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This study explores the intricate relationships between ocean circulation, the carbon cycle, and climate dynamics. It emphasizes the critical role of thermohaline circulation (THC) and examines historical data from ice cores to understand the implications of changes in flow patterns. Utilizing Stommel's box model, the research discusses carbon transport and feedback loops, including temperature and salinity influences. The study aims to highlight the importance of oceanic processes in influencing terrestrial ecosystems and the broader climate system as we face potential changes driven by global warming.
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Ocean Circulation Changes Gerrit Lohmann Carbon Course 9. January 2006 @PEP, University of Bremen, Germany
Ca CO3 sediments and rocks weathering
Topics • Long-term carbon cycle: sediments & rocks • Ocean circulation, carbon cycle & climate • Ecosystem
North Atlantic: Ice Core and Marine Data YD H1 H2 Role of the Ocean Circulation? GISP2: Grootes et al. 2000Bard et al. 2000
Ocean Circulation Methaphor conversion surface deep
Carbon flux deserts High production upwelling
Stommel (1961) Box Model Heat, freshwater surface fluxes
Stommel Box Model: Advection • Advection=Transport: q T2 from low to high latitudes, contributes to T1 • q T1 from high to low latitudes, contributes to T2 • ``upstream scheme´´: Transport along the velocity direction (also ``upwind scheme´´)
Stommel Box Model: Advection • Advection=Transport: q T2 from low to high latitudes, contributes to T1 • q T1 from high to low latitudes, contributes to T2 • ``upstream scheme´´: Transport along the velocity direction (also ``upwind scheme´´) • d/dt T1 ~ q T2 • d/dt T2 ~ q T1 • d/dt (T1-T2) = -q (T1-T2) + Fluxes
Stommel Box Model: Fluxes • ``Restoring´´: Relaxation towards local temperatures • d/dt T1 ~ -r (T1 –T10) • d/dt T2 ~ -r (T2 – T20) • d/dt (T1-T2) = -q (T1-T2) -r (T1-T2 -T10+T20 ) • ``Flux for Salinity´´: P-E (precipitation-evaporation) • dS/S0 = (P-E)/h
advection noise Surface fluxes Temperature: Salinity:
Stommel (1961) Box Model Heat, freshwater surface fluxes Z: Depth Y: meridional direction
Salinity loop • S2 low • q low • q S1 low • S2 low ------------- Positive feedback
Temperature loop • T2 high (high latitude warming) • q low • q T1 low • T2 low ------------- Negative feedback -> stable
Geostrophic motion • Flow is driven by the basic pressure gradient force (PGF) and only after the flow is initiated does the Coriolis force act. • After about a day the flow has accelerated sufficiently for the PGF and Coriolis force to balance giving the geostrophic wind.
Stommel (1961) box model On-mode Off-mode
Thermohaline circulation hysteresis Hysteresis intercomparison Rahmstorf, et al.GRL, 2005 Intermediate complexity models
Box Models • Stommel‘s model was almost completey ignored (25 years) • Rooth, 1982: Two hemisphere counterpart, unaware of the Stommel (1961) model • Rooth suggested to F. Bryan: test with a GCM
What do we learn? • Multiple equilibria: robust feature of box models, GCMs • Fundamental destabilizing mechanism: salinity feedback (feedback loop) • Stability –Hysteresis Now: • Stability depends on the basic state ?
North Atlantic: Ice Core and Marine Data YD H1 H2 Role of the Ocean Circulation? GISP2: Grootes et al. 2000Bard et al. 2000
Ocean Circulation Methaphor conversion surface deep
Conveyor belt Warm water route
Conveyor belt Cold water route
Conceptual Model of the THC (~ Rooth) S1> S2 Present Cold & Warm water route South- Equator North- Atlantic S1< S2 Glacial Cold water route
Predicted Change of the THC Rahmstorf, Nature 1999
Predicted Change of the THC by several Climate Models after IPCC, 2001