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Dissipation and Bathymetric Sensitivities in an Unstructured Mesh Global Tidal Model
  • +9
  • Coleman Blakely,
  • Guoming Ling,
  • William James Pringle,
  • María Teresa Contreras,
  • Damrongsak Wirasaet,
  • Joannes Westerink,
  • Saeed Moghimi,
  • Greg Seroka,
  • Lei Shi,
  • Edward P. Myers III,
  • Margaret Owensby,
  • Thomas Christopher Massey
Coleman Blakely
University of Notre Dame

Corresponding Author:[email protected]

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Guoming Ling
University of Notre Dame
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William James Pringle
Argonne National Laboratory
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María Teresa Contreras
University of Notre Dame
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Damrongsak Wirasaet
University of Notre Dame
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Joannes Westerink
University of Notre Dame
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Saeed Moghimi
NOAA/NOS
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Greg Seroka
NOAA/NOS Coast Survey Development Lab
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Lei Shi
National Oceanic and Atmospheric Administration (NOAA)
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Edward P. Myers III
NOAA CSDL
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Margaret Owensby
Coastal and Hydraulics Laboratory, Engineer Research and Development Center
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Thomas Christopher Massey
USACE ERDC
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Abstract

The mechanisms and geographic locations of tidal dissipation in barotropic tidal models is examined using a global, unstructured, finite element model. From simulated velocities and depths, the total dissipation within the global model is estimated. This study examines the effect that altering bathymetry can have on global tides. The Ronne ice shelf and Hudson Bay are identified as a highly sensitive region to bathymetric specification. We examine where dissipation occur and find that high boundary layer dissipation regions are very limited in geographic extent while internal tide dissipation regions are more distributed. By varying coefficients used in the parameterizations of both boundary layer and internal tide dissipation, regions that are highly sensitive to perturbations are identified. Particularly sensitive regions are used in a simple optimization technique to improve both global and local tidal results. Bottom friction coefficients are high in energetic flow regions, across the arctic ocean, and across deep ocean island chains such as the Aleutian and Ryuku Islands. Global errors of the best solution in the $M_2$ are 3.10 \si{cm} overall, 1.94 \si{cm} in areas deeper than 1000 \si{m}, and 7.74 \si{cm} in areas shallower than 1000 \si{m}. In addition to improvements in tidal amplitude, the total dissipation is estimated and compared to astronomical estimates. Greater understanding of the geographical distribution of regions which are sensitive to friction allows for a more efficient approach to optimizing tidal models.