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1.
本根据“实验3号”科学考察船在TOGA-COARE(1992年11月-1993年2月)定点(2°15'S,158°00'E)连续观测的大气,海洋资料,利用考虑风速和大气层结影响的整体输送动力学公式,计算给出了在西太平洋热带海域强对流天气过程中动量、感热和潜热等湍流通量垂直交换和水平输送的一些特性,并与该海域其它天气过程湍流通量交换和输送的特性作了比较,此外,中还讨论了更接近实际的曳力系数,感热  相似文献   

2.
马柱国  姚兰昌 《高原气象》1996,15(2):186-194
该利用TOGA-COARE强化观测期(IOP)所获得的辐射观测资料(1992年11月10日-1993年2月18日),对考察点(2°15′S,158°00′)的辐射分量进行了分析,其中包括总辐射、直接辐射、散射辐射、海表长波辐射、大气逆辐射、海表反射辐射春反照率、净辐射及有效辐射。  相似文献   

3.
西太平洋暖池区的海气通量及整体交换系数   总被引:3,自引:1,他引:2  
根据西太平洋海域弱风、高温、潮湿的大气状态特征,提出了在光滑面存在粘性副层气流中的廓线的层结订正方案。用此模式对西太平洋暖池区TOGACOAREIOP期间,在向阳红5号船(2°S,154°E)获取的海面风、温、湿梯度资料进行了处理。计算结果显示西太平洋暖池区贴水层气流中不稳定层结占50%-80%,其中很不稳定的占10.3%;该海区海气通量和整体交换系数受层结影响远大于受风速的影响;海气通量和整体交换系数随不稳定程度增加而增大,在相同风速下量值可相差4倍以上;其变化范围为0.3×10-3—3.2×10-3。由此可见,层结的影响使它们的变化大于其它海区的结果。在u10=0-10m/s范围内,中性化整体交换系数平均为CDN=1.2×10-3,CHN=1.14×10-3,CEN=1.19×10-3,与Large和Pond(1981,1982)不稳定条件的研究结果相差无几。  相似文献   

4.
热带西太平洋海面通量与气象要素关系的诊断分析   总被引:4,自引:1,他引:3  
用TOGACOARE加强期在赤道带西太平洋暖池中的观测船MoanaWave和浮标获得的小时风、温、湿、海温资料计算了海面各种通量。分析潜热通量随海面温度SST的变化特征,发现小风期潜热通量LH在某SST处出现最大值,大风时不出现此现象,即LH随SST变化的主要原因是风随SST的变化,其次是气海湿度差Δq及传输系数CE随SST的变化。用相关分析法分析小风期、西风爆发期、对流扰动期等不同时期中各通量与各气象要素的关系发现,潜热通量和动量通量主要决定于风,对感热通量起作用的主要是气海温差,降水也可通过气海温差和风影响感热通量。  相似文献   

5.
该文利用TOGA-COARE强化观测期(IOP)所获得的辐射观测资料(1992年11月10日—1993年2月18日),对考察点(2°15′S,158°00′E)的辐射分量进行了分析,其中包括总辐射、直接辐射、散射辐射、海表长波辐射、大气逆辐射、海表反射辐射及其反照率、净辐射及有效辐射。结果表明:和其它地区(如高原)比较,观测点的总辐射、直接辐射均很强;反射率小,晴天平均为0.04—0.05,阴天为0.06—0.08;海表长波辐射大而日变化小,大气逆辐射强而日变化大;有效辐射小而净辐射大。  相似文献   

6.
利用1993年ENSO事件(4月)爆发前酝酿阶段,TOGA/COARE关键区强化期(1992年11月-1993年2月)立体观测实验“向阳红五号”科学考察船定点(155°E,2°S)高空大气探测资料,分析了西太平洋暖海域上空对流上升区西侧风的垂直变化,指出:对流层上、下部各有一强风带,随着海-气ENSO异常的发展,高空强东风带和低空强西风带均呈增强趋势,最强时分别连续14天和18天达到急流标准,占相  相似文献   

