Systematic Multiscale Models for the Tropics

Systematic multi-scale perturbation theory is utilized to develop self-consistent simplified model equations for the interaction across multiple spatial and/or temporal scales in the tropics. One of these models involves simplified equations for intraseasonal planetary equatorial synoptic scale dynamics (IPESD). This model includes the self-consistent quasi-linear interaction of synoptic scale generalized steady Matsuno-Webster-Gill models with planetary scale dynamics of equatorial long waves. These new models have the potential for providing self-consistent prognostic and diagnostic models for the intraseasonal tropical oscillation. Other applications of the systematic approach reveal three different balanced weak temperature gradient (WTG) approximations for the tropics with different regimes of validity in space and time: a synoptic equatorial scale WTG (SEWTG), a mesoscale equatorial WTG (MEWTG) which reduces to the classical models treated by others, and a new seasonal planetary equatorial WTG (SPEWTG). Both the SPEWTG and MEWTG model equations have solutions with general vertical structure yet have the linearized dispersion relation of barotropic Rossby waves; thus, these models can play an important role in theories for midlatitude connections with the tropics. The models are derived both from the equatorial shallow water equations in a simplified context and also as distinguished limits from the compressible primitive equations in general.

[1]  J. Pedlosky Geophysical Fluid Dynamics , 1979 .

[2]  Rupert Klein,et al.  Asymptotic Analyses for Atmospheric Flows and the Construction of Asymptotically Adaptive Numerical Methods , 2000 .

[3]  A. Kasahara,et al.  Response of Planetary Waves to Stationary Tropical Heating in a Global Atmosphere with Meridional and Vertical Shear , 1986 .

[4]  J. Neelin On the Intepretation of the Gill Model , 1989 .

[5]  A. Matthews,et al.  Intraseasonal oscillations in 15 atmospheric general circulation models: results from an AMIP diagnostic subproject , 1996 .

[6]  R. Lindzen,et al.  On the role of sea surface temperature gradients in forcing low-level winds and convergence in the tropics , 1987 .

[7]  P. Webster Response of the Tropical Atmosphere to Local, Steady Forcing , 1972 .

[8]  J. Charney A Note on Large-Scale Motions in the Tropics , 1963 .

[9]  Andrew J. Majda,et al.  Averaging over Fast Gravity Waves for Geophysical Flows with Unbalanced Initial Data , 1998 .

[10]  Johan Nilsson,et al.  The Weak Temperature Gradient Approximation and Balanced Tropical Moisture Waves , 2001 .

[11]  A. Bourlioux,et al.  An elementary model for the validation of flamelet approximations in non-premixed turbulent combustion , 2000 .

[12]  Omar M. Knio,et al.  Numerical Simulation of a Thermoacoustic Refrigerator: II. Stratified Flow around the Stack☆ , 1998 .

[13]  Omar M. Knio,et al.  Numerical Simulation of a Thermo-AcousticRefrigerator , 1997 .

[14]  Andrew J. Majda,et al.  Averaging over fast gravity waves for geophysical flows with arbitrary potential vorticity , 1996 .

[15]  Tetsuo Nakazawa,et al.  Tropical Super Clusters within Intraseasonal Variations over the Western Pacific , 1988 .

[16]  Bin Wang,et al.  A Simple Tropical Atmosphere Model of Relevance to Short-Term Climate Variations , 1993 .

[17]  R. Klein Semi-implicit extension of a Godunov-type scheme based on low Mach number asymptotics , 1995 .

[18]  C. Bretherton,et al.  The Gill Model and the Weak Temperature Gradient Approximation , 2003 .

[19]  Bin Wang,et al.  Low-Frequency Equatorial Waves in Vertically Sheared Zonal Flow. Part II: Unstable Waves , 1996 .

[20]  J. Marsden,et al.  A mathematical introduction to fluid mechanics , 1979 .

[21]  Matthew C. Wheeler,et al.  Convectively Coupled Equatorial Waves: Analysis of Clouds and Temperature in the Wavenumber–Frequency Domain , 1999 .

[22]  T. Matsuno,et al.  Quasi-geostrophic motions in the equatorial area , 1966 .

[23]  C. Munz,et al.  The extension of incompressible flow solvers to the weakly compressible regime , 2003 .

[24]  H. Weitzner,et al.  Perturbation Methods in Applied Mathematics , 1969 .

[25]  B. Hoskins,et al.  Large-Scale Eddies and the General Circulation of the Troposphere , 1985 .

[26]  R. Klein,et al.  Extension of Finite Volume Compressible Flow Solvers to Multi-dimensional, Variable Density Zero Mach Number Flows , 2000 .

[27]  Andrew J. Majda,et al.  Large scale front dynamics for turbulent reaction-diffusion equations with separated velocity scales , 1994 .

[28]  A. E. Gill Some simple solutions for heat‐induced tropical circulation , 1980 .

[29]  N. Zeng,et al.  A Quasi-Equilibrium Tropical Circulation Model—Formulation * , 2000 .

[30]  Harry H. Hendon,et al.  The Life Cycle of the Madden–Julian Oscillation , 1994 .

[31]  Rupert Klein,et al.  Regular Article: Extension of Finite Volume Compressible Flow Solvers to Multi-dimensional, Variable Density Zero Mach Number Flows , 1999 .

[32]  A. E. Gill,et al.  Some simple analytical solutions to the problem of forced equatorial long waves , 1984 .

[33]  B. Hoskins,et al.  The initial value problem for tropical perturbations to a baroclinic atmosphere , 1991 .

[34]  A. Majda,et al.  Vorticity and incompressible flow , 2001 .

[35]  Wayne H. Schubert,et al.  The Role of Gravity Waves in Slowly Varying in Time Tropospheric Motions near the Equator , 2000 .

[36]  D. Raymond A New Model of the Madden–Julian Oscillation , 2001 .

[37]  A. Majda,et al.  Models for Stratiform Instability and Convectively Coupled Waves , 2001 .

[38]  Andrew J. Majda,et al.  Low Froude number limiting dynamics for stably stratified flow with small or finite Rossby numbers , 1998 .

[39]  O. Knio,et al.  Asymptotic vorticity structure and numerical simulation of slender vortex filaments , 1995, Journal of Fluid Mechanics.