The "Snowball Earth" hypothesis, proposed to explain the Neoproterozoic glacial episodes in the period 750-580 million years ago, suggested that the earth was globally covered by ice/snow during these events. This study addresses the problem of the forcings required for the earth to enter such a state of complete glaciation using the Community Climate System Model, version 3 (CCSM3). All of the simulations performed to address this issue employ the geography and topography of the present-day earth and are employed to explore the combination of factors consisting of total solar luminosity, CO 2 concentration, and sea ice/snow albedo parameterization that would be required for such an event to occur. The analyses demonstrate that the critical conditions beyond which runaway ice-albedo feedback will lead to global freezing include 1) a 10%-10.5% reduction in solar radiation with preindustrial greenhouse gas concentrations; 2) a 6% reduction in solar radiation with 17.5 ppmv CO 2; or 3) 6%less solar radiation and 286 ppmv CO 2 if sea ice albedo is equal to or greater than 0.60 with a snow albedo of 0.78, or if sea ice albedo is 0.58 with a snow albedo equal to or greater than 0.80. These bifurcation points are very sensitive to the sea ice and snow albedo parameterizations. Moreover, "soft Snowball" solutions are found in which tropical open water oceans stably coexist with year-round snow-covered low-latitude continents, implying that tropical continental ice sheets would actually be present. The authors conclude that a "soft Snowball" is entirely plausible, in which the global sea ice fraction may reach as high as 76% and sea ice margins may extend to 10°S(N) latitudes. © 2012 American Meteorological Society.
CITATION STYLE
Yang, J., Peltier, W. R., & Hu, Y. (2012). The initiation of modern “soft snowball” and “hard snowball” climates in CCSM3. Part I: The influences of solar luminosity, CO 2 concentration, and the sea ice/snow Albedo parameterization. Journal of Climate, 25(8), 2711–2736. https://doi.org/10.1175/JCLI-D-11-00189.1
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