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 A model of the large-scale interaction between the troposphere and the upper ocean, wind-driven circulation is formulated. Simplified parametrizations, built upon the conservation of global heat and momentum, relate the atmospheric eddy heat and momentum fluxes to the zonally averaged oceanic and atmospheric temperatures. The formulation shows that the wind-driven circulation influences the winds by controlling the strength of the oceanic northward heat transport, and thus the atmospheric northward heat transport and temperature distribution. Because the ocean takes decades to adjust to changes in the winds, the coupled system equilibrates into a state which is periodic in time, rather than steady. The period is linearly proportional to the transit time of long Rossby waves across the basin, and thus is of the order of decades for large-scale basins. Received: 15 December 1998 / Accepted: 29 October 1999  相似文献   

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Summary During the pre-onset regime of MONEX-79, the short period (1–2 weeks) time series measurements of surface meteorological elements, vertical profiles of temperature (BT) and salinity (Nansen casts) made from 5 former USSR and 2 Indian research vessels were utilised to investigate the observed near-surface heating rates at a few selected locations in the Arabian Sea. The influence of local surface heat fluxes on the upper ocean heat content variability is explored. The associated synoptic scale variability in the thermohaline structure of the upper layers is presented. The efficacy of a simple Kraus-Turner type one dimensional numerical model in simulating the observed variability of mixed layer heating rates is evaluated.With 7 Figures  相似文献   

6.
Summary The dominant surface energy budget parameters, namely the net radiation fluxes, must be precisely known for an understanding of southwest monsoon behaviour and the early stages of formation of a meteorological system, i.e. trough, low pressure, depression, cyclone etc., and break monsoon conditions over the Bay of Bengal region. The data measured during the MONEX-79 period from July 16–31 are used in order to study the fluctuations of energy fluxes and the net radiation in the month of July over the region. During this period the total energy flux is increasing from South to North with a maximum over the head of the Bay. However, the fluctuation of net radiation is not significant. There is an outstanding increase in the energy flux with anomalies of values 240 W/m2.
Zusammenfassung Für das Verständnis des Südwestmonsuns und für die Entwicklung eines meteorologischen Systems, wie Trog-Tiefdruck-Depression-Zyklone etc., sowie für die Bedingungen des Monsunendes über der Bengalischen Bucht, ist das genaue Wissen um die wichtigen Parameter der Energiebilanz an der Oberfläche, insbesondere der Strahlungsbilanz und der anderen Energieflüsse, unverzichtbar. Die Beobachtungsdaten vom 16.–31. Juli während MONEX-79 werden zum Studium der Energieflußfluktuationen und der Strahlungsbilanz für Juli in diesem Gebiet herangezogen. In dieser Periode nahm die Energieflußsumme nach Norden zu, mit einem Maximum über dem nördlichsten Teil der Bucht, während die Fluktuation der Strahlungsbilanz unbedeutend blieb. Trotzdem zeigt sich eine bedeutende Erhöhung des Energieflusses von bis zu 240 W/m2.


With 2 Figures  相似文献   

7.
The global heat balance: heat transports in the atmosphere and ocean   总被引:10,自引:0,他引:10  
The heat budget has been computed locally over the entire globe for each month of 1988 using compatible top-of-the-atmosphere radiation from the Earth Radiation Budget Experiment combined with European Centre for Medium Range Weather Forecasts atmospheric data. The effective heat sources and sinks (diabatic heating) and effective moisture sources and sinks for the atmosphere are computed and combined to produce overall estimates of the atmospheric energy divergence and the net flux through the Earth's surface. On an annual mean basis, this is directly related to the divergence of the ocean heat transport, and new computations of the ocean heat transport are made for the ocean basins. Results are presented for January and July, and the annual mean for 1988, along with a comprehensive discussion of errors. While the current results are believed to be the best available at present, there are substantial shortcomings remaining in the estimates of the atmospheric heat and moisture budgets. The issues, which are also present in all previous studies, arise from the diurnal cycle, problems with atmospheric divergence, vertical resolution, spurious mass imbalances, initialized versus uninitialized atmospheric analyses, and postprocessing to produce the atmospheric archive on pressure surfaces. Over land, additional problems arise from the complex surface topography, so that computed surface fluxes are more reliable over the oceans. The use of zonal means to compute ocean transports is shown to produce misleading results because a considerable part of the implied ocean transports is through the land. The need to compute the heat budget locally is demonstrated and results indicate lower ocean transports than in previous residual calculations which are therefore more compatible with direct ocean estimates. A Poisson equation is solved with appropriate boundary conditions of zero normal heat flux through the continental boundaries to obtain the ocean heat transport. Because of the poor observational data base, adjustments to the surface fluxes are necessary over the southern oceans. Error bars are estimated based on the large-scale spurious residuals over land of 30 W m–2 over 1000 km scales (1012 m2). In the Atlantic Ocean, a northward transport emerges at all latitudes with peak values of 1.1±0.2 PW (1 standard error) at 20 to 30°N. Comparable values are achieved in the Pacific at 20°N, so that the total is 2.1±0.3 PW. The peak southward transport is at 15 to 20°S of 1.9±0.3 PW made up of strong components from both the Pacific and Indian Oceans and with a heat flux from the Pacific into the Indian Ocean in the Indonesian throughflow. The pattern of poleward heat fluxes is suggestive of a strong role for Ekman transports in the tropical regions.  相似文献   

