Shale tectonics

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The phenomenon of rocks moving under their own means has always fascinated both scientists and the nonscientists. Salt is known to extrude and flow as a result of differences in density of the material and surrounding sediments. However, movement of fine-grained clastics as intrusive injectites or diapirs or as extrusive eruptive sand blows or mud volcanoes has captured the public's imagination and given scientists the impetus to reconsider the physics of how sediments behave in the subsurface.

Because of the burgeoning of shale gas and shale oil research, geoscientists are gaining a better understanding of the petrographic framework of shales, as well as their behavior under various pressure and temperature regimes and the manner in how fluids move thorough these strata (for a review, see Day-Stirrat et al.[1]). Advances in seismic imaging and processing technologies illuminate stratal geometries associated with shale tectonics that have led to a new understanding of the processes responsible for the geometries we observe in shale strata (see Day-Stirrat et al.[1]; Elsley and Tieman[2]). In addition, advances in modeling and understanding of how both muds and shales behave after burial have led to new geodynamic models for interpreting process from response reflected in stratal packages.[3] Field geoscientists have added to our understanding of the geochemistry and physical character of extrusive mud features and their relationship to the overall basin hydrocarbon system.[4][5][6][7] As with mobile salt, shale-cored structures are commonly closely associated with hydrocarbons in many basins around the world. In Henry et al.[8], information on the character of these strata can be found as well as documentation on drilling into mobile mud-cored anticlinal features (diapirs) in southern Trinidad.

Terminology

To develop a working classification of shale tectonics, recognition that two primary classes of features occur is critical: (1) those associated with extrusion of fluids and material that does not involve grain-to-grain contact,[4][5] and (2) those associated with larger scale deformation of apparent highly overpressured mud or shale substrates involving grain-to-grain plastic flow.[2][9] In addition, several varieties of highly fractured seep features exist.[7] These features allow fluid leakage from overpressured beds, but they do not always involve plastic or fluid-mud extrusion. Shales form a variety of nonextrusive structures, many of which resemble features generated through mobile salt movement, such as domes, welds, and walls. In contrast, muds form a variety of extrusive features, such as volcanoes, ponds, and flows and can erupt explosively.

Several terms are used to describe the processes and features of shale mobility. These include shale tectonics, mud diapirism, shale diapirism and diapirs, mobile shales, mud volcanoes, mud diatremes, mud flows, and finally, from the Greek, argillokinesis and pellitokinesis. Although many scientists continue to argue against the existence of mobile shale, the term is well entrenched in the lexicon and unlikely to go away. A GeoRef search on the topic of mobile shale resulted in 34 instances of the combined term present in the peer-reviewed literature. Mobile shale and mud are the primary subject of a 2003 publication from the Geological Society of London, Subsurface Sediment Mobilization.[10] This single publication accounts for 36 additional articles on the subject, quadrupling the previous literature offering.

Argillokinesis is a broadly applied, all-encompassing term used to describe the dynamics of uncompacted flexible clays. With broad consideration of previous literature, as well as numerous conversations with the scientific community of subsurface researchers, we propose herein to use the term shale tectonics to define the structuring within a basin associated with shale or mudstone plasticity or mobility, either as the cause of such mobility or as a result of such mobility. Mobile shales are defined as any manifestation of clay constituents (indurated or not) that show evidence of microscopic-scale fluid or plastic movement. We acknowledge that such mobility is currently poorly understood and may be some manifestation of microscopic shearing or as a reconstitution of partly indurated muds through diagenetic alteration.

Identification of subsurface mobile shale

Setting is a very important factor in the possible occurrence of mobile shales. Because shale mobility is caused by an imbalance of hydrostatic and lithostatic pressures, anything that varies the balance of forces within or around a shale mass, such as compressive tectonics, or rapid loading, will affect this balance and may initiate movement. Undeniably, the most influential variable in shale tectonics is fluid pressure. Two conditions commonly exist in regions of tectonically active muds or shales: (1) the presence of undercompacted mud at depth within the basin (this mud is presumed overpressured and held at depth by an overlying low permeability material) and (2) a triggering of overburden breach by some process that passes a critical threshold, causing sudden or gradual release of fluids, either with or without sediments. Triggers might be the gradual buildup of pressure beyond confining stresses of the overburden, sudden mass failure downslope of the overburden, regional compression, or seismicity.

