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<br /> <br />Figure 3.3-Satellite image of convective clouds on May 28. <br />1979. at 002 G.m.t. showing typical clusters. <br /> <br />within 150 km of Big Spring had minimum echo-top <br />temperatures in the 0 to -15 0 C range. Nearly 30 <br />percent of these echoes lasted more than one-half <br />hour. These results suggested that there are a rea- <br />sonable number of opportunities to examine ice- <br />phase seeding hypotheses within this region without <br />having seeding effects masked by abundant natural <br />ice from colder regions of a cloud. <br /> <br />3.4 Mesoscale Analysis <br /> <br />It has been understood for a long time that <br />convective showers develop in an unstable atmos- <br />phere where the temperature decreases with height <br />at about 5 0 C/km. By the time Texas HIPLEX began. <br />it was also understood that the occurrence of heavy <br />convective rainfall requires some organization' of <br />atmospheric motions on a scale exceeding that of <br />the local shower but smaller than that of the standard <br />weather map. It was resolved to make investigations <br />of these mesoscale systems a major part of the Texas <br />HIPLEX. To this end. a mesoscale network of rawin- <br />sonde stations was set up. and the rawinsonde data <br />were examined along with satellite cloud pictures <br />and other data. <br /> <br />Rawinsonde data were collected from one site in <br />1975 and increased to seven sites in 1979 and <br />1980. During operational days when convective <br />activity was expected. observations were made <br />every 3 hours from 1500 to 0300 G.m.t. <br /> <br />Data from the Big Spring and Midland soundings <br />were generally available for analysis and forecasting <br />in near real-time (within 2 hours of observation) <br />through the EDN. <br /> <br />The Texas HIPLEX mesoscale research conducted <br />during the summers of 1976 through 1980 was <br />designed to determine factors and environmental <br />conditions responsible for the initiation. growth. <br />maintenance. and dissipation of the several classes <br />of convective clouds. Substantial differences were <br />found between periods of convection and periods of <br />no convection. Low-level net horizontal inflow. het <br />upward transport. and upper-level net horizontal <br />outflow of total convective energy were found dur- <br />ing times of convection. By contrast. the reverse was <br />found when convective activity was absent. Water <br />vapor transport appears to be the dominant energy <br />source for convection. supplying both latent and <br />kinetic energy to the storm. Both depth and intensity <br />of convective activity wf!te correlated best with the <br />amount of water vapor transport near the surface <br />and the degree of vertical transport aloft (Scoggins <br />et al.. 1979). Horizontal outflow in the upper air was <br />shown to complement the, low-level convergence <br />and upward motion. The volume of convective cloud <br />(depth and area) contributed more to the quantity of <br />water vapor processed than did the type of organiza- <br />tion. Comparison with radar and satellite images <br />showed that mesoscale convergence and lifting are <br />responsible for most deep convection and that sink- <br />ing motion suppressed cloud development (Mat- <br />thews. 1983). <br /> <br />Figure 3.4 shows an example of strong vertical <br />motion which triggered deep convective clouds and <br />heavy precipitation. nearly 37 x 106 m3 of rainfall <br />within the rain gage network. during a convective <br />line event on July 17. 1979. The mesoscale precip- <br />itation efficiency of this system was 16 percent. indi- <br />cating that only a fraction of the total available <br />moisture was returned in the form of rainfall. This <br />suggests that there may be potential for improving <br />the efficiency of these systems. <br /> <br />With the above indications of significant mesoscale <br />control of precipitation events in west Texas. studies <br />were initiated to better understand the relationships <br />involved and their geographic variations. Matthews <br />(1980) found from analyses of satellite cloud pic- <br />tures that convection showed different degrees of <br />organization across the High Plains, Mountain- <br />generated convective storms. lines. and clusters <br />were the predominant daily convective types in Mon- <br />tana. While many isolated convective clouds occur- <br />red on any given day. days where these clouds were <br />not associated with larger scale lines and clusters <br />were few. In Kansas. days' with lines and clusters as <br />the predominant convective feature were most com- <br />mon. but days with only isolated cells also occurred. <br />Days with isolated convective cells were most com- <br />mon in Texas. but mesoscale lines and clusters were <br />observed on some days. <br /> <br />15 <br />