Abstract:The total quasi-geostrophic (QG) vertical motion is partitioned into transverse and shearwise couplets oriented parallel to, and along, the geostrophic vertical shear, respectively, in order to examine the role of rotational frontogenesis, and its associated shearwise circulation, in the life cycle of an upper-front/jet system in northwesterly flow. In particular the analysis emphasizes two aspects of that role: (1) the influence of shearwise ω on scalar frontogenesis, and (2) the effect of rotational frontoge… Show more
“…Recent studies that explore the role of latent heating during WCB ascent in creating midtropospheric positive PV anomalies and upper-tropospheric negative PV anomalies include Pomroy and Thorpe (2000), Knippertz and Wernli (2010), Lang (2011), Schemm et al (2013), and Madonna et al (2014). Cooper et al (2004) showed that penetration of stratospheric intrusions by convection can facilitate subsequent mixing into the troposphere.…”
Section: Convective Influences On Ste Near Jetsmentioning
confidence: 98%
“…Cold air advection along the UTLS jet axis has been shown to be compatible with sinking downstream of a trough at synoptic scales (Martin 2006;Lang and Martin 2010). Sawyer (1949) explored the possible role of inertial or symmetric instability in the UTLS in modifying midlatitude cyclogenesis, jet stream behavior, and meridional circulations.…”
Section: B Rwb Inertial Instability and Westerly Jetsmentioning
In simulations of midlatitude cyclones with the University of Wisconsin Nonhydrostatic Modeling System (UWNMS), mesoscale regions with large negative absolute vorticity commonly occur in the upper troposphere and lower stratosphere (UTLS), overlying thin layers of air with stratospheric values of ozone and potential vorticity (PV). These locally enhanced stratosphere-troposphere exchange (STE) events are related to upstream convection by tracing negative equivalent potential vorticity (EPV) anomalies along back trajectories. Detailed agreement between the patterns of negative absolute vorticity, PV, and EPV-each indicators of inertial instability in the UTLS-is shown to occur in association with enhanced STE signatures. Results are presented for two midlatitude cyclones in the upper Midwest, where convection develops between the subpolar and subtropical jets.Mesoscale regions of negative EPV air originate upstream in the boundary layer. As they are transported through convection, EPV becomes increasingly negative toward the tropopause. In association with the arrival of each large negative EPV anomaly, a locally enhanced poleward surge of the subpolar jet occurs, characterized by high turbulent kinetic energy and low Richardson number. Isosurfaces of wind speed show that gravity waves emanating from inertially unstable regions connect with and modulate the subpolar and subtropical jets simultaneously. Inertially unstable convective outflow surges can facilitate STE locally by fostering poleward acceleration in the UTLS, with enhanced folding of tropospheric air over stratospheric air underneath the poleward-moving jet.
“…Recent studies that explore the role of latent heating during WCB ascent in creating midtropospheric positive PV anomalies and upper-tropospheric negative PV anomalies include Pomroy and Thorpe (2000), Knippertz and Wernli (2010), Lang (2011), Schemm et al (2013), and Madonna et al (2014). Cooper et al (2004) showed that penetration of stratospheric intrusions by convection can facilitate subsequent mixing into the troposphere.…”
Section: Convective Influences On Ste Near Jetsmentioning
confidence: 98%
“…Cold air advection along the UTLS jet axis has been shown to be compatible with sinking downstream of a trough at synoptic scales (Martin 2006;Lang and Martin 2010). Sawyer (1949) explored the possible role of inertial or symmetric instability in the UTLS in modifying midlatitude cyclogenesis, jet stream behavior, and meridional circulations.…”
Section: B Rwb Inertial Instability and Westerly Jetsmentioning
In simulations of midlatitude cyclones with the University of Wisconsin Nonhydrostatic Modeling System (UWNMS), mesoscale regions with large negative absolute vorticity commonly occur in the upper troposphere and lower stratosphere (UTLS), overlying thin layers of air with stratospheric values of ozone and potential vorticity (PV). These locally enhanced stratosphere-troposphere exchange (STE) events are related to upstream convection by tracing negative equivalent potential vorticity (EPV) anomalies along back trajectories. Detailed agreement between the patterns of negative absolute vorticity, PV, and EPV-each indicators of inertial instability in the UTLS-is shown to occur in association with enhanced STE signatures. Results are presented for two midlatitude cyclones in the upper Midwest, where convection develops between the subpolar and subtropical jets.Mesoscale regions of negative EPV air originate upstream in the boundary layer. As they are transported through convection, EPV becomes increasingly negative toward the tropopause. In association with the arrival of each large negative EPV anomaly, a locally enhanced poleward surge of the subpolar jet occurs, characterized by high turbulent kinetic energy and low Richardson number. Isosurfaces of wind speed show that gravity waves emanating from inertially unstable regions connect with and modulate the subpolar and subtropical jets simultaneously. Inertially unstable convective outflow surges can facilitate STE locally by fostering poleward acceleration in the UTLS, with enhanced folding of tropospheric air over stratospheric air underneath the poleward-moving jet.
