arctic sea ice freeboard from icesat altimetry
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Arctic sea ice freeboard from ICESat altimetry NASA SNAME Luncheon, October 19 th , 2011 Vidya Renganathan Contractor, Chevron Arctic Center Changing ice conditions What is also important is the ice thickness, its distribution and its


  1. Arctic sea ice freeboard from ICESat altimetry NASA SNAME Luncheon, October 19 th , 2011 Vidya Renganathan Contractor, Chevron Arctic Center

  2. Changing ice conditions What is also important is the ice thickness, its distribution and its inter-annual variability. 2

  3. Why care about sea ice thickness? Quest for natural resources 3

  4. Why care about sea ice thickness? UNEP Chevron Arctic Center Sea routes Ice management 4

  5. Why care about sea ice thickness? Bottom force I ce force 1 0 m 1 Base Friction h Line of excavation 4 Native sand Chevron Arctic Center Ice-structure interaction 5

  6. Research Objective Can ICESat laser altimetry data provide sea ice freeboard and thickness estimates? How do the sea ice freeboards derived in this study compare with other • methods? How do the sea ice thicknesses derived in this study compare with • other methods? What are the magnitudes of uncertainty in the estimated sea ice • freeboard and thickness? 6

  7. Ice Cloud Elevation Satellite – ICESat 7 NASA

  8. Freeboard estimation from ICESat Total Freeboard = snow surface – sea surface Range (Snow) Snow surface = Orbital height – Range (Snow) Chevron Arctic Center 8

  9. Freeboard estimation from ICESat Total Freeboard = snow surface – sea surface Range 1. “Observed” = Orbital height – Range (sea (Snow) surface) Oceanographic models 2. = Geoid + Tides + Mean dynamic topography + inverse barometric effect Chevron Arctic Center 9

  10. Sea surface heights from models Sea surface = Geoid + Tides + Mean Dyn. Topo. + Inv. Barometric Effect Ice freeboard = Snow surface – Sea surface – Snow depth – errors Snow depth Freeboard Tides + Mean Dyn Topo Snow surface Geoid Chevron Arctic Center 10

  11. Geoid, Tides, Mean Dynamic Topography Mean Dyn Topo Tides Geoid UW AOTIM-5 EIGEN-GL04c model Univ. Washington Oregon State Univ. GFZ Germany 11

  12. Comparison with ‘observed sea surface’ method DNSC Feb 2006 ICESat period 12

  13. Validation of ICESat elevations in Churchill Precise leveling – Sep 2006 GPS Real-time Kinematic – Mar 2008 Co-incident field measurements were taken along the predicted ICESat track on the ground 13

  14. Validation of ICESat elevations in Churchill Surface Type ICESat – Precise leveling (m) Surface Type ICESat – GPS RTK (m) Wetlands 0.60 Sea ice < 0.10 Runway 0.20 Boreal forests 0.90 Coast > 1.0 Tidal flats 0.30 14

  15. Sea ice thickness distribution compared to Helicopter Electro-magnetic measurements – May 2006 HEM data: Christian Haas, U of A Two methods agree within 53 cm 15

  16. Sea ice thickness distribution compared to JIP Arctic Islands thickness data (APOA) 16

  17. Summary and Outlook Summary • Freeboard distributions show good agreement with ‘observed’ freeboards • Sea ice thickness shows good agreement with HEM-based thickness estimates and JIP data (APOA) • Sensitivity analysis indicates an error of about 24 cm in freeboard estimates Sensitivity analysis indicates an error of about < 98 cm in thickness estimates • Outlook • Mean Dynamic Topography was the major source of error • The accuracy of this method will improve automatically when the accuracy of the component models continues to improve in the future • An optimal Sea Surface Height estimate can be obtained by combining both ‘observed’ and modeled SSH www.ucalgary.ca/engo_webdocs/AB/10.20301_VRenganathan.pdf 17

  18. 2011 studies – Cryosat-2 radar altimeter 18

  19. Questions? 19

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