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Particle flux experiments with HAMOCC and LSG or MPIOM. E.Maier-Reimer, C.Heinze, I.Kriest, J.Segschneider, K.Six, M.Howard, J.Tjiputra, A.Winguth. 3Box models eg Harvardton Bear 20 Box eg Pandora 2.5 dimensional eg Wright/Stocker Genie LSG GCM coarse (~200 km) GCMHR (<30 km).
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Particle flux experiments with HAMOCC and LSG or MPIOM • E.Maier-Reimer, C.Heinze, I.Kriest, J.Segschneider, K.Six, M.Howard, J.Tjiputra, A.Winguth
3Box models eg Harvardton Bear 20 Box eg Pandora 2.5 dimensional eg Wright/Stocker Genie LSG GCM coarse (~200 km) GCMHR (<30 km) Hierarchy of models Onset of dynamics Understanding lacks Schlitzer
LSG vs Genie • Both aiming essentially geostrophy • fxU=-gradP • -rU (Genie, „Rayleigh“ friction) • -U t (LSG, damping of gravity waves by time discretization). Definitely more arithmetics for given resolution. • Structures similar but Genie more sluggish
HAMOCC versions • HAMOCC2: annual mean circulation, convection parameterized as diffusion, production from restoring surface P to 0 with 3 months (many Heinze et al. Papers 1989 and later). • HAMOCC3: Seasonal cycle EMR 1993 • HAMOCC4: explicit plankton dynamics and multicomponent sediment Six,EMR 1996 • HAMOCC5 competing N,P,Fe, denitrification and N-fixation Aumont, Wetzel 2002,05
Natural Radiocarbon GOSAC
Prerequisites for modeling • Realistic circulation • Realistic boundary conditions and forcing • Realistic process formulation • What happens if one or more not? • It is not foreseeable
2cm/a 15cm/a Spreading rate of midoceanic rideges,source for δ3He
Multitracer approach is a must! • Unfortunately our funding agency didn‘t perfectly agree
On remineralization profiles • (wP)z= -rP exponential profile • Suess, Martin : Fp ~ z-α (0.8< α<1) • Fz = - (r/w)F • If somehow (r/w)=a/z, F=F0z -a • How to generate a/z? • Temperature, particle aggregation with/out dust particles, mineral ballast loading
Validation of dust input through simulation of dissolved Al Gehlen, Heinze, Maier-Reimer and Measures, 2003, Global Biogeochem. Cycles
Assimilation of data • Look at data and tune parameters. • Have all model feedbacks in mind • Create the adjoint code (more by Thomas) • Winguth (1996) took δ13C for determination of glacial climate forcing with HAMOCC3 • Tjiputra (2006) did it for chlorophyll and nitrate for the full plankton model
Chlorophyll (mg-3) for the first guess integration (4 seasons)
Particle aggregation (Kriest, Evans) • θ =aggregate diameter • ε =slope of size distribution in log diagram • size spectrum P(θ)= Aθ-ε • Number of aggregates =A int θ-ε dθ • W( θ)= B θη
Vertical distribution of POC southern ocean global
Vertical distribution of POC North Atlantic Equatorial Pacific
d13C profiles atlantic/pacific NADW signature DEPTH [m] North Pacific Atlantic off Recife
D14C profiles t1/2=5700a ‘new’ deep water oldest water intermediate age (300a) old water (1000a) MPIOM/HAMOCC5 GR15L40
global Export across 90 m vs primary production
Reg. Prod (no O) New prod. from NO3 (O-isotopes) N2 algae NH3 algae Remineralization Release of NH3 locally NO3 consumption with isotopic fractionation Nitrate depleted vs P, enriched in heavy isotopes oxidation
d13c profile 12C evaporates more easily and is preferred by plankton during photosynthesis (20o/oo) remineralisation of organic matter inflow of deep water originating from low SST regions (evaporative fractionation is temperature dependent, with higher 13C in colder water) DEPTH [m] 13C profile in the North Pacific from GR15L40 MPIOM/HAMOCC5 4 years after initialisation from PO4 ? (model 13C not yet in equilibrium)