首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 390 毫秒
1.
An analytical error analysis of profile-derived fluxes of heat, moisture, and momentum, along with stability and roughness length, is performed using the accuracies of the constituent temperature, humidity, and wind speed measurements. Five experiments, representing more than two thirds of the existing marine profile data presently contained in the literature, are compared. Much of the profile data examined was used to develop the transfer coefficients presently employed by a large number of competing bulk aerodynamic flux schemes. Depending upon the experiment, typical profile-method measurement errors were found to range from 15 to 35% for a sensible heat flux of ± 10 W m-2, from 15 to 105% for a latent heat flux of ± 100 W m-2, from 10 to 40% for a stress of 0.05 N m-2, from 15 to 60% for a Monin-Obukhov stability of ± 0.05, and from 25 to 100% for a roughness length of 2 × 10-4 m. Smaller magnitude flux values were found to contain typical errors as large as 100% for sensible heat flux, 300% for latent heat flux, and 60% for stress.  相似文献   

2.
Bulk formulae for wind stress, sensible and latent heat flux are presented that are suitable for strong mesoscale events such as westerly wind bursts that contribute to the El Niño-Southern Oscillation (ENSO). Their exchange coefficients for heat and momentum have a simple polynomial dependence on wind speed and a linear dependence on air–sea temperature difference. The accuracy of these formulae are validated with respect to air–sea fluxes estimated using the standard algorithm adopted by the Tropical Ocean-Global AtmosphereCoupled-Ocean Atmosphere Response Experiment (TOGA COARE). The comparison ismade for observations from 96 Tropical Atmosphere Ocean (TAO) array and National Oceanographic Data Center (NODC) moorings in the equatorial and North Pacific Ocean spanning years 1990–1999. The bulk formulae are shown to have very small median root–mean-square differences with respect to the TOGA COARE estimates: 0.003 N m-2, 1.0 W m-2, and 10.0 W m-2 for the wind stress, sensible heat flux, and latent heat flux, respectively.The variability of air–sea fluxes during the 1997–1998 ENSO is also examined, along with a possible relationship between air–sea fluxes and surface ocean mixed layer depth (MLD). The wind stress and latent heat flux during the 1997 El Niño are found to be greater in the warm pool of the western Pacific than in the central Pacific where the ENSO is most clearly seen. These differences disappear upon the start of La Niña. The MLD in the equatorial Pacific is found to be moderately correlated to air–sea fluxes just before the start of the 1998 La Niña and poorly correlated otherwise.  相似文献   

3.
The sensible heat loss from a stand of winter wheat was calculated from radiometric measurements of crop surface temperature, measurements of air temperature, and an atmospheric resistance to momentum transfer; corresponding latent heat flux was obtained through the energy balance equation. These estimates of sensible and latent heat were compared with fluxes from the Bowen Ratio method. When radiative temperature was derived using a measured canopy emissivity of 0.98, calculations of sensible heat flux were systematically 50–100 W m-2 less than Bowen Ratio values. The two techniques agreed more closely when an apparent emissivity of 0.96 was used with an apparent reflectivity of 0.03. The mean difference between the estimates of latent heat flux was then -16 ± 32 W m-2.The surface temperature method showed less systematic error in comparison with the Bowen Ratio values than did estimates using the aerodynamic method.On leave from: University of Nottingham, School of Agriculture, Loughborough LE12 5RD.  相似文献   

