# Subduction {#subduction .reader-title}
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'Subduction' is a geological process in which the oceanic lithosphere
and some continental lithosphere is recycled into the Earth\'s mantle at
the convergent boundaries between tectonic plates. Where one tectonic
plate converges with a second plate, the heavier plate dives beneath the
other and sinks into the mantle. A region where this process occurs is
known as a 'subduction zone', and its surface expression is known as
an 'arc-trench complex'. The process of subduction has created most of
the Earth\'s continental crust.^\[1\]^ Rates of subduction are typically
measured in centimeters per year, with rates of convergence as high as
11 cm/year.^\[2\]^
Subduction is possible because the cold and rigid oceanic lithosphere is
slightly denser than the underlying asthenosphere, the hot, ductile
layer in the upper mantle. Once initiated, stable subduction is driven
mostly by the negative buoyancy of the dense subducting lithosphere. The
down-going slab sinks into the mantle largely under its own
weight.^\[3\]^
Earthquakes are common along subduction zones, and fluids released by
the subducting plate trigger volcanism in the overriding plate. If the
subducting plate sinks at a shallow angle, the overriding plate develops
a belt of deformation characterized by crustal thickening, mountain
building, and metamorphism. Subduction at a steeper angle is
characterized by the formation of back-arc basins.^\[4\]^
<div>
# Subduction and plate tectonics {#Subduction_and_plate_tectonics}
</div>
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![The simplified model of mantle convection:^\[5\]^ Oceanic plates are
subducted creating oceanic
trenches.](file:///home/geoff/Documents/wikipedia%20extra/Subduction%20-%20Wikipedia_files/Oceanic_spreading.svg.png){.moz-reader-block-img
file-width="600" file-height="450" height="255" width="340"}
According to the theory of plate tectonics, the Earth\'s lithosphere,
its rigid outer shell, is broken into sixteen larger tectonic plates and
several smaller plates. These plates are in slow motion, due mostly to
the pull force of subducting lithosphere. Sinking lithosphere at
subduction zones is a part of convection cells in the underlying ductile
mantle. This process of convection allows heat generated by radioactive
decay to escape from the Earth\'s interior.^\[6\]^
The lithosphere consists of the outermost light crust plus the uppermost
rigid portion of the mantle. Oceanic lithosphere ranges in thickness
from just a few km for young lithosphere created at mid-ocean ridges to
around 100 km (62 mi) for the oldest oceanic lithosphere.^\[7\]^
Continental lithosphere is up to 200 km (120 mi) thick.^\[8\]^ The
lithosphere is relatively cold and rigid compared with the underlying
asthenosphere, and so tectonic plates move as solid bodies atop the
asthenosphere. Individual plates often include both regions of the
oceanic lithosphere and continental lithosphere.
