2005
DOI: 10.1127/0941-2948/2005/0077
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In fluence parameters for a polar mesocyclone development

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Cited by 12 publications
(10 citation statements)
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“…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 (Klein & Heinemann, 2002) 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.…”
Section: Synoptic Overview and Katabatic Storm Developmentmentioning
confidence: 99%
“…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 (Klein & Heinemann, 2002) 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.…”
Section: Synoptic Overview and Katabatic Storm Developmentmentioning
confidence: 99%
“…We use the nonhydrostatic and anelastic atmospheric model METRAS [ Schlünzen , 1988, 1990] in a 2D version as applied earlier to cold air outbreaks by Lüpkes and Schlünzen [1996] and by Birnbaum and Lüpkes [2002] and to on‐ice flow regimes by Vihma et al [2003]. Its 3D version was applied to arctic regions by Dierer and Schlünzen [2005a, 2005b] and by Hebbinghaus et al [2006]. The model is originally a mesoscale model with horizontal grid spacing Δ x of at least 1 km in convective conditions.…”
Section: Model Descriptionmentioning
confidence: 99%
“…In addition to the standard variables from ERA5, we used the maximum Eady growth rate to assess the baroclinic instability in the atmosphere. Following earlier studies (Lindzen and Farrell, 1980;Dierer et al, 2005), we estimated the maximum Eady growth rate in the 1000 hPa to 750 hPa layer with σ E ≈ 0.31 f N | u750−u1000 z750−z1000 |, where f is the Coriolis frequency, u is the wind speed, z the height, N the Brunt-Väisälä frequency and the subscripts refer to the associated pressure levels.…”
Section: Datamentioning
confidence: 99%