4.
In different synoptic conditions and at different time scales,the analysis of the energy budgets by Bowen Ratio Method and Bulk Schemes over Huaihe River Basin during the field observation periods of HUBEX in 1999 shows that,(1) the averaged latent heat flux is an order of magnitude more than the averaged sensible heat flux during the observation period:(2) the variation of totalcloud amount is out of phase with the terms of energy budgets except for the downward longwave radiation which maybe is related to the cloud's height and class:(3) the values of sensible and latent heat fluxes are small during rain episodes,but thereafter,the values become high and then up to maximum.It is similar to the other terms of the energy budgets except for the downward longwave radiation.The diurnal variation of energy budgets indicates that the daytime precipitation exerts great influence to the energy budgets,but the nighttime precipitation makes little influence;(4) the variation of the latent heat flux is in phase with the evaporation,which indicates that the latent heat flux calculated by bulk schemes is reliable:(5) the means of the sensible and latent heat flux and momentum flux by bulk schemes for the time period from May to August are,respectively,30.71W/m2.116.81W/m2.2.86×10-2N/m2 in 1998 and 30.28W/m2,107.35W/m2,2.74×10-2N/m2 in 1999.The values of these two years are similar.During summer in 1999 the magnitude and activity of sensible heat flux are strongest in June and those of the latent heat flux are in August.  相似文献   

5.
Surface-layer meteorological observations obtained from oceanic buoys over the Korean Strait and the Yellow Sea are used to estimate surface-layer turbulent fluxes of heat, moisture and momentum over the East-Asian Marginal Seas. Special emphasis is paid towards explanation of the impact of the Tsushima warm current flowing through the Korean Strait on air–sea interface fluxes. During the active phase of the Tsushima warm current, when the difference in sea surface temperature and air temperature becomes as large as 8°C, the sensible heat flux increases to a value of about 135 W m−2, while the latent heat flux is around 200 W m−2. The study attempts to broaden our understanding on the air-sea interaction processes over the Yellow Sea and Korean Strait.  相似文献   

6.
利用苏州地区2011 年12月20 日-2012年8 月13 日的湍流观测资料对不同季节、高温、台风强天气过程下的湍流特征进行分析.结果表明:城市地区不同季节动量通量、感热通量、潜热通量日变化明显,各通量的夏季平均值、最大值均高于冬春季,夏季感热通量日最大值为160.2 W·m-2,感热在城市地表能量平衡中的作用大于潜...  相似文献   

7.
Summary The computation of the fluxes between ground surface and air in atmospheric models is based on the assumption that the surfaces parameters are horizontally homogeneous. In reality, the surface is heterogeneous, inducing a difference between the computed and realistic fluxes. Assuming that the distributions of temperature and humidity of the surface are normal, the difference of the fluxes for homogeneous and heterogeneous surface is found theoretically. The results show that the effect of the heterogeneity on the radiation flux is small, but attains a certain degree on the sensible and latent heat fluxes. However, this effect on the heat fluxes is not great when the standard deviation of the distribution of the surface parameters also is small. Only in case of great standard deviation, the difference may attain several W/m2 even the order of magnitude of 10 W/m2. Usually the computed sensible and latent heat fluxes are slightly greater for the heterogeneous case than that for homogeneous case, but when the interaction between the temperature and humidity of the surface is considered, the reverse is true. Received January 18, 2001 Revised July 31, 2001  相似文献   

8.
During slightly unstable but still very close to neutral conditions new results from two previous investigations have shown a significant increase of sensible and latent heat fluxes over the sea. The vertical heat transport during these conditions is dominated by detached eddies originating at the top of the boundary layer, bringing relatively cold and dry air to the surface. This effect can be described in numerical models by either enhanced heat transfer coefficients for sensible and latent heat (Stanton and Dalton numbers respectively) or with an additional roughness length, added to the original roughness lengths for heat and humidity. Such new expressions are developed using turbulence measurements from the Baltic Sea valid for wind speeds up to 14 m s−1. The effect of including the increased heat fluxes is investigated using two different numerical models: a regional three-dimensional climate model covering northern Europe, and a process-oriented ocean model for the Baltic Sea. During periods of several days, the latent heat flux can be increased by as much as 100 W m−2. The increase in sensible heat flux is significantly smaller since the process is only of importance in the very near-neutral regime where the sensible heat flux is very small. The long-term average effect over the Baltic Sea is of the order of several W m−2.  相似文献   

