首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到18条相似文献,搜索用时 125 毫秒
1.
中国区域人为热释放的气候强迫   总被引:4,自引:2,他引:2  
研究了1978~2008年中国地区及各省、市、自治区、特别行政区人为热释放造成的气候强迫与不同地区间的人口、能源消费状况和人为热释放的气候强迫的关系,并试图对未来人为热释放的气候强迫做出预估.结果表明,近30年中国地区平均人为热释放造成的气候强迫迅速增加,1978年其值约为0.07 W·m-2,但2008年则增至0.28 W·m-2.另外,中国人为热释放的气候强迫呈典型地域分布特征,华北、华东、华中和华南等经济发达地区明显高于周围其他地区,而西北地区整体上来说则很小,地区分布很不均匀.这种不均匀分布的特征,可能对区域气候、甚至全球气候造成影响.  相似文献   

2.
人为热释放:全球分布的估算及其气候效应的探索   总被引:1,自引:0,他引:1  
陈兵  陈良富  董理  石广玉 《大气科学》2016,40(2):289-295
人类生产和生活中大量消费各种形式的能源,除了向大气里排放温室气体和气溶胶外,还释放大量热量。人为热释放伴随着人类社会发展而长期存在,随着全球人口增长和经济发展,其影响效应不断加剧。人为热释放具有典型地域集中、不均匀分布的特征:虽然全球平均人为热释放通量仅约为0.03 W m-2,在人口密集的城市地区,人为热释放可高达每平方米数百瓦,足以影响局地气候。伴随全球经济的发展,人口的增长及城市化进程的加剧,人为热释放分布更集中,影响气候的范围逐步扩大,其对气候的影响能力逐步增强。全球气候模式的结果表明:人为热释放能够对全球大气环流产生影响,进而影响到全球气候变化。人为热释放可以导致全球地表温度增温约0.06 K,500 hPa温度场平均升温约0.04 K,尤其对北半球中高纬度升温效应明显。研究结果表明,人为热释放虽然没有温室气体如二氧化碳等影响因子对全球气候的影响那么显著,但是其仍然能够对全球气候产生影响,是全球气候变化不可忽视的影响因子。  相似文献   

3.
硫酸盐和烟尘气溶胶辐射特性及辐射强迫的模拟估算   总被引:21,自引:6,他引:21       下载免费PDF全文
张立盛  石广玉 《大气科学》2001,25(2):231-242
利用已有的硫酸盐和烟尘气溶胶折射指数资料,精确计算了这两种气溶胶从太阳短波到红外谱段的辐射特性。然后,在LLNL化学输送模式(CTM)模拟的硫酸盐和烟尘气溶胶资料及改进的气溶胶参数化基础上,在国内首次用GCM估算了这两种气溶胶引起的全球辐射强迫。结果表明:(1)西欧是全球最大的硫酸盐辐射强迫中心,最大值出现在夏季,达-5.0W/m2;(2)烟尘强迫的最大中心出现在夏季的南美和非洲中南部,为4.0W/m2;(3)南半球大陆人为气溶胶的强迫不容忽视;(4)某些地区人为气溶胶的强迫在量值上可与CO2等温室气体引起的强迫相比拟。  相似文献   

4.
温室气体和硫酸盐气溶胶的辐射强迫作用   总被引:5,自引:4,他引:5  
对GOALS4 .0海 陆 气耦合模式的相关部分进行了改进 ,主要改进包括温室气体的扩充和硫酸盐气溶胶“显式”方案的引入 ,并引入 2 0世纪温室气体的实际浓度变化以及硫循环模式模拟的硫酸盐气溶胶的三维全球浓度分布 ,模拟了温室气体和硫酸盐气溶胶造成的辐射强迫的空间分布和时间变化。全球平均的温室气体和硫酸盐气溶胶的辐射强迫分别为 2 .17W /m2 和 - 0 .2 9W /m2 ;温室气体造成的辐射强迫在空间上呈现明显的纬向结构 ,最大值 (大于 2 .5W/m2 )和最小值 (小于 1W /m2 )分别位于副热带和两极地区 ,在北半球主要工业区硫酸盐气溶胶的辐射强迫绝对值接近温室气体的辐射强迫值 (大于 - 2 .0W /m2 )。  相似文献   

