Attribution of Chemistry-Climate Model Initiative (CCMI) ozone radiative flux bias from satellites

<p>The top-of-atmosphere (TOA) outgoing longwave flux over the 9.6&thinsp;<span class="inline-formula">µm</span> ozone band is a fundamental quantity for understanding chemistry–climate coupling. However, observed TOA fluxes are hard to estimate as they exhibit consid...

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Bibliographic Details
Main Authors: L. Kuai, K. W. Bowman, K. Miyazaki, M. Deushi, L. Revell, E. Rozanov, F. Paulot, S. Strode, A. Conley, J.-F. Lamarque, P. Jöckel, D. A. Plummer, L. D. Oman, H. Worden, S. Kulawik, D. Paynter, A. Stenke, M. Kunze
Format: Article
Language:English
Published: Copernicus Publications 2020-01-01
Series:Atmospheric Chemistry and Physics
Online Access:https://www.atmos-chem-phys.net/20/281/2020/acp-20-281-2020.pdf
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Summary:<p>The top-of-atmosphere (TOA) outgoing longwave flux over the 9.6&thinsp;<span class="inline-formula">µm</span> ozone band is a fundamental quantity for understanding chemistry–climate coupling. However, observed TOA fluxes are hard to estimate as they exhibit considerable variability in space and time that depend on the distributions of clouds, ozone (<span class="inline-formula">O<sub>3</sub></span>), water vapor (<span class="inline-formula">H<sub>2</sub>O</span>), air temperature (<span class="inline-formula"><i>T</i><sub>a</sub></span>), and surface temperature (<span class="inline-formula"><i>T</i><sub>s</sub></span>). Benchmarking present-day fluxes and quantifying the relative influence of their drivers is the first step for estimating climate feedbacks from ozone radiative forcing and predicting radiative forcing evolution.</p> <p>To that end, we constructed observational instantaneous radiative kernels (IRKs) under clear-sky conditions, representing the sensitivities of the TOA flux in the 9.6&thinsp;<span class="inline-formula">µm</span> ozone band to the vertical distribution of geophysical variables, including <span class="inline-formula">O<sub>3</sub></span>, <span class="inline-formula">H<sub>2</sub>O</span>, <span class="inline-formula"><i>T</i><sub>a</sub></span>, and <span class="inline-formula"><i>T</i><sub>s</sub></span> based upon the Aura Tropospheric Emission Spectrometer (TES) measurements. Applying these kernels to present-day simulations from the Chemistry-Climate Model Initiative (CCMI) project as compared to a 2006 reanalysis assimilating satellite observations, we show that the models have large differences in TOA flux, attributable to different geophysical variables. In particular, model simulations continue to diverge from observations in the tropics, as reported in previous studies of the Atmospheric Chemistry Climate Model Intercomparison Project (ACCMIP) simulations. The principal culprits are tropical middle and upper tropospheric ozone followed by tropical lower tropospheric <span class="inline-formula">H<sub>2</sub>O</span>. Five models out of the eight studied here have TOA flux biases exceeding 100&thinsp;mW&thinsp;m<span class="inline-formula"><sup>−2</sup></span> attributable to tropospheric ozone bias. Another set of five models have flux biases over 50&thinsp;mW&thinsp;m<span class="inline-formula"><sup>−2</sup></span> due to <span class="inline-formula">H<sub>2</sub>O</span>. On the other hand, <span class="inline-formula"><i>T</i><sub>a</sub></span> radiative bias is negligible in all models (no more than 30&thinsp;mW&thinsp;m<span class="inline-formula"><sup>−2</sup></span>). We found that the atmospheric component (AM3) of the Geophysical Fluid Dynamics<span id="page282"/> Laboratory (GFDL) general circulation model and Canadian Middle Atmosphere Model (CMAM) have the lowest TOA flux biases globally but are a result of cancellation of opposite biases due to different processes. Overall, the multi-model ensemble mean bias is <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M17" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>-</mo><mn mathvariant="normal">133</mn><mo>±</mo><mn mathvariant="normal">98</mn></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="52pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="5389b518f84f2067694b56b2b3c81d83"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="acp-20-281-2020-ie00001.svg" width="52pt" height="10pt" src="acp-20-281-2020-ie00001.png"/></svg:svg></span></span>&thinsp;mW&thinsp;m<span class="inline-formula"><sup>−2</sup></span>, indicating that they are too atmospherically opaque due to trapping too much radiation in the atmosphere by overestimated tropical tropospheric <span class="inline-formula">O<sub>3</sub></span> and <span class="inline-formula">H<sub>2</sub>O</span>. Having too much <span class="inline-formula">O<sub>3</sub></span> and <span class="inline-formula">H<sub>2</sub>O</span> in the troposphere would have different impacts on the sensitivity of TOA flux to <span class="inline-formula">O<sub>3</sub></span> and these competing effects add more uncertainties on the ozone radiative forcing. We find that the inter-model TOA outgoing longwave radiation (OLR) difference is well anti-correlated with their ozone band flux bias. This suggests that there is significant radiative compensation in the calculation of model outgoing longwave radiation.</p>
ISSN:1680-7316
1680-7324