Subduction zones are where cold oceanic lithosphere sinks back into the
mantle and is recycled.^\[4\]\[9\]^ They are found at convergent plate
boundaries, where the heavier oceanic lithosphere of one plate is
overridden by the leading edge of another, less-dense plate.^\[7\]^ The
overridden plate (the *slab*) sinks at an angle most commonly between 25
and 75 degrees to the Earth\'s surface.^\[10\]^ This sinking is driven
by the temperature difference between the slab and the surrounding
asthenosphere, as the colder oceanic lithosphere is, on average, more
dense.^\[7\]^ Sediments and some trapped water are carried downwards by
the slab and recycled into the deep mantle.^\[11\]^
So far, Earth is the only planet where subduction is known to occur, and
subduction zones are its most important tectonic feature. Subduction is
the driving force behind plate tectonics, and without it, plate
tectonics could not occur.^\[12\]^ Oceanic subduction zones are located
along 55,000 km (34,000 mi) of convergent plate margins,^\[13\]^ almost
equal to the cumulative plate formation rate of 60,000 km (37,000 mi) of
mid-ocean ridges.^\[14\]^
Sea water seeps into oceanic lithosphere through fractures and pores,
and reacts with minerals in the crust and mantle to form hydrous
minerals (such as serpentine) that store water in their crystal
structures.^\[15\]^ Water is transported into the deep mantle *via*
hydrous minerals in subducting slabs.^\[16\]^ During subduction, a
series of minerals in these slabs such as serpentine can be stable at
different pressures within the slab geotherms, and may transport a
significant amount of water into the Earth\'s interior.^\[17\]^ As
plates sink and heat up, released fluids can trigger seismicity and
induce melting within the subducted plate and in the overlying mantle
wedge. This type of melting selectively concentrates volatiles and
transports them into the overlying plate. If an eruption occurs, the
cycle then returns the volatiles into the oceans and atmosphere.^\[18\]^
<div>
# Structure of subduction zones {#Structure_of_subduction_zones}
</div>
The surface expressions of subduction zones are arc-trench complexes. On
the ocean side of the complex, where the subducting plate first
approaches the subduction zone, there is often an *outer trench high* or
*outer trench swell*. Here the plate shallows slightly before plunging
downwards, as a consequence of the rigidity of the plate.^\[19\]^ The
point where the slab begins to plunge downwards is marked by an *oceanic
trench*. Oceanic trenches are the deepest parts of the ocean floor.
Beyond the trench is the *forearc* portion of the overriding plate.
Depending on sedimentation rates, the forearc may include an
accretionary wedge of sediments scraped off the subducting slab and
accreted to the overriding plate. However, not all arc-trench complexes
have an accretionary wedge. Accretionary arcs have a well-developed
forearc basin behind the accretionary wedge, while the forearc basin is
poorly developed in non-accretionary arcs.^\[20\]^
Beyond the forearc basin, volcanoes are found in long chains called
*volcanic arcs*. The subducting basalt and sediment are normally rich in
hydrous minerals and clays. Additionally, large quantities of water are
introduced into cracks and fractures created as the subducting slab
bends downward.^\[21\]^ During the transition from basalt to eclogite,
these hydrous materials break down, producing copious quantities of
water, which at such great pressure and temperature exists as a
supercritical fluid.^\[22\]^ The supercritical water, which is hot and
more buoyant than the surrounding rock, rises into the overlying mantle,
where it lowers the melting temperature of the mantle rock, generating
magma via flux melting.^\[23\]^ The magmas, in turn, rise as diapirs
because they are less dense than the rocks of the mantle.^\[24\]^ The
mantle-derived magmas (which are initially basaltic in composition) can
ultimately reach the Earth\'s surface, resulting in volcanic eruptions.
The chemical composition of the erupting lava depends upon the degree to
which the mantle-derived basalt interacts with (melts) Earth\'s crust or
undergoes fractional crystallization. Arc volcanoes tend to produce
dangerous eruptions because they are rich in water (from the slab and
sediments) and tend to be extremely explosive.^\[25\]^ Krakatoa, Nevado
del Ruiz, and Mount Vesuvius are all examples of arc volcanoes. Arcs are
also associated with most ore deposits.^\[24\]^
Beyond the volcanic arc is a back-arc region whose character depends
strongly on the angle of subduction of the subducting slab. Where this
angle is shallow, the subducting slab drags the overlying continental
crust partially with it, which produces a zone of shortening and crustal
thickening in which there may be extensive folding and thrust faulting.
