The three-dimensional structure of breaking Rossby waves in the polar wintertime stratosphere

The three-dimensional nature of breaking Rossby waves in the polar wintertime stratosphere is studied using an idealized global primitive equation model. The model is initialized with a well-formed polar vortex, characterized by a latitudinal band of steep potential vorticity (PV) gradients. Planetary-scale Rossby waves are generated by varying the topography of the bottom boundary, corresponding to undulations of the tropopause. Such topographically forced Rossby waves then propagate up the edge of the vortex, and their amplification with height leads to irreversible wave breaking. These numerical experiments highlight several nonlinear aspects of stratospheric dynamics that are beyond the reach of both isentropic two-dimensional models and fully realistic GCM simulations. They also show that the polar vortex is contorted by the breaking Rossby waves in a surprisingly wide range of shapes. With zonal wavenumber-1 forcing, wave breaking usually initiates as a deep helical tongue of PV that is extruded from the polar vortex. This tongue is often observed to roll up into deep isolated columns, which, in turn, may be stretched and tilted by horizontal and vertical shears. The wave amplitude directly controls the depth of the wave breaking region and the amount of vortex erosion. At large forcing amplitudes, the wave breaking in the middle/lower portions of the vortex destroys the PV gradients essential for vertical propagation, thus shielding the top of the vortex from further wave breaking. The initial vertical structure of the polar vortex is shown to play an important role in determining the characteristics of the wave breaking. Perhaps surprisingly, initially steeper PV gradients allow for stronger vertical wave propagation and thus lead to stronger erosion. Vertical wind shear has the notable effect of tilting and stretching PV structures, and thus dramatically accelerating the downscale stirring. An initial decrease in vortex area with increasing height (i.e., a conical shape) leads to focusing of wave activity, which amplifies the wave breaking. This effect provides a geometric interpretation of the ‘‘preconditioning’’ that often precedes a stratospheric sudden warming event. The implications for stratospheric dynamics of these and other threedimensional vortex properties are discussed.

[1]  T. Matsuno,et al.  A Dynamical Model of the Stratospheric Sudden Warming , 1971 .

[2]  John C. Gille,et al.  Transport of ozone in the middle stratosphere: evidence for planetary wave breaking , 1985 .

[3]  Tim Palmer,et al.  The «surf zone» in the stratosphere , 1984 .

[4]  C. Mechoso The Final Warming of the Stratosphere , 1990 .

[5]  R. Reynolds,et al.  The NCEP/NCAR 40-Year Reanalysis Project , 1996, Renewable Energy.

[6]  S. Yoden,et al.  A Numerical Experiment on the Breakdown of a Polar Vortex due to Forced Rossby Waves , 1993 .

[7]  Mark R. Schoeberl,et al.  A multiple‐level trajectory analysis of vortex filaments , 1995 .

[8]  P. Haynes,et al.  The Vertical-Scale Cascade in Atmospheric Tracers due to Large-Scale Differential Advection , 1997 .

[9]  M. Juckes A Shallow Water Model of the Winter Stratosphere. , 1989 .

[10]  Brian J. Hoskins,et al.  A multi-layer spectral model and the semi-implicit method , 1975 .

[11]  Mohamed Moustaoui,et al.  Comparison between vertical ozone soundings and reconstructed potential vorticity maps by contour advection with surgery , 1997 .

[12]  T. Matsuno Vertical Propagation of Stationary Planetary Waves in the Winter Northern Hemisphere , 1970 .

[13]  D. Waugh,et al.  The Dependence of Rossby Wave Breaking on the Vertical Structure of the Polar Vortex , 1999 .

[14]  A. O'Neill,et al.  Simulations of linear and nonlinear disturbances in the stratosphere , 1988 .

[15]  Mark R. Schoeberl,et al.  Intrusions into the lower stratospheric Arctic vortex during the winter of 1991–1992 , 1994 .

[16]  R. Saravanan,et al.  Three-dimensional quasi-geostrophic contour dynamics, with an application to stratospheric vortex dynamics , 1994 .

[17]  K. Labitzke The Amplification of Height Wave 1 in January 1979: A Characteristic Precondition for the Major Warming in February , 1981 .

[18]  L. Polvani,et al.  On the Subtropical Edge of the Stratospheric Surf Zone , 1995 .

[19]  W. Randel Ideas flow on Antarctic vortex , 1993, Nature.

[20]  T. Palmer,et al.  Breaking planetary waves in the stratosphere , 1983, Nature.

[21]  Christopher R. Webster,et al.  Transport out of the lower stratospheric Arctic vortex by Rossby wave breaking , 1994 .

[22]  William J. Randel,et al.  Global atmospheric circulation statistics, 1000-1 mb , 1992 .

[23]  J. McWilliams,et al.  Co-rotating stationary states and vertical alignment of geostrophic vortices with thin cores , 1998, Journal of Fluid Mechanics.

[24]  W. Randel,et al.  Climatology of Arctic and Antarctic Polar Vortices Using Elliptical Diagnostics , 1999 .

[25]  R. A. Plumb Instability of the Distorted Polar Night Vortex: A Theory of Stratospheric Warmings , 1981 .

[26]  R. Garcia,et al.  The interaction of horizontal Eddy transport and thermal drive in the stratosphere , 1990 .

[27]  L. Polvani,et al.  Rossby-wave breaking, microbreaking, filamentation, and secondary vortex formation-The dynamics of a perturbed vortex , 1992 .

[28]  D. Hartmann,et al.  The dynamics of the stratospheric polar vortex and its relation to springtime ozone depletions. , 1991, Science.

[29]  H. Arakawa AN ALTERNATIVE FORM OF POTENTIAL VORTICITY , 1941 .

[30]  T. Palmer,et al.  Simulations of an observed stratospheric warming with quasigeostrophic refractive index as a model diagnostic , 1982 .

[31]  D. Waugh Contour Surgery Simulations of a Forced Polar Vortex. , 1993 .

[32]  L. Gray,et al.  Simulation of the semi‐annual oscillation of the equatorial middle atmosphere using the Extended UGAMP General Circulation Model , 1994 .

[33]  L. Polvani,et al.  The roll-up of vorticity strips on the surface of a sphere , 1992, Journal of Fluid Mechanics.

[34]  J. Mahfouf,et al.  A Quasi-Biennial Oscillation Signal in General Circulation Model Simulations , 1993, Science.

[35]  R. Wilson,et al.  Climatology of the SKYHI Troposphere–Stratosphere–Mesosphere General Circulation Model , 1995 .

[36]  M. Juckes,et al.  A high-resolution one-layer model of breaking planetary waves in the stratosphere , 1987, Nature.

[37]  J. Hack,et al.  Description of the NCAR Community Climate Model (CCM1) , 1987 .

[38]  Warwick A. Norton,et al.  Breaking Rossby Waves in a Model Stratosphere Diagnosed by a Vortex-Following Coordinate System and a Technique for Advecting Material Contours , 1994 .

[39]  R. Garcia,et al.  Air Motions Accompanying the Development of a Planetary Wave Critical Layer , 1990 .

[40]  B. Boville Middle atmosphere version of CCM2 (MACCM2): Annual cycle and interannual variability , 1995 .