Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point

The hard snowball Earth bifurcation point is determined by the level of atmospheric carbon dioxide concentration (pCO(2)) below which complete glaciation of the planet would occur. In previous studies, the bifurcation point was determined based on the assumption that the extent of continental glacia...

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Published in:Climate Dynamics
Main Authors: Liu, Yonggang, Peltier, W. Richard, Yang, Jun, Vettoretti, Guido, Wang, Yuwei
Other Authors: Liu, YG (reprint author), Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China., Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China., Univ Toronto, Dept Phys, 60 St George St, Toronto, ON M5S 1A7, Canada.
Format: Journal/Newspaper
Language:English
Published: CLIMATE DYNAMICS 2017
Subjects:
Online Access:https://hdl.handle.net/20.500.11897/473142
https://doi.org/10.1007/s00382-016-3278-1
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spelling ftpekinguniv:oai:localhost:20.500.11897/473142 2023-05-15T16:40:11+02:00 Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point Liu, Yonggang Peltier, W. Richard Yang, Jun Vettoretti, Guido Wang, Yuwei Liu, YG (reprint author), Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China. Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China. Univ Toronto, Dept Phys, 60 St George St, Toronto, ON M5S 1A7, Canada. 2017 https://hdl.handle.net/20.500.11897/473142 https://doi.org/10.1007/s00382-016-3278-1 en eng CLIMATE DYNAMICS CLIMATE DYNAMICS.2017,48(11),3459-3474. 1907358 0930-7575 http://hdl.handle.net/20.500.11897/473142 1432-0894 doi:10.1007/s00382-016-3278-1 WOS:000402122200001 SCI Snowball Earth Bifurcation point Tropical ice sheet Atmospheric heat transport Neoproterozoic MODERN SOFT SNOWBALL CLIMATE INITIATION MODEL SIMULATIONS GLACIATIONS IMPACT HYPOTHESIS LUMINOSITY DYNAMICS Journal 2017 ftpekinguniv https://doi.org/20.500.11897/473142 https://doi.org/10.1007/s00382-016-3278-1 2021-08-01T11:12:43Z The hard snowball Earth bifurcation point is determined by the level of atmospheric carbon dioxide concentration (pCO(2)) below which complete glaciation of the planet would occur. In previous studies, the bifurcation point was determined based on the assumption that the extent of continental glaciation could be neglected and the results thereby obtained suggested that very low values of pCO(2) would be required (similar to 100 ppmv). Here, we deduce the upper bound on the bifurcation point using the coupled atmosphere-ocean climate model of the NCAR that is referred to as the Community Climate System Model version 3 by assuming that the continents are fully covered by ice sheets prior to executing the transition into the hard snowball state. The thickness of the ice sheet is assumed to be that obtained by an ice-sheet model coupled to an energy balance model for a soft snowball Earth. We find that the hard snowball Earth bifurcation point is in the ranges of 600-630 and 300-320 ppmv for the 720 and 570 Ma continental configurations, respectively. These critical points are between 10 and 3 times higher than their respective values when ice sheets are completely neglected. We also find that when the ice sheets are thinner than those assumed above, the climate is colder and the bifurcation point is larger. The key process that causes the excess cooling when continental ice sheets are thin is shown to be associated with the fact that atmospheric heat transport from the adjacent oceans to the ice sheet-covered continents is enhanced in such conditions. Feedbacks from sea-ice expansion and reduced water vapor concentration further cool the oceanic regions strongly. Ministry of Education of China; NSERC [A9627] SCI(E) ARTICLE 11 3459-3474 48 Journal/Newspaper Ice Sheet Sea ice Peking University Institutional Repository (PKU IR) Climate Dynamics 48 11-12 3459 3474
institution Open Polar
collection Peking University Institutional Repository (PKU IR)
op_collection_id ftpekinguniv
language English
topic Snowball Earth
Bifurcation point