9.
曲绍厚 《气象学报》1988,46(4):452-460
本文根据中国科学院“实验3号”科学考察船1986年10月至12月在菲律宾以东60多万平方公里辽阔的西太平洋热带海域6个连续测站上(146°E,0°;145°E,0°;150°E,0°;140°E,5°N;145°E,5°N;150°E,5°N),使用我国自行研制的小型系留气艇探测系统观测到的大气温度、湿度、气压和风等廓线资料,利用相似理论的通量-廓线关系,给出这一海域的动量通量(特别是曳力系数C_D)、感热通量和潜热通量。结果表明,这一海域上的曳力系数值C_D=(1.53±0.25)×10~(-3);该海域总是将其贮存的热量以感热形式特别是以潜热形式输送到大气中(其中感热输送仅占10%,其余主要为水汽潜热输送),使该海域成为地球上不可多见的热源。  相似文献   

10.
南疆沙漠腹地大气边界层湍流通量特征的观测研究   总被引:4,自引:0,他引:4  
利用新疆塔中站2006年4月、8月的三维风速。温度和水汽脉动资料,运用涡旋相关法计算得到了春、夏季塔中10m高度的动量、感热和潜热通量。结果表明,塔中地区地表热量输送以感热输送为主。春季每天的最大感热通量变化范围为120—320W·m^-2,月平均值为220W·m^-2;夏季最大感热通量的变化范围为140—340W·m^-2,月平均值为230W·m^-2。感热通量值在夜间为负,白天为正,符号的改变出现在日出、日落前后。夏季潜热通量最大值一般为20—60W·m^-2,平均值为27W·m^-2,潜热通量比感热通量小一个量级。春季动量通量的平均值为-0.063W·m^-2,夏季动量通量的平均值为-0.091W·m^-2。日变化规律比较明显,日出后,动量向下传输增大,在09-10时(地方时)出现一个最大值,随后动量向下传输并开始减小。  相似文献   

11.
The link between the sea-ice cover of the Amundsen Gulf and the overlying atmospheric boundary layer was explored on a weekly timestep from winter to summer 2008. The total sea-ice cover was around 97% (3% leads) from 7 January to 21 April. From 28 April to 12 May, the total sea-ice cover approached 100%. From May 19, the total sea-ice declined rapidly to its July minimum of 3%. During the winter, a turbulent internal boundary layer (IBL), attributed to the upward flux of sensible heat (mean = 46 W m−2), was present in most of the mean daily potential temperature profiles. The mean latent heat flux was 1.7 Wm−2. A turbulent IBL was also present in most of the mean daily profiles for early spring. Surface fluxes were not estimated. During late spring and early summer, a stable IBL, attributed to the downward flux of sensible heat (mean = −19 W m−2), was present in most of the potential temperature profiles. Both downward and upward fluxes of latent heat occurred in this period (means = −3.3 and 1.1 W m−2). The sensible heat flux estimates are consistent with the results of others; however, the latent heat flux estimates may be too small due to condensation/deposition within the IBL. The unconsolidated nature of the pack ice in the Amundsen Gulf, and the low sea-surface temperatures following break-up, were critical factors controlling the presence and type of IBL.  相似文献   

12.
Three recent experiments allow evaluation of the bulk transfer coefficients for momentum, water vapour and sensible heat over water bodies of different sizes. As part of a study of evaporation rates from a swamp, measurements of latent and sensible heat fluxes were made over Lake Wyangan in southern N.S.W., Australia. This lake is of several kilometers diameter. In a later experiment, Reynolds stress and sensible heat transfer were measured from a natural-gas platform standing in Bass Strait, south of mainland Australia. The most recent experiment involved the direct measurement of each of these turbulent fluxes from a fixed tower erected in Lake Michigan, U.S.A.Perhaps the most important of the results is the finding that drag coefficients measured over Bass Strait are not significantly different from those over Lake Michigan, despite the obvious differences in depth, fetch, and hence surface wave structure. At both locations, drag coefficients are found to increase slightly with increasing wind speed, while at low wind speeds they are not significantly different from those corresponding to aerodynamic smoothness.Near-neutral bulk transfer coefficients for sensible heat and for water vapour are found to be similar. An average value of about 1.4 × 10–3 is obtained.It is emphasized that stability effects should be considered in any discussion of drag coefficients or bulk transfer coefficients. Large errors can result if near-neutrality is incorrectly assumed.  相似文献   

