International Pipeline Conference — Volume I ASME 1998 IPC1998-2054 THE SIGNIFICANCE OF SOIL FREEZING FOR STRESS CORROSION CRACKING Peter J. W illiam s Thom as L. W hite J. Kenneth Torrance Geotechnical Science Laboratories, Carieton University 1125 Colonel By Drive Ottawa ON K1S 5B6 Canada Tel: (613)520 2852 Fax: (613)520 3640 E-mail: [email protected] ABSTRACT The microstructure of soils (the arrangement of pores and voids, aggregation and surface characteristics of particles) is substantially modified by freezing. Soils so modified differ, in a number of important properties, from soils not previously frozen. Furthermore, each time a soil is frozen there is a redistribution of particles, moisture and solutes. Corrosion of buried pipes is known to be related to the ground conditions. Accordingly the particular nature of frozen ground needs consideration in this respect. Studies of microstructure o f samples of freezing, frozen and unfrozen soils, many obtained from a full-scale experimental study of the effects o f freezing on a buried pipeline, have provided an explanation for measured changes in bulk geotechnical properties of the materials. The microstructure viewed by optical microscopy, reveals the soil structure as having a complex and striking dependence on freezing history. Scanning electron microscopy shows further details in clay rich soils. Freezing at tem peratures occurring in nature normally does not convert all the soil w ater to ice. The effects of particle surface forces is to reduce the freezing point of the w ater nearest a mineral surface. The distribution of solutes is radically altered, with pockets of high concentration interconnected by a liquid phase of varying concentration. A variety o f other effects, relating to chemical and mechanical properties o f soils subjected to freezing, have been demonstrated or can be postulated. Some o f these are important in corrosion phenomena. The stresses that have been shown to occur in a pipe as a result o f frost heave in the freezing soil, will also tend to increase the possibility of stress corrosion cracking. INTRODUCTION Most people would agree that understanding stress corrosion cracking (SCC) requires understanding the soil, or ground, environment o f the corroding structure. There is a significant body of knowledge on the importance of the soil conditions in those regions where the problems of SCC are greatest. The cold regions of the world are not those we think o f in this context. Yet in fact, the cold regions, those where freezing of the ground is extensive, have particular importance: in Russia the troubled pipeline network of Siberia in the permafrost regions is of great political and industrial significance. In North America we have the prestigious example of the TransAlaska oil pipeline, and the smaller, Canadian Norman Wells-Zama oil line (although no large gas pipelines at all) passing through the permafrost. In southern Canada and the northern US there are many pipelines where the adjacent soil may be frozen for much of the winter. Probably the world’s largest oil spill on land, the Russian, Komi spill of 1994, has been ascribed to corrosion problems. Those of us who study the effects of frost heave on pipelines have also considered how this failure and others might relate to the cold conditions. In fact, there may well be multiple causes. A pipe may have failed due to corrosion which had been exacerbated by the stresses associated with the frost heave displacements and also by the particular conditions for corrosion that occur in freezing ground. Even geotechnical engineers often do not realise just how significantly different freezing soil is from ’normal’, that is unfrozen, soil. Frozen soil is usually thought o f as cold and bard. Both conditions sound relatively benign. THE NATURE OF FREEZING GROUND When water freezes in small spaces it behaves differently than ’normal’water. Notably the tem perature at which freezing occurs is less than 0 ° (by up to a few degrees) and the pressure conditions of the ice and the w ater are quite different from those of ’ordinary’ or bulk ice - that is, ice which is not confined in small spaces. As much as half of the moisture content, in some clays, is unfrozen at 5 ° C. Sands and other coarse-grained soils have little unfrozen water while medium textured soils lie between these extremes. In brief, at the microscopic scale the behaviour is dictated by forces at the molecular level, associated with the interfaces between the mineral surfaces of the particles, the w ater and the ice (Williams and Smith 1991). The area of mineral particle surface in a gram of clay can be as large as the area o f a football field (consider how the area of particle surface increases as the particles are divided into smaller and smaller particles). In turn these surface forces and the distribution of the stresses at the microscopic level cause displacements of the particles and of the w ater and ice (White and Williams, 1994). Plate 1 shows the result of a single freezing (and thawing) of a silt soil. The change in the soil’s microstructure from the unfrozen state to the once-frozen state is very