In structural geology, a fold is a stack of originally planar surfaces, such as sedimentary strata, that are bent or curved during permanent deformation. Folds in rocks vary in size from microscopic crinkles to mountain-sized folds. They occur as single isolated folds or in periodic sets (known as fold trains). Synsedimentary folds are those formed during sedimentary deposition.
Folds form under varied conditions of stress, pore pressure, and temperature gradient, as evidenced by their presence in soft sediments, the full spectrum of metamorphic rocks, and even as primary flow structures in some igneous rocks. A set of folds distributed on a regional scale constitutes a fold belt, a common feature of orogenic zones. Folds are commonly formed by shortening of existing layers, but may also be formed as a result of displacement on a non-planar fault (fault bend fold), at the tip of a propagating fault (fault propagation fold), by differential compaction or due to the effects of a high-level igneous intrusion e.g. above a laccolith.
The fold hinge is the line joining points of maximum curvature on a folded surface. This line may be either straight or curved. The term hinge line has also been used for this feature.
A fold surface seen perpendicular to its shortening direction can be divided into hinge and limb portions, the limbs are the flanks of the fold and the hinge zone is where the limbs converge. Within the hinge zone lies the hinge point, which is the point of minimum radius of curvature (maximum curvature) of the fold. The crest of the fold represents the highest point of the fold surface whereas the trough is the lowest point. The inflection point of a fold is the point on a limb at which the concavity reverses; on regular folds, this is the midpoint of the limb.
The axial surface is defined as a plane connecting all the hinge lines of stacked folded surfaces. If the axial surface is planar then it is called an axial plane and can be described in terms of strike and dip.
Folds can have a fold axis. A fold axis, “is the closest approximation to a straight line that when moved parallel to itself, generates the form of the fold.” (Davis and Reynolds, 1996 after Donath and Parker, 1964; Ramsay 1967). A fold that can be generated by a fold axis is called a cylindrical fold. This term has been broadened to include near-cylindrical folds. Often, the fold axis is the same as the hinge line.
Minor folds are quite frequently seen in outcrop; major folds seldom are except in the more arid countries. Minor folds can, however, often provide the key to the major folds they are related to. They reflect the same shape and style, the direction in which the closures of the major folds lie, and their cleavage indicates the attitude of the axial planes of the major folds and their direction of overturning 
Fold tightness is defined by the size of the angle between the fold's limbs (as measured tangential to the folded surface at the inflection line of each limb), called the interlimb angle. Gentle folds have an interlimb angle of between 180° and 120°, open folds range from 120° to 70°, close folds from 70° to 30°, and tight folds from 30° to 0°. Isoclines, or isoclinal folds, have an interlimb angle of between 10° and zero, with essentially parallel limbs.
Not all folds are equal on both sides of the axis of the fold. Those with limbs of relatively equal length are termed symmetrical, and those with highly unequal limbs are asymmetrical. Asymmetrical folds generally have an axis at an angle to the original unfolded surface they formed on.
Facing and vergenceEdit
Vergence is calculated in a direction perpendicular to the fold axis.
Deformation style classesEdit
Folds that maintain uniform layer thickness are classed as concentric folds. Those that do not are called similar folds. Similar folds tend to display thinning of the limbs and thickening of the hinge zone. Concentric folds are caused by warping from active buckling of the layers, whereas similar folds usually form by some form of shear flow where the layers are not mechanically active. Ramsay has proposed a classification scheme for folds that often is used to describe folds in profile based upon the curvature of the inner and outer lines of a fold and the behavior of dip isogons. that is, lines connecting points of equal dip on adjacent folded surfaces:
|1||Cinner > Couter||Dip isogons converge|
|1A||Orthogonal thickness at hinge narrower than at limbs|
|1C||Orthogonal thickness at limbs narrower than at hinge|
|2||Cinner = Couter||Dip isogons are parallel: similar folds|
|3||Cinner < Couter||Dip isogons diverge|
Types of foldEdit
- Anticline: linear, strata normally dip away from the axial center, oldest strata in center irrespective of orientation.
- Syncline: linear, strata normally dip toward the axial center, youngest strata in center irrespective of orientation.
- Antiform: linear, strata dip away from the axial center, age unknown, or inverted.
- Synform: linear, strata dip toward the axial center, age unknown, or inverted.
- Dome: nonlinear, strata dip away from center in all directions, oldest strata in center.
- Basin: nonlinear, strata dip toward center in all directions, youngest strata in center.
