Potential Vorticity Thinking

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Presentation transcript:

Potential Vorticity Thinking Chapter 6 Potential Vorticity Thinking

Ertel potential vorticity Define The Ertel potential vorticity The 3D absolute vorticity f + w Ertel’s theorem: for frictionless adiabatic motion EPV is conserved following fluid parcels

EPV in isentropic coordinates q + Dq f + z q

Standard PV distribution Standard distribution 1 PV unit = 10-6 m2s-1 K kg-1  10 K per 100 mb at 45o lat.

Mean meridional distribution of PV tropopause latitude

A PV chart 30 September 1982

20oN cutoff high Trough B cutoff at 315 K Trough B Trough C Trough D clear at all levels Trough D clearest at 330 K 20oN 30 September 1982

330 K 24 – 29 September 1982 250 mb

Development of an Atlantic cutoff low 300 K 500 mb 40oN 20 – 25 September 1982

Vertical structure through a cutoff low

30-04-90 02-05-90 315 K 01-05-90 03-05-90

330 K 250 mb 30 September – 7 October 1982 Region 30oN - 80oN and 60oW - 60oE

330 K 250 mb 80oN 80oN 30oN 2 October 1982

+ PV anomaly   - PV anomaly  

+ PV anomaly   - PV anomaly  

Elements of PV thinking PV anomaly: defined as a deviation of PV contours from a background or reference state. e.g. troughs may be defined as positive PV anomalies (NH) resulting from equatorward displacement of PV contours relative to reference state. Conservation: emphasizes dynamical properties of flow features that depend on their material nature (e.g. propagation of Rossby waves arising from displacement of PV contours; motion of vortices due to advection of isolated regions of fluid).

Elements of PV thinking Invertibility: Given specification of a reference state, balance condition, and boundary conditions, the PV field uniquely determines (i.e. induces) the flow field. Allows inference of action at a distance. Attributability: PV field may be partitioned in a piecewise sense, allowing consideration of interactions among the respective constituents through their induced flow fields.

Elements of PV thinking Scale effect: For a given magnitude of PV, small-scale features contribute weakly to the velocity field induced by a given PV anomaly, whereas large-scale features contribute strongly to the velocity field. Scale effect depends also on the anisotropy of a PV anomaly (i.e. maximized for isotropic anomalies and reduced for increasing anisotropy).

Mechanisms for system evolution Rossby-wave dispersion: Referred to as downstream development; it is a consequence of the property of Rossby/PV waves and tropopause-based edge waves that cgroup > cphase , resulting in the sequential formation of troughs and ridges in the downstream direction and dissipation in the upstream direction.

Mechanisms for system evolution Superposition: Increase in the total perturbation energy arising from a reconfiguration of a given PV anomaly (e.g. through axisymmetrization in a deformation flow) or from a change in the relative position between separate PV anomalies. Perturbation enstrophy is conserved

Mechanisms for system evolution Exponential (modal) growth: Mutual intensification of counter-propagating wave trains on opposite-signed basic-state PV gradients in the presence of background vertical shear. Characterized by fixed vertical structure resulting from phase locking of wave trains. Total perturbation energy and enstrophy increase.

The End