globalchange  > 气候变化事实与影响
DOI: doi:10.1038/nclimate2451
论文题名:
A large ozone-circulation feedback and its implications for global warming assessments
作者: Peer J. Nowack
刊名: Nature Climate Change
ISSN: 1758-1087X
EISSN: 1758-7207
出版年: 2014-12-01
卷: Volume:5, 页码:Pages:41;45 (2015)
语种: 英语
英文关键词: Climate and Earth system modelling ; Projection and prediction ; Atmospheric chemistry ; Atmospheric dynamics
英文摘要:

State-of-the-art climate models now include more climate processes simulated at higher spatial resolution than ever1. Nevertheless, some processes, such as atmospheric chemical feedbacks, are still computationally expensive and are often ignored in climate simulations1, 2. Here we present evidence that the representation of stratospheric ozone in climate models can have a first-order impact on estimates of effective climate sensitivity. Using a comprehensive atmosphere–ocean chemistry–climate model, we find an increase in global mean surface warming of around 1 °C (20%) after 75 years when ozone is prescribed at pre-industrial levels compared with when it is allowed to evolve self-consistently in response to an abrupt 4×CO2 forcing. The difference is primarily attributed to changes in long-wave radiative feedbacks associated with circulation-driven decreases in tropical lower stratospheric ozone and related stratospheric water vapour and cirrus cloud changes. This has important implications for global model intercomparison studies1, 2 in which participating models often use simplified treatments of atmospheric composition changes that are consistent with neither the specified greenhouse gas forcing scenario nor the associated atmospheric circulation feedbacks3, 4, 5.

Starting from pre-industrial conditions, an instantaneous quadrupling of the atmospheric CO2 mixing ratio is a standard climate change experiment (referred to as abrupt4×CO2) in model intercomparison projects such as the Coupled Model Intercomparison Project phase 5 (CMIP5; ref. 1) or the Geoengineering Model Intercomparison Project2 (GeoMIP). One aim of these initiatives is to offer a quantitative assessment of possible future climate change, with the range of projections from participating models commonly used as a measure of uncertainty6. Within such projects, stratospheric chemistry, and therefore stratospheric ozone, is treated differently in individual models. In CMIP5 and GeoMIP, most participating models did not explicitly calculate stratospheric ozone changes2, 4. For abrupt4×CO2 experiments, modelling centres thus often prescribed stratospheric ozone at pre-industrial levels2, 5. For transient CMIP5 experiments, it was instead recommended to use an ozone field derived from the averaged projections of 13 chemistry–climate models3. This multi-model mean ozone data set was obtained from the Chemistry–Climate Model Validation activity phase 2 (CCMVal-2) projections run under the Special Report on Emissions Scenarios (SRES) A1b scenario for well-mixed greenhouse gases, in contrast to the representative concentration pathway (RCP) scenarios used in CMIP5. So far, research on the impacts of contrasting representations of stratospheric ozone has focused on regional effects, such as the influence of possible future Antarctic ozone recovery on the position of the Southern Hemisphere mid-latitude jet4, 7. However, its potential effect on the magnitude of projected global warming has not received much attention.

Here, we present evidence that highlights that stratospheric chemistry–climate feedbacks can exert a more significant influence on global warming projections than has been suggested8. For a specific climate change experiment, we show that the choice of how to represent key stratospheric chemical species alone can result in a 20% difference in simulated global mean surface warming. Therefore, a treatment of ozone that is not internally consistent with a particular model or greenhouse gas scenario, as is the case for some CMIP5 simulations, could introduce a significant bias into climate change projections.

The model used here is the HadGEM3-AO configuration of the UK Met Office’s Unified Model9 coupled to the United Kingdom Chemistry and Aerosols (UKCA) stratospheric chemistry scheme10 (see Methods). This comprehensive model set-up allows us to study complex feedback effects between the atmosphere, land surface, ocean and sea ice.

