Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model

The Arctic is warming 2 to 3 times faster than the global average, partly due to changes in short-lived climate forcers (SLCFs) including aerosols. In order to study the effects of atmospheric aerosols in this warming, recent past (1990–2014) and future (2015–2050) simulations have been carried out...

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Published in:Atmospheric Chemistry and Physics
Main Authors: Im, Ulas, Tsigaridis, Kostas, Faluvegi, Gregory, Langen, Peter L., French, Joshua P., Mahmood, Rashed, Thomas, Manu A., Salzen, Knut, Thomas, Daniel C., Whaley, Cynthia H., Klimont, Zbigniew, Skov, Henrik, Brandt, Jørgen
Format: Text
Language:English
Published: 2021
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Ari
Online Access:https://doi.org/10.5194/acp-21-10413-2021
https://acp.copernicus.org/articles/21/10413/2021/
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op_collection_id ftcopernicus
language English
description The Arctic is warming 2 to 3 times faster than the global average, partly due to changes in short-lived climate forcers (SLCFs) including aerosols. In order to study the effects of atmospheric aerosols in this warming, recent past (1990–2014) and future (2015–2050) simulations have been carried out using the GISS-E2.1 Earth system model to study the aerosol burdens and their radiative and climate impacts over the Arctic ( >60 ∘ N), using anthropogenic emissions from the Eclipse V6b and the Coupled Model Intercomparison Project Phase 6 (CMIP6) databases, while global annual mean greenhouse gas concentrations were prescribed and kept fixed in all simulations. Results showed that the simulations have underestimated observed surface aerosol levels, in particular black carbon (BC) and sulfate ( <math xmlns="http://www.w3.org/1998/Math/MathML" id="M3" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="6060a0eb6022af681aa55d19b3180df9"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00001.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00001.png"/></svg:svg> ), by more than 50 %, with the smallest biases calculated for the atmosphere-only simulations, where winds are nudged to reanalysis data. CMIP6 simulations performed slightly better in reproducing the observed surface aerosol concentrations and climate parameters, compared to the Eclipse simulations. In addition, simulations where atmosphere and ocean are fully coupled had slightly smaller biases in aerosol levels compared to atmosphere-only simulations without nudging. Arctic BC, organic aerosol (OA), and <math xmlns="http://www.w3.org/1998/Math/MathML" id="M4" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="544235742d8f4a0f97153436b699bab8"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00002.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00002.png"/></svg:svg> burdens decrease significantly in all simulations by 10 %–60 % following the reductions of 7 %–78 % in emission projections, with the Eclipse ensemble showing larger reductions in Arctic aerosol burdens compared to the CMIP6 ensemble. For the 2030–2050 period, the Eclipse ensemble simulated a radiative forcing due to aerosol–radiation interactions ( RF ARI ) of <math xmlns="http://www.w3.org/1998/Math/MathML" id="M6" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>-</mo><mn mathvariant="normal">0.39</mn><mo>±</mo><mn mathvariant="normal">0.01</mn></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="64pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="aafee4724c88d7325eca1cf08d50e976"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00003.svg" width="64pt" height="10pt" src="acp-21-10413-2021-ie00003.png"/></svg:svg> W m −2 , which is −0.08 W m −2 larger than the 1990–2010 mean forcing ( −0.32 W m −2 ), of which <math xmlns="http://www.w3.org/1998/Math/MathML" id="M12" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>-</mo><mn mathvariant="normal">0.24</mn><mo>±</mo><mn mathvariant="normal">0.01</mn></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="64pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="a0c6a8aaa00926f494c19262568b2d9a"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00004.svg" width="64pt" height="10pt" src="acp-21-10413-2021-ie00004.png"/></svg:svg> W m −2 was attributed to the anthropogenic aerosols. The CMIP6 ensemble simulated a RF ARI of −0.35 to −0.40 W m −2 for the same period, which is −0.01 to −0.06 W m −2 larger than the 1990–2010 mean forcing of −0.35 W m −2 . The scenarios with little to no mitigation (worst-case scenarios) led to very small changes in the RF ARI , while scenarios with medium to large emission mitigations led to increases in the negative RF ARI , mainly due to the decrease in the positive BC forcing and the decrease in the negative <math xmlns="http://www.w3.org/1998/Math/MathML" id="M25" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="66431dc7c7d5e1df65243409a551c241"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00005.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00005.png"/></svg:svg> forcing. The anthropogenic aerosols accounted for −0.24 to −0.26 W m −2 of the net RF ARI in 2030–2050 period, in Eclipse and CMIP6 ensembles, respectively. Finally, all simulations showed an increase in the Arctic surface air temperatures throughout the simulation period. By 2050, surface air temperatures are projected to increase by 2.4 to 2.6 ∘ C in the Eclipse ensemble and 1.9 to 2.6 ∘ C in the CMIP6 ensemble, compared to the 1990–2010 mean. Overall, results show that even the scenarios with largest emission reductions leads to similar impact on the future Arctic surface air temperatures and sea-ice extent compared to scenarios with smaller emission reductions, implying reductions of greenhouse emissions are still necessary to mitigate climate change.