7.
南沙海域大气湍流通量输送特征分析   总被引:23,自引:1,他引:23  
利用1994年9月在南沙群岛的渚碧礁(10°52′N,114°04′E)观测的湍流资料,采用涡旋相关法计算,给出了南沙海域的曳力系数,动量通量,感热通量和潜热通量,并与其它海气相互作用实验及HEIFE的结果作了比较,结果表明,该海域的曳力系数CD=(1.54±0.24)×10^-3。大气向海洋输送动量通量与水平风速挟方成正比,该海区无论白在还是晚上都是将其贮存的热量以潜热或感热的形式输送到大气中。  相似文献   

8.
TEMPERATURE-MEASURINGRADIO-ACOUSTICSOUNDINGSYSTEM(RASS)¥LiJianguo(李建国),WangPing(王坪)andMengZhaolin(孟昭林)TEMPERATURE-MEASURINGRA...  相似文献   

9.
CHINAGLOBALATMOSPHEREWATCHBASELINEOBSERVATORYANDITSMEASUREMENTPROGRAMTangJie(汤洁),WenYupu(温玉璞),XuXiaobin(徐晓斌),ZhengXiangdong(郑...  相似文献   

10.
STUDYONSOMEMETEOROLOGICALPROBLEMSINHHGAGRICULTURALPRODUCTION¥GaoSuhua(高素华),GuoJianping(郭建平).AnShunqing(安顺清)andWangShili(王石立)S...  相似文献   

11.
With the marine ship observation data set obtained by three cruise-phases of Chinese Xi-angyanghong 5 from November 5,1992 to February 19,1993 in the TOGA-COARE IOP at 2°S,156°E.the sea surface fluxes at this point are estimated by three different bulk schemes.Firstly.aquasi-linear relation is found between the neutral drag coefficients and wind speed.Then,the sta-bility-dependent drag and heat transfer coefficients are solved in the iterative method.Based onthus-derived transfer coefficients,the momentum,sensible and latent heat fluxes are calculated.In the warm pool region,the fluxes corresponding to the westeily winds are much greater thanthose of the easterly trade winds.The magnitude of sea surface fluxes depends upon the atmo-spheric stability as well,in particular in the case of weak wind condition.The estimated sea sur-face net heat budget shows that considerable amount of heat transport from ocean to atmosphere ismainly produced by the effective longwave radiation,latent and sensible heat fluxes.Among themthe value of latent heat flux is the largest and the sensible heat flux is the smallest.Finally,an ac-curacy analysis is made by direct measurements with the eddy-correlation method on the JapaneseR/V Hakuho board at the same time.It is shown that the bulk-derived fluxes are acceptable withmuch confidence.The estimated effective longwave radiation is used to compare with those by di-rect observations on Xiangyanghong 5.This research is compared with TOGA investigation in thetropical western Pacific.  相似文献   

12.
Through the use of the hourly wind, air temperature and humidity, sea surface temperature data measured on board the observing vessel Moana Wave and buoy in the warm pool of western Pacific during the IOP of TOGA COARE, we compute the fluxes over sea surface and analyze the characteristics of the variation ofthe latent heat flux with sea surface temperature. During weak rather than strong wind periods a maximum valueof latent heat flux appears at some points of SST, which is caused mainly by the variations of wind, then by the humidity difference between air and sea and the transfer coefficient with SAT. Using correlation analysis. we also analyze the relationship between the fluxes and meteorological elements during weak wind periods. wester lywind burst periods, and convective disturbed periods etc. The main conclusions are that the latent heat flux ismainly determined by wind, sensible heat flux by the potential temperature difference between air and sea and the momentum flux by wind. The precipitation affects the sensible heat flux through the potential temperature difference and wind.  相似文献   

