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www.bsc.es Mexico DF, 26 August 2015
Francisco J. Doblas-Reyes
BSC Earth Sciences Department Director
ICREA Research Professor
Climate Modelling, Predictions
and Projections
2
Temperatures in Barcelona airport from the ECAD dataset.
An example of what is going on
2014
4
Radiative forcing in the representative concentration pathways (RCP)
Scenarios of concentration
RCPs describe the impact on the global energy balance of the
human activity under different socio-economic scenarios.
Differences between the RCPs are clear after 2030.
5
Figure SPM.7a: Global average surface temperature change
Global-mean temperature
Global surface temperature change for the end of the 21st
century is likely to exceed 1.5°C relative to 1850 for all
scenarios.
6
Figure SPM.8a,b: CMIP5 multi-model mean spatial distribution
Temperature and precipitation
8
Figure SPM.7c: Global ocean surface pH
Ocean acidification
The ocean acidification is one of the clearest signals of the
anthropogenic climate change.
A spatial distribution of the change is also found.
9
Figure SPM.9: Global mean sea level rise
Sea level
Global mean sea level will continue to rise during the 21st
century even under mitigation scenarios.
10
Limiting climate change will require substantial and sustained
reductions of greenhouse gas emissions.
Figure SPM.10: Temperature increase vs cumulative carbon emissions
The clock is ticking
11
.
Decadal climate prediction
Predictions Historical
simulations
Observations
Atlantic multidecadal
variability (AMV)
Global mean surface air
temperature (GMST)
• C3S Climate Projections Workshop: Near-term predictions and projections, 21 April 2015
Doblas-Reyes et al. (2013, Nat. Comms.)
The initialized simulations reproduce the temperature trends
and the AMV variability and suggest that initialization corrects
the forced model response and phases in the internal
variability.
12
SST averaged over the subpolar gyre to estimate basin-wide
accumulated cyclone energy (ACE). The results are for 1-5 year
averages 1961-2006. Statistically significant scores are in bold.
Service-driven predictions
• C3S Climate Projections Workshop: Near-term predictions and projections, 21 April 2015
Caron et al. (2015, GRL)
14
What is coming up
The Sixth Coupled Model Intercomparison Project (CMIP6) is
opening the way to a new generation of experiments that will
feed into the AR6.
15
Service-driven climate research
Climate data is not climate information

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Climate Modelling, Predictions and Projections

  • 1. www.bsc.es Mexico DF, 26 August 2015 Francisco J. Doblas-Reyes BSC Earth Sciences Department Director ICREA Research Professor Climate Modelling, Predictions and Projections
  • 2. 2 Temperatures in Barcelona airport from the ECAD dataset. An example of what is going on 2014
  • 3. 4 Radiative forcing in the representative concentration pathways (RCP) Scenarios of concentration RCPs describe the impact on the global energy balance of the human activity under different socio-economic scenarios. Differences between the RCPs are clear after 2030.
  • 4. 5 Figure SPM.7a: Global average surface temperature change Global-mean temperature Global surface temperature change for the end of the 21st century is likely to exceed 1.5°C relative to 1850 for all scenarios.
  • 5. 6 Figure SPM.8a,b: CMIP5 multi-model mean spatial distribution Temperature and precipitation
  • 6. 8 Figure SPM.7c: Global ocean surface pH Ocean acidification The ocean acidification is one of the clearest signals of the anthropogenic climate change. A spatial distribution of the change is also found.
  • 7. 9 Figure SPM.9: Global mean sea level rise Sea level Global mean sea level will continue to rise during the 21st century even under mitigation scenarios.
  • 8. 10 Limiting climate change will require substantial and sustained reductions of greenhouse gas emissions. Figure SPM.10: Temperature increase vs cumulative carbon emissions The clock is ticking
  • 9. 11 . Decadal climate prediction Predictions Historical simulations Observations Atlantic multidecadal variability (AMV) Global mean surface air temperature (GMST) • C3S Climate Projections Workshop: Near-term predictions and projections, 21 April 2015 Doblas-Reyes et al. (2013, Nat. Comms.) The initialized simulations reproduce the temperature trends and the AMV variability and suggest that initialization corrects the forced model response and phases in the internal variability.
  • 10. 12 SST averaged over the subpolar gyre to estimate basin-wide accumulated cyclone energy (ACE). The results are for 1-5 year averages 1961-2006. Statistically significant scores are in bold. Service-driven predictions • C3S Climate Projections Workshop: Near-term predictions and projections, 21 April 2015 Caron et al. (2015, GRL)
  • 11. 14 What is coming up The Sixth Coupled Model Intercomparison Project (CMIP6) is opening the way to a new generation of experiments that will feed into the AR6.