13.
In this study, turbulent heat flux data from two sites within the Baltic Sea are compared with estimates from two models. The main focus is on the latent heat flux. The measuring sites are located on small islands close to the islands of Bornholm and Gotland. Both sites have a wide wind direction sector with undisturbed over-water fetch. Mean parameters and direct fluxes were measured on masts during May to December 1998.The two models used in this study are the regional-scale atmospheric model HIRLAM and the ocean model PROBE-Baltic. It is shown that both models overestimate the sensible and latent heat fluxes. The overestimation can, to a large extent, be explained by errors in the air-water temperature and humidity differences. From comparing observed and modelled data, the estimated 8-month mean errors in temperature and humidity are up to 1 °C and 1 g kg-1, respectively. The mean errors in the sensible and latent heat fluxes for the same period are approximately 15 and 30 W m-2, respectively.Bulk transfer coefficients used for calculating heat and humidity fluxes at the surface were shown to agree rather well with the measurements, at least for the unstable data. For stable stratification, the scatter in data is generally large, and it appears that the bulk formulation chosen overestimates turbulent heat fluxes.  相似文献   

14.
On March 26, 1971, eddy fluxes of momentum, sensible heat and water vapour were measured over Lake Mendota, Wisconsin, U.S.A., which was covered by an extensive snowfall. An evaporation rate of about 0.7mm day–1 (2.2 mW cm–2) was detected. Wind speeds were light and the atmosphere near the surface was highly stable. In these conditions, the average sensible heat transfer and Reynolds stress were -0.9 mW cm–2 and 0.10 dyn cm–2, respectively. Comparison with measured gradients of wind speed, temperature and humidity yield a drag coefficient of about 0.54 × 10–3, and bulk transfer coefficients for sensible and latent heat of 0.41 × 10–3 and 0.78 × 10–3, respectively, applied to 10-m data. When corrected for the effect of atmospheric stability, these three coefficients become (in the same order) 1.2 × 10–3, 0.9 × 10–3 and 2.5 × 10–3. The errors in these estimates are such that the drag coefficient is not significantly different from that corresponding to an aerodynamically smooth surface, while the heat coefficients are similar to those normally applied over liquid water surfaces.  相似文献   

15.
根据NCEP/DOE再分析资料的地面感热通量和潜热通量以及MICAPS天气图资料识别的高原低涡资料集,研究了近30年来青藏高原夏季地面热源和高原低涡生成频数的气候学特征,分析了高原地面加热与低涡生成频数的时间相关性及其物理成因.得到如下认知:夏季高原地面感热通量的气候均值为58 W m-2,近30年地面感热总体呈微弱的减小趋势.其中在1980年代初期和21世纪前10年的大部分时段,地面感热呈增大趋势,而中间时段呈波动式下降.地面感热具有准3年为主的周期振荡,1996年前后是其开始减弱的突变点.高原夏季地面潜热通量的气候均值为62 W m-2,近30年呈波动状变化并伴有增大趋势.地面潜热的周期振荡以准4年为主,地面潜热增大的突变始于2004年前后.夏季高原地面热源的气候均值为120 W m-2,其中地面感热与地面潜热对地面热源的贡献在夏季大致相当.地面热源总体呈幅度不大的减弱趋势,其中1980年代到1990年代末偏强,21世纪前6年明显偏弱,随后又转为偏强.地面热源亦呈准3年为主的周期振荡并在1997年前后发生由强转弱的突变.根据MICAPS天气图资料的识别和统计,近30来夏季高原低涡的生成频数整体呈现一定程度的线性减少趋势,低涡高发期主要集中在1980年代到1990年代中后期.低涡生成频数有准7年为主的周期振荡现象,自1990年代中期开始的低涡生成频数的减少态势在1998年前后发生了突变.夏季高原低涡生成频数与同期高原地面感热呈高度正相关,与地面潜热呈一定程度的负相关,但与同期地面热源仍呈较显著的正相关.因此,在气候尺度上,高原地面热源偏强特别是地面感热偏强的时期,对应高原低涡的多发期.本研究从气候统计的时间相关性角度揭示了高原地面加热作用对催生高原低涡乃至高原对流活动的重要性.  相似文献   

