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24 December 1991, Volume 10 Issue 4   
  • THE VORTICITY CHANGE-RATE AND ITS HEAT SOURCE FOR DEVELOPMENT OF MESO-α SCALE VORTEX DURING A PERSISTENT HEAVY RAIN OF 14-22 AUGUST 1981
  • Cheng Linsheng
  • 1991 Vol. 10 (4): 337-350. 
  • Abstract ( ) PDF (895KB) ( )
  • During the period of 14-22 August 1981, a persistent heavy rain event occurred over the adjacent region of the Shaanxi-Gansu-Sichuan Province. This heavy rain event was directly related to a persistent development of a meso-α scale vortex with shear line. Diagnoses of the vorticity change-rate reveal rhat the positive vorticity change-rate center originated over the lower levels of the Qinghai-Xizang Plateau lee side, and then a process of the superposition and coupling and vertically joining-up of the vorticity change-rate centers over upper-and lower-levels was occurred. The vertical structure and evolution of the positive vorticity change-rate centers are basically consistent with the vertical structure and evolution of the positive vorticity centers of the formation and development of the shear line-vortex. In the factors of contributing to the vorticity change-rate, the relative numeric of the nonlinear interactive vorticity change-rate is the most component;the time-mean vorticity change-rate owing to topographic forcing is important only for the formation and maintenance of the shear line-vortex;the contribution of the perturbation vorticity change-rate is worth notice only when the shear line-vortex is under an intensive development. Diagnoses of the mesoscale heat and moisture budgets reveal that the vertical integrated high value regions of the apparent heat source Q1 and apparent moisture sink Q2 are basically consistent with regions of developing shear line-vortex and heavy rain. The vertical profiles of temporal-and spatial-averaged Q1 and Q2 indicate that the maximum heating interval of the Q1 appears between 570 hPa and 400 hPa, while the maximum interval of the Q2 appears between 650 hPa and 550 hPa. The heating due to convective eddy flux convergence of the sensible and latent heat is about half the amount of latent heat due to condensation.