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Ice lens

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263: 94: 161: 140: 288: 53:, wedging the soil or rock apart. Ice lenses grow parallel to the surface and several centimeters to several decimeters (inches to feet) deep in the soil or rock. Studies from 1990 have demonstrated that rock fracture by ice segregation (i.e., the fracture of intact rock by ice lenses that grow by drawing water from their surroundings during periods of sustained subfreezing temperatures) is a more effective weathering process than the freeze-thaw process which older texts proposed. 20: 206:). Premelted water exists as a thin layer on the surface of ice. Under premelting conditions, ice and water can coexist at temperatures below -10 °C in a porous medium. The Gibbs-Thomson effect results in water migrating down a thermal gradient (from higher temperatures to lower temperatures); Dash states, “…material is carried to colder regions…” This can also be viewed energetically as favoring larger ice particles over smaller ( 186: 279:
forms in soil. If the ice layer resulted from cooling from a single direction (e.g., the top) the rock fracture tends to lie close to the surface (e.g., 1–2 cm in chalk). If the ice layer results from freezing from both sides (e.g., above and below) the rock fracture tends to lie deeper (e.g., 2–3.5 cm in chalk).
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Rocks routinely contain pores of varying size and shape, regardless of origin or location. Rock voids are essentially small cracks, and serve as the location from which a crack can propagate if the rock is placed in tension. If ice accumulates in a pore asymmetrically, the ice will place the rock in
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A key phenomenon for understanding ice segregation in soil or porous rock (also referred to as an ice lens due to its shape) is premelting, which is the development of a liquid film on surfaces and interfaces at temperatures significantly below their bulk melting temperature. The term premelting is
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have been observed below Antarctic ice sheets; these are believed to result from ice lenses forming in the debris. In the faster flowing glacial regions, the ice sheet is sliding over water saturated sediments (glacial till) or actually being floated upon a layer of water. The till and water served
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The formation of an ice sphere can happen when an object is about 0.5–1.0 ft above where the water reaches repeatedly. The water will form a thin layer of ice on any surface it reaches. Each wave is an advancement and recession of water. The advancement soaks everything on the shore. When the
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Differential frost heave producing complex patterns will occur if the correct conditions exist. Feedback from one year's frost heave influences the effects in subsequent years. For example, a small increase in overburden will affect the depth of ice formation and heaving in the subsequent years.
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Mutron confirmed that ice initially forms in pores and creates small microfractures parallel to the surface. As ice accumulates, the ice layer grows outward in what is frequently characterized as an ice-lens parallel to the surface. Ice will form in water-permeable rock in much the same way as it
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forms, the sphere needs a base that is not water. Most commonly on vegetation, the sphere starts as a dot of ice on a branch or stem. As waves soak the shore in water and briefly expose the soaked objects to freezing temperatures, the dot begins to grow as each thin layer wraps itself around the
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is unable to warm the ice lens boundary. Hence the area through which the water is diffusing continues to cool until another ice segregation layer forms below the first layer. With sustained cold weather, this process can repeat, producing multiple ice layers (ice lenses), all parallel to the
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Walder and Hallet developed models that predict rock crack-growth locations and rates consistent with fractures actually observed in the field. Their model predicted that marble and granite grow cracks most effectively when the temperatures range from a −4 °C to −15 °C; in this range
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If the ice layer resulted from a cooling from a single direction (e.g., the top) the fracture tends to lie close to the surface (e.g., 1–2 cm in chalk). If the ice layer results from freezing from both sides (e.g., above and below) the fracture tends to lie deeper (e.g., 2–3.5 cm in
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Ice lens growth within the bedrock below the glacier is projected during the summer months when there is ample water at the base of the glacier. Ice lenses will form within the bedrock, accumulating until the rock is sufficiently weakened that it shears or spalls off. Layers of rock along the
