THE EFFECTS OF CONVECTION ON A SIMULATED MARINE CYCLONE

Citation
G. Balasubramanian et Mk. Yau, THE EFFECTS OF CONVECTION ON A SIMULATED MARINE CYCLONE, Journal of the atmospheric sciences, 51(16), 1994, pp. 2397-2417
Citations number
43
Categorie Soggetti
Metereology & Atmospheric Sciences
ISSN journal
00224928
Volume
51
Issue
16
Year of publication
1994
Pages
2397 - 2417
Database
ISI
SICI code
0022-4928(1994)51:16<2397:TEOCOA>2.0.ZU;2-4
Abstract
A hydrostatic, primitive equation model is used to simulate an oceanic cyclone with idealized initial conditions. The model uses a pressure coordinate in the vertical with a grid spacing of 100 mb. In the horiz ontal a grid spacing of 25 km is used, which should be nearly sufficie nt to resolve slantwise convection. The model produces an explosive mo ist cyclone with an intense bent-back warm front. The thermal gradient in the bent-back warm frontal region exceeds 8 K/100 km, in agreement with recent observations. Before rapid deepening, the model atmospher e becomes unstable to slantwise convection in the warm frontal region. After the spinup period, buckling in the angular momentum and theta(e ) surfaces are noted. It is suggested that the descending motion and t he associated dry slot over the cyclone center may arise from the desc ending branch of the slantwise convection on the warm side of the warm front. The descent may be augmented by the evaporation of liquid wate r. After the explosive deepening period, the stratification in both th e warm front and the bent-back warm front exhibits neutrality to slant wise convection. The Ertel potential vorticity (EPV) inversion techniq ue developed by Davis and Emanuel is used to obtain the perturbation g eopotential at 900-mb, 500-mb, and 300-mb levels due to EPV anomalies at different levels. The inversion is applied at the mature stage of t he cyclone at 45 h. It is found that there is a positive EPV anomaly a long the regions of the warm front and bent-back warm front, and it ac counts for 40% of the perturbation geopotential at 900 and 500 mb over the cyclone center. The contribution of low-level EPV anomaly in the moist cyclone to the perturbation geopotential at 500 mb over the cycl one center is twice that in the dry case. The circulation of the inver ted nondivergent wind fields in the moist run shows a small-scale cycl onic vortex and the presence of cold advection in the bent-back warm f rontal region. The contribution of the upper-level EPV anomaly to the 900-mb perturbation geopotential is also significant in the moist cycl one. The physical mechanism for the latter effect can be traced to an increase in vorticity advection in the middle troposphere in associati on with the formation of the bent-back warm front. This finding is in agreement with the authors' recent two-layer model results, which show that the bent-back warm front represents a region of cold advection t hat can in turn lead to an intensification of the upper-level wave. Th e contribution of the 1000-mb theta anomaly in the mature moist cyclon e is smaller than that of the dry run because of the convection-induce d cold advection in the bent-back warm front.