Abstract
Using the global environmental multiscale (GEM) model, we investigate the impact of increasing model resolution from 2° to 0.3° on Atlantic tropical cyclone activity. There is a clear improvement in the realism of Atlantic storms with increased resolution, in part, linked to a better representation of African easterly waves. The geographical distribution of a Genesis Potential Index, composed of large-scales fields known to impact cyclone formation, coincides closely in the model with areas of high cyclogenesis. The geographical distribution of this index also improves with resolution. We then compare two techniques for achieving local high resolution over the tropical Atlantic: a limited-area model driven at the boundaries by the global 2° GEM simulation and a global variable resolution model (GVAR). The limited-area domain and high-resolution part of the GVAR model coincide geographically, allowing a direct comparison between these two downscaling options. These integrations are further compared with a set of limited-area simulations employing the same domain and resolution, but driven at the boundaries by reanalysis. The limited-area model driven by reanalysis produces the most realistic Atlantic tropical cyclone variability. The GVAR simulation is clearly more accurate than the limited-area version driven by GEM-Global. Degradation in the simulated interannual variability is partly linked to the models failure to accurately reproduce the impact of atmospheric teleconnections from the equatorial Pacific and Sahel on Atlantic cyclogenesis. Through the use of a smaller limited-area grid, driven by GEM-Global 2°, we show that an accurate representation of African Easterly Waves is crucial for simulating Atlantic tropical cyclone variability.
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Notes
In the cases where two minima in pressure were recorded within a <2° radius of each other, the highest pressure coordinate was discarded.
This value was chosen in order to allow direct comparison with the storms stored in the National Hurricane Center best track database (HURDAT; available online at http://www.nhc.noaa.gov/pastall.shtml).
The jumpy looking tracks in GEM 2°, and to a lesser extent in GEM 1°, are caused by the coarse resolution of these simulations.
Details on MPI are given in Appendix.
\(\hbox{SOI} =\frac{\hbox{Standardized MSLP Tahiti}- \hbox{Standardized MSLP Darwin}}{\hbox{Monthly standard deviation}}.\)
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Acknowledgements
The authors would like to thank ECMWF for making the ERA-40 reanalyses available and the National Hurricane Center for the use of their tropical cyclone best track data (HURDAT). The authors are also grateful to Kerry Emanuel for making the MPI FORTRAN routine available, to Bernard Dugas for many helpful discussions and to Fabrice Chauvin and an anonymous reviewer for their valuable recommendations in improving this paper. This research was supported by the Natural Sciences and Engineering Research Council of Canada and the Mathematics of Information Technology and Complex Systems (MITACS, grant number 61851).
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A maximum potential intensity
A maximum potential intensity
The definition of maximum potential intensity is described in detail in Emanuel (1995) and Bister and Emanuel (1998). A Fortran subroutine to evaluate MPI provided by Kerry Emanuel is available at ftp://texmex.mit.edu/pub/emanuel/TCMAX. The formula used is
where V m is the maximum wind speed a storm can reach in current atmospheric condition (MPI), T s is the ocean temperature, T 0 them mean outflow temperature, C k the exchange coefficient for enthalpy and C d the drag coefficient. CAPE is the vertical integral of parcel buoyancy as a function of surface temperature, pressure, and specific humidity, as well as the vertical profile of virtual temperature. CAPE* is the value of CAPE for an air parcel lifted from saturation at sea level at the radius of maximum winds and CAPEb is the CAPE of the boundary layer air.
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Caron, LP., Jones, C.G. & Winger, K. Impact of resolution and downscaling technique in simulating recent Atlantic tropical cylone activity. Clim Dyn 37, 869–892 (2011). https://doi.org/10.1007/s00382-010-0846-7
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DOI: https://doi.org/10.1007/s00382-010-0846-7