Figure 1 shows the evolution of global and annual mean surface temperature anomalies (ΔTsurf) from eight different climate integrations, two of which were carried out with interactive stratospheric chemistry and six with different prescribed monthly mean fields of the following chemically and radiatively active gases: ozone, methane and nitrous oxide (see Table 1 for details). Experiments labelled A are pre-industrial control runs. Experiment B is an abrupt4×CO2 run with fully interactive chemistry, and experiments labelled C are non-interactive abrupt4×CO2 runs in which the chemical fields were prescribed at pre-industrial levels. We conducted two versions of each non-interactive experiment to test the effect of using zonal mean fields (label 2, for example, A2) instead of full three-dimensional (3D) fields (label 1, for example, A1). The time development of ΔTsurf shows a clear difference of nearly 20% between the abrupt4×CO2 experiments B and C1/C2, indicating a much larger global warming in C1/C2 as a consequence of missing composition feedbacks. The primary driver of these differences is changing ozone, with methane and nitrous oxide making much smaller contributions (see below). Fields averaged over the final 50 years of the interactive experiment B were imposed from the beginning in the abrupt4×CO2 experiments B1 and B2. These simulations show a close agreement with experiment B in terms of ΔTsurf, implying that the global mean energy budget can be comparatively well reproduced with this treatment of composition changes, despite the neglect of transient changes in their abundances.

Figure 1: Temporal evolution of the annual and global mean surface temperature anomalies.
Temporal evolution of the annual and global mean surface temperature anomalies.

All anomalies (°C) are shown relative to the average temperature of experiment A. Solid lines show the interactive chemistry runs (A, B), dashed lines show the 3D climatology experiments (A1, B1, C1) and dotted lines show the 2D climatology experiments (A2, B2, C2). For clarity, lines for the abrupt4×CO2 experiments start after year one so that they are not joined with those of the corresponding control experiments. The last 50 years of the abrupt4×CO2 experiments are highlighted in the inset panel with the straight lines marking the average temperature in each set of experiments over the last 20 years.

Model set-up.

A version of the recently developed Hadley Centre Global Environmental Model version 3 in the Atmosphere Ocean configuration (HadGEM3 AO) from the United Kingdom Met Office has been employed here9. It consists of three submodels, representing the atmosphere plus land surface, ocean and sea ice.

For the atmosphere, the Met Office’s Unified Model version 7.3 is used. The configuration used here is based on a regular grid with a horizontal resolution of 3.75° longitude by 2.5° latitude and comprises 60 vertical levels up to a height of 84 km, and so includes a full representation of the stratosphere. Its dynamical core is non-hydrostatic and employs a semi-Lagrangian advection scheme. Subgrid-scale features such as clouds and gravity waves are parameterized.

The ocean component is the Nucleus for European Modelling of the Ocean (NEMO) model version 3.0 coupled to the Los Alamos sea ice model Community Ice CodE (CICE) version 4.0. It contains 31 vertical levels reaching down to a depth of 5 km. The NEMO configuration used in this study deploys a tripolar, locally anisotropic grid that has 2° resolution in longitude everywhere, but an increased latitudinal resolution in certain regions with up to 0.5° in the tropics.

Atmospheric chemistry is represented by the UKCA model in an updated version of the detailed stratospheric chemistry configuration10 that is coupled to the Met Office’s Unified Model. A simple tropospheric chemistry scheme is included that provides for emissions of 3 chemical species and constrains surface mixing ratios of 6 further species. This includes the surface mixing ratios of nitrous oxide (280 ppbv) and methane (790 ppbv), which effectively keeps their concentrations in the troposphere constant at approximately pre-industrial levels. Changes in photolysis rates in the troposphere and the stratosphere are calculated interactively using the Fast-JX photolysis scheme27.

Linear climate feedback theory.

