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Innovative methods for tropical cyclone genesis

Outline . Introduction: Flosolver LabProblem of Tropical cyclone (TC) genesis/track predictionTC genesisVortex merger theoryPrediction methodTC track Effect of new boundary layer Conclusion. Flosolver Lab. 1980's

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Innovative methods for tropical cyclone genesis

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    1. Innovative methods for tropical cyclone genesis/track prediction T. N. Venkatesh Flosolver Unit National Aerospace Laboratories Bangalore, INDIA tnv@flosolver.nal.res.in

    2. Outline Introduction: Flosolver Lab Problem of Tropical cyclone (TC) genesis/track prediction TC genesis Vortex merger theory Prediction method TC track Effect of new boundary layer Conclusion

    3. Flosolver Lab 1980’s – denial regime – in-house ``supercomputer’’ development India’s first parallel computer in 1986 Six generations

    4. Flosolver Lab NAL / Flosolver : parallel computer for fluid dynamics Atmospheric modelling for nearly two decades

    5. Tropical cyclones Of both scientific and practical interest Track, intensity prediction Genesis Storm surge Accurate track forecasts have considerable societal value. Genesis prediction, could help in advanced warning

    6. TC Genesis: Gray’s conditions Warm sea waters ( > 27 degrees) Weak vertical shear of wind Latitude greater than 5 degrees Conditions suitable for moist convection

    7. Earlier theories : CISK Conditional Instability of the Second Kind Charney 1964 Growth at realistic length and time scales Short wavelength cutoff Energy source

    8. Earlier theories : WISHE Air – Sea interaction Emanuel, 1986 Integral view of moisture/heating Finite amplitude nature Energy source

    9. Vortex merger theory (PhD Thesis: T. N. Venkatesh, IISc, April 2003) Stage 1: Mid -level mesoscale vortices interact. If this interaction results in merger, the second stage is reached Stage 2: This larger vortex increases in strength due to the air-sea interaction mechanism

    10. Numerical simulations Stage 1: 2 D vortex patch studies Critical distance for merger of regular configurations of vortex patches These occur at length and time scales relevant to atmospheric vortices

    11. Two patches

    12. Two patches

    13. Three patches

    14. Three patches

    15. Four patches

    16. Four patches

    17. Critical distance for merger

    18. Stage 2 Axisymmetric model Clouds Boundary layer ... Mid-level vortices decay, but a deep vortex which extends down to the boundary layer amplifies

    19. Observational Evidence from IR Images Merger of MCVs prior to TC formation using satellite images and observed wind fields

    20. Prediction method R_cg : Average distance of the systems from centroid L : Average radius of the systems r*(n) : Critical radius of merger

    21. Vortex merger index Calculated from satellite IR images From the CIMSS website (3 hour intervals) Studies in the Bay of Bengal Real-time tests since October 2002 Can give advance warning for formation by about 48 hours Geophysical Research Letters, Vol 31, L04105, February 2004 Four seasons : Eight events 6 lead to TC formation 2 False alarms (depressions formed)

    22. The merger index

    23. Test cases

    24. Recent seasons

    25. Possible use of additional data from Megha-Tropiques Mesoscale structures (MCSs, MCVs) Validate theory Earlier detection of MCS/MCVs Velocity fields ?

    26. Track prediction

    27. NMITLI project on “Mesoscale modelling for monsoon related predictions” NAL, IISc, TIFR team – Option A software Development of a new prediction code to be run efficiently on NMITLI hardware Reengineered NCMRF T-80 code forms the backbone for the present model: Written in Fortran 90 New boundary layer module New radiation module Grid clustering

    28. NMITLI Code – Version 1 Operational on Flosolver MK6 Rewritten in Fortran 90 Seed code: NCMRWF/NCEP GCM T-80 Incorporates new physics modules Boundary layer Radiation Engineered software Code length reduced Nanjundiah & Sinha, Current Science, 1999

    29. New boundary layer scaling at low winds Tropics characterized by convection at low winds Monin-Obukhov not applicable Usual fix: Gustiness parameter (Hack et al, 1993) New parameterization in NMITLI code for weakly forced convection “Heat-flux scaling for weakly forced turbulent convection in the atmosphere” K. G. Rao and R. Narasimha, JFM 2005 Based on data from MONTBLEX-90 (Narasimha, Sikka and Prabhu 1997) and BLX-83 (Stull 1994)

    32. Implementation of new parameterization Weakly forced convection Drag is a linear function of wind speed Heat flux is independent of wind speed Define matching velocity -Vm V > Vm use M-O estimates V < Vm use Heat flux scaling Match at Vm Integrated into the NMITLI GCM and tested Values of Vm : 1, 3, 5 m/s

    33. Low resolution : 80 Modes :Old BL

    34. Low resolution : 80 Modes: New BL

    35. Higher resolution :120 Modes: Old BL

    36. Higher resolution:120 Modes: New BL

    37. Higher resolution:120 Modes: New BL

    38. Orissa Supercyclone 1999 Track errors

    39. Track improvement : Preliminary analysis Surface force on the TC due to the PBL computed Within a radius of 8 grid lengths (approximately 640 km) from centre of TC Total torque

    40. Preliminary analysis: Stress fields

    41. Surface force on TC

    42. Possible use of additional data from Megha-Tropiques Surface fluxes Heat Moisture Accurate fixing of the Initial position of the Tropical Cyclone

    43. Concluding remarks Tropical Cyclone genesis New prediction method Results are encouraging Further work is necessary Tropical Cyclone track Use of a new boundary layer scaling improves track simulation significantly Additional data from the Megha-Tropiques satellite would help in refining these schemes

    49. Cyclone 03B, 2003 Track errors

    50. Radiation Module Long wave - new code based on work of Varghese etal Valid from surface to 100 km Accurate near the surface Integrated into NMITLI Code Version 1 CPU time Being optimized Look up table

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