clear. We all know how important the microstructure of steel is for its properties and it should come as no surprise that the microstructure of a soil has effects on the mechanical, hydraulic, chemical, and geotechnical properties. How significant is freezing of the ground likely to be in the question of stress corrosion cracking? Because the properties of freezing soils are so different to those of unfrozen soils, they must be considered in the analysis of SCC in the cold regions. Copyright © 1998 by ASME Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab the pipeline (Williams et al. 1993), there are a variety o f less direct effects which may be even more important. If the soil which has experienced frost heave thaws, its strength falls to a value lower, probably much lower, than it had prior to <*>) Plate 1. (a) Micrograph of Caen silt, unfrozen (b) Similar m aterial after one freeze-thaw cycle (both frames are 13.5 mm wide in reality). UNIQUE CHARACTERISTICS OF FREEZING SOILS Mechanical properties: These are dominated by creep and by the process of frost heave. The former is the tendency to deform over long periods of time at rather small stresses, notwithstanding the demonstrably high strength under short term loading. Frost heave is a related phenomenon best known as causing irregular uplift of the ground surface where winters are cold; frost heave may disrupt driveways or highways, building foundations and underground services (Ladanyi and Andersland 1995). It is less widely known that it is due to the movement of water from unfrozen soil to the freezing zone giving rise to layers of ice within the frozen soil (PI. 2). Known only to specialists is that the water, in a still liquid state within solid-frozen soil, moves slowly along microscopic pathways in tiny pores and along particle surfaces to freeze at some lower temperature where it gives rise to high stresses and small deformations within the rock-like material. A pipeline buried in frozen ground will often experience high stresses on this account with a slowly developing deformation (Williams 1989). In addition to the direct effects of frost heave on Plate 2. Frozen silt soil (sample approx. 8 cm high) showing ice layers. freezing. A pipeline may subside -the essential problem of oil pipelines in permafrost - or if a gas line, it may be displaced upwards by buoyancy in the water saturated soil. The weakened soil following thaw, on sloping ground will be exposed to risk of erosion by surface meltwater such as to expose the pipe. There is abundant evidence (PI. 3 ) o f all these effects in the Russian pipeline system in the permafrost regions (Williams, 1992, Kharionovsky, 1992). The problems associated with thaw have been tackled in the TransAlaska pipeline, although at great expense, and in the Norman Wells - Zama oil line. There remains the problem of SCC. Even when the stresses originating through freezing and thawing are held within acceptable operating limits, these stresses are a factor in the development of SCC over the life-time of the pipeline. The thermodynamic processes associated with freezing of soils must be considered, because of the stresses they produce in a pipe. Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab Plate 4 (cont’d). (b) sim ilar m aterial contaminated with 10 parts per million aviation diesel and exposed to two further freeze-thaw cycles. P late 3. Pipeline deformed by frost heave and exposed by erosion of thawed frost heaved materials. Siberia. When w ater freezes pure ice is formed and dissolved materials are excluded. Solutes become concentrated in the water that remains (in certain circumstances, for example, sea ice, the crystalline ice may come to enclose a small body o f highly concentrated solution or even o f precipitate - but the dissolved material does not become integral with the ice). In frozen soils the solutes will be concentrated in unfrozen w ater located on the surface of particles and in small pores, and there may be pockets o f highly concentrated solution. Physico-chemical properties: The effects of freezing are so fundamental, as is evidenced by the modification of microstructure, that it is not surprising they modify the chemistry of the soil as well as its physics. M ore surprising is the degree to which a small admixture, literally parts p er million of certain chemicals, can cause substantial modifications o f the microstructure (Pis. 4 and 5) of soils exposed to freezing (W hite and Coutard 1998) . This is further evidence of the close and sensitive relations of soil chemistry to soil microstructure in freezing conditions. Plate 5. Electron micrographs of sam e m aterial as in Plate 4 (b). An aggregate structure has developed with the individual a l t grains closely packed into th e aggregates, with large c h a n n e ls between intersections o f aggregates, (a) image length approx 0 3 mm Plate. 