8.
Summary One method of computing the seasonal heat budget of the atmosphere involves the seasonal heat storage in the oceans. On the basis of bathythermograph data and ocean surface temperatures, the heat added to, or released by the ocean was computed month by month. The heat stored in the ocean was then compared withGabites' estimate of the heat added by radiation and by means of the latent heat of water vapor. From this comparison, the heating of the atmosphere was approximated. In middle latitudes, the net heating of the atmosphere is close to zero during most of the year, so that even the sign of the atmospheric heating is in doubt there. During most of the year, the atmosphere undergoes net heating in low latitudes, and net cooling in high latitudes. The excess is removed by motions of the atmosphere and the ocean.
Zusammenfassung Eine Methode, das jahreszeitliche Wärmebudget der Atmosphäre zu berechnen, hat auch der Wärmespericherung in den Ozeanen Rechnung zu tragen. Auf Grund von Wasserthermographenwerten und Ozeanoberflächentemperaturen wurden die dem Ozean zugeführten oder von ihm abgegebenen Wärmemengen monatsweise berechnet. Die im Ozean gespeicherte Wärme wurde dann mit der vonGabites aufgestellten Schätzung der durch Strahlung und durch die latente Wärme des Wasserdampfs zugeführten Wärmeenge verglichen und von dieser Vergleichung wurde auf die Erwärmung der Atmosphäre geschlossen. In mittleren Breiten liegt der Erwärmungszuwachs der Atmosphäre während des Großteils des Jahres bei Null, so daß sogar das Vorzeichen der Erwärmung zweifelhaft ist. Während des Großteils des Jahres erfährt die Atmosphäre dagegen in niederen Breiten einen Wärmezuwachs, in hohen Breiten einen Überschuß an Abkühlung. Diese Überschüsse werden durch Bewegungsvorgänge in der Atmosphäre und im Ozean verfrachtet.

Résumé Une méthode visant à calcular le bilan thermique annuel de l'atmosphère doit tenir compte de la chaleur mise en réserve dans les mers. Des mesures de température de l'eau de mer en profondeur et en surface permettent d'établir les quantités de chaleur fournies mensuellement à la mer ou enlevée à celle-ci. La chaleur accumulée fut alors comparée à celle qu'estimeGabites en considérant la chaleur fournie par rayonnement et par la chaleur latente de la vapeur d'eau; on en a tiré une conclusion relative au réchauffement de l'atmosphère. Aux latitudes moyennes, l'accroissement de chaleur de cette dernière est voisine de zéro la plus grande partie de l'année, de sorte que même le signe est douteux. Aux latitudes basses par contre l'atmosphère reçoit de la chaleur pendant la plus grande partie de l'année; elle en perd aux latitudes élevées. Ces gains et ces pertes s'équilibrent in globo par les mouvements de l'air et de l'eau.


With 4 Figures

Presented at the 11th General Assembly, IUGG (IAM), Toronto, Septemer 1957.

