3 research outputs found
Copernicus Ocean State Report, issue 6
The 6th issue of the Copernicus OSR incorporates a large range of topics for the blue, white and green ocean for all European regional seas, and the global ocean over 1993â2020 with a special focus on 2020
Calculation of the vertical net energy flux using an energy budget equation for the land surface
In dieser Arbeit wird auf unterschiedliche Berechnungsmethoden fĂŒr den vertikalenNettoenergiefluss durch die ErdoberflĂ€che eingegangen. DafĂŒr werden drei unterschiedliche Methoden verwendet, zum einen die direkte Berechnung aus der Nettostrahlung und den turbulenten FlĂŒssen wie man sie in Reanalysen wie ERA5 herunterladen kann. Eine weitere Berechnungsmöglichkeit stellt die Berechnung ĂŒber eine atmosphĂ€rische SĂ€ule dar. Die dritte Methode ist eine diagnostische Auswertung einer Gleichung fĂŒr die Beschreibung des BodenwĂ€rmestromes ĂŒber der LandoberflĂ€che. Zuerst werden die dafĂŒr benötigten theoretischen Grundlagen erlĂ€utert. ImAnschluss daran werden die verwendeten Daten und Methoden beschrieben. Dadurch ist die Basis fĂŒr den Vergleich der unterschiedlichen Berechnungsmethoden fĂŒr den vertikalen Nettoenergiefluss geschaffen.
Ein Vergleich der Berechnungsmethoden und eineDiskussion derUnterschiede ist von groĂem Interesse. DafĂŒr wird als Untersuchungsgebiet die LandoberflĂ€che von 40 ±N bis 90 ±N herangezogen. Da dies einen sehr groĂen Bereich darstellt wird auch auf einzelne Teilbereiche eingegangen. Ăber LandoberflĂ€chen ist die Konsistenz zwischen den vertikalen NettoenergieflĂŒssen auf der jahreszeitlichen Zeitskala vernĂŒnftig. Inkonsistenzen treten in höher gelegenen Gebieten nahe steiler Orographie auf. Die Gleichung fĂŒr die LandoberflĂ€che, wie sie hier vorgestellt wird, scheint ĂŒber Eisschilden nicht zu funktionieren, wahrscheinlich wegen der unterschiedlichen DatenreprĂ€sentation dort.In this thesis different calculation methods for the vertical net energy flux through the Earthâs surface are discussed. Three different methods are used for this purpose, firstly the direct calculation from the net radiation and the turbulent fluxes as they can be downloaded from reanalyses like ERA5. Another calculation possibility is the calculation over an atmospheric column. The third method is the diagnostic evaluation of an equation for the description of the soil heat flux over the land surface. At first the necessary theoretical foundations are explained. Afterwards the data and methods used are described. This provides the basis for comparing the different methods of calculating the vertical net energy flow.
A comparison of the calculation methods and a discussion of the differences is of great interest. For this purpose, the land surface from40 ±Nto 90 ±Nis used as a study area. Since this is a very large area, individual sub-areas are also dealt with. Over land surfaces the consistency between the net vertical energy fluxes is reasonable on the seasonal time scale. Inconsistencies emerge in high surface regions and near steep orography. The land surface equation as it is presented here does not seem to work over ice sheets, likely because of different data representation there
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Diagnostic evaluation of river discharge into the Arctic Ocean and its impact on oceanic volume transports
This study analyses river discharge into the Arctic Ocean using state-of-the-art reanalyses such as the fifth-generation European Reanalysis (ERA5) and the reanalysis component from the Global Flood Awareness System (GloFAS). GloFAS, in its operational version 2.1, combines the land surface model (Hydrology Tiled European Centre for Medium-Range Weather Forecasts â ECMWF â Scheme for Surface Exchanges over Land, HTESSEL) from ECMWFâs ERA5 with a hydrological and channel routing model (LISFLOOD). Furthermore, we analyse GloFAS' most recent version 3.1, which is not coupled to HTESSEL but uses the full configuration of LISFLOOD.
Seasonal cycles as well as annual runoff trends are analysed for the major Arctic watersheds â Yenisei, Ob, Lena, and Mackenzie â where reanalysis-based runoff can be compared to available observed river discharge records. Furthermore, we calculate river discharge over the whole pan-Arctic region and, by combination with atmospheric inputs, storage changes from the Gravity Recovery and Climate Experiment (GRACE) and oceanic volume transports from ocean reanalyses, we assess closure of the non-steric water volume budget. Finally, we provide best estimates for every budget equation term using a variational adjustment scheme.
Runoff from ERA5 and GloFAS v2.1 features pronounced declining trends induced by two temporal inhomogeneities in ERA5's data assimilation system, and seasonal river discharge peaks are underestimated by up to 50â% compared to observations. The new GloFAS v3.1 product exhibits distinct improvements and performs best in terms of seasonality and long-term means; however, in contrast to gauge observations, it also features declining runoff trends. Calculating runoff indirectly through the divergence of moisture flux is the only reanalysis-based estimate that is able to reproduce the river discharge increases measured by gauge observations (pan-Arctic increase of 2â% per decade). In addition, we examine Greenlandic discharge, which contributes about 10â% of the total pan-Arctic discharge and features strong increases mainly due to glacial melting.
The variational adjustment yields reliable estimates of the volume budget terms on an annual scale, requiring only moderate adjustments of less than 3â% for each individual term. Approximately 6583±84âkm3 of freshwater leaves the Arctic Ocean per year through its boundaries. About two-thirds of this is contributed by runoff from the surrounding land areas to the Arctic Ocean (4379±25âkm3âyrâ1), and about one-third is supplied by the atmosphere. However, on a seasonal scale budget residuals of some calendar months were too large to be eliminated within the a priori spreads of the individual terms. This suggests that systematical errors are present in the reanalyses and ocean reanalysis data sets, which are not considered in our uncertainty estimation