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___________________________ Status of CCMI and Evaluation of Chemistry in CMIP6 WACCM ________________________ Doug Kinnison, Chuck Bardeen, and the entire WACCM Team. WACCM Working Group Meeting Breckenridge Colorado June 21, 2016.
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Kinnison WKWG 2016 Final v1 - CESM® · 2016. 8. 14. · Current CCMI Publications. Currently have ~30 Science publication in progress. Garcia, R. R. Anne K. Smith, D. Kinnison 1,

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  • ___________________________Status of CCMI and Evaluation of

    Chemistry in CMIP6 WACCM________________________

    Doug Kinnison, Chuck Bardeen, and the entire WACCM Team.

    WACCM Working Group MeetingBreckenridge Colorado

    June 21, 2016.

  • Outline

    • Status of CCMI simulations.

    • Preliminary Comparison of CCMI with CMIP6 (SD only)

    • Halogen, GHG LBCs for CMIP6 (New Capability)

  • CESM1 (WACCM4) - CCMI

    CCMI: CESM1 (WACCM) – CAM4 column physics – 2 degree Res.

    • TSMLT Chemistry, ~180 species, >450 gas-phase rxns; 17 heterogeneous rxns on sulfate, NAT, and Water-Ice.

    • Solar Variability (Lean ETF; SPEs & Auroral NOx).

    • Halogen (LL, VSL); GHGs (CO2, CH4, N2O).

    • Sulfate SAD time series (including Volcanoes).

    • QBO nudged to observed winds.

    • SD simulation using MERRA met.

  • CESM1-WACCM4 CCMI Simulations: Status

    Scenario Period Ocean RCP Members Completed

    CMOR#

    REFC1 1955-2014 Data - 5 Done

    REFC1-PI 1850-1960 Data - 1 -

    REFC1SD 1979-2014 Data - 1 Done

    REFC2 1960-2100 Interactive RCP6.0 3 Done

    SENC2 2001-2100 Interactive RCP4.5 1 Done

    SENC2 2001-2100 Interactive RCP8.5 3 Done

    SENC2-fGHG1960 1960-2100 Interactive RCP6.0 3 Soon

    SENC2-fODS1960 1960-2100 Interactive RCP6.0 3 Soon

    SENC2-fODS2000 2000-2100 Interactive RCP6.0 3 Soon

    SENC2-nVSL 1955-2100 Interactive RCP6.0 1 Soon

    #CMOR’izing addressed by Simone Tilmes and Gary Strand.

  • Current CCMI Publications.

    Currently have ~30 Science publication in progress.

    Garcia, R. R. Anne K. Smith, D. Kinnison1, Á. de la Cámara, and D. Murphy, Modification of the gravity wave parameterization in the Whole Atmosphere Community Climate Model: Motivation and results, in review, JGR, 2016.

    Solomon, S., D. J. Ivy, D. Kinnison, M. J. Mills, R. R. Neely III, A. Schmidt, Emergence of Healing in the Antarctic Ozone Layer, accepted, Science, 2016.

    Tilmes, S., J.-F. Lamarque, L. K. Emmons, D. Kinnison, D. Marsh, R. R. Garcia, A. K. Smith, R. R. Neeley, A. Conley, F. Vitt, Maria Val Martin, H. Tanimoto, I. Simpson, D. R. Blake, and N. Blake, Representation of the Community Earth System Model (CESM1) CAM4-Chem within the Chemistry-Climate Model Initiative, Geosci. Model Dev., 9, 1853–1890, doi:10.5194/gmd-9-1853-2016.

    Jackman, C. H., D. R. Marsh, D. E. Kinnison, C. J. Mertens, and E. L. Fleming, Atmopspheric changes caused by galactic cosmic rays over the period 1960-2010, Atmos. Chem. Phys. , doi:10.5194/acp-16-5853-2016.

    Garcia, R. R., M. Lopez-Puertas, B. Funke, D. E. Kinnison, D. R. Marsh, L. Qian, On the secular trend of COx and CO2 in the lower thermosphere, J. Geophys. Res., 121, 3634-3644, doi:10.1002/2015JD024553.

    Solomon, S., D. E. Kinnison, J. Bandoro, R.Garcia, Simulations of Polar Ozone Depletion: An Update, J. Geophys. Res., 120, 7958-7974, doi:10.1002/2015JD0233652015.