The theory is based on the following equation described by Gregory et al.11

where N is the change in global mean net TOA radiative imbalance (W m−2), F is the effective forcing (W m−2), ΔTsurf is the global mean surface temperature change (°C), and α is the climate feedback parameter (W m−2°C−1). Thus, α can be obtained by regressing N as a function of time against ΔTsurf relative to a control climate. Here, the positive sign convention is used, meaning that a negative α implies a stable climate system. The theory assumes that the net climate feedback parameter can be approximated by a linear superposition of processes that contribute to the overall climate response to an imposed forcing. This can be expressed in the form of a linear decomposition of the α parameter into process-related parameters

with λi, for example, being λwater feedback, λclouds and so on. Similarly, one can decompose the climate feedback parameter into separate radiative components12, 23, 25

providing individual SW and LW components for CS radiative fluxes and the CRE. In this method, the CRE contains direct CREs and indirect cloud masking effects, for example, due to persistent cloud cover that masks surface albedo changes in the all-sky calculation25, 26.

Radiative transfer experiments.

The radiative transfer calculations were carried out using the radiation code from the coupled model simulations28, 29. The inferred all-sky radiative effects due to the changes in ozone and stratospheric water vapour between experiments B and C1 were diagnosed using a base climatology (temperature, pressure, humidity and so on) taken from the last 50 years of C1 and perturbing around this state with the B minus C1 ozone or stratospheric water vapour fields over the same time period. The calculations employ the fixed dynamical heating method15, in which stratospheric temperatures are adjusted to re-establish radiative equilibrium in the presence of the imposed perturbation (see ref. 30 for details). The radiative forcing is then diagnosed as the imbalance in the total (LW + SW) net (down minus up) tropopause fluxes. Note that the changes in ozone and stratospheric water vapour described in the study could be considered as a part forcing and part climate feedback. For example, the increase in ozone in the mid and upper stratosphere in Fig. 3a is linked to the CO2-induced cooling at these levels, and may therefore not be strongly correlated with surface temperature change. In contrast, the decrease in ozone in the tropical mid- and lower stratosphere is driven by the strengthening in the Brewer–Dobson circulation, which is more closely linked to tropospheric temperature change21. However, for the purposes of quantifying the radiative contribution of the composition changes to the evolution of global climate in the experiments, we impose them diagnostically in the offline code as a pseudo radiative forcing agent.

  1. Taylor, K. E., Stouffer, R. J. & Meehl, G. A. An overview of CMIP5 and the experiment design. Bull. Am. Meteorol. Soc. 93, 485498 (2012).
  2. Kravitz, B. et al. An overview of the Geoengineering Model Intercomparison Project (GeoMIP). J. Geophys. Res. 118, 1310313107 (2013).
  3. Cionni, I. et al. Ozone database in support of CMIP5 simulations: Results and corresponding radiative forcing. Atmos. Chem. Phys. 11, 1126711292 (2011).
  4. Eyring, V. et al. Long-term ozone changes and associated climate impacts in CMIP5 simulations. J. Geophys. Res. 118, 50295060 (2013).
  5. Jones, C. D. et al. The HadGEM2-ES implementation of CMIP5 centennial simulations. Geosci. Model Dev. 4, 543570 (2011).
  6. Knutti, R. & Sedláček, J. Robustness and uncertainties in the new CMIP5 climate model projections. Nature Clim. Change 3, 369373 (2013).
  7. Son, S-W. et al. The impact of stratospheric ozone recovery on the Southern Hemisphere westerly jet. Science 320, 14861489 (2008).
  8. Dietmüller, S., Ponater, M. & Sausen, R. Interactive ozone induces a negative feedback in CO2-driven climate change simulations. J. Geophys. Res. 119,
URL: http://www.nature.com/nclimate/journal/v5/n1/full/nclimate2451.html
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资源类型: 期刊论文
标识符: http://119.78.100.158/handle/2HF3EXSE/4915
Appears in Collections:气候变化事实与影响
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气候变化与战略

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Peer J. Nowack. A large ozone-circulation feedback and its implications for global warming assessments[J]. Nature Climate Change,2014-12-01,Volume:5:Pages:41;45 (2015).
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