  • 12. 15 Service-driven climate research Climate data is not climate information

Editor's Notes

  1. Figure SPM.5 | Radiative forcing estimates in 2011 relative to 1750 and aggregated uncertainties for the main drivers of climate change. Values are global average radiative forcing (RF, Footnote 14), partitioned according to the emitted compounds or processes that result in a combination of drivers. The best estimates of the net radiative forcing are shown as black diamonds with corresponding uncertainty intervals; the numerical values are provided on the right of the figure, together with the confidence level in the net forcing (VH – very high, H – high, M – medium, L – low, VL – very low). Albedo forcing due to black carbon on snow and ice is included in the black carbon aerosol bar. Small forcings due to contrails (0.05 W m–2, including contrail induced cirrus), and HFCs, PFCs and SF6 (total 0.03 W m–2) are not shown. Concentration-based RFs for gases can be obtained by summing the like-coloured bars. Volcanic forcing is not included as its episodic nature makes is difficult to compare to other forcing mechanisms. Total anthropogenic radiative forcing is provided for three different years relative to 1750. For further technical details, including uncertainty ranges associated with individual components and processes, see the Technical Summary Supplementary Material. {8.5; Figures 8.14–8.18; Figures TS.6 and TS.7} Footnote 14: The strength of drivers is quantified as Radiative Forcing (RF) in units watts per square metre (W m–2) as in previous IPCC assessments. RF is the change in energy flux caused by a driver, and is calculated at the tropopause or at the top of the atmosphere. In the traditional RF concept employed in previous IPCC reports all surface and tropospheric conditions are kept fixed. In calculations of RF for well-mixed greenhouse gases and aerosols in this report, physical variables, except for the ocean and sea ice, are allowed to respond to perturbations with rapid adjustments. The resulting forcing is called Effective Radiative Forcing (ERF) in the underlying report. This change reflects the scientific progress from previous assessments and results in a better indication of the eventual temperature response for these drivers. For all drivers other than well-mixed greenhouse gases and aerosols, rapid adjustments are less well characterized and assumed to be small, and thus the traditional RF is used. {8.1}
  2. Complete caption of Figure SPM.7: Figure SPM.7 | CMIP5 multi-model simulated time series from 1950 to 2100 for (a) change in global annual mean surface temperature relative to 1986–2005, (b) Northern Hemisphere September sea ice extent (5-year running mean), and (c) global mean ocean surface pH. Time series of projections and a measure of uncertainty (shading) are shown for scenarios RCP2.6 (blue) and RCP8.5 (red). Black (grey shading) is the modelled historical evolution using historical reconstructed forcings. The mean and associated uncertainties averaged over 2081−2100 are given for all RCP scenarios as colored vertical bars. The numbers of CMIP5 models used to calculate the multi-model mean is indicated. For sea ice extent (b), the projected mean and uncertainty (minimum-maximum range) of the subset of models that most closely reproduce the climatological mean state and 1979 to 2012 trend of the Arctic sea ice is given (number of models given in brackets). For completeness, the CMIP5 multi-model mean is also indicated with dotted lines. The dashed line represents nearly ice-free conditions (i.e., when sea ice extent is less than 106 km2 for at least five consecutive years). For further technical details see the Technical Summary Supplementary Material {Figures 6.28, 12.5, and 12.28–12.31; Figures TS.15, TS.17, and TS.20}
  3. Complete caption of Figure SPM.7: Figure SPM.7 | CMIP5 multi-model simulated time series from 1950 to 2100 for (a) change in global annual mean surface temperature relative to 1986–2005, (b) Northern Hemisphere September sea ice extent (5-year running mean), and (c) global mean ocean surface pH. Time series of projections and a measure of uncertainty (shading) are shown for scenarios RCP2.6 (blue) and RCP8.5 (red). Black (grey shading) is the modelled historical evolution using historical reconstructed forcings. The mean and associated uncertainties averaged over 2081−2100 are given for all RCP scenarios as colored vertical bars. The numbers of CMIP5 models used to calculate the multi-model mean is indicated. For sea ice extent (b), the projected mean and uncertainty (minimum-maximum range) of the subset of models that most closely reproduce the climatological mean state and 1979 to 2012 trend of the Arctic sea ice is given (number of models given in brackets). For completeness, the CMIP5 multi-model mean is also indicated with dotted lines. The dashed line represents nearly ice-free conditions (i.e., when sea ice extent is less than 106 km2 for at least five consecutive years). For further technical details see the Technical Summary Supplementary Material {Figures 6.28, 12.5, and 12.28–12.31; Figures TS.15, TS.17, and TS.20}
