Interdependence of the growth of the Northern Hemisphere ice sheets during the last glaciation: The role of atmospheric circulation

23Citations
Citations of this article
34Readers
Mendeley users who have this article in their library.

Abstract

The development of large continental-scale ice sheets over Canada and northern Europe during the last glacial cycle likely modified the track of stationary waves and influenced the location of growing ice sheets through changes in accumulation and temperature patterns. Although they are often mentioned in the literature, these feedback mechanisms are poorly constrained and have never been studied throughout an entire glacial-interglacial cycle. Using the climate model of intermediate complexity CLIMBER-2 coupled with the 3-D ice-sheet model GRISLI (GRenoble Ice Shelf and Land Ice model), we investigate the impact of stationary waves on the construction of past Northern Hemisphere ice sheets during the past glaciation. The stationary waves are not explicitly computed in the model but their effect on sea-level pressure is parameterized. We tested different parameterizations to study separately the effect of surface temperature (thermal forcing) and topography (orographic forcing) on sea-level pressure, and therefore on atmospheric circulation and ice-sheet surface mass balance. Our model results suggest that the response of ice sheets to thermal and/or orographic forcings is rather different. At the beginning of the glaciation, the orographic effect favors the growth of the Laurentide ice sheet, whereas Fennoscandia appears rather sensitive to the thermal effect. Using the ablation parameterization as a trigger to artificially modify the size of one ice sheet, the remote influence of one ice sheet on the other is also studied as a function of the stationary wave parameterizations. The sensitivity of remote ice sheets is shown to be highly sensitive to the choice of these parameterizations with a larger response when orographic effect is accounted for. Results presented in this study suggest that the various spatial distributions of ice sheets could be partly explained by the feedback mechanisms occurring between ice sheets and atmospheric circulation. © 2014 Author(s).

Figures

  • Fig. 1. Difference between sea-level pressure and its zonal mean in winter (DJF) for (a) NCEP reanalysis, (b) with only thermal parameterization (TH), (c) with only orographic parameterization (ORO) and (d) for the sum of the two parameterizations (OTH) (hPa).
  • Table 1. Experimental set-up. For each experiment, the 1st part of the name (NONE, TH, ORO, OTH) corresponds to the stationary wave parameterization while the second part corresponds to the ablation formulation: REF indicates the couple σLIS0 − σ FIS
  • Fig. 2. Summer surface temperature at 125 ka in NONE-REF experiment (parameterization of SLP are removed) (a), difference of summer surface air temperature between TH-REF (thermal parameterization) and NONE-REF (b); ORO-REF (orographic parameterization) and NONE-REF (c) and OTH-REF (combination of both thermal and orographic parameterization) and NONE-REF (c) at 125 ka. Same for the snow accumulation (e–h). The green line represents the limit where the ice thickness difference exceeds −500 m.
  • Fig. 3. Ice thickness (colors) and ice-sheet height (contours, isolines every 500 m) simulated at 115 ka with the four parameterizations (m).
  • Fig. 4. The left part of the figure shows the evolution of Fennoscandian ice volume (a) for the reference experiments (solid lines, black when the waves are off, blue for the thermal parameterization, red for the orographic parameterization, and green when the two effects are on) and for the experiments with a smaller σFIS0 (plotted line, same color code). (b) shows the Laurentide ice volume for the same experiments. The right part of the figure shows the evolution of the Laurentide ice volume (c) for the reference experiments (solid lines) and for the ones with smaller σLIS0 (dotted lines), then the Fennoscandian ice volume (d) for the same experiments. For all panels, the evolution of ice volume is shown for the inception.
  • Fig. 5. Summer surface temperature differences between NONE-FIS and NONE-REF at 125 ka (a) and 120 ka (b). The yellow line represents the limit where the ice thickness difference exceeds 500 m.
  • Fig. 6. Azonal sea-level pressure (in hPa) at 120 and 115 ka for OTH (a–b) and TH experiments (e–f), respectively, and accumulation (in meter water equivalent) at 120 and 115 ka for OTH (c–d) and TH experiments (g-h). Grey lines indicate the limits of the ice sheets.
  • Fig. 7. The left part of the figure shows the evolution of Fennoscandian ice volume (a) for the reference experiments (solid lines, black when the waves are off, blue for the thermal parameterization, red for the orographic parameterization, and green when the two effects are on) and for the experiments with a smaller σFIS0 (plotted line, same color code). (b) shows the Laurentide ice volume for the same experiments. The right part of the figure shows the evolution of the Laurentide ice volume (c) for the reference experiments (solid lines) and for the ones with smaller σLIS0 (dotted lines), then the Fennoscandian ice volume (d) for the same experiments. For all panels, the evolution of ice volume is shown for the all glaciation.

References Powered by Scopus

The NCEP/NCAR 40-year reanalysis project

26400Citations
N/AReaders
Get full text

Climate and atmospheric history of the past 420,000 years from the Vostok ice core, Antarctica

4791Citations
N/AReaders
Get full text

Global glacial isostasy and the surface of the ice-age earth: The ICE-5G (VM2) model and GRACE

2230Citations
N/AReaders
Get full text

Cited by Powered by Scopus

Evolution of the large-scale atmospheric circulation in response to changing ice sheets over the last glacial cycle

105Citations
N/AReaders
Get full text

Orbital control of western North America atmospheric circulation and climate over two glacial cycles

91Citations
N/AReaders
Get full text

Constraint on the penultimate glacial maximum Northern Hemisphere ice topography (≈140 kyrs BP)

79Citations
N/AReaders
Get full text

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Cite

CITATION STYLE

APA

Beghin, P., Charbit, S., Dumas, C., Kageyama, M., Roche, D. M., & Ritz, C. (2014). Interdependence of the growth of the Northern Hemisphere ice sheets during the last glaciation: The role of atmospheric circulation. Climate of the Past, 10(1), 345–358. https://doi.org/10.5194/cp-10-345-2014

Readers over time

‘13‘14‘15‘16‘17‘18‘19‘20‘21‘22‘23‘24‘2502468

Readers' Seniority

Tooltip

PhD / Post grad / Masters / Doc 13

50%

Researcher 9

35%

Professor / Associate Prof. 3

12%

Lecturer / Post doc 1

4%

Readers' Discipline

Tooltip

Earth and Planetary Sciences 20

83%

Environmental Science 3

13%

Arts and Humanities 1

4%

Save time finding and organizing research with Mendeley

Sign up for free
0