- Monocline: linear, strata dip in one direction between horizontal layers on each side.
- Chevron: angular fold with straight limbs and small hinges
- Recumbent: linear, fold axial plane oriented at a low angle resulting in overturned strata in one limb of the fold.
- Slump: typically monoclinal, the result of differential compaction or dissolution during sedimentation and lithification.
- Ptygmatic: Folds are chaotic, random and disconnected. Typical of sedimentary slump folding, migmatites and decollement detachment zones.
- Parasitic: short-wavelength folds formed within a larger wavelength fold structure - normally associated with differences in bed thickness
- Disharmonic: Folds in adjacent layers with different wavelengths and shapes
(A homocline involves strata dipping in the same direction, though not necessarily any folding.)
Causes of foldingEdit
When a sequence of layered rocks is shortened parallel to its layering, this deformation may be accommodated in a number of ways, homogeneous shortening, reverse faulting or folding. The response depends on the thickness of the mechanical layering and the contrast in properties between the layers. If the layering does begin to fold, the fold style is also dependent on these properties. Isolated thick competent layers in a less competent matrix control the folding and typically generate classic rounded buckle folds accommodated by deformation in the matrix. In the case of regular alternations of layers of contrasting properties, such as sandstone-shale sequences, kink-bands, box-folds and chevron folds are normally produced.
Many folds are directly related to faults, associated with their propagation, displacement and the accommodation of strains between neighboring faults.
Fault bend foldingEdit
Fault-bend folds are caused by displacement along a non-planar fault. In non-vertical faults, the hanging-wall deforms to accommodate the mismatch across the fault as displacement progresses. Fault bend folds occur in both extensional and thrust faulting. In extension, listric faults form rollover anticlines in their hanging walls. In thrusting, ramp anticlines form whenever a thrust fault cuts up section from one detachment level to another. Displacement over this higher-angle ramp generates the folding.
Fault propagation foldingEdit
Fault propagation folds or tip-line folds are caused when displacement occurs on an existing fault without further propagation. In both reverse and normal faults this leads to folding of the overlying sequence, often in the form of a monocline.
When a thrust fault continues to displace above a planar detachment without further fault propagation, detachment folds may form, typically of box-fold style. These generally occur above a good detachment such as in the Jura Mountains, where the detachment occurs on middle Triassic evaporites.
Folding in shear zonesEdit
Shear zones that approximate to simple shear typically contain minor asymmetric folds, with the direction of overturning consistent with the overall shear sense. Some of these folds have highly curved hinge-lines and are referred to as sheath folds. Folds in shear zones can be inherited, formed due to the orientation of pre-shearing layering or formed due to instability within the shear flow.
Folding in sedimentsEdit
Recently-deposited sediments are normally mechanically weak and prone to remobilization before they become lithified, leading to folding. To distinguish them from folds of tectonic origin, such structures are called synsedimentary (formed during sedimentation).
Slump folding: When slumps form in poorly consolidated sediments, they commonly undergo folding, particularly at their leading edges, during their emplacement. The asymmetry of the slump folds can be used to determine paleoslope directions in sequences of sedimentary rocks.
Dewatering: Rapid dewatering of sandy sediments, possibly triggered by seismic activity, can cause convolute bedding.
The emplacement of igneous intrusions tends to deform the surrounding country rock. In the case of high-level intrusions, near the Earth's surface, this deformation is concentrated above the intrusion and often takes the form of folding, as with the upper surface of a laccolith.
The compliance of rock layers is referred to as competence: a competent layer or bed of rock can withstand an applied load without collapsing and is relatively strong, while an incompetent layer is relatively weak. When rock behaves as a fluid, as in the case of very weak rock such as rock salt, or any rock that is buried deeply enough, it typically shows flow folding (also called passive folding, because little resistance is offered): the strata appear shifted undistorted, assuming any shape impressed upon them by surrounding more rigid rocks. The strata simply serve as markers of the folding. Such folding is also a feature of many igneous intrusions and glacier ice.
Folding of rocks must balance the deformation of layers with the conservation of volume in a rock mass. This occurs by several mechanisms.
Flexural slip allows folding by creating layer-parallel slip between the layers of the folded strata, which, altogether, result in deformation. A good analogy is bending a phone book, where volume preservation is accommodated by slip between the pages of the book.
The fold formed by the compression of competent rock beds is called "flexure fold".