Graue[11] published a set of criteria that, when met, are conducive to shale tectonics and mud extrusion. These criteria are as follows.

  • Rocks that have low mechanical strength, that are commonly undercompacted, and that have a low degree of consolidation.
  • Compressive tectonic stress to provide ductile deformation and increased pore pressures.
  • Structural culminations that focus decompacted water and hydrocarbons.
  • Carrier beds for migrating fluids and gases.

In AAPG Memoir 8, Diapirs and Diapirism, Musgrave and Hicks[12] provided a set of characteristics for what appear to be displaced shale masses in the Gulf of Mexico: (1) low-velocity sound transmission, in the range of 6500–8500 ft/s (1981.2–2590.8 m/s) with very little increase in velocity with depth; (2) low density, estimated to be in the range of 2.1–2.3 g/cm3; (3) low resistivity, approximately 0.5 ohm m; and (4) high fluid pressure, about 90% of the overburden pressure. Other authors (Henry et al.[8]) have documented sonic velocities in near surface (~0–3500 ft [~0–1070 m] below surface) mobile muds of onshore Trinidad to be lower than that of water! Authors from a range of disciplines have attributed these behaviors to high fluid pressure within the shales. At times, these densities are reduced to the point that the shales will rise as a mass in a diapiric fashion that is similar to that of salt. However, such behavior is not widely documented.

Improved seismic technologies have allowed a step change forward in the interpretation of shale tectonics in the subsurface with many previously interpreted mobile masses now much better defined. In some instances, improved imaging techniques have shown features previously interpreted as shale diapirs to be tightly folded anticlinal cores (Elsley and Tieman[2]). However, other instances exist in which shale substrates do appear to show inflation and upward mobility (Wiener et al.[9]). Because criteria for interpreting mobile shales are not well documented in literature, many of the characteristics that were developed for interpreting mobile salts have been applied to shale basins, albeit with mixed success. In addition, in basins where both salt and shale occur, geoscientists commonly fail to differentiate mobile shales from mobile salts in seismic images. To rectify this deficiency, the following criteria for differentiating salt and shale are provided.

  • Shale welds are less prevalent in shale systems than salt welds are in salt systems.
  • Shales have a much slower velocity than salt. Salt will be underlain by seismic pull-up versus no pull-up beneath shale features.
  • Salt requires a pipe several kilometers wide to facilitate vertical migration. In contrast, fluids migrating through shales will crack and hydraulically fracture a zone through which they will migrate upward.
  • Shale may flow laterally but will develop overhangs of less than 6 km (3.7 mi). In contrast, salt overhangs may be on the order of tens of kilometers.
  • Ductile behavior of shales is unlikely above 80°C (176°F), and brittle behavior is more likely. Therefore, this temperature will provide a plasticity basement within a basin to constrain interpretation of tectonically active shales.
  • Salt volumes tend to be underestimated in interpretations of seismic data. In contrast, shale mass volumes are commonly overestimated by geophysical interpreters (Van Rensbergen and Morley[13]) because of the manner in which geophysical data are processed. The apparent pull-up of beds around shale diapirs is caused by overmigration of the shale mass and treating its velocity as one would a salt.

Future directions

Areas remain in which additional advances can be made in the study of shale tectonics. As exploration and development of hydrocarbons move into deeper waters along continental margins, our ability to seismically image shale versus salt must improve if we are to deduce the role that these very different materials play in deep-water fold-belt evolution. Improved understanding of how muds behave at grain-to-grain scale when buried will inform modelers and improve our understanding of diagenetic processes in shales.

At present, many intriguing questions remain regarding shale tectonics and mobile muds. How do we get fluid and plastic muds extruded at the sea floor that appear on seismic data to have originated well below the lithifaction depth of shales (see Day-Stirrat et al.[1] for a review)? What is the physical interaction between mud-volcano pipes and underlying hydrocarbon reservoirs? Some researchers have shown that no hydraulic links between these crosscutting strata exist (DeVille et al.[14]). Do shales truly inflate as salts do above a regional stratigraphic datum? Evidence in Nigeria seems to suggest that they do (see Wiener et al.[9]). Why have we not identified more basins in which such regional inflation of shale occurs? Is there truly such a thing as a shale diapir or is this term a misdirected application of terminology? And of course, there is always the terminology itself. Although a laborious task to standardize, because this is the language by which scientific communities communicate their ideas, some attention must be paid to its clarification.

