Crack nucleation mechanism in saline ice

A mechanism for crack nucleation in saline ice is presented, by considering a planar array of hexagonal grains containing the brine pockets as a model of poly crystalline saline ice. It is shown through a thermodynamic analysis that important local stresses arise associated with the internal pressure which builds up inside a brine pocket due to a drop in the temperature. As the temperature drops, the water inside the brine freezes, and because of the variation in the water density on freezing, this results in a buildup of pressure inside the pocket. For typical field conditions, assuming elastic behavior for the matrix, pressures as high as 7 MPa are estimated. Next, using a finite element method, the stress concentration at a grain triple junction is determined under the influence of the stress field associated with a nearby brine pocket. The resulting stress state is used to determine the condition for crack nucleation. The analysis is restricted to only elastic deformation regimes with isotropic grains, albeit with elastic constants corresponding to extreme values in a single freshwater ice crystal. The mechanism discussed here provides an explanation for the widely observed brine channels in sea ice. In addition, the effect of the externally applied stress is also considered, and the resulting stress singularities at the grain triple junctions analyzed by an asymptotic method as well as by a numerical solution. Both the strength and an approximate energy criteria suggest crack nucleation from the brine pocket surface towards the grain triple junction. The results are shown to be consistent with the experimental observations.

[1]  M. Williams,et al.  Stress Singularities Resulting From Various Boundary Conditions in Angular Corners of Plates in Extension , 1952 .

[2]  C. Knight Polygonization of Aged Sea Ice , 1962, The Journal of Geology.

[3]  S. Sjölind A constitutive model for ice as a damaging visco-elastic material , 1987 .

[4]  M. Ashby,et al.  Pressure sintering by power law creep , 1975 .

[5]  J. Hutchinson,et al.  Three-Dimensional Effects in Microcrack Nucleation in Brittle Polycrystals , 1990 .

[6]  D. Cole Crack nucleation in polycrystalline ice , 1988 .

[7]  M. Wu,et al.  Crack nucleation due to elastic anisotropy in polycrystalline ice , 1990 .

[8]  K. O. Bennington Some Crystal Growth Features of Sea Ice , 1963, Journal of Glaciology.

[9]  E. Schulson,et al.  The Strength and Ductility of Ice Under Tension , 1988 .

[10]  M. Wu,et al.  Elastic anisotropy and micro-damage processes in polycrystalline ice Part I: Theoretical formulation , 1992, International Journal of Fracture.

[11]  M. F. Ashby,et al.  Rate-controlling processes in the creep of polycrystalline ice , 1983 .

[12]  M. Wu,et al.  Elastic anisotropy and micro-damage processes in polycrystalline ice , 1992 .

[13]  M. Dudley,et al.  Dynamic observation of dislocation sources at grain boundaries in ice , 1992 .

[14]  T. H. Jacka The time and strain required for development of minimum strain rates in ice , 1984 .

[15]  Wilfrid A. Nixon,et al.  The Structure and Tensile Behavior of First-Year Sea Ice and Laboratory-Grown Saline Ice , 1990 .

[16]  J. Hutchinson,et al.  Microcracking in Ceramics Induced by Thermal Expansion or Elastic Anisotropy , 1988 .

[17]  B. J. Mason The spontaneous crystallization of supercooled water , 1952 .

[18]  A. Evans Microfracture from thermal expansion anisotropy—I. Single phase systems , 1978 .

[19]  S. Nanthikesan,et al.  Crack nucleation due to elastic anisotropy in porous ice , 1990 .

[20]  J. Dundurs,et al.  Effect of Elastic Constants on Stress In A Composite Under Plane Deformation , 1967 .

[21]  J. A. Richter-Menge,et al.  Preliminary Results of Direct Tension Tests on First-Year Sea Ice Samples , 1991 .

[22]  P. Visagie Pressures Inside Freezing Water Drops , 1969, Journal of Glaciology.