Fracture density modeling¶
The fracture density approach in PISM is based on [106] and assumes a macroscopic measure for the abundance of (partly microscale) crevasses and rifts that form in ice (shelves) and that can be transported with the ice flow as represented in a continuum ice-flow model. This approach is similar to the Continuum Damage Mechanics (CDM) (e.g. [107] and [108]) introducing a damage state variable (\(\phi\) or \(D\)) that equals zero for fully intact ice and one for fully fractured ice, that can be interpreted as a loss of all load bearing capacity.
The feedback of damage to the ice flow (creep) works within the existing constitutive framework by introducing a linear mapping between the actual physical (damaged) state of the material and an effective state that is compatible with a homogeneous, continuum representation of the creep law (Eq. 6 in [109]).
Fractures form above a critical stress threshold \(\sigma_{\text{cr}}\) in the ice (e.g. von Mises criterion, maximum stress criterion or fracture toughness from Linear Elastic Fracture Mechanics) with a fracture growth rate proportional to \(\gamma\) (Eq. 2 in [109]), that is related to the strain rate (longitudinal spreading or effective strain rate; Eq. 9 in [106]). Fracture healing is assumed to occur with a defined healing rate below a strain rate threshold (scaled with the difference to the threshold or constant; Eq. 11 in [106]).
The fracture growth constant \(\gamma\) (fracture_density
.gamma
) is ignored if
fracture_density
.borstad_limit
is set.
To enable this model, set fracture_density
.enabled
.
Parameters
Prefix: fracture_density.
borstad_limit
(no) Model fracture growth according to the constitutive law in [110] (Eq. 4), ignoringfracture_density
.gamma
.constant_fd
(no) Keep fracture density fields constant in time but include its softening effect.constant_healing
(no) Use a constant healing rate \(-\gamma_h \dot{\epsilon}_h\) independent of the local strain rate.fd2d_scheme
(no) Use an alternative transport scheme to reduce numerical diffusion (Eq. 10 in [109])fracture_weighted_healing
(no) Multiply the healing rate by \(1 - D\), i.e. assume that highly damaged ice heals slower. This mechanism can be combined withfracture_density
.constant_healing
.gamma
(1) fracture growth constant \(\gamma\)gamma_h
(0) fracture healing constant \(\gamma_{h}\)healing_threshold
(2e-10 1/s) fracture healing strain rate threshold \(\dot \epsilon_{h}\)include_grounded_ice
(no) Model fracture density in grounded areas (e.g. along ice stream shear zones) in addition to ice shelvesinitiation_threshold
(70000 Pa) fracture initiation stress threshold \(\sigma_{\text{cr}}\)lefm
(no) Use the mixed-mode fracture toughness stress criterion based on Linear Elastic Fracture Mechanics, Eqs. 8-9 in [109]max_shear_stress
(no) Use the maximum shear stress criterion for fracture formation (Tresca or Guest criterion in literature), which is more stringent than the default von Mises criterion, see Eq. 7 in [109]phi0
(0) Fracture density value used at grid points where ice velocity is prescribed. This assumes that all ice entering a shelf atbc_mask
locations has the same fracture density.softening_lower_limit
(1) Parameter controlling the strength of the feedback of damage on the ice flow. If \(1\): no feedback, if \(0\): full feedback (\(\epsilon\) in Eq. 6 in [109])
Testing
See the scripts in example/ross/fracture
for a way to test different damage options
and parameter values. Build a setup for the Ross Ice Shelf and let the damage field
evolve, with fracture bands reaching all the way from the inlets to the calving front.
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