An interpretation of baroclinic initial value problems: results for simple basic states with nonzero interior PV gradientsde Vries, H., Methven, J. ORCID: https://orcid.org/0000-0002-7636-6872, Frame, T. H. A. ORCID: https://orcid.org/0000-0001-6542-2173 and Hoskins, B. J. (2009) An interpretation of baroclinic initial value problems: results for simple basic states with nonzero interior PV gradients. Journal of the Atmospheric Sciences, 66 (4). pp. 864-882. ISSN 1520-0469 Full text not archived in this repository. It is advisable to refer to the publisher's version if you intend to cite from this work. See Guidance on citing. To link to this item DOI: 10.1175/2008JAS2774.1 Abstract/SummaryIn the Eady model, where the meridional potential vorticity (PV) gradient is zero, perturbation energy growth can be partitioned cleanly into three mechanisms: (i) shear instability, (ii) resonance, and (iii) the Orr mechanism. Shear instability involves two-way interaction between Rossby edge waves on the ground and lid, resonance occurs as interior PV anomalies excite the edge waves, and the Orr mechanism involves only interior PV anomalies. These mechanisms have distinct implications for the structural and temporal linear evolution of perturbations. Here, a new framework is developed in which the same mechanisms can be distinguished for growth on basic states with nonzero interior PV gradients. It is further shown that the evolution from quite general initial conditions can be accurately described (peak error in perturbation total energy typically less than 10%) by a reduced system that involves only three Rossby wave components. Two of these are counterpropagating Rossby waves—that is, generalizations of the Rossby edge waves when the interior PV gradient is nonzero—whereas the other component depends on the structure of the initial condition and its PV is advected passively with the shear flow. In the cases considered, the three-component model outperforms approximate solutions based on truncating a modal or singular vector basis.
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