If the angle of subduction steepens or rolls back, the upper plate
lithosphere will be put in tension instead, often producing a back-arc
basin.^\[26\]^
The arc-trench complex is the surface expression of a much deeper
structure. Though not directly accessible, the deeper portions can be
studied using geophysics and geochemistry. Subduction zones are defined
by an inclined zone of earthquakes, the Wadati--Benioff zone, that dips
away from the trench and extends down below the volcanic arc to the
660-kilometer discontinuity. Subduction zone earthquakes occur at
greater depths (up to 600 km (370 mi)) than elsewhere on Earth
(typically less than 20 km (12 mi) depth); such deep earthquakes may be
driven by deep phase transformations, thermal runaway, or dehydration
embrittlement.^\[27\]\[28\]^ Seismic tomography shows that some slabs
can penetrate the lower mantle^\[29\]\[30\]^ and sink clear to the
core--mantle boundary.^\[31\]^ Here the residue of the slabs may
eventually heat enough to rise back to the surface as mantle
plumes.^\[32\]\[33\]^
Subduction typically occurs at a moderately steep angle by the time it
is beneath the volcanic arc. However, anomalous shallower angles of
subduction are known to exist as well as some that are extremely
steep.^\[34\]^
- Flat slab subduction (subduction angle less than 30°) occurs when the
slab subducts nearly horizontally. The relatively flat slab can extend
for hundreds of kilometers under the upper plate. This geometry is
commonly caused by the subduction of buoyant lithosphere due to
thickened crust or warmer lithosphere. Recent studies have also shown
a strong correlation that older and wider subduction zones are related
to flatter subduction dips. This provides an explanation as to why
flat subduction only presently occurs in the eastern pacific as only
these regions were old and wide enough to support flat slab subduction
and why the Laramide flat slab subduction and South China flat slab
subduction were possible.^\[35\]^ Hu ultimately proposes that a
combination of subduction age and slab characteristics provide the
strongest controls over subduction dips.^\[36\]^ Because subduction of
slabs to depth is necessary to drive subduction zone volcanism,
flat-slab subduction can be invoked to explain volcanic gaps.
Flat-slab subduction is ongoing beneath part of the Andes, causing
segmentation of the Andean Volcanic Belt into four zones. The flat-slab
subduction in northern Peru and the Norte Chico region of Chile is
believed to be the result of the subduction of two buoyant aseismic
ridges, the Nazca Ridge and the Juan Fernández Ridge, respectively.
Around Taitao Peninsula flat-slab subduction is attributed to the
subduction of the Chile Rise, a spreading ridge.^\[37\]\[38\]^
The Laramide Orogeny in the Rocky Mountains of the United States is
attributed to flat-slab subduction.^\[39\]^ During this orogeny, a broad
volcanic gap appeared at the southwestern margin of North America, and
deformation occurred much farther inland; it was during this time that
the basement- cored mountain ranges of Colorado, Utah, Wyoming, South
Dakota, and New Mexico came into being. The most massive subduction zone
earthquakes, so-called \"megaquakes\", have been found to occur in
flat-slab subduction zones.^\[40\]^
- Steep-angle subduction (subduction angle greater than 70°) occurs in
subduction zones where Earth\'s oceanic crust and lithosphere are cold
and thick and have, therefore, lost buoyancy. Recent studies have also
correlated steep angled subduction zones with younger and less
extensive subduction zones. This would explain why most modern
subduction zones are relatively steep. The steepest dipping subduction
zone lies in the Mariana Trench, which is also where the oceanic
lithosphere of Jurassic age is the oldest on Earth exempting
ophiolites. Steep-angle subduction is, in contrast to flat-slab
subduction, associated with back-arc extension^\[41\]^ of the upper
plate, creating volcanic arcs and pulling fragments of continental
crust away from continents to leave behind a marginal sea.