Tropical ice sheet
Atmospheric heat transport
Neoproterozoic
MODERN SOFT SNOWBALL
CLIMATE
INITIATION
MODEL
SIMULATIONS
GLACIATIONS
IMPACT
HYPOTHESIS
LUMINOSITY
DYNAMICS
spellingShingle Snowball Earth
Bifurcation point
Tropical ice sheet
Atmospheric heat transport
Neoproterozoic
MODERN SOFT SNOWBALL
CLIMATE
INITIATION
MODEL
SIMULATIONS
GLACIATIONS
IMPACT
HYPOTHESIS
LUMINOSITY
DYNAMICS
Liu, Yonggang
Peltier, W. Richard
Yang, Jun
Vettoretti, Guido
Wang, Yuwei
Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
topic_facet Snowball Earth
Bifurcation point
Tropical ice sheet
Atmospheric heat transport
Neoproterozoic
MODERN SOFT SNOWBALL
CLIMATE
INITIATION
MODEL
SIMULATIONS
GLACIATIONS
IMPACT
HYPOTHESIS
LUMINOSITY
DYNAMICS
description The hard snowball Earth bifurcation point is determined by the level of atmospheric carbon dioxide concentration (pCO(2)) below which complete glaciation of the planet would occur. In previous studies, the bifurcation point was determined based on the assumption that the extent of continental glaciation could be neglected and the results thereby obtained suggested that very low values of pCO(2) would be required (similar to 100 ppmv). Here, we deduce the upper bound on the bifurcation point using the coupled atmosphere-ocean climate model of the NCAR that is referred to as the Community Climate System Model version 3 by assuming that the continents are fully covered by ice sheets prior to executing the transition into the hard snowball state. The thickness of the ice sheet is assumed to be that obtained by an ice-sheet model coupled to an energy balance model for a soft snowball Earth. We find that the hard snowball Earth bifurcation point is in the ranges of 600-630 and 300-320 ppmv for the 720 and 570 Ma continental configurations, respectively. These critical points are between 10 and 3 times higher than their respective values when ice sheets are completely neglected. We also find that when the ice sheets are thinner than those assumed above, the climate is colder and the bifurcation point is larger. The key process that causes the excess cooling when continental ice sheets are thin is shown to be associated with the fact that atmospheric heat transport from the adjacent oceans to the ice sheet-covered continents is enhanced in such conditions. Feedbacks from sea-ice expansion and reduced water vapor concentration further cool the oceanic regions strongly. Ministry of Education of China; NSERC [A9627] SCI(E) ARTICLE 11 3459-3474 48
author2 Liu, YG (reprint author), Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China.
Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing 100871, Peoples R China.
Univ Toronto, Dept Phys, 60 St George St, Toronto, ON M5S 1A7, Canada.
format Journal/Newspaper
author Liu, Yonggang
Peltier, W. Richard
Yang, Jun
Vettoretti, Guido
Wang, Yuwei
author_facet Liu, Yonggang
Peltier, W. Richard
Yang, Jun
Vettoretti, Guido
Wang, Yuwei
author_sort Liu, Yonggang
title Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
title_short Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
title_full Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
title_fullStr Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
title_full_unstemmed Strong effects of tropical ice-sheet coverage and thickness on the hard snowball Earth bifurcation point
title_sort strong effects of tropical ice-sheet coverage and thickness on the hard snowball earth bifurcation point
publisher CLIMATE DYNAMICS
publishDate 2017
url https://hdl.handle.net/20.500.11897/473142
https://doi.org/10.1007/s00382-016-3278-1
genre Ice Sheet
Sea ice
genre_facet Ice Sheet
Sea ice
op_source SCI
op_relation CLIMATE DYNAMICS.2017,48(11),3459-3474.
1907358
0930-7575
http://hdl.handle.net/20.500.11897/473142
1432-0894
doi:10.1007/s00382-016-3278-1
WOS:000402122200001
op_doi https://doi.org/20.500.11897/473142
https://doi.org/10.1007/s00382-016-3278-1
container_title Climate Dynamics
container_volume 48
container_issue 11-12
container_start_page 3459
op_container_end_page 3474
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