Transform fault
A transform fault or transform boundary, is a
Most such faults are found in oceanic crust, where they accommodate the lateral offset between segments of divergent boundaries, forming a zigzag pattern. This is a result of oblique seafloor spreading where the direction of motion is not perpendicular to the trend of the overall divergent boundary. A smaller number of such faults are found on land, although these are generally better-known, such as the San Andreas Fault and North Anatolian Fault.
Nomenclature
Transform boundaries are also known as conservative plate boundaries because they involve no addition or loss of lithosphere at the Earth's surface.[3]
Background
Geophysicist and geologist
Difference between transform and transcurrent faults
Transform faults are closely related to transcurrent faults and are commonly confused. Both types of fault are strike-slip or side-to-side in movement; nevertheless, transform faults always end at a junction with another plate boundary, while transcurrent faults may die out without a junction with another fault. Finally, transform faults form a tectonic plate boundary, while transcurrent faults do not.
Mechanics
Faults in general are focused areas of deformation or
Transform faults and divergent boundaries
Transform faults are commonly found linking segments of divergent boundaries (
Transform faults move differently from a strike-slip fault at the mid-oceanic ridge. Instead of the ridges moving away from each other, as they do in other strike-slip faults, transform-fault ridges remain in the same, fixed locations, and the new ocean seafloor created at the ridges is pushed away from the ridge. Evidence of this motion can be found in paleomagnetic striping on the seafloor.
A paper written by geophysicist Taras Gerya theorizes that the creation of the transform faults between the ridges of the mid-oceanic ridge is attributed to rotated and stretched sections of the mid-oceanic ridge.[7] This occurs over a long period of time with the spreading center or ridge slowly deforming from a straight line to a curved line. Finally, fracturing along these planes forms transform faults. As this takes place, the fault changes from a normal fault with extensional stress to a strike-slip fault with lateral stress.[8] In the study done by Bonatti and Crane,[who?] peridotite and gabbro rocks were discovered in the edges of the transform ridges. These rocks are created deep inside the Earth's mantle and then rapidly exhumed to the surface.[8] This evidence helps to prove that new seafloor is being created at the mid-oceanic ridges and further supports the theory of plate tectonics.
Active transform faults are between two tectonic structures or faults. Fracture zones represent the previously active transform-fault lines, which have since passed the active transform zone and are being pushed toward the continents. These elevated ridges on the ocean floor can be traced for hundreds of miles and in some cases even from one continent across an ocean to the other continent.
Types
In his work on transform-fault systems, geologist Tuzo Wilson said that transform faults must be connected to other faults or tectonic-plate boundaries on both ends; because of that requirement, transform faults can grow in length, keep a constant length, or decrease in length.[5] These length changes are dependent on which type of fault or tectonic structure connect with the transform fault. Wilson described six types of transform faults:
Growing length: In situations where a transform fault links a spreading center and the upper block of a subduction zone or where two upper blocks of subduction zones are linked, the transform fault itself will grow in length.[5]
Constant length: In other cases, transform faults will remain at a constant length. This steadiness can be attributed to many different causes. In the case of ridge-to-ridge transforms, the constancy is caused by the continuous growth by both ridges outward, canceling any change in length. The opposite occurs when a ridge linked to a subducting plate, where all the lithosphere (new seafloor) being created by the ridge is subducted, or swallowed up, by the subduction zone.[5] Finally, when two upper subduction plates are linked there is no change in length. This is due to the plates moving parallel with each other and no new lithosphere is being created to change that length.
Decreasing length faults: In rare cases, transform faults can shrink in length. These occur when two descending subduction plates are linked by a transform fault. In time as the plates are subducted, the transform fault will decrease in length until the transform fault disappears completely, leaving only two subduction zones facing in opposite directions.[5]
Examples
The most prominent examples of the mid-oceanic ridge transform zones are in the Atlantic Ocean between South America and Africa. Known as the St. Paul, Romanche, Chain, and Ascension fracture zones, these areas have deep, easily identifiable transform faults and ridges. Other locations include: the East Pacific Ridge located in the South Eastern Pacific Ocean, which meets up with San Andreas Fault to the North.
Transform faults are not limited to oceanic crust and spreading centers; many of them are on
In
Other examples include:
- Middle East's Dead Sea Transform fault
- Pakistan's Chaman Fault
- Turkey's North Anatolian Fault
- North America's Queen Charlotte Fault
- Myanmar's Sagaing Fault
See also
- Fracture zone – Linear feature on the ocean floor
- Leaky transform fault – Transform fault producing new crust
- List of tectonic plate interactions – Movements of Earth's lithosphere
- Plate tectonics – Movement of Earth's lithosphere
- Strike-slip tectonics – Deformation dominated by horizontal movement in Earth's lithosphere
- Structural geology – Science of the description and interpretation of deformation in the Earth's crust
References
- ISBN 978-1-4786-2660-2.
- ^ Kearey, K. A. (2007). Global Tectonics. Hoboken, NJ, USA: John Wiley & Sons. pp. 84–90.
- ^ "Plate Tectonics". British Geological Survey. 2020. Retrieved 16 February 2020.
- ^ Reid, H.F., (1910). The Mechanics of the Earthquake. in The California Earthquake of April 18, 1906, Report of the State Earthquake Investigation Commission, Carnegie Institution of Washington, Washington D.C.
- ^ S2CID 4294401.
- ^ Sykes, L.R. (1967). Mechanism of earthquakes and nature of faulting on the mid-oceanic ridges, Journal of Geophysical Research, 72, 5–27.
- S2CID 10943308.
- ^ .
- ^ .
- International Tectonic Dictionary – AAPG Memoir 7, 1967
- The Encyclopedia of Structural Geology and Plate Tectonics – Ed. by Carl K. Seyfert, 1987