5.
全球气候模式对东亚地区地表短波辐射的模拟检验   总被引:2,自引:1,他引:1       下载免费PDF全文
利用WCRPCMIP3提供的18个全球气候模式输出结果, 检验了其对东亚地区地表短波辐射的模拟能力, 结果表明:多模式集合的多年平均地表短波辐射模拟偏高约8.7 W/m 2, 晴空地表短波辐射模拟偏高约3.4 W/m 2, 地表短波云辐射强迫模拟偏低约5.3 W/m2, 模式间的标准差分别达到9.6, 7.8 W/m2和8 W/ m2; 多模式集合能够很好地模拟出地表短波辐射的纬向平均季节变化的位相特征, 但在量值上还有较大的差距; 模拟偏差分析表明, 多模式集合的区域年平均地表短波辐射、晴空地表短波辐射、地表短波云辐射强迫的均方根偏差分别为34.7, 17.1 W/m 2和29.1 W/ m2, 表明云在地表短波辐射的模拟偏差中起着重要作用; 多模式集合能够很好地模拟出地表入射短波辐射年变化的线性减小趋势, 但模式高估了晴空入射辐射的减小趋势, 而模拟的云辐射强迫变化趋势与ERA 40完全相反。  相似文献   

6.
为减少不同气候模式评估气溶胶气候效应的差异,第六次耦合模式比较计划(Coupled Model Intercomparison Project Phase 6,CMIP6)直接给定了人为气溶胶强迫数据。因此,有必要基于此强迫数据重新评估气溶胶气候效应。本研究首先将CMIP6给出的描述人为气溶胶强迫的模块引入南京信息工程大学(Nanjing University of Information Science and Technology,NUIST)的地球系统模式(The NUIST Earth System Model,NESM)。之后,利用NESM模式评估地球辐射收支平衡对此人为气溶胶强迫的响应,并分析模式模拟结果的不确定性。评估给出的人为气溶胶有效辐射强迫为-0. 45(±0. 28) W·m~(-2)。其中,气溶胶直接辐射效应为-0. 34(±0. 01) W·m~(-2),与第二次气溶胶比较计划(The second phase of Aerosol Comparisons between Observations and M odels,Aero ComⅡ)的评估结果基本一致;气溶胶对云辐射强迫的影响(包括半直接效应和间接效应)为-0. 10(±0. 30) W·m~(-2),明显受到模式内部变率的干扰,具有较大的不确定性。  相似文献   

7.
依据1990~2013年江苏省能源消费统计资料和1990、1995、2000、2005、2010年的人口空间分布数据,估计江苏省人为热排放量、探讨其时空分布特征并预测其未来变化趋势。研究结果表明,20多年来江苏省的人为热排放量持续增长,从1990年全省平均的0.59 W/m~2增加到2013年的2.85 W/m~2。排放的空间分布也不均匀,总体上江苏南部地区的排放通量高于江苏北部。近些年江苏省的人为热排放已成为区域问题,高值区已连接成片,2010年江苏省大部分地区的人为热排放高于2.5 W/m~2,南部主要城市排放通量大于10 W/m~2、北部城市也多大于5 W/m~2。江苏各城市的城区人为热排放通量稳步增长,2002年后增长加速、增量最高可达到2 W m~(-2) a~(-1)。在2030年和2050年江苏省的平均人为热排放通量将分别达到5.7 W/m~2和9.1 W/m~2,可能对中国东部的气候和大气环境产生重要影响。  相似文献   

8.
沙尘气溶胶辐射强迫全球分布的模拟研究   总被引:7,自引:2,他引:5  
张华  马井会  郑有飞 《气象学报》2009,67(4):510-521
为了定景了解沙尘气溶胶对气候的影响,文中利用一个改进的辐射传输模式,结合伞球气溶胶数据集(G-ADS),计算了晴空条件下,冬夏两季沙尘气溶胶的直接辐射强迫在对流层顶和地面的全球分布,并讨论了云对沙尘气溶胶辐射强迫的影响.计算结果表明,对北半球冬季和夏季而言,在对流层顶沙尘气溶胶的全球短波辐射强迫的平均值分别为-0.477和-0.501 W/m2;长波辐射强迫分别为0.11和0.085 W/m2;全球平均短波地面辐射强迫冬夏两季分别为-1.362和-1.559 W/m2;长波辐射强迫分别为0.274和0.23 W/m2.沙尘气溶胶在对流层顶和地面的负辐射强迫的绝对值郁随太阳天顶角的余弦和地表反照率的增加而增大;地表反照率对沙尘气溶胶辐射强迫的强度和分布都有重要影响.研究指出:云对沙尘气溶胶的直接辐射强迫的影响不仅取决于云量,而且取决于云的高度和云水路径,以及地面反照率和太阳高度角等综合因素.中云和低云对沙尘气溶胶在对流层顶的短波辐射强迫的影响比高云明显.云的存在都使对流层顶长波辐射强迫减少,其中低云的影响最为明显.因此,在估算沙尘气溶胶总的直接辐射强迫时,云的贡献不可忽视.  相似文献   