Typically, folding is thought to occur by simple buckling of a planar surface and its confining volume. The volume change is accommodated by layer parallel shortening the volume, which grows in thickness. Folding under this mechanism is typical of a similar fold style, as thinned limbs are shortened horizontally and thickened hinges do so vertically.
If the folding deformation cannot be accommodated by a flexural slip or volume-change shortening (buckling), the rocks are generally removed from the path of the stress. This is achieved by pressure dissolution, a form of metamorphic process, in which rocks shorten by dissolving constituents in areas of high strain and redepositing them in areas of lower strain. Folds created in this way include examples in migmatites and areas with a strong axial planar cleavage.
Mechanics of foldingEdit
The rheology of the layers being folded determines characteristic features of the folds that are measured in the field. Rocks that deform more easily form many short-wavelength, high-amplitude folds. Rocks that do not deform as easily form long-wavelength, low-amplitude folds.
Layers of rock that fold into a hinge need to accommodate large deformations in the hinge zone. This results in voids between the layers. These voids, and especially the fact that the water pressure is lower in the voids than outside of them, act as triggers for the deposition of minerals. Over millions of years, this process is capable of gathering large quantities of trace minerals from large expanses of rock and depositing them at very concentrated sites. This may be a mechanism that is responsible for the veins. To summarize, when searching for veins of valuable minerals, it might be wise to look for highly folded rock, and this is the reason why the mining industry is very interested in the theory of geological folding.
Anticlinal traps are formed by folding of rock. For example, if a porous sandstone unit covered with low permeability shale is folded into an anticline, it may contain hydrocarbons trapped in the crest of the fold. Most anticlinal traps are created as a result of sideways pressure, folding the layers of rock, but can also occur from sediments being compacted.
- M.J. Fleury, The description of folds, Proceedings of the Geologists' Association, Volume 75, Issue 4, 1964, Pages 461-492, ISSN 0016-7878, https://doi.org/10.1016/S0016-7878(64)80023-7.
- Sudipta Sengupta; Subir Kumar Ghosh; Kshitindramohan Naha (1997). Evolution of geological structures in micro- to macro-scales. Springer. p. 222. ISBN 0-412-75030-9.
- RG Park (2004). "Fold axis and axial plane". Foundations of structural geology (3rd ed.). Routledge. p. 26. ISBN 0-7487-5802-X.
- Barnes, J. W., & Lisle, R. J. (2013). "5 Field Measurements and Techniques". Basic geological mapping: 4th Edition. John Wiley & Sons. p. 79. ISBN 978-1-118-68542-6.CS1 maint: multiple names: authors list (link)
- Lisle, Richard J (2004). "Folding". Geological Structures and Maps: 3rd Edition. Elsevier. pp. 33. ISBN 0-7506-5780-4.
- See, for example, R. G. Park (2004). "Figure 3.12: Fold classification based upon dip diagrams". Foundations of structural geology (3rd ed.). Routledge. p. 31 ff. ISBN 0-7487-5802-X.
- Neville J. Price; John W. Cosgrove (1990). "Figure 10.14: Classification of fold profiles using dip isogon patterns". Analysis of geological structures. Cambridge University Press. p. 246. ISBN 0-521-31958-7.
- Park, R.G. (2004). Foundation of Structural Geology (3 ed.). Routledge. p. 33. ISBN 978-0-7487-5802-9.
- Ramsay, J.G.; Huber M.I. (1987). The techniques of modern structural geology. 2 (3 ed.). Academic Press. p. 392. ISBN 978-0-12-576922-8. Retrieved 2009-11-01.
- Withjack, M.O.; Schlische (2006). "Geometric and experimental models of extensional fault-bend folds". In Buiter S.J.H. & Schreurs G. (ed.). Analogue and numerical modelling of crustal-scale processes. Special Publications 253. R.W. Geological Society, London. pp. 285–305. ISBN 978-1-86239-191-8. Retrieved 2009-10-31.
- Rowland, S.M.; Duebendorfer E.M.; Schieflebein I.M. (2007). Structural analysis and synthesis: a laboratory course in structural geology (3 ed.). Wiley-Blackwell. p. 301. ISBN 978-1-4051-1652-7. Retrieved 2009-11-01.
- Jackson, C.A.L.; Gawthorpe R.L.; Sharp I.R. (2006). "Style and sequence of deformation during extensional fault-propagation" (PDF). Journal of Structural Geology. 28 (3): 519–535. Bibcode:2006JSG....28..519J. doi:10.1016/j.jsg.2005.11.009. Retrieved 2009-11-01.
