Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth

One of the critical issues of the Snowball Earth hypothesis is the CO<sub>2</sub> threshold for triggering the deglaciation. Using Community Atmospheric Model version 3.0 (CAM3), we study the problem for the CO<sub>2</sub> threshold. Our simulations show large differences fro...

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Main Authors: W. R. Peltier, F. Ding, J. Yang, Y. Hu
Format: Article
Language:English
Published: Copernicus Publications 2011-01-01
Series:Climate of the Past
Online Access:http://www.clim-past.net/7/17/2011/cp-7-17-2011.pdf
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spelling doaj-ad155ba616284af5b489584260ad8ed32020-11-24T23:54:59ZengCopernicus PublicationsClimate of the Past1814-93241814-93322011-01-0171172510.5194/cp-7-17-2011Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball EarthW. R. PeltierF. DingJ. YangY. HuOne of the critical issues of the Snowball Earth hypothesis is the CO<sub>2</sub> threshold for triggering the deglaciation. Using Community Atmospheric Model version 3.0 (CAM3), we study the problem for the CO<sub>2</sub> threshold. Our simulations show large differences from previous results (e.g. Pierrehumbert, 2004, 2005; Le Hir et al., 2007). At 0.2 bars of CO<sub>2</sub>, the January maximum near-surface temperature is about 268 K, about 13 K higher than that in Pierrehumbert (2004, 2005), but lower than the value of 270 K for 0.1 bar of CO<sub>2</sub> in Le Hir et al. (2007). It is found that the difference of simulation results is mainly due to model sensitivity of greenhouse effect and longwave cloud forcing to increasing CO<sub>2</sub>. At 0.2 bars of CO<sub>2</sub>, CAM3 yields 117 Wm<sup>−2</sup> of clear-sky greenhouse effect and 32 Wm<sup>−2</sup> of longwave cloud forcing, versus only about 77 Wm<sup>−2</sup> and 10.5 Wm<sup>−2</sup> in Pierrehumbert (2004, 2005), respectively. CAM3 has comparable clear-sky greenhouse effect to that in Le Hir et al. (2007), but lower longwave cloud forcing. CAM3 also produces much stronger Hadley cells than that in Pierrehumbert (2005). <br><br> Effects of pressure broadening and collision-induced absorption are also studied using a radiative-convective model and CAM3. Both effects substantially increase surface temperature and thus lower the CO<sub>2</sub> threshold. The radiative-convective model yields a CO<sub>2</sub> threshold of about 0.21 bars with surface albedo of 0.663. Without considering the effects of pressure broadening and collision-induced absorption, CAM3 yields an approximate CO<sub>2</sub> threshold of about 1.0 bar for surface albedo of about 0.6. However, the threshold is lowered to 0.38 bars as both effects are considered.http://www.clim-past.net/7/17/2011/cp-7-17-2011.pdf
collection DOAJ
language English
format Article
sources DOAJ
author W. R. Peltier
F. Ding
J. Yang
Y. Hu
spellingShingle W. R. Peltier
F. Ding
J. Yang
Y. Hu
Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
Climate of the Past
author_facet W. R. Peltier
F. Ding
J. Yang
Y. Hu
author_sort W. R. Peltier
title Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
title_short Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
title_full Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
title_fullStr Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
title_full_unstemmed Model-dependence of the CO<sub>2</sub> threshold for melting the hard Snowball Earth
title_sort model-dependence of the co<sub>2</sub> threshold for melting the hard snowball earth
publisher Copernicus Publications
series Climate of the Past
issn 1814-9324
1814-9332
publishDate 2011-01-01
description One of the critical issues of the Snowball Earth hypothesis is the CO<sub>2</sub> threshold for triggering the deglaciation. Using Community Atmospheric Model version 3.0 (CAM3), we study the problem for the CO<sub>2</sub> threshold. Our simulations show large differences from previous results (e.g. Pierrehumbert, 2004, 2005; Le Hir et al., 2007). At 0.2 bars of CO<sub>2</sub>, the January maximum near-surface temperature is about 268 K, about 13 K higher than that in Pierrehumbert (2004, 2005), but lower than the value of 270 K for 0.1 bar of CO<sub>2</sub> in Le Hir et al. (2007). It is found that the difference of simulation results is mainly due to model sensitivity of greenhouse effect and longwave cloud forcing to increasing CO<sub>2</sub>. At 0.2 bars of CO<sub>2</sub>, CAM3 yields 117 Wm<sup>−2</sup> of clear-sky greenhouse effect and 32 Wm<sup>−2</sup> of longwave cloud forcing, versus only about 77 Wm<sup>−2</sup> and 10.5 Wm<sup>−2</sup> in Pierrehumbert (2004, 2005), respectively. CAM3 has comparable clear-sky greenhouse effect to that in Le Hir et al. (2007), but lower longwave cloud forcing. CAM3 also produces much stronger Hadley cells than that in Pierrehumbert (2005). <br><br> Effects of pressure broadening and collision-induced absorption are also studied using a radiative-convective model and CAM3. Both effects substantially increase surface temperature and thus lower the CO<sub>2</sub> threshold. The radiative-convective model yields a CO<sub>2</sub> threshold of about 0.21 bars with surface albedo of 0.663. Without considering the effects of pressure broadening and collision-induced absorption, CAM3 yields an approximate CO<sub>2</sub> threshold of about 1.0 bar for surface albedo of about 0.6. However, the threshold is lowered to 0.38 bars as both effects are considered.
url http://www.clim-past.net/7/17/2011/cp-7-17-2011.pdf
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