2013
DOI: 10.1002/qj.2074
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The structure and evolution of lower stratospheric frontal zones. Part II: The influence of tropospheric ascent on lower stratospheric frontal development

Abstract: The intensification of frontal characteristics in the region above the mid-latitude jet core within the lower stratospheric portion of an upper-level jet front system (ULJF) is known as lower stratospheric frontogenesis. Four recent cases of lower stratospheric frontogenesis in southwesterly flow are examined in order to elucidate the interaction between lower stratospheric dynamical processes and tropospheric ascent that characterizes such developments. In all of the cases examined the lower stratospheric fro… Show more

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Cited by 12 publications
(45 citation statements)
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“…Grams et al 2013b). A similar impact of strong latent heat release on the upper-level flow has been reported for midlatitude weather systems (e.g., Ahmadi-Givi et al 2004;Grams et al 2011;Lang and Martin 2013;Teubler and Riemer 2016).…”
Section: Background On Tc-extratropical Flow Interactionsupporting
confidence: 73%
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“…Grams et al 2013b). A similar impact of strong latent heat release on the upper-level flow has been reported for midlatitude weather systems (e.g., Ahmadi-Givi et al 2004;Grams et al 2011;Lang and Martin 2013;Teubler and Riemer 2016).…”
Section: Background On Tc-extratropical Flow Interactionsupporting
confidence: 73%
“…The divergent outflow and initial ridge building results from the diabatically driven strong ascent and associated latent heat release in the TC inner core and later at the midlatitude baroclinic zone yielding a net transport of lower-tropospheric air with low values of potential vorticity (PV) to the tropopause (e.g., DiMego and Bosart 1982;Bosart and Lackmann 1995;Torn 2010;Grams et al 2013b). Also, other weather systems such as predecessor rain events (PREs; Galarneau et al 2010;Moore et al 2013) and warm conveyor belts (WCBs; e.g., Carlson 1980;Madonna et al 2014b) occur surrounding an ET event, exhibit strong diabatic outflow, and may modify the upper-level Rossby wave pattern in a similar manner as the actual ET (Ahmadi-Givi et al 2004;Grams et al 2011;Bosart et al 2012;Lang and Martin 2013;Moore et al 2013;Madonna et al 2014a;Galarneau 2015;Teubler and Riemer 2016). The diabatic nature of this interaction alters the behavior of Rossby waves expected from a purely dry dynamical perspective.…”
Section: Introductionmentioning
confidence: 99%
“…While the upper‐tropospheric front is often highlighted as the main dynamical structure in a tropopause jet–front system, the analyses of Lang and Martin (2012, 2013b) emphasized the fact that via the thermal wind relationship, frontal development can also occur in the lower‐stratospheric vertical shear zone above a tropopause jet streak (i.e. ‘the region of the jet stream axis with the greatest winds’; American Meteorological Society, ).…”
Section: Introductionmentioning
confidence: 99%
“…Cross‐section through a characteristic tropopause jet– front system: potential temperature (every 4 K, thin grey contours), wind speed (every 10 m s −1 starting at 40 m s −1 , black contours), the dynamic tropopause (thick black line), and the magnitude of the potential temperature gradient (every 1 K (100 km) −1 starting at 2 K (100 km) −1 , grey shading). The figure is from Lang and Martin (2013b).…”
Section: Introductionmentioning
confidence: 99%
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