- Reicherter, K., Froitzheim, N., Jarosinki, M., Badura, J., Franzke, H.-J., Hansen, M., Hübscher, C., Müller, R., Poprawa, P., Reinecker, J., Stackebrandt, W, Voigt,T., von Eynatten, H. & Zuchiewicz, W. (2008). "19. Alpine Tectonics north of the Alps". In McCann, T. (ed.). The Geology of Central Europe. Geological Society, London. pp. 1233–1285. ISBN 978-1-86239-264-9. Retrieved 2009-10-31.CS1 maint: uses authors parameter (link)
- Carreras, J.; Druguet E.; Griera A. (2005). "Shear zone-related folds". Journal of Structural Geology. 27 (7): 1229–1251. Bibcode:2005JSG....27.1229C. doi:10.1016/j.jsg.2004.08.004. Retrieved 2009-10-31.
- Bradley, D.; Hanson L. (1998). "Paleoslope Analysis of Slump Folds in the Devonian Flysch of Maine" (PDF). Journal of Geology. 106 (3): 305–318. Bibcode:1998JG....106..305B. doi:10.1086/516024. Retrieved 2009-10-31.
- Nichols, G. (1999). "17. Sediments into rocks: post-depositional processes". Sedimentology and stratigraphy. Wiley-Blackwell. p. 355. ISBN 978-0-632-03578-6. Retrieved 2009-10-31.
- Hyne, N.J. (2001). Nontechnical guide to petroleum geology, exploration, drilling, and production. PennWell Books. p. 598. ISBN 978-0-87814-823-3. Retrieved 2009-11-01.
- Orchuela, I.; Lara M.E.; Suarez M. (2003). "Productive Large Scale Folding Associated with Igneous Intrusions: El Trapial Field, Neuquen Basin, Argentina" (PDF). AAPG Abstracts. Retrieved 2009-10-31.
- Arvid M. Johnson; Raymond C. Fletcher (1994). "Figure 2.6". Folding of viscous layers: mechanical analysis and interpretation of structures in deformed rock. Columbia University Press. p. 87. ISBN 0-231-08484-6.
- Park, R.G. (1997). Foundations of structural geology (3rd ed.). Routledge. p. 109. ISBN 0-7487-5802-X.; RJ Twiss; EM Moores (1992). "Figure 12.8: Passive shear folding". Structural geology (2nd ed.). Macmillan. pp. 241–242. ISBN 0-7167-2252-6.
- Hudleston, P.J. (1977). "Similar folds, recumbent folds and gravity tectonics in ice and rocks". Journal of Geology. 85 (1): 113–122. Bibcode:1977JG.....85..113H. doi:10.1086/628272. JSTOR 30068680.
- Barnes, J. W.; Lisle, R. J. (2013). "Field Measurements and Techniques". Basic Geological Mapping (4th ed.). John Wiley & Sons. p. 79. ISBN 978-1-118-68542-6.
|The Wikibook Historical Geology has a page on the topic of: Folds|
|Wikimedia Commons has media related to folds.|
- Davis, George H.; Reynolds, Stephen J. (1996). "Folds". Structural Geology of Rocks and Regions. New York: John Wiley & Sons. pp. 372–424. ISBN 0-471-52621-5.
- Donath, F.A.; Parker, R.B. (1964). "Folds and Folding". Geological Society of America Bulletin. 75: 45–62. doi:10.1130/0016-7606(1964)75[45:FAF]2.0.CO;2. ISSN 0016-7606.
- Energy Education, page=
- Lisle, Richard J. (2004). "Folding". Geological Structures and Maps (3rd ed.). Elsevier. pp. 33. ISBN 0-7506-5780-4 – via Archive Foundation.
- McKnight, Tom L.; Hess, Darrel (2000). "The Internal Processes: Folding". Physical Geography: A Landscape Appreciation. Upper Saddle River, NJ: Prentice Hall. pp. 409–14. ISBN 0-13-020263-0 – via Archive Foundation.
- Mark Peletier, p. 
- Pollard, David D.; Fletcher, Raymond C. (2005). Fundamentals of Structural Geology. Cambridge University Press. ISBN 0-521-83927-0 – via Archive Foundation.
- Ramsay, J.G., 1967, Folding and fracturing of rocks: McGraw-Hill Book Company, New York, 560pp.