Sensitivity of the dynamics of Pine Island Glacier, West Antarctica, to climate forcing for the next 50 years

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Abstract

Pine Island Glacier, a major contributor to sea level rise in West Antarctica, has been undergoing significant changes over the last few decades. Here, we employ a three-dimensional, higher-order model to simulate its evolution over the next 50 yr in response to changes in its surface mass balance, the position of its calving front and ocean-induced ice shelf melting. Simulations show that the largest climatic impact on ice dynamics is the rate of ice shelf melting, which rapidly affects the glacier speed over several hundreds of kilometers upstream of the grounding line. Our simulations show that the speedup observed in the 1990s and 2000s is consistent with an increase in sub-ice-shelf melting. According to our modeling results, even if the grounding line stabilizes for a few decades, we find that the glacier reaction can continue for several decades longer. Furthermore, Pine Island Glacier will continue to change rapidly over the coming decades and remain a major contributor to sea level rise, even if ocean-induced melting is reduced.

Figures

  • Figure 1. (a) Initial modeled 2008 velocity of Pine Island Glacier, overlain on a MODIS Mosaic of Antarctica with initial grounding line position (white) and glacier centerline (black). (b) Ice front positions used in the sensitivity study.
  • Figure 2. Mesh resolution (in m) used in the simulations; the white box shows the region represented in Figs. 6 and 10.
  • Figure 3. (a) Basal melting rate (in m yr−1) from the MITgcm filled with constant values (50 m yr−1) over areas not covered by the MITgcm. (b) Basal melting rate values (in m yr−1) from the MITgcm represented as a function of ice shelf base depth.
  • Figure 4. (a) Thickness change (in m) and (b) velocity change (in m yr−1) during the 10 yr relaxation period overlain on a MODIS Mosaic of Antarctica. Black line represents the grounding line.
  • Figure 5. Modeled velocity sensitivity (left column) and volume above floatation sensitivity (right column) to (a, b) surface mass balance; (c, d) ice front position and (e, f) ice shelf melting. Solid lines in the left column represent the ice velocity at the end of the simulation and dashed line the initial velocity after ice front retreat when ice front position is changed.
  • Figure 6. Grounding line position at the beginning of the experiments (blue line), and at the end of the melting experiments in the case of β = 1 (red line) and β = 2 (black line) overlain on the bedrock elevation. The mesh resolution is 500 m (a) and 250 m (b) in the grounding line area.
  • Figure 7. Changes in observed and modeled velocities in m yr−1 on a logarithmic scale. (a) Modeled year 11–year 1, (b) modeled year 15–year 1, (c) modeled year 15–year 11, (d), observed 2006–1996, (e) observed 2010–1996, (f) observed 2011–2006. Modeled velocities are from the increased basal melting experiment (melting multiplied by 1.5).
  • Figure 8. Modeled velocity sensitivity (a) and volume above floatation sensitivity (b) to increased ice shelf melting over a limited time. Ice shelf melting is multiplied by 1.5 during the first 0 (red), 5 (yellow), 15 (green) and 50 (blue) yr of the simulation.

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CITATION STYLE

APA

Seroussi, H., Morlighem, M., Rignot, E., Mouginot, J., Larour, E., Schodlok, M., & Khazendar, A. (2014). Sensitivity of the dynamics of Pine Island Glacier, West Antarctica, to climate forcing for the next 50 years. Cryosphere, 8(5), 1699–1710. https://doi.org/10.5194/tc-8-1699-2014

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