2001
DOI: 10.1061/(asce)0887-381x(2001)15:3(135)
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Ice Rubble Behavior in Punch Tests

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Cited by 15 publications
(3 citation statements)
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“…We uphold the Coulomb‐frictional limit on the contact interface: false‖σtijfalse‖0.25emμfalse‖σnijfalse‖, and excess elastic energy is recorded as frictional heat loss. Increases in contact strength by freezing can be added to the right‐hand side of the above equation through a time and temperature‐dependent cohesion term (e.g., Azarnejad & Brown, 2001), but is not included here. The normal and tangential forces on the ice floes for the momentum equations (Equations and ) are found by decomposing the tangential stress according to the contact orientation: fnij=(σtijbold-italicnfalse^ij)Aij, and ftij=(σtijbold-italictfalse^ij)Aij, where bold-italicnfalse^ and bold-italictfalse^ are unit‐length normal and tangential vectors for the i and j particle pair.…”
Section: Ridging Parameterization For Large‐scale Simulationsmentioning
confidence: 99%
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“…We uphold the Coulomb‐frictional limit on the contact interface: false‖σtijfalse‖0.25emμfalse‖σnijfalse‖, and excess elastic energy is recorded as frictional heat loss. Increases in contact strength by freezing can be added to the right‐hand side of the above equation through a time and temperature‐dependent cohesion term (e.g., Azarnejad & Brown, 2001), but is not included here. The normal and tangential forces on the ice floes for the momentum equations (Equations and ) are found by decomposing the tangential stress according to the contact orientation: fnij=(σtijbold-italicnfalse^ij)Aij, and ftij=(σtijbold-italictfalse^ij)Aij, where bold-italicnfalse^ and bold-italictfalse^ are unit‐length normal and tangential vectors for the i and j particle pair.…”
Section: Ridging Parameterization For Large‐scale Simulationsmentioning
confidence: 99%
“…and excess elastic energy is recorded as frictional heat loss. Increases in contact strength by freezing can be added to the right-hand side of the above equation through a time and temperature-dependent cohesion term (e.g., Azarnejad & Brown, 2001), but is not included here. The normal and tangential forces on the ice floes for the momentum equations (Equations 1 and 2) are found by decomposing the tangential stress according to the contact orientation:…”
Section: Ridging Parameterization For Large-scale Simulationsmentioning
confidence: 99%
“…The initial tests performed in laboratories were direct shear box tests [7][8][9]. Subsequently, biaxial shear tests [10][11][12][13], triaxial shear tests [14,15] and punch-through tests [16][17][18] have been conducted. Based on laboratory tests, an elastic-perfectly plastic model based on the Mohr-Coulomb law was proposed to describe ice rubble behavior [19,20].…”
Section: Introductionmentioning
confidence: 99%