地表热通量测量中的问题

由于缺乏对土壤表面发生的各种过程的了解，往往会导致土壤表面热通量测量的不正确。基想根据地表以下一些度处的抛弃爱量测量资料准确地确定地表的热通量，不但要考虑则板以上的热量存同，而且要考虑到测板以下的潜热损耗。如果忽略热储量就会导致大的误差，如忽略潜热过程，则会有更大的误差。     

空气热储存和垂直平流对干旱均匀裸土地表能量平衡的影响

利用"内蒙古微气象观测蒸发试验"的数据,估算了我国西北干旱区典型均匀裸土下垫面条件下的空气热储存和垂直平流输送,并分析了空气热储存项和垂直平流输送项对干旱区地表能量不闭合的影响。研究发现:由于干旱区温度梯度大,热力抬升作用较强,即使在均匀下垫面条件下也存在可观的垂直平流输送。在地表能量平衡方程中引入空气热储存项和垂直平流输送项之后,二者对能量不闭合的平均补偿分别达到1.0 W/m2和7.1 W/m2,闭合度分别提高2%和14%,地表能量不平衡残差平均值由26.4 W/m2减小到18.2 W/m2,地表能量闭合度由82%提升到98%,干旱区地表能量平衡有明显改善。     

半干旱草原下垫面能量平衡特征及土壤热通量对能量闭合率的影响

土壤热通量在半干旱草原下垫面能量平衡研究中极为重要,土壤热通量估计不够准确是导致地表能量不平衡的一个重要原因。利用2008年6—9月锡林郭勒草原主生长期地表辐射、通量和土壤温度梯度观测资料,研究中纬度半干旱草原下垫面地表能量平衡特征。首先,在分析能量平衡各分量月平均日变化特征的基础上,通过对土壤热流量板观测的5 cm深度土壤热通量(G)的相位前移,研究了土壤热通量相位滞后对地表能量平衡产生的影响;其次,利用谐波分析方法,通过计算地表土壤热通量(Gs),分析了地表到热流量板之间的土壤热量储存对地表能量平衡的影响。结果表明:(1)将土壤热通量相位前移30 min,湍流通量与可利用能量(Rn-G)线性回归的斜率从0.835增加到0.842,地表能量闭合率提高了0.7%,但仍有15.8%的能量不闭合;(2)考虑了地表到热流量板之间的土壤热量储存之后,湍流通量与可利用能量之间的回归斜率达到0.979,能量不闭合程度仅为2.1%。     

土壤热异常对地表能量平衡影响初探

将来自土壤深部的热通量引入off line的陆面过程模式 (NCAR—LSM ) ,通过长达 2a的数值试验对比分析了它对各层次土壤温度和地表能量平衡的影响。　　在土壤底部引入 5W /m2 的热通量使底层土壤显著升温 ,但升温随着接近表层而迅速衰减。积分 3个月后 ,由地下进入地表的热流量增幅可达 1W/m2 以上 ,并持续增大到 5W /m2 ,地表最大升温约 0 .5K ,同时地表感热、蒸发潜热及长波辐射通量均有 1W /m2 左右的正异常 ;若将土壤热传导系数放大一个量级以加速热量交换 ,则地表升温提高到 1K以上 ,长波辐射增加 3W /m2 以上 ,超过了气溶胶全球平均的辐射效应。结果表明 :一定量值的土壤热异常对地表能量平衡和短期气候变化 (10 -1～ 10 1a)有着不可忽略的影响。同时 ,深入的资料分析、完善的陆面过程模式以及它与大气模式的耦合试验也是亟待进行的相关工作。     

