Understanding Balanced Vortex Dynamics in Tropical Cyclones

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Exploring the application of Potential Vorticity (PV) thinking in understanding tropical cyclones, focusing on Wayne Schubert's contributions to balanced vortex dynamics. The discussion covers the beauty of PV-thinking in relation to baroclinic instability, the analogy between baroclinic wave dynamics and balanced vortex equations, and the insights gained from nonhydrostatic, axisymmetric equations.


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  1. PV-Thinking and Tropical Cyclones: Wayne Schubert s Contribution to Balanced Vortex Dynamics Kerry Emanuel Lorenz Center MIT

  2. Main Points What s wrong with comprehensive complexity? The beauty of PV-thinking in understanding baroclinic instability Wayne Schubert s application of PV thinking to tropical cyclones The analogy between surface semigeostrophy for baroclinic wave dynamics and an extension of Wayne s transformed balanced vortex equations for tropical cyclones

  3. Nonhydrostatic, Axisymmetric Equations u t v t u r v r u z v z v r + + = + v c + , u w f D p v u r v r + + = + + , u w f u D v w t w r w z + + = + + , u w c g D p v w z 2 1 r r c ( ) ( ) + + = 0, ru w v v 2 t c z p v s s r s z + + = + , v v v u w D R s t L Density temperature + , v s q v v v c Diffusion of x, Radiation D R p x + conservation of water

  4. Nonhydrostatic, Axisymmetric Equations u t v t u r v r u z v z v r + + = + v c + , u w f D p v u r v r + + = + + , u w f u D v w t w r w z + + = + + , u w c g D p v w z 2 1 r r c ( ) ( ) + + = 0, ru w v v 2 t c z p v s s r s z + + = + , v v v u w D R s t Density temperature L + , v s q v v v c Diffusion of x, Radiation D R p x + conservation of water

  5. Simulation Understanding Comprehensive complexity is no virtue in modelling, but rather an admission of failure -- Ian James

  6. Semi-geostrophy and PV-thinking (after Brian Hoskins) V d V d dt g Geostrophic momentum approximation: dt v g + , X x f Geostrophic coordinates: u g Y y f 1 2 ( ) + + 2 g 2 g u v Rephrasing of geopotential:

  7. Semi-geostrophic Eady Problem: Constant potential vorticity, qg, between two plates 1 f 1 q ( ) + + = 1 Invertibility: XX YY 2 g Conservation of on boundaries: + + = = 0 on Z 0, U V H g g X Y Z All the dynamics collapse to conservation of potential temperature on the two boundaries

  8. Baroclinic Instability Image credit: Kerry Emanuel

  9. Wayne Schubert* extended the semigeostrophic framework to semigradient axisymmetric vortices 1 2 1 2 + = 2 2 fR rV fr M Coordinate transform: R "Potential Radius" 1 g = q Potential vorticity: f Z 3 = R r r Z r r + 2 0 f qR R Invertibility: 2 Z R *Schubert, W. H., and J. J. Hack, 1983: Transformed Eliassen-balanced vortex model. J. Atmos. Sci., 40, 1571-1583.

  10. Eady Analogy Except for their eyes, TCs are nearly zero saturation PV vortices 1 * q f * e g 0 * e Z Neutrality to slantwise moist convection ( ) * e ln d 1 r 1 r ( ) = c T T Invertibility: p b o 2 2 MdM b t e Lower boundary condition: Boundary layer Neglects downdraft flux through PBL top d dM dt + = e e e M dt Surface drag Surface enthalpy flux

  11. Angular momentum and *e from nonhydrostatic, axisymmetric simulation:

  12. As with Eady model, all the dynamics collapses to evolution of e in boundary layer and at tropopause Together with upper boundary condition that assumes that the Richardson Number equals its critical value, one may derive and approximate equation for TC intensification, assuming that the core of the storm is always saturated: V C ( ) = 2 pot 2 max k h V V max 2 C V k pot h = tanh V V max pot 2

  13. Comparison to axisymmetric, nonhydrostatic model

  14. Summary Much has been learned about tropical cyclone dynamics through Wayne Schubert s semi-gradient equations Like baroclinic waves, the action in tropical cyclone occurs in the boundary layer and at or near the tropopause, because the interior (saturation) potential vorticity is passive Unlike in baroclinic waves, reversible boundary advection is unimportant compared to surface enthalpy fluxes and drag Supergradient winds in the boundary layer appear to have little effect on the interior flow or on surface winds

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