See also

References

  1. 1.0 1.1 1.2 Day-Stirrat, R. J., A. McDonnell, and L. J. Wood, 2010, Diagenetic and seismic concerns associated with interpretation of deeply buried "mobile shales," in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 5–27.
  2. 2.0 2.1 2.2 Elsley, G. R., and H. Tieman, 2010, A comparison of prestack depth and prestack time imaging of the Paktoa complex, Canadian Beaufort MacKenzie Basin, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 79–90.
  3. Albertz, M., C. Beaumont, and S. J. Ings, 2010, Geodynamic modeling of sedimentation-induced overpressure, gravitational spreading, and deformation of passive margin mobile shale basins, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 29–62.
  4. 4.0 4.1 Battani, A., A. Prinzhofer, E. Deville, and C. J. Ballentine, 2010, Trinidad mud volcanoes: The origin of the gas, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 223–236.
  5. 5.0 5.1 Delisle, G., M. Teschner, E. Faber, B. Panahi, I. Guliev, and C. Aliev, 2010, First approach in quantifying fluctuating gas emissions of methane and radon from mud volcanoes in Azerbaijan, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 209–222.
  6. McNeil, D. H., J. R. Dietrich, D. R. Issler, S. E. Grasby, J. Dixon, and L. D. Stasiuk, 2010, A new method for recognizing subsurface hydrocarbon seepage and migration using altered foraminifera from a gas chimney in the Beaufort-Mackenzie basin, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, 195–208.
  7. 7.0 7.1 Warren, J. K., A. Cheung, and I. Cartwright, 2010, Organic geochemical, isotopic, and seismic indicators of fluid flow in pressurized growth anticlines and mud volcanoes in modern deep-water slope and rise sediments of offshore Brunei Darussalam: Implications for hydrocarbon exploration in other mud- and salt-diapir provinces, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 161–194.
  8. 8.0 8.1 Henry, M., M. Pentilla, and D. Hoyer, 2010, Observations from exploration drilling in an active mud volcano in the southern basin of Trinidad, West Indies, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 63–78.
  9. 9.0 9.1 9.2 Wiener, R. W., M. G. Mann, M. T. Angelich, and J. B. Molyneux, 2010, Mobile shale in the Niger Delta: Characteristics, structure, and evolution, in L. Wood, ed., Shale tectonics: AAPG Memoir 93, p. 145–160.
  10. Van Rensbergen, O., R. R. Hillis, A. J. Maltman, and C. K. Morley, 2003, Subsurface sediment mobilization: Introduction, in P. Van Rensbergen, R. R. Hillis, A. J. Maltman, and C. K. Morley, eds., Subsurface sediment mobilization: Geological Society (London) Special Publication 216, p. 1–8.
  11. Graue, K., 2000, Mud volcanoes in deepwater Nigeria: Marine and Petroleum Geology, v. 17, p. 959–974.
  12. Musgrave, A. W., and W. G. Hicks, 1968, Outlining shale masses by geophysical methods, in E. Braunstein and G. D. O'Brien, eds., Diapirism and diapirs: AAPG Memoir 8, p. 122–136.
  13. Van Rensbergen, P., and C. K. Morley, 2000, 3D seismic study of a shale expulsion syncline at the base of the Champion Delta, offshore Brunei and its implications for the early structural evolution of large delta systems: Marine and Petroleum Geology, v. 17, p. 861–872.
  14. Deville, E., S.-H. Guerlais, Y. Callec, R. Griboulard, P. Huyghe, S. Lallemant, A. Mascle, M. Noble, and J. Schmitz, 2006, Liquefied vs. stratified sediment mobilization processes: Insight from the south of the Barbados accretionary prism: Tectonophysics, v. 428, p. 33–47, doi:10.1016/j.tecto.2006.08.011.

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