format Text
author Im, Ulas
Tsigaridis, Kostas
Faluvegi, Gregory
Langen, Peter L.
French, Joshua P.
Mahmood, Rashed
Thomas, Manu A.
Salzen, Knut
Thomas, Daniel C.
Whaley, Cynthia H.
Klimont, Zbigniew
Skov, Henrik
Brandt, Jørgen
spellingShingle Im, Ulas
Tsigaridis, Kostas
Faluvegi, Gregory
Langen, Peter L.
French, Joshua P.
Mahmood, Rashed
Thomas, Manu A.
Salzen, Knut
Thomas, Daniel C.
Whaley, Cynthia H.
Klimont, Zbigniew
Skov, Henrik
Brandt, Jørgen
Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
author_facet Im, Ulas
Tsigaridis, Kostas
Faluvegi, Gregory
Langen, Peter L.
French, Joshua P.
Mahmood, Rashed
Thomas, Manu A.
Salzen, Knut
Thomas, Daniel C.
Whaley, Cynthia H.
Klimont, Zbigniew
Skov, Henrik
Brandt, Jørgen
author_sort Im, Ulas
title Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
title_short Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
title_full Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
title_fullStr Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
title_full_unstemmed Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model
title_sort present and future aerosol impacts on arctic climate change in the giss-e2.1 earth system model
publishDate 2021
url https://doi.org/10.5194/acp-21-10413-2021
https://acp.copernicus.org/articles/21/10413/2021/
long_lat ENVELOPE(147.813,147.813,59.810,59.810)
geographic Arctic
Ari
geographic_facet Arctic
Ari
genre Arctic
black carbon
Climate change
Sea ice
genre_facet Arctic
black carbon
Climate change
Sea ice
op_source eISSN: 1680-7324
op_relation doi:10.5194/acp-21-10413-2021
https://acp.copernicus.org/articles/21/10413/2021/
op_doi https://doi.org/10.5194/acp-21-10413-2021
container_title Atmospheric Chemistry and Physics
container_volume 21
container_issue 13
container_start_page 10413
op_container_end_page 10438
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spelling ftcopernicus:oai:publications.copernicus.org:acp91939 2023-05-15T14:58:16+02:00 Present and future aerosol impacts on Arctic climate change in the GISS-E2.1 Earth system model Im, Ulas Tsigaridis, Kostas Faluvegi, Gregory Langen, Peter L. French, Joshua P. Mahmood, Rashed Thomas, Manu A. Salzen, Knut Thomas, Daniel C. Whaley, Cynthia H. Klimont, Zbigniew Skov, Henrik Brandt, Jørgen 2021-07-09 application/pdf https://doi.org/10.5194/acp-21-10413-2021 https://acp.copernicus.org/articles/21/10413/2021/ eng eng doi:10.5194/acp-21-10413-2021 https://acp.copernicus.org/articles/21/10413/2021/ eISSN: 1680-7324 Text 2021 ftcopernicus https://doi.org/10.5194/acp-21-10413-2021 2021-07-12T16:22:14Z The Arctic is warming 2 to 3 times faster than the global average, partly due to changes in short-lived climate forcers (SLCFs) including aerosols. In order to study the effects of atmospheric aerosols in this warming, recent past (1990–2014) and future (2015–2050) simulations have been carried out using the GISS-E2.1 Earth system model to study the aerosol burdens and their radiative and climate impacts over the Arctic ( >60 ∘ N), using anthropogenic emissions from the Eclipse V6b and the Coupled Model Intercomparison Project Phase 6 (CMIP6) databases, while global annual mean greenhouse gas concentrations were prescribed and kept fixed in all simulations. Results showed that the simulations have underestimated observed surface aerosol levels, in particular black carbon (BC) and sulfate ( <math xmlns="http://www.w3.org/1998/Math/MathML" id="M3" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="6060a0eb6022af681aa55d19b3180df9"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00001.