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granite may develop fractures enclosing ice 3 meters in length in a year. When the temperature is higher the ice which is formed does not apply enough pressure to cause the crack to propagate. When the temperature is below this range the water is less mobile and cracks grow more slowly.
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The basic condition for ice segregation and frost heaving is existence of a region in soil or porous rock which is relatively permeable, is in a temperature range which allows the coexistence of ice and water (in a premelted state), and has a temperature gradient across the region.
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wave recedes, it's left exposed to freezing temperatures. This brief moment of exposure causes a thin layer of ice to form. When that formation is suspended in the air by dead vegetation or erect objects, the ice will begin to form a sphere or teardrop-like shape. Similar to how a
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Frost heave is common in arctic tundra because the permafrost maintains ground frozen at depth and prevents snowmelt and rain from draining. As a result, conditions are optimal for deep ice lens formation with large ice accumulations and significant soil displacement.
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No ice forms under some conditions. At higher overburden pressures and at relatively warm surface temperatures, ice segregation cannot occur; the liquid present freezes within the pore space, with no bulk ice segregation and no measurable surface deformation or frost
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interface between glaciers and the bedrock are freed, producing much of the sediments in these basal regions of glaciers. Since the rate of glacier movement is dependent upon the characteristics of this basal ice, research is ongoing to better quantify the phenomena.
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warms the ice lens boundary, reducing the temperature gradient and controlling the rate of further ice segregation. Under these conditions, ice grows in a single layer which gets progressively thicker. The surface is displaced and soil repositioned or rock
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to reduce friction between the base of the ice sheet and the bedrock. These subglacial waters come from surface water which seasonally drains from melting at the surface, as well as from ice-sheet base melting.
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tension in a plane perpendicular to the ice accumulation direction. Hence the rock will crack along a plane perpendicular to the direction of ice accumulation, which is effectively parallel to the surface.
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The ice initially forms with small microfractures parallel to the surface. As ice accumulates the ice layer grows outward in what is frequently characterized as an ice-lens parallel to the surface.
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Time-dependent models of the frost heave indicate that over a long enough period the short-separation perturbations damp out, while mid-range perturbations grow and come to dominate the landscape.
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Ice forms rapidly when liquid is readily available. When liquid is readily available, the segregated ice (ice lens) grows parallel to the exposed cold surface. It grows rapidly until the
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regions (alpine, subpolar and polar) has often been attributed to the freezing and volumetric expansion of water trapped within pores and cracks, the majority of frost heaving and of
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Peterson, R. A.; Krantz , W. B. (2008). "Differential frost heave model for patterned ground formation: Corroboration with observations along a North American arctic transect".
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used to describe the reduction in the melting temperature (below 0 °C) which results from the surface curvature of water that's confined in a porous medium (the
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Ice forms in a different pattern when liquid is less readily available. When liquid is not readily available, the segregated ice (ice lens) grows slowly. The
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It is possible to develop analytic models using these principles; they predict the following characteristics, which are consistent with field observations:
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Rempel, A.W.; Wettlaufer, J.S.; Worster, M.G. (2001). "Interfacial Premelting and the Thermomolecular Force: Thermodynamic Buoyancy".
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Murton, Julian B.; Peterson, Rorik; Ozouf, Jean-Claude (17 November 2006). "Bedrock Fracture by Ice Segregation in Cold Regions".
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Suspended ice forms into a sphere or tear drop like shape after being repeatedly soaked by waves and frozen by surrounding air.
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surface. The formation of multiple layers (multiple lenses) producing more extensive frost damage within rocks or soils.
