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Radiative Feedback Analysis of CO2 Doubling and LGM Experiments

Radiative Feedback Analysis of CO2 Doubling and LGM Experiments. JSPS 5 th University Allied Workshop (2 July 2008, Sunroute-Plaza Tokyo). ○ M. Yoshimori, A. Abe-Ouchi CCSR, University of Tokyo and T. Yokohata National Institute for Environmental Studies. Climate Sensitivity.

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Radiative Feedback Analysis of CO2 Doubling and LGM Experiments

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  1. Radiative Feedback Analysis of CO2 Doubling and LGM Experiments JSPS 5th University Allied Workshop(2 July 2008,Sunroute-Plaza Tokyo) ○M. Yoshimori, A. Abe-Ouchi CCSR, University of Tokyo and T. Yokohata National Institute for Environmental Studies

  2. Climate Sensitivity • Climate sensitivity is a convenient metric that represents gross size of the climate change response. • Often expressed in terms of temperature change due to doubling of CO2 • “Chaney report” (1979): 1.5-4.5 K • IPCC TAR (2001): 1.5-4.5 K; IPCC AR4 (2007): 2.0-4.5 K • Perturbed physics ensemble Murphy et al., 2004 Stainforth et al., 2005 There is still a substantial range of uncertainty in the estimate of climate sensitivity, particularly in the higher end. Needs more constraint!

  3. Constraining climate sensitivity (1) • Last 150 years or so • Large uncertainty in forcing (esp. indirect effect of aerosols) • Effect of ocean heat uptake • Last 1-2 millennia • Relatively small forcing (solar forcing) with large uncertainties (incl. volcanic forcing) • Consensus on the global or hemispheric mean temperature reconstruction remains to be made

  4. Constraining climate sensitivity (2) Last Glacial Maximum (LGM) ~ 21,000 years ago • Relatively known forcing • Estimation from reconstructions/data • Hoffert and Covey, 1992; Hansen et al., 1993, Lea, 2004 • Comparison between models with specific sensitivities and data • Manabe and Broccoli, 1985; Hewitt and Mitchell, 1997; Broccoli, 2000; Hewitt et al., 2001 • Comparison between perturbed physics ensembles and data • Annan et al., 2005; Schneider von Deimling et al., 2006 But, fundamental questions remain to be explored: • Climate sensitivity may be determined differently between future warming and ice ages (Hewitt and Mitchell 1997, Crucifix 2006, Hargreaves et al., 2007) ? If so, why?

  5. Model Experiments and Feedback Analysis • Purpose • To quantify the strength of individual feedback processes for 2xCO2 and LGM experiments and to reveal similarities and differences • To obtain ideas on how temperature changes are determined in those experiments in themodel • Model • AGCM (T42/L20)-slab version of MIROC3.2: jointly developed by CCSR/NIES/FRCGC • Experiments • Preindustrial simulation (CTRL) • Doubling of atmospheric CO2 (2xCO2) • Last Glacial Maximum (LGM) • CTRL+LGMgreenhouse gas (LGMGHG)

  6. sfc albedo temperature mixing ratio clouds PRPFeedback Analysis(Wetharald and Manabe, 1988) feedback P:radiative damping, WV:water vapor, LR:lapse rate A:surface albedo, C:cloud :climate sensitivity [K/(W/m**2)] SW fluxat TOA RadiationModel LW fluxat TOA

  7. sfc albedo temperature mixing ratio clouds PRPFeedback Analysis(Wetharald and Manabe, 1988) feedback P:radiative damping, WV:water vapor, LR:lapse rate A:surface albedo, C:cloud :climate sensitivity [K/(W/m**2)] DSW fluxat TOA RadiationModel Water VaporFeedback DLW fluxat TOA

  8. Adjusted Stratosphere Radiative Forcing LGM Ice Sheets Sea level , vegetation, and dust distribution changes are not included in the forcing.

  9. Climate Sensitivity w.r.t CTRL Less positive feedback in the LGM experiment compared to the 2xCO2 experiment. *include the effect of q-flux difference due to different land-sea mask **include the thermodynamic effect of elevated surface due to LGM ice sheets

  10. Global, annual mean feedback strength w.r.t CTRL Colman, 2003 +MIROC3.2 The total feedback strength in the LGM experiment is weaker than the 2xCO2 experiment, and it results from the weaker shortwave cloud feedback.

  11. Water Vapor Feedback (DR/DT, W/m2/K) DT: normalized by global mean values DT: normalized by the zonal mean values • Water vapor feedback per 1K warming is larger in the tropics. • The water vapor feedback is weaker in the LGM experiment compared to the 2xCO2 experiment because fractionally less tropical forcing in the LGM.

  12. Lapse Rate Feedback (W/m2/K) • Lapse feedback is negative (positive) in the low (high) latitudes. • The lapse rate feedback is stronger in the LGM experiment compared to the 2xCO2 experiment because fractionally more extratropical forcing in the LGM.

  13. Albedo Feedback (W/m2/K) Albedo feedback occurs in lower (higher) latitudes in cooling (warming) experiments.

  14. Cloud Feedback (W/m2/K) The difference in the cloud feedback between LGMand 2xCO2 experiments is primarily due to shortwave component.

  15. Cloud Amount 2xCO2-CTRL CTRL LGM-CTRL LGM-2xCO2

  16. Summary • Radiative forcing, climate sensitivity, and climate feedback strength is quantitatively evaluated in a consistent manner for 2xCO2, LGMGHG, LGM experiments using MIROC3.2. • The comparison between 2xCO2 and LGMGHG experiments reveals that there is an asymmetry in the cloud feedback between warming and cooling experiments. • The comparison between LGM and LGMGHG experiments further reveal that the LGM ice sheets causes additional weakening in the cloud feedback, and it occurs in the shortwave component. • These results suggest that a model with high climate sensitivity in the warming experiment does not necessarily yields the high climate sensitivity in the LGM. Nevertheless, the difference in climate sensitivity between the LGM and 2xCO2 is relatively small compared to the intermodel spread in the 2xCO2 experiment, and paleoclimate studies may be able to provide some constraint.

  17. End

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