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Abstract

Uncertainties in projections of future climate change have not lessened substantially in past decades. Both models and observations yield broad probability distributions for long-term increases in global mean temperature expected from the doubling of atmospheric carbon dioxide, with small but finite probabilities of very large increases. We show that the shape of these probability distributions is an inevitable and general consequence of the nature of the climate system, and we derive a simple analytic form for the shape that fits recent published distributions very well. We show that the breadth of the distribution and, in particular, the probability of large temperature increases are relatively insensitive to decreases in uncertainties associated with the underlying climate processes.
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References and Notes

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There are ambiguities surrounding feedback terminology in the climate literature. Hansen et al. (22) reversed the definition of feedback factor and gain from what is conventional in electronics (2325). The convention adopted by Hansen et al. (22) has permeated much, but not all, of the climate literature [compare with (2628)]. For the standard electronics definitions, it can be shown that the feedback factor is proportional to the fraction of the system response fed back into the system input and that the gain is the proportion by which the output has gained (i.e., been amplified) by the inclusion of the feedbacks. In this study, we retain the traditional electronics definitions. See also the SOM.
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Researchers (17, 18) estimated mean and SD of feedback factors calculated from two different suites of climate models. First, Colman (17) found a mean and SD of (0.11, 0.06) for the albedo feedback factor; (0.17, 0.11) for the cloud feedback factor; and (0.42, 0.06) for the water vapor and lapse rate feedbacks combined. Second, Soden and Held (18) found a mean and SD of (0.09, 0.02) for the albedo feedback factor; (0.22, 0.12) for the cloud feedback factor; and (0.31, 0.04) for the water vapor and lapse rate feedbacks combined. The water vapor and lapse rate feedbacks are typically combined because models show a strong negative correlation between the two. Although the combined feedback for water vapor and lapse rate has the largest magnitude, the greatest contributor to uncertainty is the cloud feedback.
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The curve from (5) is a numerical calculation from climate observations and uses an equation isomorphic to Eq. 3.
30
We thank P. Guttorp, J. M. Wallace, D. Hartmann, D. Battisti, C. Bretherton, E. Steig, D. Stolar, and S. Warren for insightful comments on drafts of the manuscript; M. R. Allen, M. Cane, and one anonymous reviewer for constructive suggestions that substantially improved the manuscript; and H. J. Smith, the editor. G.H.R. thanks Yale University for support as a Flint Visiting Professor.

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Published In

Science
Volume 318Issue 585026 October 2007
Pages: 629 - 632

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Received: 7 May 2007
Accepted: 14 September 2007

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Gerard H. Roe*
Department of Earth and Space Sciences, University of Washington, Seattle, WA 98195, USA.
Marcia B. Baker
Department of Earth and Space Sciences, University of Washington, Seattle, WA 98195, USA.

Notes

* To whom correspondence should be addressed. E-mail: [email protected]

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Science
Volume 318|Issue 5850
26 October 2007
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Received:7 May 2007
Accepted:14 September 2007
Published in print:26 October 2007
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