    Sakazaki, T., T. Sasaki, M. Shiotani, Y. Tomikawa, and D. Kinnison, Zonally uniform tidal oscillations in tropical stratosphere, Geophys. Res. Lett., , 42, 9553-9560, doi:10.1002/ 2015GL066054.2015.

    Randall, C, V. Harvey, L. Holt, D. Marsh, D. E. Kinnison , B. Funke, P. F. Bernath, Simulation of energetic particle precipitation effects during the 2003-2004 Arctic winter, J. Geophy. Res., Space Phys., 120, 5035-5048, doi:10.1002/2015JA021196, 2015.

  • Daily and Monthly Ozone will be used for input for non-interactive CMIP6 models.

    TOZ [63S-90S] - October

    1850 1900 1950 2000 2050 2100Year

    150

    200

    250

    300

    350

    400

    450To

    tal C

    olum

    n O

    zone

    (DU)

    REFC1 [data ocean]REFC2 [interactive ocean]REFC1SD [MERRA]Observations

    Thin black line ~1980 TOZSymbols are individual realizations3-point smoothing for solid lines

  • The SD simulation gets most of the NH depletion – but not all (issues with T-bias, SAD input).

    TOZ [63N-90N] - March

    1850 1900 1950 2000 2050 2100Year

    300

    350

    400

    450

    500

    550To

    tal C

    olum

    n O

    zone

    (DU)

    REFC1 [data ocean]REFC2 [interactive ocean]REFC1SD [MERRA]Observations

    Thin black line ~1980 TOZ

    Symbols are individual realizations

    3-point smoothing for solid lines

  • CESM Column Physics

    CAM4/WACCM4 CAM5.1 CAM5.5/WACCM5.5Horizontal Resolution 1.9˚x2.5˚ 1.9˚x2.5˚ 0.95˚x1.25˚Vertical Layers 26/66 30 32/70Boundary Layer HB UW CLUBBShallow Convection Hack UW CLUBBDeep Convection ZM ZM ZMMacrophysics R&K UW CLUBBMicrophysics R&K MG 1.0 MG 2.0Radiation CAMRT RRTMG RRTMGAerosols Bulk MAM3 MAM4

    NOTE: MAM4 includes prognostic stratospheric sulfates.

    NEXT: Will show how only year 2011 SD simulations (88-levels).

  • Evaluation of Stratospheric Chemistry (SD-WACCM / MERRA)

    increases the variability of ClONO2, in terms of both high and low extremes. The high extremes are linked to therapid formation of ClONO2 from enhanced ClOwhenever NO2 is available, while the low extremes reflect effectiveheterogeneous removal that subsequently drives ClONO2 toward zero if heterogeneous chemistry is sufficientlyrapid compared to the rate of reformation of ClONO2. Variations linked to wave activity that lead to sporadiclow and high temperatures, and transport air from sunlight to darkness and vice versa, strongly affect theClONO2 extremes. Arnone et al. [2012] show MIPAS observations of high ClONO2 inside the edge of the Arcticvortex at times, similar to that presented here for Antarctica. It is important to note that the computedvariability of the reference and LIQUIDS#2 model values decreases substantially as temperatures increase in thespring, again illustrating the fact that not only the abundance but also the variability of ClONO2 is tightly linkedto the rate of heterogeneous chemistry. MIPAS data display a similar marked decrease in variability after aboutday 275 in Figure 10. The LIQUIDS#2 case yields minimum ClONO2 mixing ratios that are higher than theircounterparts in ACE and MIPAS data (particularly after about day 250 in the latter), indicating a premature netrecovery into the ClONO2 reservoir (as suggested by the behavior of HCl in Figure 8 as well). At this latitudeand altitude, the model reference case is able to match the extremes of both ACE and MIPASobservations of ClONO2, although there is a clear bias in the reference model probability distributionfunction for days 260–280, where WACCM displays too many high values and too few low ones.

    Figure S5 shows similar results as those of Figure 10 but for latitudes deeper in the vortex, 75–85°S, near 30hPa, where the reference model values appear to overestimate somewhat both the high and low extremesduring days 260–280. It is noticeable that the reference model is closer to the MIPAS range than theLIQUIDS#2 case throughout the season.

    In summary, Figures 3, 4, 8, and 10 illustrate how the abundance, variability, and timing of the seasonalevolution of ClONO2 provide a particularly sensitive indicator of chemical processing that is key to ozonedepletion and its timing.

