The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description

We present the Potsdam Parallel Ice Sheet Model (PISM-PIK), developed at the Potsdam Institute for Climate Impact Research to be used for simulations of large-scale ice sheet-shelf systems. It is derived from the Parallel Ice Sheet Model (Bueler and Brown, 2009). Velocities are calculated by superpo...

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Main Authors: R. Winkelmann, M. A. Martin, M. Haseloff, T. Albrecht, E. Bueler, C. Khroulev, A. Levermann
Format: Article
Language:English
Published: Copernicus Publications 2011-09-01
Series:The Cryosphere
Online Access:http://www.the-cryosphere.net/5/715/2011/tc-5-715-2011.pdf
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spelling doaj-c8078fa5e41045d09cb58eea2f81f0ea2020-11-24T23:29:30ZengCopernicus PublicationsThe Cryosphere1994-04161994-04242011-09-015371572610.5194/tc-5-715-2011The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model descriptionR. WinkelmannM. A. MartinM. HaseloffT. AlbrechtE. BuelerC. KhroulevA. LevermannWe present the Potsdam Parallel Ice Sheet Model (PISM-PIK), developed at the Potsdam Institute for Climate Impact Research to be used for simulations of large-scale ice sheet-shelf systems. It is derived from the Parallel Ice Sheet Model (Bueler and Brown, 2009). Velocities are calculated by superposition of two shallow stress balance approximations within the entire ice covered region: the shallow ice approximation (SIA) is dominant in grounded regions and accounts for shear deformation parallel to the geoid. The plug-flow type shallow shelf approximation (SSA) dominates the velocity field in ice shelf regions and serves as a basal sliding velocity in grounded regions. Ice streams can be identified diagnostically as regions with a significant contribution of membrane stresses to the local momentum balance. All lateral boundaries in PISM-PIK are free to evolve, including the grounding line and ice fronts. Ice shelf margins in particular are modeled using Neumann boundary conditions for the SSA equations, reflecting a hydrostatic stress imbalance along the vertical calving face. The ice front position is modeled using a subgrid-scale representation of calving front motion (Albrecht et al., 2011) and a physically-motivated calving law based on horizontal spreading rates. The model is tested in experiments from the Marine Ice Sheet Model Intercomparison Project (MISMIP). A dynamic equilibrium simulation of Antarctica under present-day conditions is presented in Martin et al. (2011).http://www.the-cryosphere.net/5/715/2011/tc-5-715-2011.pdf
collection DOAJ
language English
format Article
sources DOAJ
author R. Winkelmann
M. A. Martin
M. Haseloff
T. Albrecht
E. Bueler
C. Khroulev
A. Levermann
spellingShingle R. Winkelmann
M. A. Martin
M. Haseloff
T. Albrecht
E. Bueler
C. Khroulev
A. Levermann
The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
The Cryosphere
author_facet R. Winkelmann
M. A. Martin
M. Haseloff
T. Albrecht
E. Bueler
C. Khroulev
A. Levermann
author_sort R. Winkelmann
title The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
title_short The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
title_full The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
title_fullStr The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
title_full_unstemmed The Potsdam Parallel Ice Sheet Model (PISM-PIK) – Part 1: Model description
title_sort potsdam parallel ice sheet model (pism-pik) – part 1: model description
publisher Copernicus Publications
series The Cryosphere
issn 1994-0416
1994-0424
publishDate 2011-09-01
description We present the Potsdam Parallel Ice Sheet Model (PISM-PIK), developed at the Potsdam Institute for Climate Impact Research to be used for simulations of large-scale ice sheet-shelf systems. It is derived from the Parallel Ice Sheet Model (Bueler and Brown, 2009). Velocities are calculated by superposition of two shallow stress balance approximations within the entire ice covered region: the shallow ice approximation (SIA) is dominant in grounded regions and accounts for shear deformation parallel to the geoid. The plug-flow type shallow shelf approximation (SSA) dominates the velocity field in ice shelf regions and serves as a basal sliding velocity in grounded regions. Ice streams can be identified diagnostically as regions with a significant contribution of membrane stresses to the local momentum balance. All lateral boundaries in PISM-PIK are free to evolve, including the grounding line and ice fronts. Ice shelf margins in particular are modeled using Neumann boundary conditions for the SSA equations, reflecting a hydrostatic stress imbalance along the vertical calving face. The ice front position is modeled using a subgrid-scale representation of calving front motion (Albrecht et al., 2011) and a physically-motivated calving law based on horizontal spreading rates. The model is tested in experiments from the Marine Ice Sheet Model Intercomparison Project (MISMIP). A dynamic equilibrium simulation of Antarctica under present-day conditions is presented in Martin et al. (2011).
url http://www.the-cryosphere.net/5/715/2011/tc-5-715-2011.pdf
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