MPO 674 Lecture 9 2/10/15 Hypotheses 1. Singular Vector structures are dependent on the barotropic instability condition in the initial vortex. 2. The spreading in TC track forecasts is due to instabilities in the storm and its environment. Singular Vectors Solve “analysis error covariance optimals” via Result: perturbation structures that grow, in a linear sense, to maximize total energy within a verification region around the tropical cyclone. Compute here for barotropic version of Spectral Element Ocean Model (SEOM, Iskandarani 2008), with initial vortices on f- and beta-planes. Yamaguchi et al. (2011, JAS) Necessary condition for barotropic instability NOT satisfied Transient growth, upshear tilt vanishes. f-plane Necessary condition for barotropic instability satisfied SVs capture barotropic instability, faster growth. Yamaguchi et al. (2011, JAS) beta-plane: Sinlaku Yamaguchi et al. (2011, JAS) beta-plane: Sinlaku Yamaguchi et al. (2011, JAS) Results 1 H: SV structures are dependent on the barotropic instability condition in the initial vortex. • f-plane: initial vortices don’t meet barotropic instability condition: – – – • f-plane: initial vortices meet barotropic instability condition: – – • SVs tilted against shear, grow via Orr mechanism Leading singular value increases with Vmax, decreases with RMW Locations of SVs move outward with RMW SVs initially tilted against shear, period of transient growth SV then locks into normal mode structure, grows exponentially Beta-plane: – – All 1st and 2nd SVs have a wavenumber 1 structure at topt Some dependence on resolution Hypotheses 1. Singular Vector structures are dependent on the barotropic instability condition in the initial vortex. 2. The spreading in TC track forecasts is due to instabilities in the storm and its environment. Ensemble prediction systems NCEP: use Ensemble Transform to initialize ensemble. ECMWF: use Singular Vectors to initialize ensemble. What mechanisms cause the spreading of the ensemble members? ECMWF NCEP Background steering 0h Asymmetric propagation 12 h Yamaguchi and Majumdar (2010, MWR) Theory Ensemble perturbation Shading: Streamfunction Contour: Temperature Baroclinic instability centered on the vortex Perturbation draws eddy available potential energy from mean flow Yamaguchi and Majumdar (2010, MWR) Radial heat flux Wind 0h 6h 12 h Eddy APE is converted into EKE wind perturbation grows where radial heat flux is positive 18 h Yamaguchi and Majumdar (2010, MWR) Results 2 H: The spreading in TC track forecasts is due to instabilities in the storm and its environment. • Growth of advection flow perturbations for Sinlaku is larger in ECMWF than NCEP. • Perturbation growth in ECMWF ensemble associated with – – – 1) baroclinic energy conversion in a vortex, 2) baroclinic energy conversion in midlatitude waves, 3) barotropic energy conversion in a vortex.
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