One of the main ingredients for mesocyclogenesis is the presence of strong changes in wind speed over distance and direction with height, also known as horizontal and vertical
wind shear. This shear classically coincides with the presence of a strong
trough which may lead to an
extratropical cyclone, a type of
cyclone that forms through the interactions between cold and warm air, known as
baroclinicity. The pressure and temperature gradients between warm and cold air cause these changes in the wind with height and over distance. The resulting sheared wind field is said to have horizontal
vorticity, or the local tendency of the flowing fluid (here, air) to rotate, which is a property inherent to any flow where velocity gradients exist. The associated vorticity is often incorrectly depicted as a horizontally-rolling vortex that is directly tilted into the vertical by a rising updraft. However, in the majority of cases, the environment is horizontally homogenous with said vortexes being absent. Horizontal vorticity can instead be thought as an imaginary paddle wheel that is set spinning by the winds that change with height. These winds move the top and bottom of the wheel at different speeds along the horizontal direction, causing it to twist along its axis. This local tendency for rotation, or twisting, is what the updraft reorients, rather than a literal tube or vortex of rotating air. When an updraft forms in this environment, ascending
air parcels encounter faster sheared air across height, which is entrained and turbulently mixed at the edge of the updraft, exchanging horizontal
momentum. The rising air at the edge of the updraft speeds up sideways faster than it is moving inward, forcing inner slower air to then also move faster horizontally. Air parcels then begin to curve as they move towards and overshoot the updraft's
center of low pressure, following into a spiral as the process repeats. As the air parcels curve they also rotate about their axis due to the wind shear's twisting motion. This curving, spiraling or rotating motion of the wind can exist without the air necessarily spinning as a vortex. As the low-level mesocyclone continues to ingest horizontal vorticity, vorticity maximums or vortex patches (areas of slight rotation or transient vortices) may form alongside the boundary where the updraft and its downdrafts – the cool and moist
forward flank downdraft (FFD) and the, often, warmer and more buoyant
rear flank downdraft (RFD) – meet due to the interactions between the warmer and cooler air masses. Surges in the RFD often coincide with the consolidation of these vortex patches, and may lead to tornadogenesis as a result. This is visually indicated by the formation of a
wall cloud or other low cloud structures near the surface as the updraft strengthens from its interactions with the RFD. The gallery below shows the three stages of development of a mesocyclone and a view of the storm relative motion on radar of a mesocyclone-producing tornado over
Greensburg, Kansas on 4 May 2007. The storm was in the process of producing
an EF5 tornado at the time of the image. File:Meso-1.svg|Wind shear (red) sets air spinning (green). File:Meso-2.svg|The updraft (blue) 'tips' the spinning air upright. File:Meso-3.svg|The updraft then starts rotating. File:Greensburg3 small.gif|Radar view of a mesocyclone. Note that at the time of this image, an
EF5 tornado was on the ground. == Identification ==