Dedicated to Dr.Anders K. Ångström on the occasion of his 70th birthday.  相似文献   

9.
Turbulent fluctuations of wind and temperature were measured using a three-component sonic anemometer at 8 m on a 30 m micro-meteorological tower erected at the Indian Institute of Technology (IIT) Kharagpur (22.3° N, 87.2° E), India, as part of the Monsoon Trough Boundary Layer Experiment (MONTBLEX). Diurnal and nocturnal variations of fluxes of sensible heat and momentum were estimated by the eddy correlation technique from 42 observations, each of 10 min duration during 6–8 July in the monsoon season of 1989. The estimated heat flux shows a diurnal trend while the momentum flux shows variability but no particular trend. The nocturnal heat flux changes sign intermittently.Fluctuations of vertical wind velocity wand temperature when normalised with the respective scaling parameters u *and * are found to scale with Z/L in accordance with the Monin-Obukhov similarity hypothesis: % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqOXdy2aaS% baaSqaaiaadEhaaeqaaOGaamiEaiaacIcacaWGAbGaai4laiaadYea% caGGPaWaaWbaaSqabeaacaaIXaGaai4laiaaiodaaaaaaa!3FE8!\[\phi _w x(Z/L)^{1/3} \], % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqOXdy2aaS% baaSqaaiabeI7aXbqabaGccaWG4bGaaiikaiaadQfacaGGVaGaamit% aiaacMcadaahaaWcbeqaaiaaigdacaGGVaGaaG4maaaaaaa!40A2!\[\phi _\theta x(Z/L)^{1/3} \] during unstable conditions and % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqOXdy2aaS% baaSqaaiaadEhaaeqaaOGaamiEaiaacIcacaWGAbGaai4laiaadYea% caGGPaaaaa!3D90!\[\phi _w x(Z/L)\], % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqOXdy2aaS% baaSqaaiabeI7aXbqabaGccaWG4bGaaiikaiaadQfacaGGVaGaamit% aiaacMcadaahaaWcbeqaaiabgkHiTiaaigdaaaaaaa!401F!\[\phi _\theta x(Z/L)^{ - 1} \] during stable conditions. Correlation coefficients for heat and momentum flux % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4SdC2aaS% baaSqaaiaadEhacqaH4oqCaeqaaaaa!3A71!\[\gamma _{w\theta } \] and uwshow stability dependence. For unstable conditions, % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4SdC2aaS% baaSqaaiaadEhacqaH4oqCaeqaaaaa!3A71!\[\gamma _{w\theta } \] increases with increasing ¦Z/L¦ whereas uwdecreases. During stable conditions, % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4SdC2aaS% baaSqaaiaadEhacqaH4oqCaeqaaaaa!3A71!\[\gamma _{w\theta } \] decreases with increasing Z/L while uwdecreases very slowly from a value -0.36 to -0.37.  相似文献   

10.
Summary This study addresses the relationship between the Indian summer monsoon (ISM) and the coupled atmosphere/ocean system in the tropical Pacific on the interannual time scales. High positive correlations are found between ISM rainfall and both mixed layer sea water temperature (SWT) and sea surface temperature (SST) anomalies of the tropical western Pacific in the following winter. Negative correlations between ISM rainfall and SST in the central/eastern Pacific also appear to be most significant in the following winter. These parameters are correlated with each other mainly on a biennial time scale. Lag-correlations between the zonal wind and SST along the the equatorial Pacific show that the westerly (easterly) surface wind stress anomalies over the central/western Pacific are greatly responsible for the formation of negative (positive) SST/SWT anomalies in the western Pacific and positive (negative) SST/SWT anomalies in the central/eastern Pacific. Furthermore, it is evidenced that these lagcorrelations are physically based on the anomalies in the large-scale convection over the Asian monsoon region and the associated east-west circulation over the tropical Pacific, which first appear during the Indian summer monsoon season and evolve during the following autumn and winter. These results strongly suggest that the Asian summer monsoon may have an active, rather than a passive, role on the interannual variability, including the ENSO events, of the coupled atmosphere/ocean system over the tropical Pacific.With 9 Figures  相似文献   

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Results from nine coupled ocean-atmosphere simulations have been used to investigate changes in the relationship between the variability of monsoon precipitation over western Africa and tropical sea surface temperatures (SSTs) between the mid-Holocene and the present day. Although the influence of tropical SSTs on the African monsoon is generally overestimated in the control simulations, the models reproduce aspects of the observed modes of variability. Thus, most models reproduce the observed negative correlation between western Sahelian precipitation and SST anomalies in the eastern tropical Pacific, and many of them capture the positive correlation between SST anomalies in the eastern tropical Atlantic and precipitation over the Guinea coastal region. Although the response of individual model to the change in orbital forcing between 6 ka and present differs somewhat, eight of the models show that the strength of the teleconnection between SSTs in the eastern tropical Pacific and Sahelian precipitation is weaker in the mid-Holocene. Some of the models imply that this weakening was associated with a shift towards longer time periods (from 3–5 years in the control simulations toward 4–10 years in the mid-Holocene simulations). The simulated reduction in the teleconnection between eastern tropical Pacific SSTs and Sahelian precipitation appears to be primarily related to a reduction in the atmospheric circulation bridge between the Pacific and West Africa but, depending on the model, other mechanisms such as increased importance of other modes of tropical ocean variability or increased local recycling of monsoonal precipitation can also play a role.  相似文献   

