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This study investigates the influence of vorticity advection on the development of upper-level jet/front systems using quasi-geostrophic diagnosis. It analyzes the role of PV extrusion, isentropes, and Sawyer-Eliassen circulation in cyclonic shear. Traditional frontogenesis is compared to the new spin on vorticity advection by the thermal wind shear curvature.
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Quasi-geostrophic Diagnosis of the Influence of Vorticity Advection on the Development of Upper-level Jet/Front Systems Jonathan E. Martin Department of Atmospheric and Oceanic Sciences University of Wisconsin-Madison
500 hPa q 1800 UTC 17 November 2013
17 November Tropopause Trench Dynamic Tropopause Surface: 1800 UTC 17 November 2013
17 November Tropopause Trench Dynamic Tropopause Surface: 1800 UTC 17 November 2013
High PV extruded into the troposphere creates upper vorticity maxima that spawn lower tropo- spheric cyclones
Sloping isentropes provide parcel pathways for stratosphere/troposphere exchange High PV extruded into the troposphere creates upper vorticity maxima that spawn lower tropo- spheric cyclones
Lower stratospheric fronts Sloping isentropes provide parcel pathways for stratosphere/troposphere exchange High PV extruded into the troposphere creates upper vorticity maxima that spawn lower tropo- spheric cyclones
Sawyer-Eliassen circulation at jet core with cold air advection along the jet
Sawyer-Eliassen circulation at jet core with cold air advection along the jet
Sawyer-Eliassen circulation at jet core with cold air advection along the jet
Sawyer-Eliassen circulation at jet core with cold air advection along the jet
Sawyer-Eliassen circulation at jet core with cold air advection along the jet
. . . J Shearing deformation of an along-front θ gradient Geostrophic CAA in cyclonic shear
Rotunno et al. (1994) refer to geostrophic CAA in cyclonic shear as the “Shapiro effect”
Geostrophic vorticity maxima
Geostrophic vorticity maxima QG subsidence maxima (NVA by the thermal wind)
Does not change Traditional Frontogenesis
A New Spin on Vorticity Advection by the Thermal Wind shear curvature Shear is the component of the gradient of perpendicular to in Cartesian coordinates (Bell and Keyser 1993)
A New Spin on Vorticity Advection by the Thermal Wind shear curvature Shear is the component of the gradient of perpendicular to in Cartesian coordinates (Bell and Keyser 1993)
A New Spin on Vorticity Advection by the Thermal Wind shear curvature Shear is the component of the gradient of perpendicular to in Cartesian coordinates (Bell and Keyser 1993)