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Sea ice cover (shaded) and EADY growth rate (isolines) for the homogeneous case at 16 UTC. Sea ice cover isolines from 60 % to 80 %, increment 5 %. EADY growth rate isolines from 0·10 −4 s −1 to 1·10 −4 1 −1 , increment 2·10 −5 1 −1 . 

Sea ice cover (shaded) and EADY growth rate (isolines) for the homogeneous case at 16 UTC. Sea ice cover isolines from 60 % to 80 %, increment 5 %. EADY growth rate isolines from 0·10 −4 s −1 to 1·10 −4 1 −1 , increment 2·10 −5 1 −1 . 

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Polar mesocyclones are small-scale, short-living phenomena in the Arctic and Antarctic. Their forecast is difficult due to a lack of knowledge of initial and boundary conditions. Idealised sensitivity studies are performed with the mesoscale atmosphere - sea ice model METRAS-MESIM to evaluate the relevance of the large-scale meteorological situatio...

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... this time areas of enhanced baroclinicity develop over the ice as a result of the ice drift caused by the mesocyclone. These regions occur where the sea ice concentration is reduced during the mesocyclone passage (Figure 7). Thus, the action of a mesocyclone on the sea ice can be the reason for enhanced baroclinicity, which finally can result in an intensification of a mesocyclone. ...

