((860,1240))、NDWI_((860,1640))、NDWI_((1240,1640))和NDWI_((860,970))用于反演低矮植被CWC和VWC。基于模拟数据的结果表明,4个植被水分指数与ln (CWC)都存在明显的线性关系,基于该关系建立了CWC估算模型。该模型可以直接用于低矮植被CWC估算,并通过VWC与CWC之间的经验关系间接计算得到VWC。模型模拟结果也表明,由于NDWI_((860,1640))和NDWI_((1240,1640))高度相关(R~2=0.99),两者可以提供相似且相对较好的低矮植被CWC估算精度。基于地面实测数据的验证结果与基于模拟数据的结果表现出很好的一致性,即基于NDWI_((860,1640))和NDWI_((1240,1640))估算的VWC都有相似且较高的精度,决定系数(R~2)都为0.88,均方根误差(RMSE)分别为0.4558 kg/m~2和0.4380 kg/m~2。利用Landsat 5 TM数据对NDWI_((860,1640))估算效果的验证结果显示,模型估算CWC与地面实测CWC的R~2为0.84,RMSE为0.1342 kg/m~2,估算VWC的RMSE为0.5651 kg/m~2。本文提出的基于NDWI_((860,1640))和NDWI_((1240,1640))的CWC/VWC估算模型可被用于低矮植被的长势监测和干旱监测,为低矮植被覆盖地表的土壤水分反演提供高质量的植被水分信息。  相似文献   
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号