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Four hours of model time are simulated and history files are saved every 5 seconds. Data are analyzed using three-dimensional raytracing techniques, Lagrangian parcel analysis, and traditional horizontal slices of model parameters including wind vectors. Animations of isosurfaces, particle sheets and bundles, and wind vectors are presented in order to elucidate the morphology of these of the low-level vorticity maxima which are found throughout the simulation.
Throughout the course of the simulation, vorticity maxima are found behind the leading edge of the gust front along the right flank. These features contain values of vertical vorticity (ζ) often exceeding 0.1 s-1 for minutes at a time. These vortices tend to originate below the main updraft near the point of occlusion where tornadogenesis is typically observed. Their formation typically coincides with a slight lowering of the cloud base and a small pressure deficit (no greater than about 7 mb). The stronger vortices exhibit a strong storm-relative rotational signature, while the weaker vortices appear as kinks in plots of low-level storm-relative winds.
Almost without exception, these vortices propagate away from the location of the main supercell updraft along the flanking line. At times up to six vortex maxima occur concurrently. Three-dimensional isosurface animations indicate that these vortices form from the ground upward and occasionally extend several kilometers in length. Preliminary Lagrangian parcel analysis suggests that vortex stretching below and along the flank of the strongest winds of the updraft precedes vortex strengthening.
Recent observational and modeling studies suggest that vortex features with similar characteristics to those found in this study may play a significant role in tornadogenesis. Vortex mergers and vortex stretching have both been suggested as mechanisms for tornadogenesis, and at 100 meter horizontal grid spacing these small, localized regions of vertical vorticity are plentiful in favorable locations during this simulated supercell.
While conclusions at the time of this writing are scant, our current data indicates that features on the scale of a few hundred meters in diameter may be plentiful during the evolution of supercell thunderstorms. Higher resolution simulations will indicate whether these features are properly resolved or whether smaller-diameter swirling features of large vorticity are plentiful in similar environments.
Click on the image below for a larger view.
Supplementary URL: http://research.orf.cx/sls2004