半干旱草地地表土壤热通量的计算及其对能量平衡的影响

利用2008年7月兰州大学半干旱气候与环境观测(SACOL)站的观测资料,对比分析了地表土壤热通量的三种计算方法,即谐波法、温度预报校正法(TDEC法)以及结合自校正热通量板(HFP01SC)测量的温度积分法(ITHP法);进而分析了三种不同方法的计算结果对地表能量平衡的影响。比较5cm深度处谐波法和TDEC法的计算结果与HFP01SC的实测结果,三者的相位基本一致,相互之间均具有很好的线性关系;谐波法与TDEC法的计算值较为接近,但分别比HFP01SC的实测值偏大了2%和6%(主要发生在夜间)。对于地表的土壤热通量(G0),谐波法与TDEC法两者的计算结果仅偏差约1%;TDEC法与ITHP法的计算结果之间也具有很好的线性关系(R2=0.99),但偏差达到9%左右。相对于HFP01SC的实测结果,由谐波法和TDEC法计算的G0可将SACOL站的地表能量闭合率分别提高6%和7%左右;利用温度积分法将HFP01SC的实测结果校正到地表后,地表能量闭合率也提高了约6%。因此,在对涡动相关通量做了常规订正的情况下,当充分考虑了土壤热存储后,SACOL站的地表能量闭合率可提高6%～7%,达到82%～83%左右。     

一种城市地表能量平衡模式在上海的模拟评估

利用一整年的上海城区常规气象和地表能量平衡观测资料,驱动和检验了局地城市地表能量(水分)平衡模式(SUEWS/LUMPS)在上海地区的模拟能力,并对模式输入参数进行了部分本地化。模拟结果表明,SUEWS模式较好地再现了各辐射通量的日变化形态,对净辐射通量(Q~*)中午日峰值低估约为25 W·m~(-2);模式对四个季节向下长波辐射通量(L_↓)的日变化幅度均被低估,对向上长波辐射通量(L_↑)的模拟明显优于L_↓。SUEWS/LUMPS模式对感热通量(Q_H)各季节(春季除外)日峰值出现时次均有准确模拟,而对Q_H量值各季节均为低估;SUEWS模式在夏、秋季对白天潜热通量(Q_E)的模拟均优于LUMPS模式,而在冬、春季的模拟情况两者接近;SUEWS模式成功再现了储热通量(△Q_S)冬、春、秋季早、晚正负值转换时间,而在夏季滞后了2 h,模拟的△Q_S量值季节差异性较大。对模式误差随气温、风速及风向变化进行分析表明,在较高气温和较大风速下,Q_H、Q_E均表现为低估误差增大,而△Q_S则相反,表现为更显著地高估;风向的影响主要表现为模式未考虑东面密集建筑群而使得Q_H较明显低估约为-50 W·m~(-2),而西侧公园绿地的存在使得Q_H高估约15 W·m~(-2)。     

上海秋冬季地表能量平衡及CO2通量特征分析

利用2012年11月11日至2013年1月20日上海秋冬季涡动相关通量观测资料,对比分析地表能量平衡和CO₂通量在不同天气条件下的日变化特征。结果表明：2012-2013年上海晴天和多云天气条件下,最大能量通量为储热项,其次为感热项;用于蒸发的潜热通量项最小,低于50 w·m^-2。储热项日峰值出现在11时,出现时间早于净辐射通量,而在日落前转为负值。感热项日变化曲线并不以12时为中心呈对称分布,日落后感热项仍为明显正值。中午至日落时波文比值为3以上。感热通量受风向影响最大,在主导风向为西北风时,感热通量日峰值从其他风向的175 w·m^-2左右减小至120 w·m^-2左右。霾和云对短波辐射均表现为衰减作用,云的衰减作用明显大于霾。云使地表向上长波辐射和净长波辐射明显减少,而使大气逆辐射增加。晴天条件下,全天表现为CO₂排放源,且日变化呈双峰型,两个峰值出现时间正好对应上下班高峰时段,傍晚峰值大于早上峰值。     

地表通量的计算问题

该文简略地评述了地表通量（动车，感热和潜热通量）计算的用途，方法，某些结果以及不同方法的优缺点，对于未来的工作也提出了建议。     

西北干旱区及高原上卫星遥感非均匀地表区域能量通量研究

介绍了目前利用Landsat TM和NOAA/AVHRR遥感资料进行非均匀地表区域地表能量通量和蒸发(蒸散)量研究的进展和存在的难点问题，并提出了解决问题的可能途径。     

