A Maxwell elasto-brittle rheology for sea ice modelling

被引:87
作者
Dansereau, Veronique [1 ]
Weiss, Jerome [2 ]
Saramito, Pierre [3 ]
Lattes, Philippe [4 ]
机构
[1] Univ Grenoble, CNRS UMR 5183, Lab Glaciol & Geophys Environm, Grenoble, France
[2] Univ Grenoble, CNRS UMR 5275, Inst Sci Terre, Grenoble, France
[3] Univ Grenoble, CNRS UMR 5224, Lab Jean Kuntzmann, Grenoble, France
[4] TOTAL SA, DGEP, DEV, TEC,GEO, Paris, France
关键词
VISCOELASTIC DAMAGE MODEL; SATELLITE MEASUREMENTS; FRACTURE; DEFORMATION; CREEP; LOCALIZATION; SIMULATION; MECHANICS; SLIP; LAW;
D O I
10.5194/tc-10-1339-2016
中图分类号
P9 [自然地理学];
学科分类号
0705 ; 070501 ;
摘要
A new rheological model is developed that builds on an elasto-brittle (EB) framework used for sea ice and rock mechanics, with the intent of representing both the small elastic deformations associated with fracturing processes and the larger deformations occurring along the faults/leads once the material is highly damaged and fragmented. A viscous-like relaxation term is added to the linear-elastic constitutive law together with an effective viscosity that evolves according to the local level of damage of the material, like its elastic modulus. The coupling between the level of damage and both mechanical parameters is such that within an undamaged ice cover the viscosity is infinitely large and deformations are strictly elastic, while along highly damaged zones the elastic modulus vanishes and most of the stress is dissipated through permanent deformations. A healing mechanism is also introduced, counterbalancing the effects of damaging over large timescales. In this new model, named Maxwell-EB after the Maxwell rheology, the irreversible and reversible deformations are solved for simultaneously; hence drift velocities are defined naturally. First idealized simulations without advection show that the model reproduces the main characteristics of sea ice mechanics and deformation: strain localization, anisotropy, intermittency and associated scaling laws.
引用
收藏
页码:1339 / 1359
页数:21
相关论文
共 79 条
[1]  
Agnon A., 1995, DAMAGE DISTRIBUTION, P65
[2]   From diffuse to localised damage through elastic interaction [J].
Amitrano, D ;
Grasso, JR ;
Hantz, D .
GEOPHYSICAL RESEARCH LETTERS, 1999, 26 (14) :2109-2112
[3]  
[Anonymous], 2012, OCEAN SCI, DOI DOI 10.5194/os-8-633-2012
[4]   Patterns and collective behavior in granular media: Theoretical concepts [J].
Aranson, Igor S. ;
Tsimring, Lev S. .
REVIEWS OF MODERN PHYSICS, 2006, 78 (02) :641-692
[5]   Nonlocal integral formulations of plasticity and damage:: Survey of progress [J].
Bazant, ZP ;
Jirásek, M .
JOURNAL OF ENGINEERING MECHANICS, 2002, 128 (11) :1119-1149
[6]  
BAZANT ZP, 1976, J ENG MECH DIV-ASCE, V102, P331
[7]   A damage mechanics assessment of the Larsen B ice shelf prior to collapse: Toward a physically-based calving law [J].
Borstad, C. P. ;
Khazendar, A. ;
Larour, E. ;
Morlighem, M. ;
Rignot, E. ;
Schodlok, M. P. ;
Seroussi, H. .
GEOPHYSICAL RESEARCH LETTERS, 2012, 39
[8]   Presentation of the dynamical core of neXtSIM, a new sea ice model [J].
Bouillon, Sylvain ;
Rampal, Pierre .
OCEAN MODELLING, 2015, 91 :23-37
[9]   FRICTION OF ROCKS [J].
BYERLEE, J .
PURE AND APPLIED GEOPHYSICS, 1978, 116 (4-5) :615-626
[10]   Onset of aseismic creep on major strike-slip faults [J].
Cakir, Ziyadin ;
Ergintav, Semih ;
Ozener, Haluk ;
Dogan, Ugur ;
Akoglu, Ahmet M. ;
Meghraoui, Mustapha ;
Reilinger, Robert .
GEOLOGY, 2012, 40 (12) :1115-1118