  4. Figure SPM.8, Panels a and b Complete caption of Figure SPM.8: Figure SPM.8 | Maps of CMIP5 multi-model mean results for the scenarios RCP2.6 and RCP8.5 in 2081–2100 of (a) annual mean surface temperature change, (b) average percent change in annual mean precipitation, (c) Northern Hemisphere September sea ice extent, and (d) change in ocean surface pH. Changes in panels (a), (b) and (d) are shown relative to 1986–2005. The number of CMIP5 models used to calculate the multi-model mean is indicated in the upper right corner of each panel. For panels (a) and (b), hatching indicates regions where the multi-model mean is small compared to natural internal variability (i.e., less than one standard deviation of natural internal variability in 20-year means). Stippling indicates regions where the multi-model mean is large compared to natural internal variability (i.e., greater than two standard deviations of natural internal variability in 20-year means) and where at least 90% of models agree on the sign of change (see Box 12.1). In panel (c), the lines are the modelled means for 1986−2005; the filled areas are for the end of the century. The CMIP5 multi-model mean is given in white colour, the projected mean sea ice extent of a subset of models (number of models given in brackets) that most closely reproduce the climatological mean state and 1979 to 2012 trend of the Arctic sea ice extent is given in light blue colour. For further technical details see the Technical Summary Supplementary Material. {Figures 6.28, 12.11, 12.22, and 12.29; Figures TS.15, TS.16, TS.17, and TS.20}
  5. Complete caption of Figure SPM.7: Figure SPM.7 | CMIP5 multi-model simulated time series from 1950 to 2100 for (a) change in global annual mean surface temperature relative to 1986–2005, (b) Northern Hemisphere September sea ice extent (5-year running mean), and (c) global mean ocean surface pH. Time series of projections and a measure of uncertainty (shading) are shown for scenarios RCP2.6 (blue) and RCP8.5 (red). Black (grey shading) is the modelled historical evolution using historical reconstructed forcings. The mean and associated uncertainties averaged over 2081−2100 are given for all RCP scenarios as colored vertical bars. The numbers of CMIP5 models used to calculate the multi-model mean is indicated. For sea ice extent (b), the projected mean and uncertainty (minimum-maximum range) of the subset of models that most closely reproduce the climatological mean state and 1979 to 2012 trend of the Arctic sea ice is given (number of models given in brackets). For completeness, the CMIP5 multi-model mean is also indicated with dotted lines. The dashed line represents nearly ice-free conditions (i.e., when sea ice extent is less than 106 km2 for at least five consecutive years). For further technical details see the Technical Summary Supplementary Material {Figures 6.28, 12.5, and 12.28–12.31; Figures TS.15, TS.17, and TS.20}
  6. Complete caption of Figure SPM.7: Figure SPM.7 | CMIP5 multi-model simulated time series from 1950 to 2100 for (a) change in global annual mean surface temperature relative to 1986–2005, (b) Northern Hemisphere September sea ice extent (5-year running mean), and (c) global mean ocean surface pH. Time series of projections and a measure of uncertainty (shading) are shown for scenarios RCP2.6 (blue) and RCP8.5 (red). Black (grey shading) is the modelled historical evolution using historical reconstructed forcings. The mean and associated uncertainties averaged over 2081−2100 are given for all RCP scenarios as colored vertical bars. The numbers of CMIP5 models used to calculate the multi-model mean is indicated. For sea ice extent (b), the projected mean and uncertainty (minimum-maximum range) of the subset of models that most closely reproduce the climatological mean state and 1979 to 2012 trend of the Arctic sea ice is given (number of models given in brackets). For completeness, the CMIP5 multi-model mean is also indicated with dotted lines. The dashed line represents nearly ice-free conditions (i.e., when sea ice extent is less than 106 km2 for at least five consecutive years). For further technical details see the Technical Summary Supplementary Material {Figures 6.28, 12.5, and 12.28–12.31; Figures TS.15, TS.17, and TS.20}
  7. Figure SPM.9 | Projections of global mean sea level rise over the 21st century relative to 1986–2005 from the combination of the CMIP5 ensemble with process-based models, for RCP2.6 and RCP8.5. The assessed likely range is shown as a shaded band. The assessed likely ranges for the mean over the period 2081–2100 for all RCP scenarios are given as coloured vertical bars, with the corresponding median value given as a horizontal line. For further technical details see the Technical Summary Supplementary Material {Table 13.5, Figures 13.10 and 13.11; Figures TS.21 and TS.22}
  8. Figure SPM.10 | Global mean surface temperature increase as a function of cumulative total global CO2 emissions from various lines of evidence. Multi-model results from a hierarchy of climate-carbon cycle models for each RCP until 2100 are shown with coloured lines and decadal means (dots). Some decadal means are labeled for clarity (e.g., 2050 indicating the decade 2040−2049). Model results over the historical period (1860 to 2010) are indicated in black. The coloured plume illustrates the multi-model spread over the four RCP scenarios and fades with the decreasing number of available models in RCP8.5. The multi-model mean and range simulated by CMIP5 models, forced by a CO2 increase of 1% per year (1% yr–1 CO2 simulations), is given by the thin black line and grey area. For a specific amount of cumulative CO2 emissions, the 1% per year CO2 simulations exhibit lower warming than those driven by RCPs, which include additional non-CO2 forcings. Temperature values are given relative to the 1861−1880 base period, emissions relative to 1870. Decadal averages are connected by straight lines. For further technical details see the Technical Summary Supplementary Material. {Figure 12.45; TS TFE.8, Figure 1}
  9. CMIP5 decadal predictions. Global-mean near-surface air temperature and AMV against GHCN/ERSST3b for forecast years 2-5.