Laserfiche WebLink
<br />layers which tend to focus the effect of lifting on the release of <br />convective instability. Meso-p convergence may be produced by <br />several mechanisms such as: dry line~ jet streak~ low-level jet~ <br />local differential heating and meso-a frontal systems. Wind shear <br />plays a role in unloading precipitation in updrafts, establishing <br />regions of strong upper-level divergence which maintains mesoscale <br />updraft regions~ and transferring horizontal momentum to the convec- <br />tive cells which control their movement and evolution of updraft/ <br />downdraft couplets. <br /> <br />4. Mesosynoptic convective systems form in an environment with <br />synoptic-scale forcing having sufficient instability and moisture <br />to generate convective clouds and precipitation. These systems <br />result from frontal systems~ cyclonic systems~ easterly waves and <br />upslope flow which produce widespread lifting. Mesoscale convective <br />triggers hypothesized in 1.2.2 and 1.2.3 above may be superimposed on <br />the synoptic lifting pattern to produce meso-o areas of more intense <br />convective precipitation along squall lines or in embedded showers <br />and thunderstorms. In these cases mesoscale lifting produces areas <br />of more intense convective activity within regions of widespread <br />synoptic-scale stratiform precipitation. <br /> <br />Table 1.1 provides a quantitative definition of scale and organiza- <br />tion of cells for each type of event based upon satellite image struc- <br />ture and radar echo characteristics. The satellite provides a unique <br />overview of cloud structure which clearly defines the cloud organiza- <br />tion~ the extent of clouds and cloud type. Radar provides a more quan- <br />titative analf'iS of detailed echo :ize and individual echo properties. <br />