Abstract
The water vapour feedback is the largest physical climate feedback. It also gives the second-largest contribution to the range of uncertainty in climate sensitivity in General Circulation Models (GCMs). Tracing these differences back to their physical causes in the hope of constraining climate sensitivity requires an appropriate quantification. Yet the Intergovernmental Panel on Climate Change judge that the conventional diagnosis of a “water vapour feedback” and a “lapse rate feedback” provides little insight into differences between GCMs’ climate sensitivities. We show that the conventionally diagnosed water vapour feedback is in fact formally useless for investigating differences between GCMs’ climate sensitivities—the anticorrelation between conventional “water vapour feedback” and “lapse rate feedback” makes the correlation between the “water vapour feedback” and their sum insignificant: i.e. statistically, knowing this “feedback” allows one to conclude nothing about the sum and thence about climate sensitivity. This follows primarily from how little relative humidity (RH) changes with climate change in GCMs. A more detailed physical analysis concludes that the overall mean decrease of RH on warming seen in GCMs is robustly physically based. This and other physical arguments then suggest that the stronger the positive “water vapour feedback”, the less sensitive climate can be expected to be. A diagnosis based on the “partly-Simpsonian” model of water vapour feedback avoids these problems. On the conventional view of the water vapour feedback, naive extrapolation of variations within present-day climate suggests that parts of our planet are close to locally reaching conditions that would allow a run-away water vapour greenhouse effect once they were extensive enough. Of course this has never occurred in geological history, and is not seen in Earth-like GCMs. Again, the “partly-Simpsonian” approach provides a simple qualitative explanation, by showing that the water vapour feedback can only cancel part of the basic Planck’s Law negative feedback.
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Notes
Conventions vary, but here “λ” means the net radiative response to global-mean temperature changes, in Wm−2/K, inversely proportional to climate sensitivity, and negative for a net negative feedback, i.e. a stable system.
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Acknowledgments
This work was funded by the joint DECC, DEFRA and MoD Integrated Climate Programme—DECC/Defra (GA01101), MoD (CBC/2B/0417_Annex C5), with writing up partly funded by NERC contract NE/D012287/1 and EU contract GOCE-505539. I am grateful to many Met Office colleagues, particularly Catherine Senior and Mark Ringer, for their support, and Keith Williams for the HadSM3 simulations. At AOPP it formed part of a doctoral project, where I am again grateful to many colleagues, particularly my supervisor Professor David Andrews, Myles Allen, Mark Munro, Stu Teasdale, Pardeep Pall and Simon Crooks. The multi-model analysis relies entirely on the valuable tabulations of Soden and Held (2006). Both content and presentation have benefitted greatly from comments from reviewers.
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Ingram, W. Some implications of a new approach to the water vapour feedback. Clim Dyn 40, 925–933 (2013). https://doi.org/10.1007/s00382-012-1456-3
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DOI: https://doi.org/10.1007/s00382-012-1456-3