9.
基于NCEP/NCAR再分析资料及6个CMIP6全球气候模式模拟资料,对1961—2014年北半球湿热指数表征的热不舒适天数与风寒指数表征的冷不舒适天数历史变化进行归因分析,并预估未来(2015—2100年)4种不同情景下不舒适天数的变化趋势。结果表明:历史时期北半球中低(中高)纬度地区热(冷)不舒适天数偏多且不舒适天数显著增加(减少)。其中,高纬度(中纬度)地区能够检测到历史全强迫,人为强迫和温室气体强迫的影响,且温室气体强迫主导了冷(热)不舒适天数变化。低纬度地区,热不舒适天数显著增加可归因于人为温室气体强迫作用,气溶胶强迫能够产生相反的作用降低热不舒适的发生率,冷不舒适天数则受气候系统内部的调控作用。未来热(冷)不舒适天数将持续增加(减少),其中ssp585与ssp370情景下舒适度变化显著,ssp126与ssp245情景下,2080年后北半球人类遭受的冷热不舒适感将维持在稳定的水平。  相似文献   

10.
对气溶胶气候效应开展分类评估并探讨诊断方法的合理性。人为气溶胶辐射效应对计算云辐射强迫的影响为0.38 W·m~(-2)。诊断评估气溶胶对云辐射强迫的影响需要排除这个偏差。两种基于不同试验设计诊断得出的半直接效应分别为0.21和0.09 W·m~(-2),存在显著差异。主要原因可能是人为气溶胶影响云辐射强迫的不同机制之间在模式模拟过程中不断地相互交织,不是简单的线性叠加关系。模式诊断得出的Twomey效应不仅包括Twomey效应本身,还包括Twomey效应引起的部分快速调整。总之,利用模式评估分析人为气溶胶气候效应需要注意审查试验设计和诊断方法的合理性。  相似文献   

11.
Stable light data from Defense Meteorological Satellite Program (DMSP)/Operational Linescan System (OLS) satellites and authoritative energy consumption data distributed by National Bureau of Statistics of China were applied to estimating the distribution of anthropogenic heat release in China from 1992 to 2009. A strong linear relationship was found between DMSP/OLS digital number data and anthropogenic heat flux density (AHFD). The results indicate that anthropogenic heat release in China was geographically concentrated and was fundamentally correlated with economic activities. The anthropogenic heat release in economically developed areas in northern, eastern, and southern China was much larger than other regions, whereas it was very small in northwestern and southwestern China. The mean AHFD in China increased from 0.07 W m-2 in 1978 to 0.28 W m-2 in 2008. The results indicate that in the anthropogenic heat-concentrated regions of Beijing, the Yangtze River Delta, and the Pearl River Delta, the AHFD levels were much higher than the average. The effect of aggravating anthropogenic heat release on climate change deserves further investigation.  相似文献   

12.
Comparisons are made of long-term empirical and model-estimated patterns of solar irradiance forcing during a 200-year period (1650-1850), which precedes any apparent anthropogenic influence on climate. This interval encompasses a considerable range (approximately 4 W/m2) of estimated variation in solar output, including the "Maunder" and "Dalton" Minima of solar irradiance, and an intervening interval of relatively high values of irradiance, but does not encroach into the industrial era wherein it is difficult to separate solar and anthropogenic influences. Particular emphasis is placed on comparing empirical and modeled patterns of forced surface temperature variation. The empirical patterns bear a greater similarity to the pattern of forced response of a coupled ocean-atmosphere general circulation model (AOGCM) than with an independent model simulation result using an ocean with specified heat transport, both in terms of the spatial pattern of response and implied global mean sensitivity to forcing. Heightened sensitivity in the western Pacific warm pool apparent in the empirical response pattern, is not observed in the forced response of the coupled model. It is possible that this pattern is the result of feedback processes not currently reproduced in course-resolution coupled models. The greatest empirical response is found at the multidecadal-to-century (> 40 year period) time scale, for which the forcing is dominated by the roughly 90-year Gleissberg Cycle of irradiance. This indicates a global-mean sensitivity (approximately 0.3 K/W/m2), which is close to the coupled model result (approximately 0.4 K/W/m2). At decadal time scales (8-25 year period), for which the forcing is dominated by the 11-year and 22-year period solar cycles), the temperature sensitivity is moderately reduced, and its spatial pattern of response is dominated by an apparent resonance with known decadal modes of climate variability.  相似文献   