13.
Summary Based on observed rainfall data of India Meteorological Department (IMD), correlation coefficients (CCs) have been computed between Indian summer monsoon rainfall (ISMR) and sea surface temperature (SST) anomalies over different Nino regions and standardised pressure difference between Tahiti and Darwin. Significant positive CCs are found between the Southern Oscillation Index (SOI) in winter and subsequent June rainfall over India. Concurrent with and subsequent to Indian summer monsoon, SOI shows significant positive CC with the mean rainfall of July to September (JAS). Significant negative CCs are found between JAS mean rain and the concurrent and following SST anomalies over Nino-3.4 region. On the basis of these correlations, it is proposed that the entire period of summer monsoon from June to September could be divided into two sub-periods such as: early summer (June) and mid-late summer (July to September) monsoon for prediction of ISMR in the extended range.In order to examine the characteristics of atmospheric circulation during some El-Nino years, divergent flow at 200hPa and omega field at 500hPa based on NCEP/NCAR reanalysis have been studied in detail. Major significant southward shift of upper level divergent field from India are related to El-Nino and this shift may be responsible for causing droughts during several El-Nino years over India. Also vertical wind fields at 500hPa show sinking motion over large parts of India and west Pacific and ascending motion over southern Indian Ocean, central and eastern Pacific during major drought years.  相似文献   

14.
Studies of climate change 6,000 years before present using atmospheric general circulation models (AGCMs) suggest the enhancement and northward shift of the summer Asian and African monsoons in the Northern Hemisphere. Although enhancement of the African monsoonal precipitation by ocean coupling is a common and robust feature, contradictions exist between analyses of the role of the ocean in the strength of the Asian monsoon. We investigated the role of the ocean in the Asian monsoon and sought to clarify which oceanic mechanisms played an important role using three ocean coupling schemes: MIROC, an atmosphere–ocean coupled general circulation model [C]; an AGCM extracted from MIROC coupled with a mixed-layer ocean model [M]; and the same AGCM, but with prescribed sea surface temperatures [A]. The effect of “ocean dynamics” is quantified through differences between experiments [C] and [M]. The effect of “ocean thermodynamics” is quantified through differences between experiments [M] and [A]. The precipitation change for the African and Asian monsoon area suggested that the ocean thermodynamics played an important role. In particular, the enhancement of the Asian monsoonal precipitation was most vigorous in the AGCM simulations, but mitigated in early summer in ocean coupled cases, which were not significantly different from each other. The ocean feedbacks were not significant for the precipitation change in late summer. On the other hand, in Africa, ocean thermodynamics contributed to the further enhancement of the precipitation from spring to autumn, and the ocean dynamics had a modest impact in enhancing precipitation in late summer.  相似文献   

15.
利用1979—2012年日本气象厅次表层海温资料和NCEP/NCAR再分析资料,分析了前期冬季热带太平洋次表层海温与东亚夏季风的关系,并讨论了其可能机制。结果表明,前期冬季热带太平洋次表层海温与后期东亚夏季风强弱有显著的相关关系。冬季次表层海温呈现东正西负的类El Nio分布型时,夏季副热带高压偏强,西北太平洋地区受反气旋型环流控制,能将大量的水汽输送到长江和淮河流域,有利于水汽在该区域辐合,为夏季降水偏多创造了条件,此时东亚夏季风活动整体偏弱,反之亦然。但类El Nio分布型对东亚夏季气候变化的影响较类La Nia分布型更显著。此外,冬季热带太平洋次表层海温可能通过其自身能够持续性地影响东亚—太平洋地区的大气环流异常,次表层海温随季节变化有明显的发展和移动趋势:冬季西太平洋暖池次表层冷(暖)海温不断堆积,沿温跃层向东传播使得中东太平洋次表层海温逐渐变冷(暖),冷(暖)海温上翻加强使得海表温度异常,进一步影响到西太平洋副热带高压的位置和强度,并在东亚地区形成经向遥相关波列,通过西北太平洋地区异常反气旋(气旋)环流的作用,影响东亚地区大气环流以及气候变化。  相似文献   