4 (a) Optical micrograph of Caen silt after exposure to two cycles of freeze-thaw. Thermal properties: The fact of freezing is always important for thermal properties. The conversion of w ater to ice requires the extraction of latent heat of fusion, 334 J g m 1. By contrast, to lower the tem perature of w ater by one degree C requires the removal of only 4.12 J g m 1. This means that tem perature changes will occur much more slowly in freezing ground. Ground freezing is a climatic effect and the thermal properties are important over the whole Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab facility at the Centre de Geomorphologie, CNRS, Caen, France, (extensively reported, see Geotechnical Science Laboratories, 1997). The experiment showed how a pipe could be deformed as a consequence of differential frost heave arising from a transition from silty to sandy soil (Figure 1 and Fremond and Mikkoia 1993, Williams et al. 1992). The results of this study continue to be analysed and with the slow-down in plans for extraction o f oil and gas in the Canadian Arctic, the design response for pipelines in permafrost is still unclear. It was established that slow heaving and accompanying deformation occurs in frozen ground when the soil is a degree or so below freezing point and is therefore frozen solid (Smith and Patterson, 1989). Furthermore the associated heaving stress is transmitted to the pipe and the effect may increase with time even after there is a quasi-steady tem perature state. Plate 5 (coat’d) (b) further enlargement, o f angle aggregate seen in left centre o f (a> Chilled Air Ground Surface -Q.7S*C E range of studies associated with cold terrain. Quite generally, therefore, therm al properties will have to be considered in SCC although the significance is not as immediately relevant as the direct frost-heave induced stresses. Biological properties: It is wrong to think of frozen ground as a barren material with respect to biological activity. Apart from the living organisms that survive in ice (such as the algae which may give a pinkish colour to glacier ice, or the bacteria leading to deterioration of frozen foods with tim e) the often large amounts of still mobile w ater provide an environment for a range of microbiological organisms. In so far as organisms such as bacteria are believed to play an im portant role in SCC, it should be noted that this should also be true in freezing ground -although the organisms will probably be fewer and their activities less than in unfrozen materials. SIGNIFICANCE OF THE PROPERTIES OF FREEZING SOIL FOR THE PROCESSES OF STRESS CORROSION CRACKING In speaking generally of the importance o f soil freezing in pipelines it is im portant to rem em ber that gas pipelines are often colder than the surrounding ground and therefore can cause freezing. Oil pipelines in the cold regions are frequently warmer than the natural soil and thus are particularly associated with problems of thawing. Stress corrosion cracking needs to be considered from both points of view. Indeed, many pipelines will be exposed to conditions where tem perature gradients are, at different times, towards and away from the pipe. Certainly the direction of the temperature gradient is very important when considering in detail what occurs in the soil at freezing temperatures. Frost heave: Two main effects of frost heave must be considered. Firstly, frost heave itself may be sufficient to render a pipeline inoperable (Williams 1989). If the pipeline is already weakened by SCC then com pared to otherwise similar ground freezing conditions, the frost heave is likely to be a still larger threat to the pipeline. Secondly, the SCC process itself is accelerated by the stresses produced in the pipe by frost heave. Concern over the uncertain magnitude of the mechanical effects of frost heave led to a major experimental study of an 11" diameter gas pipe placed in freezing ground in a controlled environment «V ft ////A ■ Û ////À : . ■' ' : .• -■ 18 m <■) V p i o * E i m p i i v SOi Figure 1. (a) arrangement o f pipeline in experimental facility (b) deformation of pipe caused by freezing o f soil (note vertical scale is mm, horizontal is m). In the experiment the pipe was held at a lower (freezing) tem perature than the soil. It was observed that a cavity developed below the pipe and running throughout its length in the silt section. During the period of freezing, occasional observations revealed substantial accumulations of ice in the cavity. The cavity could be clearly seen on excavation following thaw (PI. 6). The cavity appears to be analogous to that known to form naturally under boulders as these are lifted relative to the soil matrix, to ultimately appear as a 'growing stone’ at the ground surface (Washburn 1979, Williams and Smith 1991). Similar effects result in fence posts, utility poles and similar being progressively Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab Plate 6. Cavity below pipe, following freeze-thaw cycle, revealed by excavation (the cavity is seen as the dark opening immediately below the pipe). displaced upwards sometim es to the extent of their falling over. The mechanism, or more probably, mechanisms, have been widely discussed in the geological literature. Broadly speaking, the object (in this case the pip e) is either heaved up by a growing ice accumulation below the pipe, or the pipe is pulled up by expanding freezing soil adhering to it laterally. In