13.
Quantifying the radiative forcing due to aerosol–cloud interactions especially through cirrus clouds remains challenging because of our limited understanding of aerosol and cloud processes. In this study, we investigate the anthropogenic aerosol indirect forcing (AIF) through cirrus clouds using the Community Atmosphere Model version 5 (CAM5) with a state-of-the-art treatment of ice nucleation. We adopt a new approach to isolate anthropogenic AIF through cirrus clouds in which ice nucleation parameterization is driven by prescribed pre-industrial (PI) and presentday (PD) aerosols, respectively. Sensitivities of anthropogenic ice AIF (i.e., anthropogenic AIF through cirrus clouds) to different ice nucleation parameterizations, homogeneous freezing occurrence, and uncertainties in the cloud microphysics scheme are investigated. Results of sensitivity experiments show that the change (PD minus PI) in global annual mean longwave cloud forcing (i.e., longwave anthropogenic ice AIF) ranges from 0.14 to 0.35 W m–2, the change in global annual mean shortwave cloud forcing (i.e., shortwave anthropogenic ice AIF) from–0.47 to–0.20 W m–2, and the change in net cloud forcing from–0.12 to 0.05 W m–2. Our results suggest that different ice nucleation parameterizations are an important factor for the large uncertainty of anthropogenic ice AIF. Furthermore, improved understanding of the spatial and temporal occurrence characteristics of homogeneous freezing events and the mean states of cirrus cloud properties are also important for constraining anthropogenic ice AIF.  相似文献   

14.
Richard VanCuren 《Climatic change》2012,112(3-4):1071-1083
Exploiting surface albedo change has been proposed as a form of geoengineering to reduce the heating effect of anthropogenic increases in greenhouse gases (GHGs). Recent modeling experiments have projected significant negative radiative forcing from large-scale implementation of albedo reduction technologies (“cool” roofs and pavements). This paper complements such model studies with measurement-based calculations of the direct radiation balance impacts of replacement of conventional roofing with “cool” roof materials in California. This analysis uses, as a case study, the required changes to commercial buildings embodied in California’s building energy efficiency regulations, representing a total of 4300 ha of roof area distributed over 16 climate zones. The estimated statewide mean radiative forcing per 0.01 increase in albedo (here labeled RF01) is ?1.38 W/m2. The resulting unit-roof-area mean annual radiative forcing impact of this regulation is ?44.2 W/m2. This forcing is computed to counteract the positive radiative forcing of ambient atmospheric CO2 at a rate of about 41 kg for each square meter of roof. Aggregated over the 4300 ha of cool roof estimated built in the first decade after adoption of the State regulation, this is comparable to removing about 1.76 million metric tons (MMT) of CO2 from the atmosphere. The point radiation data used in this study also provide perspective on the spatial variability of cool roof radiative forcing in California, with individual climate zone effectiveness ranging from ?37 to ?59 W/m2 of roof. These “bottom-up” calculations validate the estimates reported for published “top down” modeling, highlight the large spatial diversity of the effects of albedo change within even a limited geographical area, and offer a potential methodology for regulatory agencies to account for the climate effects of “cool” roofing in addition to its well-known energy efficiency benefits.  相似文献   

15.
Estimation of anthropogenic heat emission in the Gyeong-In region of Korea   总被引:1,自引:0,他引:1  
The anthropogenic heat emission in the Gyeong-In region of Korea in 2002 is estimated based on the energy consumption statistics data. The energy consumption over the region is categorized into four energy sectors: electricity use, transportation, point sources, and area sources. The estimated annual mean anthropogenic heat emissions in Seoul, Incheon, and Gyeonggi are found to be 55, 53, and 28 W m?2, respectively. A major contributing energy sector to anthropogenic heat emission in the Gyeong-In region is area sources including the residential, commercial, and small industrial sectors, which account for 40% of the total heat emission from the three administrative districts, and transportation and electricity use follow. The distributions of the annual, monthly, and hourly mean anthropogenic heat emission for all energy sectors are presented in the 0.01° longitude × 0.01° latitude grid domain. The presently estimated anthropogenic heat emission data can be used in mesoscale meteorological and environmental modeling in the Gyeong-In region.  相似文献   