Effects of the Soil Heat Flux Estimates on Surface Energy BalanceClosure over a Semi-Arid Grassland

Soil heat flux is important for surface energy balance (SEB), and inaccurate estimation of soil heat flux often leads to surface energy imbalance. In this paper, by using observations of surface radiation fluxes and soil temperature gradients at a semi-arid grassland in Xilingguole, Inner Mongolia, China from June to September 2008, the characters of the SEB for the semi-arid grassland were analyzed. Firstly, monthly averaged diurnal variations of SEB components were revealed. A 30-min forward phase displacement of soil heat flux (G) observed by a fluxplate at the depth of 5-cm below the soil surface was conducted and its effect on the SEB was studied. Secondly, the surface soil heat flux (Gs) was computed by using harmonic analysis and the effect of the soil heat storage between the surface and the fluxplate on the SEB was examined. The results show that with the 30-min forward phase displacement of observed G, the slope of the ordinary linear regression (OLR) of turbulent fluxes (H+LE) against available energy (Rn–G) increased from 0.835 to 0.842, i.e., the closure ratio of SEB increased by 0.7%, yet energy imclosure of 15.8% still existed in the SEB. When Gs, instead of G was used in the SEB equation, the slope of corresponding OLR of (H+LE) against (Rn–Gs) reached 0.979, thereby the imclosure ratio of SEB was reduced to only 2.1%.     

Interdecadal Variations of the Western Pacific Subtropical High and Surface Heat Flux over East Asia and Their Relationship

The interdecadal variation of intensity of the western Pacific subtropical high(WPSH) during the period 1951-2001 is studied by using data from the National Climate Center(NCC),China Meteorological Administration.The characteristics of the circulations at 500 hPa and the surface heat flux over East Asia are also analyzed based on the NCEP/NCAR monthly reanalysis data.The results reveal that the WPSH and the circulations exhibit interdecadal variations around 1978,with enhancing intensities.The interseasonal persistence of the WPSH intensity alters correspondingly to some extent,which is more significant during 1978-2001 than during 1951-1978.The surface heat flux over East Asia also displays a remarkable interdecadal variation,which leads that of the WPSH intensity.The key variation areas of the surface sensible heat flux(SSHF) are mainly located over the eastern and western Tibetan Plateau around the late 1960s.However,the difference of the SSHF between the eastern and western Plateau exhibits a change in the mid 1970s,close to the time of the abrupt climate change of the WPSH intensity.The SSHF of the Plateau stably increases in the west and decreases in the east before the mid-late 1960s,while it stably increases in the east and decreases in the west after the mid-1970s.On the other hand,the key variation area of the surface latent heat flux(SLHF) is mainly situated over the West Pacific(WP),where the SLHF anomaly in spring changes from positive to negative in the south before 1978,but from negative to positive in the north after 1978;while in summer it turns from positive to negative all over the WP after 1978.The interdecadal variation of SLHF in both spring and summer corresponds well to the interdecadal variation of the WPSH intensity in the same season.The notable correlation between the WPSH intensity and SSHF(or SLHF) maintains without any change although each of these qnantities varies on the interdecadal scale.     

SST日变化对西太平洋暖池海表热通量季节内变化的影响

基于利用日最大太阳辐射、日平均海面风和日降水量近似计算海表温度(SST)日变化的振幅的方法，发展了一个计算SST日循环的参数化方案。利用周平均SST强迫美国国家大气研究中心(NCAR)的CCM3大气模式进行了有、无考虑SST日变化的比较试验。热带海洋与全球大气计划之耦合海气响应实验(TOGA COARE)的强化观测期间IMET浮标的逐时海表观测资料不仅验证了该参数化方案的合理性，也表明了利用参数化方案对强迫场SST迭加日变化使CCM3较真实地模拟出西太平洋暖池海表热通量的季节内变化的位相结构。     

SST日变化对西太平洋暖池海表热通量季节内变化的影响(英文)