13.
Aircraft turbulence data from the Autonomous Ocean Sampling Network project were analyzed and compared to the Coupled Ocean–Atmosphere Response Experiment (COARE) bulk parametrization of turbulent fluxes in an ocean area near the coast of California characterized by complex atmospheric flow. Turbulent fluxes measured at about 35 m above the sea surface using the eddy-correlation method were lower than bulk estimates under unstable and stable atmospheric stratification for all but light winds. Neutral turbulent transfer coefficients were used in this comparison because they remove the effects of mean atmospheric conditions and atmospheric stability. Spectral analysis suggested that kilometre-scale longitudinal rolls affect significantly turbulence measurements even near the sea surface, depending on sampling direction. Cross-wind sampling tended to capture all the available turbulent energy. Vertical soundings showed low boundary-layer depths and high flux divergence near the sea surface in the case of sensible heat flux but minimal flux divergence for the momentum flux. Cross-wind sampling and flux divergence were found to explain most of the observed discrepancies between the measured and bulk flux estimates. At low wind speeds the drag coefficient determined with eddy correlation and an inertial dissipation method after corrections were applied still showed high values compared to bulk estimates. This discrepancy correlated with the dominance of sea swell, which was a usually observed condition under low wind speeds. Under stable atmospheric conditions measured sensible heat fluxes, which usually have low values over the ocean, were possibly affected by measurement errors and deviated significantly from bulk estimates.  相似文献   

14.
本文用热平衡方法估算了1984年夏季张掖地区的平均感热、潜热输送以及对热量和水份的滞凝系数,对该地的平均热状况特征进行了研究,在张掖地区,感热通量及热量滞凝系数随高度增加,而潜热通量及水份滞凝系数则减小;热力参数与辐射参数一样,也存在着3—5天的中期振荡周期,热力参数及辐射参数相应振荡的位相差都很小,而谱相关则大多在50%以上。可以用辐射参数的平均值来估计近地面层感热和潜热输送的平均状况。张掖地区的热状况平均特征基本上与1979年QXPMEX结果一致。  相似文献   

15.
Turbulent surface heat fluxes (latent and sensible heat) are the two most important parameters through which air–sea interaction takes place at the ocean–atmosphere interface. These fluxes over the global ocean are required to drive ocean models and to validate coupled ocean–atmosphere global models. But because of inadequate in situ observations these are the least understood parameters over the tropical Indian Ocean. Surface heat fluxes also contribute to the oceanic heat budget and control the sea surface temperature in conjunction with upper ocean stratification and ocean currents. The most widely used flux products in diagnostic studies and forcing of ocean general circulation models are the ones provided by the National Centres for Environment Prediction (NCEP) reanalysis. In this study we have compared NCEP reanalysed marine meteorological parameters, which are used for turbulent heat fluxes, with the moored buoy observation in the south-eastern Arabian Sea. The NCEP latent heat flux (LHF) and sensible heat flux (SHF) derived from bulk aerodynamic formula are also compared with that of ship and buoy derived LHF and SHF. The analysis is being carried out during the pre-monsoon and monsoon season of 2005. The analysis shows that NCEP latent as well as sensible heat fluxes are largely underestimated during the monsoon season, however, it is reasonably comparable during the pre-monsoon period. This is largely due to the underestimation of NCEP reanalysis air temperature (AT), wind speed (WS) and relative humidity (RH) compared to buoy observations. The mean differences between buoy and NCEP parameters during the monsoon (pre-monsoon) period are ~21% (~14%) for WS, ~6% (~3%) for RH, and ~0.75% (0.9%) for AT, respectively. The sudden drop in AT during rain events could not be captured by the NCEP data and, hence, large underestimations in SHF. During the pre-monsoon period, major contribution to LHF variations comes from WS, however, both surface winds and relative humidity controls the LHF variations during the monsoon. LHF is mainly determined by WS and RH during the monsoon and, WS is the main contributor during the pre-monsoon.  相似文献   