16.
Data collected during the Indo-Soviet Monsoon-77 expedition are used to determine quadratic expressions for the universal constants A and B, as functions of the stability parameter, . A quadratic expression has also been obtained for u *, in terms of the surface wind u s. It is shown, from the mean values of q and E , that the entire area covered by the expedition could be divided into four regions around the point 13° N, 78° E. The mean thermal characteristic of each region differs. It is shown that the northeastern quadrant is most favourable for the sustenance of a tropical storm once it has formed.  相似文献   

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Theoretical and Applied Climatology - In this study, factors responsible for the deficit Indian Summer Monsoon (ISM) rainfall in 2014 and 2015 and the ability of Indian Institute of Tropical...  相似文献   

19.
Aerological observations carried out on board ORV Sagarkanya at a stationary location (20° N, 89° E) over the Head Bay of Bengal during August 18–21, 1990 were analysed to study the thermodynamic structure of the marine boundary layer in relation to a monsoon depression which formedin situ with its centre at 20° N, 88° E. The q(mixing ratio) reversal observed at 850 hPa prior to formation of the low pressure area shifted to a higher level (h<700 hPa) with the formtion of the low. Positive buoyancy below 850 hPa prior to the formation of the low indicated conditions favourable for deep convection. When the low pressure area intensified into a depression, negative buoyancy was observed at lower levels.  相似文献   

20.
Summary Recent investigations have shown that the poleward flux of angular momentum across latitutde 30° N can be regarded essentially as an edey flux due to macroturbulence. Since the principal source region of atmospheric angular momentum is the frictional layer in the trade-wind zone it is necessary to have a mechanism which explains the transport of the angular momentum up to the upper troposphere and the tropopause level and into the planetary jet stream aroundlatitude 30° N. In the present paper it is shown that this transport can easily be explained by assuming the existence of a mean meridional circulation between the Equator and latitude 30°N. The mass transport in this meridional circulation cell can be computed from the empirical data for the poleward eddy flux of angular momentum presented byY. Mintz. The same data can then also be used to estimte the excess of precipitation over evaporation in the equatorial zone of the ascending branch of the circulation.
Zusammenfassung Neuere Untersuchungen haben gezeigt, daß der Polwärtstransport des Rotationsimpulses über Breite 30° N hinaus im wesentlichen als Austauschströmung durch Makroturbulenz aufgefaßt werden kann. Da dase Hauptquellgebieet des atmosphärischen Rotationsimpulses die Reibungs-schicht der Passatzone ist, ist es notwendig, einen Mechanismus zu finden, der die Verlagerung des Rotationsimpulses bis in die obere Troposphäre und das Tropenpasausenniveau und in den planetarischen jet stream rund um den Brietenkreis 30° N erklärt. In der vorliegenden Arbiet wird gezeigt, daß diese Verlagerung durch die Annahme ener mittleren Meridionalzirkulation zwischen dem Äquator und 30° N leicht erklärt werden kann. Der Massentransport in dieser Meridionalzirkulationszelle kann aus den Empirischen Daten berechnet werden, dieY. Mintz für den turbulenten Polwärtstransport des Rotationsimpulses angegeben hat. Dieselben Werten können auch benützt werden, um den überschuß des Niederschlags über die Verdungstung in der Äquatorialzone des aufsteigenden Zirkulationszweiges zu berechnen.

Résumé De récentes recherches ont montré que le flux du moment cinétique dirigé vers le pôle à travers la région de 30° lat. N peut être considéré comme étant essentiellement unflux dû à la macroturbulence. Etant donné que la source principale du moment cinétique atmosphérique est située dans la couche de friction dans la zone des vents alizés, il est nécessaire de trouver un mécanisme qui expliquerait le transport du moment cinétique vers la haute troposphère et le niveau de la tropopause ainsi que dans le jet stream planétaire autour du 30ème degré de latitude nord. Dans l'article suivant l'auteur montre comment il est possible d'expliquer facilement ce transport en admettant l'existence d'une circulation méridienne moyenne entre l'équateur et 30° lat. N. Le transport de masse dans cette cellule de circulation méridienne peut être calculé à partir des données empiriques indiquées parY. Mintz concernant le flux du moment cinétique dû à la turbulence et dirigé vers de pôle. Les mêmes données peuvent aussi être employées pour estimer l'excès des précipitations sur l'évaporation dans la zone équatoriale de la branche ascendante de la circulation.
  相似文献   

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