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... This converging flow constitutes a low-level baroclinic instability and enhances cyclonic vorticity due to vortex stretching, thereby increasing the PV anomaly . As a measure for baroclinicity we calculate the maximum Eady growth rate (σ max in s −1 ; Dierer & Schluenzen, 2005;Eady, 1949;Lindzen & Farrell, 1980) that describes how well deep pressure systems can develop in a weather situation over a specific area, with positive values favoring cyclogenesis: ...
... Within the next 6 hr, the katabatic flow from Ammassalik triggers a polar low with closed isobars on 29 February at 00 UTC and a core pressure of less than 980 hPa (Figure 2e). Converging flow, differential cold air advection decreasing with height in the Ammassalik area trigger the formation of the polar low near the sea ice edge, where polar lows frequently form and intensify (Bracegirdle & Gray, 2009;Dierer & Schluenzen, 2005). There is also a two-way interaction of the polar low-level and the upper-level trough. ...
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... METRAS ist zur Prüfung der implementierten numerischen Verfahren mit analytischen Lösun gen und zur weiteren Validierung mit Messungen und Ergebnissen anderer mesoskaliger Modelle verglichen worden (Bigalke, 1992;Dierer & Schluenzen, 2005;Grawe et al., 2013;Lüpkes et al., 2012;Ries et al., 2010;Schlünzen, 1992;Thunis et al., 2003). Die bei den Modellrechnungen genutzten Parametrisierungen und numerischen Methoden wurden detailliert untersucht (Lüpkes & Schlünzen, 1996;Schlünzen & Katzfey, 2003;Schroeder et al., 2006;Von Salzen et al., 1996;Schroeder et al., 2005;Augustin et al., 2008;Bohnenstengel & Schlünzen, 2009;Schroeder & Schlünzen, 2006;Schlünzen et al., 2011). ...
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... MIZ parameters such as its position, width, configuration, and mesoscale circulations in the ocean in the MIZ area are determined in many respects by interaction with the atmosphere (Guest et al., 1995). The position and configuration, in turn, influence the CAO large scale parameters (Pagowski and Moore, 2001) and the creation of MCs (Heine mann, 1996;Dierer and Schluenzen, 2005), while small scale inhomogeneities impact the values of the heat and momentum fluxes within the MIZ (Lüpkes and Birnbaum, 2005), as well as the organization of convection into rolls over the ocean . ...
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... The mesoscale transport and fluid model METRAS (Schlünzen, 1990;Lüpkes and Schlünzen, 1996) is a three-dimensional non-hydrostatic mesoscale numerical atmospheric model. It has been previously applied to Germany (Schlünzen, 1992;Renner and Münzenberg, 2003;Schlünzen and Katzfey, 2003;Schüler and Schlünzen, 2006;Schlünzen and Meyer, 2007;Bohnenstengel, 2011, Buschbom et al., 2012, Spain (Augustin et al., 2008), China (Wu and Schlünzen, 1992;Sheng et al., 2000), coastal areas (Niemeier and Schlünzen, 1993), the Arctic (Dierer and Schlünzen, 2005;Hebbinghaus et al., 2007;Lüpkes et al., 2008;Ries et al., 2010), and the urban climate of London (Thompson, 2008;Grawe et al., 2012 submitted) with horizontal resolutions ranging from 1 km to 18 km. A detailed description of METRAS is given in Schlünzen et al. (2012a). ...
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... The mesoscale transport and fluid model METRAS (Schlünzen, 1990;Lüpkes and Schlünzen, 1996) is a three-dimensional non-hydrostatic mesoscale numerical atmospheric model. It has been previously applied to Germany (Schlünzen, 1992;Renner and Münzenberg, 2003;Schlünzen and Katzfey, 2003;Schüler and Schlünzen, 2006;Schlünzen and Meyer, 2007;Bohnenstengel, 2011, Buschbom et al., 2012, Spain (Augustin et al., 2008), China (Wu and Schlünzen, 1992;Sheng et al., 2000), coastal areas (Niemeier and Schlünzen, 1993;Boettcher et al., 2015), the Arctic (Dierer and Schlünzen, 2005;Hebbinghaus et al., 2007;Lüpkes et al., 2008;Ries et al., 2010) and the urban climate of London (Thompson, 2008;Grawe et al., 2012) with horizontal resolutions ranging from 1 km to 18 km. A detailed description of METRAS is given in Schlünzen et al. (2012a). ...
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In the framework of the interdisciplinary project KLIMZUG-NORD, adaptation measures to climate change are developed for the Metropolitan Region of Hamburg. For the development of these measures it is crucial to know how the urban climate of Hamburg, a city with a population of 1.8 Mio, will alter due to climate change. Regional climate models provide climate projections on a horizontal resolution of up to 10 km, which is still too coarse to sufficiently simulate urban related phenomena such as the urban heat island (UHI). Therefore, these climate projections have to be downscaled. Since the computational amount increases rapidly with increasing horizontal resolution, a statistical-dynamical method for the UHI was developed. As a first step of the downscaling method, synoptic situations which are relevant for the UHI are determined. This is done combining objective weather type classification of ERA-40 reanalysis data using k-means-based cluster analysis and a regression-based statistical model for the observed UHI of Hamburg. The meteorological variables and domain used for the weather type classification are chosen to explain the variability of the UHI as best as possible. The second step is the simulation of the resulting synoptic situations with the mesoscale meteorological model METRAS providing a horizontal resolution of 1 km. To get the average UHI for a certain period, the simulation results are statistically recombined according to the frequency of the synoptic weather types. This is done for present and future climate simulations for the A1B scenario conducted with the regional climate models REMO and CLM and for the A2 scenario conducted with the regional climate model CCAM to identify changes in Hamburg's UHI. In this presentation the method will be presented with focus on the weather type classification and on the simulation results for the summer season.
... This large variability is mainly due to synoptic scale and mesoscale disturbances passing through the Fram Strait. The development of these atmospheric disturbances is influenced by the sea-ice characteristics (Dierer and Schlünzen, 2005). Via turbulent momentum-and heat fluxes mesoscale structures like fronts and polar cyclones are linked to surface characteristics such as roughness or sea-ice distribution. ...
... Valkonen et al. (2008) found the sea-ice concentration to play an important role for the near-ground temperature and wind field during a study in the Weddell Sea. For the simulation of a mesoscale cyclone passage with dynamic changes in the sea-ice distribution, a strong influence on the heat fluxes has been found when compared to simulations with constant sea-ice distribution (Dierer and Schlünzen, 2005). Here the development of an on-ice moving trough in the Fram Strait on 7 March 2002 is investigated. ...
... The simulations are performed with the mesoscale transport and fluid model METRAS (Schlünzen, 1990; Lüpkes and Schlünzen, 1996). Parametrization options that have been proven to deliver most realistic results for high latitude applications have been chosen (Lüpkes and Birnbaum, 2005; Dierer et al., 2005). The model treats the sea ice as invariant with respect to position and the characteristics mentioned (except sea-ice temperature). ...
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The impacts of the sea-ice characteristics distribution, roughness, temperature and thermal conductivity on an on-ice moving trough in the Fram Strait on 7 March 2002 are investigated. The situation is simulated with the mesoscale transport and fluid model METRAS and the named characteristics are varied within the range of observational uncertainty. The test cases are evaluated against aircraft measurements performed within the 'Fram Strait Cyclone Experiment 2002'. The model's sensitivity on the changes in sea-ice characteristics is quantified by statistical means. The strongest impacts on the near-ground temperature are found from sea-ice temperature, manifesting as an overall bias, and the positioning of the sea-ice edge, manifesting as a phase error. Only higher than natural homogenization of the sea-ice cover leads to some reduction of the amplitude error. A reduction of the sea-ice surface roughness is performed by applying an unrealistically small roughness length of ! z(0) = 1 mm. This reduces the negative wind speed bias, enhances the advection of contrasting air masses and improves the frontal sharpness. The thermal conductivity has the smallest influence. The lateral forcing taken from 'European Centre for Medium-Range Weather Forecasts' (ECMWF) reanalyses shows the strongest effect on the limited area model performance.
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