Semigeostrophic moist frontogenesis in a Lagrangian model

Abstract A geometric technique for solving the Lagrangian conservation form of the semigeostrophic equations is extended to study moist frontogenesis. Model elements are required to conserve θ E and the frontogenesis is forced by a deformation flow. The boundary-layer elements ahead of the surface front are conditionally unstable but initially unsaturated. As they are forced to ascend at the surface front these elements saturate and appear at a new equilibrium position after implicitly releasing latent heat. This leads to the formation of a ‘lens’ of moist air at mid-levels some 200 km behind the surface front. In terms of dry potential vorticity, a positive anomaly has been created in the region where the elements saturate and a corresponding negative anomaly is created at the site of the lens. The inclusion of cooling using a simple model to mimic evaporational effects is found to have a significant effect on the overall evolution of the moist front.

[1]  K. Emanuel Observational evidence of slantwise convective adjustment , 1988 .

[2]  David Bolton The Computation of Equivalent Potential Temperature , 1980 .

[3]  David J. Knight a Numerical Modeling Study of Frontogenesis and Cold-Frontal Rainbands. , 1988 .

[4]  M. Cullen,et al.  An Extended Lagrangian Theory of Semi-Geostrophic Frontogenesis , 1984 .

[5]  Peter H. Haynes,et al.  On the Evolution of Vorticity and Potential Vorticity in the Presence of Diabatic Heating and Frictional or Other Forces , 1987 .

[6]  M. Holt,et al.  An analytical model of the growth of a frontal discontinuity , 1990 .

[7]  M. Cullen Solutions to a model of a front forced by deformation , 1983 .

[8]  T. W. Harrold Mechanisms influencing the distribution of precipitation within baroclinic disturbances , 1973 .

[9]  B. Hoskins,et al.  Conditional symmetric instability - a possible explanation for frontal rainbands , 1979 .

[10]  G. Shutts,et al.  A Geometric Model of Balanced, Axisymmetric Flows with Embedded Penetrative Convection , 1988 .

[11]  R. Gall,et al.  On the minimum scale of surface fronts , 1987 .

[12]  Francis P. Bretherton,et al.  Atmospheric Frontogenesis Models: Mathematical Formulation and Solution , 1972 .

[13]  R. Carbone A Severe Frontal Rainband. Part I. Stormwide Hydrodynamic Structure , 1982 .

[14]  G. Shutts Balanced Flow States Resulting from Penetrative, Slantwise Convection , 1987 .

[15]  K. Emanuel,et al.  Frontogenesis in the presence of small stability to slantwise convection , 1985 .

[16]  K. Emanuel Frontal Circulations in the Presence of Small Moist Symmetric Stability , 1985 .

[17]  M. Shapiro,et al.  The Frontal Hydraulic Head: A Micro-α Scale (̃1 km) Triggering Mechanism for Mesoconvective Weather Systems , 1985 .

[18]  Keith A. Browning,et al.  Air motion and precipitation growth at a cold front , 1970 .