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Dash, G.; A. W. Rempel; J. S. Wettlaufer (2006). "The physics of premelted ice and its geophysical consequences".
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and lens growth in the near-surface frozen regions. Ice segregation results in rock fracture and frost heave.
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Walder, Joseph; Hallet, Bernard (March 1985). "A theoretical model of the fracture of rock during freezing".
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Bell, Robin E. (27 April 2008). "The role of subglacial water in ice-sheet mass balance".
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of buildings and displace soil in regular patterns. Moist, fine-grained soil at certain
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in cold regions. Frost heaving creates debris and dramatically shapes landscapes into
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Ice will form in water-permeable rock in much the same way as it forms in soil.
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formed in arctic tundra as a result of periodically spaced ice lens formation.
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and upward thrust of the ground surface. This process can distort and crack
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previous layer. Over time, they form spheres or teardrop-like formations
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Ice Formation on coarse shore of Copper Harbor, Upper Peninsula Michigan.
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Ice lens growing within glacial till and bedrock beneath glacial ice.
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Ice forms in layers which are parallel to the overlying surface.
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of soils and fracture of bedrock, which are fundamental to
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10.1130/0016-7606(1985)96<336:ATMOTF>2.0.CO;2
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Although rock fracture in 7: 181:Understanding the phenomena 10: 1155: 635:American Geophysical Union 531:American Geophysical Union 459:American Geophysical Union 255: 240:heat liberated by freezing 232:heat liberated by freezing 1098: 1072: 1000: 944: 868: 740: 601:10.1103/RevModPhys.78.695 575:American Physical Society 156:Subglacial ice formations 982:Stratified slope deposit 734:Periglacial environment 404:Physical Review Letters 372:10.1126/science.1132127 252:Ice lens growth in rock 16:Ice within soil or rock 891:Fluvio-thermal erosion 517:Rempel, A. W. (2008). 292: 267: 194: 165: 144: 102: 27: 1053:Massenerhebung effect 758:Cryoplanation terrace 619:Rempel, A.W. (2007). 290: 265: 188: 168:Bands of sediment or 163: 142: 96: 58:frost induced heaving 22: 644:10.1029/2006JF000525 548:10.1029/2007JF000870 467:10.1029/2007JG000559 298:condensation nucleus 283:Ice sphere formation 204:Gibbs-Thomson effect 135:Ice lenses in tundra 89:Common frost heaving 936:Zero-curtain effect 686:1985GSAB...96..336W 583:2006RvMP...78..695D 539:2008JGRF..113.1013R 496:2008NatGe...1..297B 417:2001PhRvL..87h8501R 364:2006Sci...314.1127M 358:(5802): 1127–1129. 945:Soils and deposits 293: 268: 195: 166: 145: 103: 28: 1134:Erosion landforms 1116: 1115: 1108:Template:Glaciers 864: 863: 490:(5802): 297–304. 483:Nature Geoscience 320:; July 18, 2012, 101:in cold climates. 1146: 1049:Alpine tree line 1034:Antarctic tundra 1019:Arctic tree line 901:Frost weathering 828:Patterned ground 824: 823: 798:Protalus rampart 788:Periglacial lake 727: 720: 713: 704: 703: 698: 697: 665: 656: 655: 653: 651: 646: 616: 605: 604: 594: 562: 553: 552: 550: 514: 508: 507: 477: 471: 470: 446: 437: 436: 398: 392: 391: 345: 328: 326:10.1130/G33330.1 314: 258:Frost weathering 208:Ostwald ripening 193:(picture) growth 66:complex patterns 1154: 1153: 1149: 1148: 1147: 1145: 1144: 1143: 1119: 1118: 1117: 1112: 1094: 1068: 1024:Antarctic oasis 996: 940: 916:Methane release 911:Ice segregation 860: 822: 763:Glacial erratic 736: 731: 701: 666: 659: 649: 647: 617: 608: 592:10.1.1.462.1061 563: 556: 515: 511: 504:10.1038/ngeo186 478: 474: 447: 440: 399: 395: 346: 331: 315: 311: 307: 285: 260: 254: 183: 158: 137: 91: 86: 78:ice segregation 17: 12: 11: 5: 1152: 1142: 1141: 1136: 1131: 1114: 1113: 1111: 1110: 1105: 1099: 1096: 1095: 1093: 1092: 1087: 1082: 1076: 1074: 1070: 1069: 1067: 1066: 1056: 1046: 1041: 1036: 1031: 1026: 1021: 1016: 1010: 1008: 998: 997: 995: 994: 989: 984: 979: 974: 969: 964: 959: 954: 948: 946: 942: 941: 939: 938: 933: 928: 923: 918: 913: 908: 903: 898: 893: 888: 883: 878: 872: 870: 866: 865: 862: 861: 859: 858: 853: 848: 843: 838: 832: 830: 821: 820: 815: 810: 805: 800: 795: 790: 785: 780: 775: 770: 765: 760: 755: 750: 744: 742: 738: 737: 730: 729: 722: 715: 707: 700: 699: 657: 606: 567:Rev. 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Index


Pingo
moisture
diffused
soil
rock
lens
frost induced heaving
weathering
complex patterns
periglacial
bedrock
ice segregation

frost heave
Frost heave
saturated
soil
deformation
pavement
foundations
temperatures


glacial till

palsa
Gibbs-Thomson effect
Ostwald ripening
heat liberated by freezing

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