either case, at thaw the extraneous object is unlikely to settle back at its original level because o f small stones, gravel etc that tend to fall into the space vacated by the ice. T he significance o f the cavity and the attendant soil shear is that they show the forces which freezing can exert and which may disrupt a protective coating. The formation o f discrete ice masses in freezing soils is an effect of the fine-porous nature of the soil and water migration in the direction of the tem perature gradient. A space between the pipe surface and disturbed coating may offer the thermodynamic conditions for ice accumulation, close or attaching to the steel surface. This may be an analogous situation to the disbondment of coatings in the presence o f montmorillonite (shrinking and swelling) clays (Wilmott, pers. comm.). Particularly significant would be the presence of small soil masses trapped between the pipe and the coating, as may accidentally occur. If w ater can reach the entrapped soil through a punctured coating, further ice accumulation there is likely with further disruption o f the coating. Solutes might also be concentrated close to the pipe surface. PHYSICO-CHEMICAL EFFECTS OF FREEZING IN RELATION TO CORROSION AND STRESS CORROSION CRACKING The water in soils generally contains dissolved salts in low concentrations (certain soils, in salt marshes, solonetz soils and others, of course contain high concentrations and require special attention). As the soil w ater freezes the salts excluded from the ice become concentrated in the remaining water. The films are important in frost heave. They must also be continuous paths of relatively high electrical conductivity through the frozen soils. The effects will be greater the finer-grained the soil, because of the larger amounts of mineral surface and therefore of film water in such soils. Because o f the water that remains unfrozen, dissolved materials are mobile. The permeability of frozen soils to water, although sounding a contradiction in terms, is in fact regarded by many as the most important topic for research in to the geotechnical behaviour of freezing ground. In fine-grained soils movements of water, towards lower tem perature, are responsible for the continuing frost heave of the frozen material over time. As the w ater moves it carries ions with it - advective transport - in the directions of the temperature gradient. Cbuvilin et al., (1996) describe the movement of ions in the water films around soil particles. Nye (in Dash et al. 1998) discusses the unfrozen w ater al crystal interfaces in ice, which represents another possible path for ion movement, through ice occupying pores or ice layers in the soil. Chemical diffusion o f ions occurs in the unfrozen water in the frozen soil but this is generally in the opposite direction because solutes move from high to low concentrations (and the higher concentrations occur at the lower tem peratures). In fine-grained soils the advective transport towards and into the freezing layer exceeds chemical diffusion in the opposite direction, when frost heave is actively occurring (Chuvilin 1998). A complication is the adsorption of ions on to mineral particle surfaces. Ion exchange is significant, with certain ion species being held more strongly than others by the particle surfaces. Consequently the relative importance of movements o f different ions by the advection process or by diffusion becomes a complex question. There may be small, near-microscopic, pockets of w ater in the freezing soil having high concentrations of dissolved materials. Layers of ground of considerable thickness, known as cryopegs, can also remain unfrozen because o f their high concentration of dissolved materials. Cryopegs are particularly likely in coarse grained soils where quantities o f unfrozen w ater are small and the freezing process is different. Coarse-grained soils without any fine material do not accumulate excess ice on freezing and discrete layers of ice are not formed. In situations of constraint or loading on the frozen layer, when the pore w ater turns into ice the increase in volume is accommodated by w ater being pushed ahead of the freezing layer into the unfrozen material. Dissolved materials excluded from the ice are concentrated in this water. The result is a layer of unfrozen soil, at the interface between the frozen and unfrozen ground, at a tem perature just below 0 ° C . This is the origin of the cryopegs, which are widely reported and extensively discussed in the Russian literature. They occur below and within the permafrost. They are not commonly reported in Canada. It may be that the different climatic history of the permafrost in Russia explains the extensive, very large cryopegs there, but it seems probable that smaller cryopegs (maybe localised, metre-thick layers) will occur in the near-surface permafrost regions of North America, especially where the deposits are coarse-grained. These diverse aspects of the physical chemistry and thermodynamics of freezing soils are the subject of current research prompted by the global significance o f freezing processes (Dash et al. 1998) -climate change, agronomy in cold regions, and pollution in freezing ground (White and Williams 1998, Chuvilin 1998, and Virtual Conference, 1997). The fundamental importance in geotechnical engineering of the freezing of soils has been realised in recent decades. Nevertheless the potential importance o f freezing o f soil in stress-corrosion cracking appears to have been largely overlooked. Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab CONCLUSIONS The characteristics o f frozen ground differ radically from those of unfrozen ground in ways that are significant for SCC. In particular: 1. Continuing accumulations of ice within freezing ground give rise to pervasive and often large stresses and deformations in buried pipelines 2. The ice accumulations can be disruptive of protective coatings. 3. The freezing porous soil medium has a high concentration of ions in films on particle surfaces. 4. In spite of its apparently relatively inert and solid nature, frozen ground is perm eable to w ater and ions can be transported by advective transport. As a result of the thermodynamic conditions, extremely high hydraulic gradients develop in association with temperature gradients in freezing groundJons also move under concentration gradients and gradients of electrokinetic potential. 5. Metre-thick layers of soil remain unfrozen at temperatures below 0 0 C because o f high concentrations of solutes excluded from ice. 6. In cold regions, research into the pipeline environment with respect to stress corrosion cracking must consider the role of the special characteristics o f freezing ground. References Chuvilin, E .M , 1998, "Migration of Ions in Freezing and Frozen Soils," Proceedings, Conference on Contamination in Freezing Ground, Cambridge 1997. Polar Record (Cambridge Univ. Press) Special Issue (in press). Chuvilin, E M , Smirnova, O.G. and Kochetkova, N .Y , 1996, "Evaluating the Ionic Permeability of Frozen Soils and Ice," Sth Chinese Conference o f Glaciology and Geocryology, Lanzhou, China, 52-60 Dash, J .G , W ertlaufer J. and Unterscheiner N , 1998, "Ice in the Natural and Endangered Environment," Proceedings, NATO Advanced Study Institute. M aratea, Italy. Springer Verlag. Fremond M. and Mikkola, M , 1993, "Thermomechanical modelling o f freezing soil, in Gas Pipelines, Oil Pipelines and Civil Engineering in Arctic Climates," 1993, Proceedings of a Seminar, Caen and Paris. Geotechnical Science Laboratories, Carleton University, Ottawa. Geotechnical Science Laboratories, 1997. Reports and publications on the France-Canada Ground Freezing Project. (A listing of more than 50 items), available: Geotech. Sci. Labs., Carleton Univ., Ottawa, or on Web-site: httpVAvww.carleton.ca/GSL Kharionovsky, V , 1992, "Enhancing Arctic Gas-pipeline Reliability," Procceedings, International Conference on Pipeline Reliability. Calgary. CANM ET and Gulf Publishing Co. Vol.l, D-3-1 9. Ladanyi, B. and Andersland, OJ3., 1995. "An Introduction to Frozen Ground Engineering." Chapman and Hall, 352 pp. Riseborough, D.W. Williams, P J , Smith M .W , 1993. Pipelines Buried in Freezing Soil: A comparison of Two Ground-thermal Conditions." Proceedings of the 12th International Conference on Offshore Mechanics and Arctic Engineering, American Society of Mechnical Engineers, Bood No. G00681 - 1993, pp. 187-193. Smith M.W. and Patterson, D £ , 1989, "Detailed Observations on the Nature of Frost Heaving at a Field Scale. Can. Geot. Jour. Vol. 26, 2, 306-312. Virtual Conference 1997, "Contaminants in Freezing Ground" (in clu d es in te r n a tio n a l b ib lio g ra p h y ), o n W e b site: http://wwwireezinggroundcontam.org Washburn, A i^ , 1979, "Geocryology", Edward Arnold. 409pp. White T.L. and Coutard, J.-P , 1998, "Modification of Silt Microstructure by Hydrocarbon Contamination in Freezing Ground," Proceedings, Conference on Contamination in Freezing Ground. Polar Record. Cambridge, (in press). White, TD . and Williams, P J , 1994, "Cryogenic Alteration of Frost-susceptible Soils," Proceedings, 7th. International Sympposium on Freezing Ground, Nancy, France. 17-24. Williams, P J , 1989, T ipelines and Permafrost. Science in a Cold Climate," 2nd. E d , 3rd. printing. Carleton Univ. Press, Ottawa. 129 pp. Williams, P J . and Smith, M .W , 1991, T h e Frozen Earth. Fundamentals of Geocryology," Cambridge. 306 pp. Williams, P J , 1992, "Gas Pipelines and the Challenge of the Cold Regions: An Experimental Study," Proceedings, International Conference on Pipeline Reliability, Calgary, CANMET and Gulf Publishing Co. Vol. 1, Ü-2-1-12. Williams, P J , Riseborough D .W , and Smith, M .W , 1993, "The France-Canada Joint Study o f Deformation of an Experimental Pipeline by Differential Frost Heave," Int. Jour. Polar and Offshore Engineering. Vol. 3, 1, 56-60. Wilmot, M , 1997, Personal communication: Lecture at CANMET. Yershov, E D , 1998, "General Geocryology," A translation from the Russian. Cambridge University Press (in press). Downloaded From: https://proceedings.asmedigitalcollection.asme.org/pdfaccess.ashx?url=/data/conferences/asmep/89945/ on 06/18/2017 Terms of Use: http://www.asme.org/ab
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