    4.4. Transport and ClONO2

    Figure 11 examines the zonally averaged budget of ClONO2 in the reference case for Antarctica, by showingthe contributions of chemistry and advective transport to the calculated rate of change of ClONO2 in SD-WACCM

    Figure 8. Evolution of zonally averaged chemical species at (left) 80°S and (right) 70°S near 30 hPa, for the (top) referenceand (bottom) LIQUIDS#2 cases. Concentrations of ozone and HCl calculated by SD-WACCM (lines) are compared to MLSsatellite data (crosses), and calculated abundances of related species are also indicated.

    Journal of Geophysical Research: Atmospheres 10.1002/2015JD023365

    SOLOMON ET AL. POLAR OZONE DEPLETION 7969

    Amazing representation of stratospheric chemistry. Comparisons above are made with: Aura MLS (HCl, O3); MIPAS (ClONO2).

    Wegner, T, D. E. Kinnison, R. R. Garcia, S. Madronich, and S. Solomon, Polar Stratospheric Clouds in SD-WACCM4, J. Geophys. Res., VOL. 118, 1-12, doi:10.1002/jgrd.50415, 2013.

    Solomon, S., D. E. Kinnison, J. Bandoro, R.Garcia, Simulations of Polar Ozone Depletion: An Update, J. Geophys. Res., 120, 7958-7974, doi:10.1002/2015JD0233652015.

    31hPa

  • Agreement not as well represented in SD-WACCM / GEOS5 (1-deg) CMIP6 (between days 270-290)?

    31hPa

  • ClOx Activation is lower in CMIP6?

    Evaluation of Stratospheric Chemistry (SD)

    Net Activation is lower in CMIP6 near day 280.

    31hPa, 80S

    Less ICE Activation

  • Evaluation of Stratospheric Chemistry (SD) - lower down.61hPa, 74S

    Ozone depletion is also less in CMIP6 (relative to obs). However, in much better agreement at 61hPa vs 31hPa.

    ICE SAD is lower in magnitude in CMIP6 (relative to CCMI). This may be partially why ozone depletion is underestimated in CMIP6 near day 280.

  • CCMI: H2O, HNO3, and Temperature

    Overall – pretty amazing agreement.

  • CMIP6: H2O, HNO3, and Temperature

    XXHNO3 (higher) and H2O (lower) are not as well represented in CMIP6.

    Temperature is consistent between both model systems.

  • Transport / Mixing Differences?

  • Chemistry Summary

    • Specified Dynamics simulations were conducted for year 2011 using the CCMI (2-deg; WACCM4) and CMIP6 (1-deg).

    • There are some difference between the high latitude polar results published in Solomon et al., JGR 2015 (CCMI) versus the what is currently derived in CMIP6. The agreement is worse at lower pressures (higher altitude).

    • This might be due to changes in transport/mixing. It could alsobe partially dependent on the magnitude of SAD ICE, which is lower in CMIP6 vs CCMI.

    • More work (ASAP) is needed to understand the SD CCMI / CMIP6 differences.

  • New Lower Boundary Conditions for CMIP6

    Malte Meinshausen et al., Historical greenhouse gas concentrations for CMIP6, to be submitted to GMD, 2016

    Key improvements from CMIP6:

    • Latitudinal gradients• Seasonal gradients

    Ground-based and aircraft observation are used.

  • Methyl Bromide, CH3Br (pptv)

    Impressive representation of the latitudinal gradient in CH3Br. Not having this gradient makes comparisons to aircraft campaigns (in the NH) problematic. Values for present day approaching 1960s conditions (~1.5 years, lifetime controlled by reaction with OH).

  • Methyl Chloroform, CH3CCl3 (pptv)

    The atmosphere is almost free of MCF (lifetime ~5 years; lifetime controlled with OH)!

  • Pretty consistent with CMIP5 historical time series, except observations are now used from 2005 forward (lifetime ~9 years; lifetime controlled with OH)!.

    Methane, CH4 (ppbv)

  • Pretty consistent with CMIP5 historical time series, except observations are now used from 2005 forward (lifetime ~9 years; lifetime controlled with OH)!.

    Carbon Dioxide, CO2 (ppmv)

  • Carbon Dioxide, CO2 (ppmv), global average.

    Increasing at a rapid rate – near 400 ppmv in 2014!

    ?

  • Thank you for your attention.