“…It is clear that the effective horizontal rotational frontogenesis (Figure 2a) is much smaller than that afforded by tilting (Figure 2b), suggesting a predominant role for tilting in changing the geostrophic temperature advection. Lang and Martin (2010) proposed a conceptual model, illustrated in their figure 13, which suggested that the development of along-flow geostrophic cold air advection was dependent on both kinematic rotation of ∇θ and alongflow tilting. Given the re-evaluation of the kinematics offered in this response, it is likely that rotation by deformation provides the kinematic contribution that we mistakenly attributed to the vorticity in our original paper.…”
Section: Rotation Of ∇φmentioning
confidence: 99%
“…The role of that vertical circulation in initiating geostrophic cold air advection along the flow is particularly at issue in Schultz (2012). Lang and Martin (2010) entered an ongoing debate between two competing hypotheses regarding the initiation of geostrophic cold air advection in the upper frontogenesis process and attempted to devise a more complete explanation that borrowed from both. Rotunno et al (1994, hereafter RSS94), using idealized baroclinic channel model simulations, examined the intensification of an upper-level front from a nearly equivalent barotropic initial state.…”
Schultz (2012) proposes that our previous arguments regarding the initiation of along-flow geostrophic cold air advection during the upper frontogenesis process are incomplete. The core of his criticism, and the motivation for his call to include additional diagnostic calculations, hinges upon the assertion that the vertical vorticity can rotate isentropes relative to isohypses. In this response we derive an expression for the rate of change of ∇φ that demonstrates that vorticity rotates ∇θ and ∇φ equally, in accord with our original statement to that effect. The derived expression also provides motivation to propose a revision of our previous conceptual model, highlighting the role of deformation instead of vorticity in the differential rotation of ∇θ relative to ∇φ that can contribute to the initiation of along-flow geostrophic temperature advection.
“…Sutcliffe, 1947;Trenberth, 1978), which exists along the jet axis when geostrophic cold air advection is present along an ULJF. Keyser and Pecnik (1987) showed that subsidence through the jet core is upper frontogenetic, thus the establishment of geostrophic cold air advection along the jet has been described as an important aspect of the upper front life cycle (Rotunno et al, 1994;Schultz and Doswell, 1999;Lang and Martin, 2010). An environment characterized by geostrophic warm air advection through the jet core shifts the thermally direct (indirect) circulation in the jet entrance (exit) region toward the cyclonic (anticyclonic) side, so that the jet core is conversely characterized by ascent (Figure 3(c)).…”
The structure, evolution and dynamics of two lower stratospheric frontal zones are examined from a basic state variables perspective. The case studies highlight the asynchronous evolution of the lower stratospheric and upper tropospheric frontal portions of upper level jet-front (ULJF) systems, as well as some substantial differences in lower stratospheric frontal development that occur in southwesterly and northwesterly flow. The evolution of the ULJF in northwesterly flow was characterized by an initially intense but weakening lower stratospheric front along with an initially weak but intensifying upper tropospheric front. Throughout the evolution, geostrophic cold air advection in cyclonic shear characterized a substantial portion of the lower stratospheric front. This circumstance supported subsidence through the local jet core within the cold upper troposphere, weakening the lower stratospheric front via tilting. This subsidence extended downward below the jet core where it is suggested to have played a role in the early stages of upper tropospheric frontogenesis. In the southwesterly flow case, the evolution of the ULJF was characterized by a strengthening lower stratospheric front and a weakening upper
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