Numerical simulations of freely-evolving turbulence generated by baroclinic instability, in both quasigeostrophic and Boussinesq models, verify the predictions and reveal that the jump in stratification has two effects: it alters the Green's function in the region of the jump, and it produces a peak in PV near the jump, approaching a Dirac delta-function as δ → 0. When the Green's function is integrated against this sharp PV distribution, contributions far from the jump (|z| ≫ δ) are suppressed, and the kinetic energy spectrum flattens. This occurs for a range of wavenumbers above the deformation wavenumber associated with the vertical extent H0 of the domain, f/(N0H0), but smaller than a wavenumber associated with the vertical scale of the jump, Kδ = f/(Nd δ). The vertical distribution of the flattened spectrum decays over a distance proportional to δ. Implications of these results for observations of geostrophic turbulence in the upper ocean will be discussed.
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