The Influence of Physical Processes on Extratropical Singular Vectors

An investigation is made of the impact of a full linearized physical (moist) parameterization package on extratropical singular vectors (SVs) using the ECMWF integrated forecasting system (IFS). Comparison is made for one particular period with a dry physical package including only vertical diffusion and surface drag. The crucial extra ingredient in the full package is found to be the large-scale latent heat release. Consistent with basic theory, its inclusion results in a shift to smaller horizontal scales and enhanced growth for the SVs. Whereas, for the dry SVs, T42 resolution is sufficient, the moist SVs require T63 to resolve their structure and growth. A 24-h optimization time appears to be appropriate for the moist SVs because of the larger growth of moist SVs compared with dry SVs. Like dry SVs, moist SVs tend to occur in regions of high baroclinicity, but their location is also influenced by the availability of moisture. The most rapidly growing SVs appear to enhance or reduce large-scale rain in regions ahead of major cold fronts. The enhancement occurs in and ahead of a cyclonic perturbation and the reduction in and ahead of an anticyclonic perturbation. Most of the moist SVs for this situation are slightly modified versions of the dry SVs. However, some occur in new locations and have particularly confined structures. The most rapidly growing SV is shown to exhibit quite linear behavior in the nonlinear model as it grows from 0.5 to 12 hPa in 1 day. For 5 times this amplitude the structure is similar but the growth is about half as the perturbation damps a potential vorticity (PV) trough or produces a cutoff, depending on its sign.

[1]  Roberto Buizza,et al.  Singular Vectors: The Effect of Spatial Scale on Linear Growth of Disturbances. , 1995 .

[2]  M. Stoelinga A Potential Vorticity-Based Study of the Role of Diabatic Heating and Friction in a Numerically Simulated Baroclinic Cyclone , 1996 .

[3]  A. Blackadar The vertical distribution of wind and turbulent exchange in a neutral atmosphere , 1962 .

[4]  F. Molteni,et al.  The ECMWF Ensemble Prediction System: Methodology and validation , 1996 .

[5]  B. Farrell The initial growth of disturbances in a baroclinic flow , 1982 .

[6]  R. Buizza Impact of horizontal diffusion on T21, T42, and T63 singular vectors , 1998 .

[7]  Roberto Buizza,et al.  The nature of singular vector growth and structure , 2000 .

[8]  E. Lorenz A study of the predictability of a 28-variable atmospheric model , 1965 .

[9]  Ronald M. Errico,et al.  Singular-Vector Perturbation Growth in a Primitive Equation Model with Moist Physics , 1999 .

[10]  Leonard A. Smith,et al.  Linear Regime Duration: Is 24 Hours a Long Time in Synoptic Weather Forecasting? , 2001 .

[11]  Jean-François Mahfouf,et al.  Influence of physical processes on the tangent‐linear approximation , 1999 .

[12]  Roberto Buizza,et al.  Computation of optimal unstable structures for a numerical weather prediction model , 1993 .

[13]  Roberto Buizza,et al.  Tropical singular vectors computed with linearized diabatic physics , 2001 .

[14]  Roberto Buizza,et al.  The Singular-Vector Structure of the Atmospheric Global Circulation , 1995 .

[15]  B. Hoskins,et al.  Simple Initial Value Problems and Mechanisms for Baroclinic Growth , 2001 .

[16]  Roberto Buizza,et al.  Optimal perturbation time evolution and sensitivity of ensemble prediction to perturbation amplitude , 1995 .

[17]  Paul J. Valdes,et al.  On the Existence of Storm-Tracks. , 1990 .

[18]  R. Buizza Localization of optimal perturbations using a projection operator , 1994 .

[19]  B. Hoskins Theory of Extratropical Cyclones , 1990 .

[20]  T. Palmer,et al.  Ensemble prediction of tropical cyclones using targeted diabatic singular vectors , 2001 .

[21]  Ronald M. Errico,et al.  An examination of the accuracy of the linearization of a mesoscale model with moist physics , 1999 .

[22]  Roberto Buizza,et al.  Sensitivity of optimal unstable structures , 1994 .

[23]  K. Emanuel,et al.  Baroclinic Instability in an Environment of Small Stability to Slantwise Moist Convection. Part I: Two-Dimensional Models , 1987 .

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