TY - JOUR
T1 - Three-dimensional numerical modeling of convection produced by interacting thunderstorm outflows. Part I
T2 - control simulation and low-level moisture variations.
AU - Droegemeier, K. K.
AU - Wilhelmson, R. B.
PY - 1985
Y1 - 1985
N2 - The Klemp-Wilhelmson three-dimensional numerical cloud model is used to investigate cloud development along intersecting thunderstorm outflow boundaries. The model initial environment is characterized by a temperature and moisture profile typically found in strong convective situations, and the initial wind field is prescribed by a constant unidirectional shear of 2.9 m s-1 km-1 from 0.8 to 8.9 km, with a constant wind everywhere else. The wind shear vector is perpendicular to the line containing the two initial outflow-producing clouds (which are spaced 16 km apart and are triggered by thermal impulses centered at the top of the boundary layer). The dynamics of the outflow collision are documented using time-dependent, kinematic air parcel trajectories and thermodynamic data. We find that ambient air in the outflow collision region is literally 'squeezed' out of the way as the two outflows collide. Some of this air is lifted to saturation, triggering two convective clouds. The upshear member of the pair has a head start in development, and since the two clouds are growing close together and competing for the same air, the upshear cloud is the strongest. In addition, the downshear cell is suppressed because it grows into the region occupied by the upshear cell's downdraft and rain region. -from Authors
AB - The Klemp-Wilhelmson three-dimensional numerical cloud model is used to investigate cloud development along intersecting thunderstorm outflow boundaries. The model initial environment is characterized by a temperature and moisture profile typically found in strong convective situations, and the initial wind field is prescribed by a constant unidirectional shear of 2.9 m s-1 km-1 from 0.8 to 8.9 km, with a constant wind everywhere else. The wind shear vector is perpendicular to the line containing the two initial outflow-producing clouds (which are spaced 16 km apart and are triggered by thermal impulses centered at the top of the boundary layer). The dynamics of the outflow collision are documented using time-dependent, kinematic air parcel trajectories and thermodynamic data. We find that ambient air in the outflow collision region is literally 'squeezed' out of the way as the two outflows collide. Some of this air is lifted to saturation, triggering two convective clouds. The upshear member of the pair has a head start in development, and since the two clouds are growing close together and competing for the same air, the upshear cloud is the strongest. In addition, the downshear cell is suppressed because it grows into the region occupied by the upshear cell's downdraft and rain region. -from Authors
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U2 - 10.1175/1520-0469(1985)042<2381:TDNMOC>2.0.CO;2
DO - 10.1175/1520-0469(1985)042<2381:TDNMOC>2.0.CO;2
M3 - Article
AN - SCOPUS:0022264245
SN - 0022-4928
VL - 42
SP - 2381
EP - 2403
JO - Journal of the Atmospheric Sciences
JF - Journal of the Atmospheric Sciences
IS - 22
ER -