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The future of ice sheets and sea ice: Between reversible retreat and unstoppable loss

Dirk Notz
PNAS December 8, 2009 106 (49) 20590-20595; https://doi.org/10.1073/pnas.0902356106
Dirk Notz
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  • For correspondence: dirk.notz@zmaw.de
  1. Edited by Hans Joachim Schellnhuber, Environmental Change Institute, Oxford, United Kingdom, and approved September 22, 2009 (received for review March 3, 2009)

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    Fig. 1.

    Evolution of minimum Arctic sea-ice extent from 1953 until 2008. The blue line shows the minimum sea-ice extent, and the bars at the bottom show the change in extent from one year to the next.

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    Fig. 2.

    Comparison of the impact of a certain amount of summer melt on the ice-covered area for two different ice-thickness distributions. The black line shows which percentage of a certain area is covered by ice that is thicker than the ice thickness indicated along the x axis at the beginning of the melt season (cumulative ice-thickness distribution). A shows a possible cumulative thickness distribution of thick ice and B shows that of thinner ice. The colored lines indicate the shift of the ice-thickness distribution for a uniform melting during summers of 0.5 m (cold summer, blue), 0.75 m (normal summer, green) and 1.0 m (warm summer, red), respectively. Note the much stronger variability of the remaining ice-covered area in the case with thinner ice. The Inset shows roughly the noncumulative ice-thickness distribution for each case. Here, the y axis indicates normalized area that is covered by the ice thickness shown along the x axis.

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    Fig. 3.

    Schematic comparison of the ice-thickness evolution of first-year ice (blue) and of preexisting ice (red). The snow on top of the ice is represented by the shaded blue and red areas. The atmospheric and oceanic boundary conditions for this simulation, including the incoming radiation, sensible and latent heat fluxes, and the amount of snowfall, are given by Arctic climatological mean values as summarized by Maykut and Untersteiner (66). For simplicity, the ice growth was simulated by a zero-layer model (see ref. 67) and there is no feedback from the ice to the atmospheric or oceanic forcing. Ice formation of the first-year sea ice was prescribed to start on November 1, two months after the end of the melting season of the preexisting ice. Note that, nevertheless, the newly forming ice reaches a larger maximum thickness than the preexisting ice because of the thinner isolating snow-cover on top of the former.

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The future of ice sheets and sea ice: Between reversible retreat and unstoppable loss
Dirk Notz
Proceedings of the National Academy of Sciences Dec 2009, 106 (49) 20590-20595; DOI: 10.1073/pnas.0902356106

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The future of ice sheets and sea ice: Between reversible retreat and unstoppable loss
Dirk Notz
Proceedings of the National Academy of Sciences Dec 2009, 106 (49) 20590-20595; DOI: 10.1073/pnas.0902356106
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Proceedings of the National Academy of Sciences: 106 (49)
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  • Article
    • Abstract
    • The Ice–Albedo Feedback
    • The Small Ice-Cap Instability
    • Arctic Sea Ice
    • Antarctic Sea Ice
    • Greenland and WAIS
    • Conclusion and Summary
    • Acknowledgments
    • Footnotes
    • References
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