16.
RCP4.5: a pathway for stabilization of radiative forcing by 2100   总被引:3,自引:2,他引:1  
Representative Concentration Pathway (RCP) 4.5 is a scenario that stabilizes radiative forcing at 4.5?W?m?2 in the year 2100 without ever exceeding that value. Simulated with the Global Change Assessment Model (GCAM), RCP4.5 includes long-term, global emissions of greenhouse gases, short-lived species, and land-use-land-cover in a global economic framework. RCP4.5 was updated from earlier GCAM scenarios to incorporate historical emissions and land cover information common to the RCP process and follows a cost-minimizing pathway to reach the target radiative forcing. The imperative to limit emissions in order to reach this target drives changes in the energy system, including shifts to electricity, to lower emissions energy technologies and to the deployment of carbon capture and geologic storage technology. In addition, the RCP4.5 emissions price also applies to land use emissions; as a result, forest lands expand from their present day extent. The simulated future emissions and land use were downscaled from the regional simulation to a grid to facilitate transfer to climate models. While there are many alternative pathways to achieve a radiative forcing level of 4.5?W?m?2, the application of the RCP4.5 provides a common platform for climate models to explore the climate system response to stabilizing the anthropogenic components of radiative forcing.  相似文献   

17.
水文循环过程受气候变化与人类活动的共同作用,区分气候内部自然变率与人类活动作用于水循环贡献对于增加气候变化的理解非常重要。本研究利用近期发展的考虑地下水取用水与灌溉影响的全球陆气耦合模式进行数值模拟,基于最优指纹法分析探讨中国东部季风区黄河、淮河、海河、珠江、长江、松花江流域水循环变化(地表温度、降水、径流、蒸散发)及归因。结果表明:大部分流域的地表温度年际变化在1965~2005年间检测到包括温室气体气溶胶人为排放、臭氧与土地利用变化产生的外强迫效应,显示在长期对于地表温度起主要作用的可能为上述强迫;1965~2005年降水年际变化仅在淮河及长江下游检测到上述强迫效应,且在长江下游效应占主导。在1965~1984年间,地表温度的年际变化在海河流域检测到由于地下水取水灌溉产生的外强迫效应,并且该效应占主导。在1982~2005年径流年际变化中,在淮河、长江下游及黄河下游处检测到了由于温室气体排放、气溶胶人为排放、臭氧变化及土地利用变化等产生的外强迫效应但无法有效分离,显示该信号在这些地区可能不为主导效应;1982~2005年间的蒸散发年际变化在珠江、长江下游同样检测到了上述强迫效应,并且该效应在长江下游占主导效应。  相似文献   

18.
Estimation of the Distribution of Global Anthropogenic Heat Flux   总被引:1,自引:0,他引:1       下载免费PDF全文
The radiance lights data in 2006 from the National Oceanic and Atmospheric Administration Air Force Defense Meteorological Satellite Program/Operational Linescan System (DMSP/OLS) and authoritative energy data distributed by the United State Energy Information Administration were applied to estimate the global distribution of anthropogenic heat flux.A strong linear relationship was found to exist between the anthropogenic heat flux and the DMSP/OLS radiance data.On a global scale,the average value of anthropogenic heat flux is approximately 0.03 W m 2 and 0.10 W m 2 for global land area.The results indicate that global anthropogenic heat flux was geographically concentrated and distributed,fundamentally correlating to the economical activities.The anthropogenic heat flux concentrated in the economically developed areas including East Asia,Europe,and eastern North America.The anthropogenic heat flux in the concentrated regions,including the northeastern United States,Central Europe,United Kingdom,Japan,India,and East and South China is much larger than global average level,reaching a large enough value that could affect regional climate.In the center of the concentrated area,the anthropogenic heat flux density may exceed 100 W m 2,according to the results of the model.In developing areas,including South America,Central and North China,India,East Europe,and Middle East,the anthropogenic heat flux can reach a level of more than 10 W m 2 ;however,the anthropogenic heat flux in a vast area,including Africa,Central and North Asia,and South America,is low.With the development of global economy and urban agglomerations,the effect on climate of anthropogenic heat is essential for the research of climate change.  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