基于利用日最大太阳辐射、日平均海面风和日降水量近似计算海表温度（SST）日变化的振幅的方法,发展了一个计算SST日循环的参数化方案。利用周平均SST强迫美国国家大气研究中心（NCAR）的CCM3大气模式进行了有、无考虑SST日变化的比较试验。热带海洋与全球大气计划之耦合海气响应实验（TOGA COARE）的强化观测期间 IMET浮标的逐时海表观测资料不仅验证了该参数化方案的合理性,也表明了利用参数化方案对强迫场SST迭加日变化使CCM3较真实地模拟出西太平洋暖池海表热通量的季节内变化的位相结构。     

麦田通量数据质量控制及能量闭合性分析

近地面层能量不闭合是涡度相关系统观测中普遍存在的难点问题。为了提高涡度相关系统通量观测数据的质量,选取郑州农业气象试验站2009年10月—2010年6月整个冬小麦生长季的通量观测资料,对30 min通量数据进行野点剔除、数据插补和Webb-Pearman-Leuning(WPL)校正等数据预处理。用两种方法(OLS和EBR)评价了该地区麦田生态系统能量平衡状况。结果表明:处理后的数据质量有明显提升,日平均湍流能增加7.09 W·m~(-2),日平均CO2通量减少0.0730 mg·m~(-2)·s~(-1)。农田涡度相关系统观测的能量平衡比率(EBR)日变化规律明显:早晨和傍晚昼夜交替时EBR波动最大,白天能量闭合状况优于夜间;暖季EBR大部分都在1左右浮动,能量平衡闭合程度较高,而冬季能量平衡闭合程度比暖季偏低。能量通量和湍流通量有较强的相关性,决定系数R2=0.8066,能量闭合度为88%,存在能量不闭合现象。     

Latent Heat Flux from Small Sheltered Lakes

The dependency of the latent heat flux on the over-water fetch on lakes surrounded by tall, dense forest was studied by making use of measurements made on two different-sized lakes. The measurements were made during the NOPEX (Northern Hemisphere Climate-Processes Land Surface Experiment) field campaign. It was found that, in the case of a typical Scandinavian lake with a size of less than 10 km², the latent heat flux will increase as a function of over-water fetch due to the increase of wind speed and in spite of the increased air humidity. This also has implications on area-averaged fluxes: when two lakes having similar shorelines, lake water temperatures and solar radiation conditions are compared, then the evaporation per unit area is smaller from the smaller lake. When the lakes are large, with fetches of several kilometres, then the significance of sheltering is small. If point measurements are used for the estimation of area-averaged latent heat fluxes from lakes with short fetches and forested shorelines then the distance of the measuring site from the shoreline should be taken into account, otherwise errors of tens of percent may occur.     

不同土壤类型的热通量变化特征

利用2004—2007年中国科学院中国生态系统研究网络(CERN)生态站实测土壤热通量、辐射等资料,分析了不同土壤类型表层热通量的日变化和季节变化,以及不同土壤类型的热通量与总辐射、净辐射的关系。结果表明,由于导热率越大,热量传输就越快;热容量越小,热量传输也越快,造成土壤热通量的日较差和年较差较大,所以黄绵土和紫色土的表层热通量日较差最大(220～280 W.m-2),高寒草甸土和水稻土最小(55W.m-2);季节变化中土壤表层热通量的年较差变化范围在12～28W.m-2之间,灰漠土最大,为28W.m-2,热通量年较差从大到小依次为灰漠土、黄绵土、盐碱潮土、红壤土、紫色土、沼泽土、水稻土和高寒潮土,高寒潮土最小,为12W.m-2。不同土壤类型的热通量与总辐射、净辐射呈正相关关系,但不同土壤类型的土壤热通量在12:00(地方时)所占净辐射的比例各不相同,高寒草甸土最小,约为8%;黄绵土最大,为38%,多数土壤的热通量占净辐射的比例在15%～20%之间,这充分表明不同土壤类型表层热通量的传输存在很大差异。