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Atlantic Multidecadal Variability and the role of natural forcing in BCM

Atlantic Multidecadal Variability and the role of natural forcing in BCM. Odd Helge Otterå, Mats Bentsen, Lingling Suo and Helene Langehaug (Nansen/Bjerknes). Bergen Climate Model (version 2). ARPEGE. ARPEGE Resolution: T42, ~2.8x2.8, 31 layers Volcanic aerosols implemented MICOM

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Atlantic Multidecadal Variability and the role of natural forcing in BCM

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  1. Atlantic Multidecadal Variability and the role of natural forcing in BCM Odd Helge Otterå, Mats Bentsen, Lingling Suo and Helene Langehaug (Nansen/Bjerknes)

  2. Bergen Climate Model (version 2) ARPEGE • ARPEGE • Resolution: T42, ~2.8x2.8, 31 layers • Volcanic aerosols implemented • MICOM • Resolution: ~2.4x2.4, 35 isopycnic layers • New pressure gradient formulation • Reference pressure at 2000 m • Incremental remapping for tracer advection (better conservation) • Thermodynamic and dynamic sea-ice modules • GELATO: multi-category ice • NERSC: one ice layer only MICOM

  3. Performed simulations with BCM CONTROL600: All forcings kept constant at pre-industrial (1850) level NATURAL600: Same as CONTROL600, but with historic total solar irradiance (TSI) and volcanic aerosol variations for the last 600 years All150: Same as NATURAL600, but with variations in well-mixed greenhouse gases and tropospheric sulfate aerosols. Total of 5 ensemble members performed.

  4. Atlantic Merdional Overturning Circulation CONTROL600 16.6 Sv Otterå et al 2009, GMD, in press

  5. Comparison to Levitus for control Southern Ocean problem! Otterå et al 2009, GMD, in press

  6. Sea ice and NA surface ocean circulation Otterå et al 2009, GMD, in press

  7. Ventilation sites in BCM (control run) • Late winter Mixed Layer Depth (MLD) averaged over 700 years. • MLD > 1100 m in 10 winters: • 3 convection regions • Greenland Sea • Labrador Sea • Irminger Sea Courtesy of H. Langehaug

  8. Regression of MLD & AMOC Max MLD in GS ~17yrs after max AMOC Max MLD in LS ~8yrs before max AMOC Regression between the Mixed Layer Depth averaged over the convection regions and the AMOC. MLDLS is leading AMOC Courtesy of H. Langehaug

  9. Another way to investigate the propagation of intermediate and deep water masses… Max MLD in LS ~8yrs before max AMOC Lag=-20yrs Lag=-10yrs Lag=0yrs Anomalies in the thickness of the intermediate layer (interface σθ=27.75) is regressed with AMOC Max MLD in GS ~17yrs after max AMOC Lag=30yrs Lag=10yrs Lag=20yrs Courtesy of H. Langehaug

  10. Natural run: Applied forcing(Crowley et al. 2003) Effective solar constant Dalton Minimum Maunder Minimum Spörer Minimum Krakatoa 1883 Kuwae 1452 Tambora 1815 Otterå et al 2009

  11. Settlement on Iceland & Greenland Today Little Ice Age Reconstructed and observed N Hemisphere temperature Temperature anomaly (ºC) Year Mann et al. 2008

  12. Simulated NH response Krakatoa 1883 Kuwae 1452 Tambora 1815 Otterå et al 2009

  13. Simulated time-latitude variability of SAT (ALL forcing run, relative 1961-1990)

  14. 1816 – The year without a summerFollowing the 1815 Tambora eruption(relative 1500-1899) Mary Shelley

  15. The winter warming phenomenon Composite of 10 largest tropical eruptions

  16. Simulated time-latitude variability of SAT (ALL forcing run, relative 1961-1990)

  17. Simulated Early Warming in the Arctic2 m temperature, 60-90oN Suo et al, in prog

  18. Atlantic Multidecadal Oscillation (AMO) Average SST 75W-7.5W; 0-60N Sutton & Hodson, 2005, Science

  19. Observed AMO Simulated AMO °C per SD-AMO

  20. Observed AMO Simulated AMO °C per SD-AMO

  21. Similarities between observed and simulated ✓ NH Temperature (1400-2000) ✓ AMO (1860-2000) and ✓ Early Warming (1930-50) for NATURAL and all members of ALLforcing, but not for CTRL

  22. Natural forcing as a pacemaker for Atlantic multidecadal variability? Otterå et al 2009

  23. Power spectrum for AMO and AMOC (shading: 60-100 yr) Control600 Natural600 More power on 60-100 yr time scales in NATURAL Otterå et al 2009

  24. Variability in the simulated strength of AMOC is – mainly – governed by Labrador Sea mixing with a lag of about 8 years. Holds for both CTRL and NATURAL. ~ 8 yr lag

  25. Lag-correlations (30 yr filter): AMO vs LabSea/AMOC/RadTOA CONTROL600 NATURAL600 LS density and AMOC lead by 15 and 8 years No lag with Rad TOA; LS density and AMOC lag by 5 and 15 years Otterå et al 2009

  26. Lag-correlations (unfiltered time series): Forcing vs LabSea/AMOC/RadTOA NATURAL600 Volcanoes plays a key role!

  27. Surface T and Atlantic streamfunction regressed onto AMO About 90 yr cycle

  28. AMOC linked to the derivative of the AMO (AMO ROC): Atmosphere link? AMOC SLP regressed onto the AMO ROC index

  29. AMO vs other climate parameters

  30. EOF1 NAO-index: reconstructed vs model pc1 10 yr running mean

  31. Reconstructions from Gardar Drift G. inflata Sortable silt warm strong Winter temp Overf low cold weak Courtesy of Tor Mjell and U. Ninnemann

  32. Upper ocean (300 m) temperature regressed on AMO-index (lag 0) The Gardar Drift region anti-correlates with the AMO-index in the simulation

  33. Simulated winter temperature Gardar drift vs AMO-index

  34. Preliminary summary Main features of the observed multidecadal variability in the Atlantic region are simulated by the model The simulated multidecadal variability is strongly linked to changes in the combined effect of solar irradiance and aerosol variations, rather than to internal variability from the ocean component (2) needs to be supported by other models/studies The simulated AMOC in BCM is out of phase with AMO  strong AMOC in cold times and vice versa If these findings are robust, decadal-scale predictability experiments need to take into account future changes in solar irradiance and aerosol variations (volcanoes included)

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