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00001.png"/></svg:svg> ), by more than 50 %, with the smallest biases calculated for the atmosphere-only simulations, where winds are nudged to reanalysis data. CMIP6 simulations performed slightly better in reproducing the observed surface aerosol concentrations and climate parameters, compared to the Eclipse simulations. In addition, simulations where atmosphere and ocean are fully coupled had slightly smaller biases in aerosol levels compared to atmosphere-only simulations without nudging. Arctic BC, organic aerosol (OA), and <math xmlns="http://www.w3.org/1998/Math/MathML" id="M4" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="544235742d8f4a0f97153436b699bab8"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00002.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00002.png"/></svg:svg> burdens decrease significantly in all simulations by 10 %–60 % following the reductions of 7 %–78 % in emission projections, with the Eclipse ensemble showing larger reductions in Arctic aerosol burdens compared to the CMIP6 ensemble. For the 2030–2050 period, the Eclipse ensemble simulated a radiative forcing due to aerosol–radiation interactions ( RF ARI ) of <math xmlns="http://www.w3.org/1998/Math/MathML" id="M6" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>-</mo><mn mathvariant="normal">0.39</mn><mo>±</mo><mn mathvariant="normal">0.01</mn></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="64pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="aafee4724c88d7325eca1cf08d50e976"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00003.svg" width="64pt" height="10pt" src="acp-21-10413-2021-ie00003.png"/></svg:svg> W m −2 , which is −0.08 W m −2 larger than the 1990–2010 mean forcing ( −0.32 W m −2 ), of which <math xmlns="http://www.w3.org/1998/Math/MathML" id="M12" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>-</mo><mn mathvariant="normal">0.24</mn><mo>±</mo><mn mathvariant="normal">0.01</mn></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="64pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="a0c6a8aaa00926f494c19262568b2d9a"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00004.svg" width="64pt" height="10pt" src="acp-21-10413-2021-ie00004.png"/></svg:svg> W m −2 was attributed to the anthropogenic aerosols. The CMIP6 ensemble simulated a RF ARI of −0.35 to −0.40 W m −2 for the same period, which is −0.01 to −0.06 W m −2 larger than the 1990–2010 mean forcing of −0.35 W m −2 . The scenarios with little to no mitigation (worst-case scenarios) led to very small changes in the RF ARI , while scenarios with medium to large emission mitigations led to increases in the negative RF ARI , mainly due to the decrease in the positive BC forcing and the decrease in the negative <math xmlns="http://www.w3.org/1998/Math/MathML" id="M25" display="inline" overflow="scroll" dspmath="mathml"><mrow class="chem"><msubsup><mi mathvariant="normal">SO</mi><mn mathvariant="normal">4</mn><mrow><mn mathvariant="normal">2</mn><mo>-</mo></mrow></msubsup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="29pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="66431dc7c7d5e1df65243409a551c241"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-21-10413-2021-ie00005.svg" width="29pt" height="17pt" src="acp-21-10413-2021-ie00005.png"/></svg:svg> forcing. The anthropogenic aerosols accounted for −0.24 to −0.26 W m −2 of the net RF ARI in 2030–2050 period, in Eclipse and CMIP6 ensembles, respectively. Finally, all simulations showed an increase in the Arctic surface air temperatures throughout the simulation period. By 2050, surface air temperatures are projected to increase by 2.4 to 2.6 ∘ C in the Eclipse ensemble and 1.9 to 2.6 ∘ C in the CMIP6 ensemble, compared to the 1990–2010 mean. Overall, results show that even the scenarios with largest emission reductions leads to similar impact on the future Arctic surface air temperatures and sea-ice extent compared to scenarios with smaller emission reductions, implying reductions of greenhouse emissions are still necessary to mitigate climate change. Text Arctic black carbon Climate change Sea ice Copernicus Publications: E-Journals Arctic Ari ENVELOPE(147.813,147.813,59.810,59.810) Atmospheric Chemistry and Physics 21 13 10413 10438