16.
The role of a river of small dimensions in driving the surface exchange of sensible and latent heat fluxes at the bottom of a valley is investigated using large-eddy simulation (LES). Simulations were performed using different valley topographies, river widths and large-scale wind speed and direction. In all cases, the river acted as a sink of both sensible and latent heat during daytime. Despite the general agreement concerning the flux direction above the river surface, specific differences exist between the simulations. The topography enhances the wind divergence caused by the river, and the larger negative surface fluxes above the river occur when there are no slopes, a consequence of larger wind speeds above the river. For large-scale winds aligned with the valley axis, the surface fluxes depend on the large-scale wind speed, but this dependence is reduced if the large-scale wind is perpendicular to the valley axis. There is a minimum of temperature and a maximum of specific humidity above the river surface. The scalar budgets show that sensible heat flux converges above the river, being balanced by the warm air subsidence at the centre of the valley. Latent heat fluxes, on the other hand, converge above the river surface, and they are balanced by the horizontal advection of humidity towards the river margins.  相似文献   

17.
1998年南海季风试验期间海 气通量的估算   总被引:2,自引:0,他引:2       下载免费PDF全文
根据1998年南海季风试验西沙海面铁塔梯度观测资料,利用总体(Bulk)系数法和多层结通量廓线法对西沙海面的海-气通量进行了估算,得出两种方法估算的潜热通量、感热通量基本一致。总体系数法估算的潜热通量比多层结通量廓线法略大1~3 W·m-2,感热通量小0~1.5 W·m-2。一般而言,季风爆发期间潜热输送逐渐增加;季风爆发前期夜间潜热通量比季风爆发后期大;季风爆发后期,白天潜热通量明显大于爆发初期和中期。感热通量季风爆发前海面向大气输送,爆发后期大气向海面输送。动量通量和摩擦速度随风速增加。  相似文献   

18.
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   

19.
Abstract

This study reports on tower measurements from the intertidal zone taken during the ice‐free period between August 1 and September 20, 1985. Sea and air temperatures showed ranges of 8 and 14°C, respectively, and both were colder during onshore than during offshore winds. Onshore winds were associated with a nearly saturated atmosphere whereas offshore ones were quite dry. Surface albedo was twice as great for low tide as for high tide. The ratio net/solar radiation was 13% less at low tide owing to both the larger albedo and the stronger long‐wave radiation loss. Heat fluxes into the bottom sediments were small with net gains in August and net losses in September. During the day, heat storage in the water was large and positive. This occurred even with the tide out, when the ponded water continued to warm. At night the water gave up heat, both for low and high tide, and especially late in the season. The latent heat flux was always positive and was largest by day during low tide and by night during high tide. The sensible heat flux was positive for onshore winds and often negative for offshore winds. Under all wind directions heat storage constituted 60% of net radiation, the latent heat flux 35% and the remainder was proportioned equally between the sensible heat flux and the flux into the bottom sediments.  相似文献   

20.
热带太平洋-印度洋海温异常综合模的数值模拟   总被引:1,自引:0,他引:1  
通过数值模拟及结果的合成分析,对热带太平洋-印度洋异常海温综合模态的三维热力结构、动力结构及其发生发展的可能机制进行了研究.数值模拟结果的分析表明,太平洋、印度洋海温异常的综合模态在表层、次表层的表现都很明显,即在赤道西印度洋、中东太平洋的海温偏高(低)时,赤道西太平洋、东印度洋的海温偏低(高),该模态还存在着显著的年变化特征、年际变化特征以及年代际变化特征.数值模拟的合成分析结果表明,异常的海表风应力引起表层洋流异常,表层洋流异常及由其引起的海表高度异常可导致次表层海水环流的异常,海洋环流异常导致的平流热输送异常是海温形成异常综合模态的主要原因之一,垂直输送是形成次表层海温综合模态的主要原因.平流热输送过程对海表温度变异的贡献是:在事件发生到盛期阶段促进了次表层海温异常综合模态的形成,在盛期到消亡阶段次表层的平流过程阻碍其进一步发展;短波辐射是海洋的主要热力来源,海表面异常的净短波辐射通量、潜热通量是表层海温形成异常模态的主要热力学原因,异常的海表面净短波辐射通量、潜热通量、感热通量在到达盛期阶段后抑制其进一步发展.  相似文献   

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