16.
Profile and eddy-correlation (heights of 4 and 10 m) measurements performed on the Pasterze glacier (Austria) are used to study the characteristics of the stable boundary layer under conditions of katabatic and large-scale forcing. We consider cases where large-scale forcing results in a downslope (or following) ambient wind. The analysis of averaged spectra and cospectra reveals low frequency perturbations that have a large influence on the variances of temperature and horizontal wind components and also alter the cospectra of momentum and sensible heat flux. Only the spectrum of the vertical wind speed is comparable to universal spectra. The low frequency perturbations occur as brief intermittent events and result in downward entrainment of ambient air thereby producing enhanced downward sensible heat fluxes and downward as well as upward momentum fluxes with various magnitudes and timescales. After the variances were high pass filtered, the normalised standard deviations of wind speed and temperature compare favourably to findings in the literature within the range 0>z/L>0.5. For larger z/L they deviate as a result of an increased influence from low frequency perturbations and thus non-stationarity. In line with this, the turbulent kinetic energy budget (at 4 m height) indicates that production (shear) is in balance with destruction (buoyancy and dissipation) within the range 0>z/L>0.3. Non-dimensional gradients of wind speed within the range 0>z/L>0.3 have a slope of about 3.5. The scatter for the dimensionless temperature gradient is quite large, and the slope is comparable to that for wind speed gradients. For z/L>0.3 the imbalance in the turbulent kinetic energy budget grows and non-dimensional gradients for wind speed and temperature deviate considerably from accepted values as a result of increased non-stationarity. Average roughness lengths for momentum and sensible heat flux derived from wind speed and temperature profiles are respectively 1 × 10-3 m and 6 × 10-5 m, consistent with the literature. The ratio (z0h/z0m) compares to those predicted by surface renewal models. A variation of this ratio with the roughness Reynolds number is not indicated by our data.  相似文献   

17.
Increased heat fluxes near a forest edge   总被引:1,自引:0,他引:1  
Summary ?Observations of sensible and latent heat flux above forest downwind of a forest edge show these fluxes to be larger than the available energy over the forest. The enhancement averages to 56 W m−2, or 16% of the net radiation, at fetches less than 400 m, equivalent to fetch to height ratios less than 15. The enhancement of turbulent energy fluxes is explained by advection and increases with the difference in temperature and humidity of the air over the upwind area as compared to the forest. The relatively high temperature and humidity of the upwind air are not caused by high surface heat fluxes, but are explained by the relatively low aerodynamic roughness of the upwind surface. Although the heat fluxes over forest are enhanced, the momentum fluxes are almost adjusted to the underlying forest. The different behaviour of heat and momentum fluxes is explained by absorption of momentum by pressure gradients near the forest edge. It is concluded that fetch requirements to obtain accurate surface fluxes from atmospheric observations need to be more stringent for scalar fluxes as compared to momentum fluxes. Received November 23, 2001; accepted May 13, 2002  相似文献   

18.
东海黑潮区潜热变化对中国春季降水的影响及其影响过程   总被引:2,自引:0,他引:2  
本文利用美国NCEP/NCAR再分析资料、哈德来(Hadley)中心海温数据、国家气候中心的观测站降水和客观分析海气通量(OAFlux)潜热感热通量资料,研究了1960~2010年春季黑潮区潜热输送对中国春季降水的影响及其影响过程。本文以黑潮流经的中国东部海域及邻近海域为研究对象,该区域是黑潮的主体区域,在文中简称为东海黑潮区。对中国东海以及邻近海域海温与降水的分析表明,在夏季该区域可能以大气强迫海洋为主,而在春冬两季可能主要为海洋强迫大气为主,秋季则可能为不明显的海气相互作用。在春季西北太平洋区域中感热和潜热都对黑潮流经的区域有比较好的敏感性,黑潮流经区域感热和潜热的气候平均值分别约为30 W m-2与120 W m-2;春季的感热通量标准差大值区主要集中在日本以西区域,潜热通量标准差主要集中在中国东海区域与日本东南区域(即东海黑潮区域)。春季潜热EOF第一模态的主要变化就集中在东海黑潮流域。相关分析与合成分析的结果表明,当黑潮潜热指数为正时,华南地区春季降水偏多,长江以北地区偏少,反之亦然。在物理过程分析中,黑潮潜热指数大于0.8时,长江以南的中国大陆有比较强盛的异常北风,使得水汽无法输送到更北的地区,导致在华南地区水汽的积累,并且在海面出现有利于降水的垂直运动异常延伸到大陆上,使华南地区降水增多,而长江以北的东部地区由于水汽输送偏弱,导致水汽积累偏少,从而降水减少。当黑潮指数小于-0.8时,有较强盛的异常南风,有利于水汽输送到北方地区,水汽在华北地区积累,导致长江以北出现降水正异常,而华南地区由于南风偏强,水汽输送加强,导致水汽无法在此区域积累,并且出现不利于降水的垂直运动异常,从而导致降水偏少。  相似文献   

19.
The Summer Surface Energy Balance of the High Antarctic Plateau   总被引:1,自引:0,他引:1  
The summertime surface energy balance (SEB) at Kohnen station, situated on the high Antarctic plateau (75°00′ S, 0°04′ E, 2892m above sea level) is presented for the period of 8 January to 9 February 2002. Shortwave and longwave radiation fluxes were measured directly; the former was corrected for problems associated with the cosine response of the instrument. Sensible and latent heat fluxes were calculated using the bulk method, and eddy-correlation measurements and the modified Bowen ratio method were used to verify these calculated fluxes. The calculated sub-surface heat flux was checked by comparing calculated to measured snow temperatures. Uncertainties in the measurements and energy-balance calculations are discussed. The general meteorological conditions were not extraordinary during the period of the experiment, with a mean 2-m air temperature of −27.5°C, specific humidity of 0.52×10−3kg kg−1 and wind speed of 4.1ms−1. The experiment covered the transition period from Antarctic summer (positive net radiation) to winter (negative net radiation), and as a result the period mean net radiation, sensible heat, latent heat and sub-surface heat fluxes were small with values of −1.1, 0.0, −1.0 and 0.7 Wm−2, respectively. Daily mean net radiation peaked on cloudy days (16 Wm−2) and was negative on clear-sky days (minimum of −19 W m−2). Daily mean sensible heat flux ranged from −8 to +10 Wm−2, latent heat flux from −4 to 0 Wm−2 and sub-surface heat flux from −8 to +7 Wm−2.  相似文献   

20.
利用青藏高原中部聂荣地区草地下垫面2014年7~8月近地层气象要素梯度观测及湍流观测数据,分析讨论了该地区观测期间的基本气象要素特征、能量平衡特征以及能量输送特征,主要结论如下:(1)向下、向上短波辐射和净辐射日变化规律一致,向下、向上长波辐射日变化平缓。反照率呈"U"型分布,早晚大,中午小,聂荣夏季地表平均反照率为0.20。(2)在夏季白天,聂荣地区净辐射大部分以潜热的形式加热大气。考虑了土壤浅层热储存和垂直运动引起的平流输送后,能量闭合率由0.65提高到0.80,闭合率有显著的提高。(3)在不稳定层结下,动量总体输送系数CD平均值为4.7×10~(-3)和热量总体输送系数CH平均值为3.5×10~(-3);在稳定层结下,CD平均值为3.4×10~(-3),CH平均值为1.8×10~(-3);C_D和C_H在近中性层结下的平均值分别为4.30×10~(-3)和2.39 10~(-3)。  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