<div>
# Life cycle of subduction zones {#Life_cycle_of_subduction_zones}
</div>
<div>
# # Initiation of subduction {#Initiation_of_subduction}
</div>
Although stable subduction is fairly well understood, the process by
which subduction is initiated remains a matter of discussion and
continuing study. Subduction can begin spontaneously if the denser
oceanic lithosphere can founder and sink beneath the adjacent oceanic or
continental lithosphere through vertical forcing only; alternatively,
existing plate motions can induce new subduction zones by horizontally
forcing the oceanic lithosphere to rupture and sink into the
asthenosphere.^\[42\]\[43\]^ Both models can eventually yield
self-sustaining subduction zones, as the oceanic crust is metamorphosed
at great depth and becomes denser than the surrounding mantle rocks. The
compilation of subduction zone initiation events back to 100 Ma suggests
horizontally-forced subduction zone initiation for most modern
subduction zones,^\[43\]^ which is supported by results from numerical
models^\[44\]\[45\]^ and geologic studies.^\[46\]\[47\]^ Some analogue
modeling shows, however, the possibility of spontaneous subduction from
inherent density differences between two plates at specific locations
like passive margins and along transform faults.^\[48\]\[49\]^ There is
evidence this has taken place in the Izu-Bonin-Mariana subduction
system.^\[50\]\[51\]^ Earlier in Earth\'s history, subduction is likely
to have initiated without horizontal forcing due to the lack of relative
plate motion, though a proposal by A. Yin suggests that meteorite
impacts may have contributed to subduction initiation on early
Earth.^\[52\]^
Though the idea of subduction initiation at passive margins is popular,
there is no modern day example for this type of subduction
nucleation.^\[53\]^ This is likely due to the strength of the oceanic or
transitional crust at the continental passive margins, suggesting that
if the crust did not break in its first 20 million years of life, it is
unlikely to break in the future under normal sedimentation loads. Only
with additional weaking of the crust, through hotspot magmatism or
extensional rifting, would the crust be able to break from its continent
and begin subduction.
Subduction can continue as long as the oceanic lithosphere moves into
the subduction zone. However, the arrival of buoyant continental
lithosphere at a subduction zone can result in increased coupling at the
trench and cause plate boundary reorganization. The arrival of
continental crust results in *continental collision* or *terrane
accretion* that may disrupt subduction.^\[54\]^ Continental crust can
subduct to depths of 250 km (160 mi) where it can reach a point of no
return.^\[55\]\[33\]^ Sections of crustal or intraoceanic arc crust
greater than 15 km (9.3 mi) in thickness or oceanic plateau greater than
30 km (19 mi) in thickness can disrupt subduction. However, island arcs
subducted end-on may cause only local disruption, while an arc arriving
parallel to the zone can shut it down.^\[54\]^ This has happened with
the Ontong Java Plateau and the Vitiaz Trench.^\[56\]^
<div>
# Characteristics and effects {#Characteristics_and_effects}
</div>
Subduction zones host a unique variety of rock types created by the
high-pressure, low-temperature conditions a subducting slab encounters
during its descent.^\[57\]^ The metamorphic conditions the slab passes
through in this process create and destroy water bearing (hydrous)
mineral phases, releasing water into the mantle. This water lowers the
melting point of mantle rock, initiating melting.^\[58\]^ Understanding
the timing and conditions in which these dehydration reactions occur is
key to interpreting mantle melting, volcanic arc magmatism, and the
formation of continental crust.^\[59\]^
A metamorphic facies is characterized by a stable mineral assemblage
specific to a pressure-temperature range and specific starting material.
Subduction zone metamorphism is characterized by a low temperature,
high-ultrahigh pressure metamorphic path through the zeolite,
prehnite-pumpellyite, blueschist, and eclogite facies stability zones of
subducted oceanic crust.^\[60\]^ Zeolite and prehnite-pumpellyite facies
assemblages may or may not be present, thus the onset of metamorphism
may only be marked by blueschist facies conditions.^\[61\]^ Subducting
slabs are composed of basaltic crust topped with pelagic
sediments;^\[62\]^ however, the pelagic sediments may be accreted onto
the forearc-hanging wall and not subducted.^\[63\]^ Most metamorphic
phase transitions that occur within the subducting slab are prompted by
the dehydration of hydrous mineral phases. The breakdown of hydrous
mineral phases typically occurs at depths greater than 10 km
(6.2 mi).^\[64\]^ Each of these metamorphic facies is marked by the
presence of a specific stable mineral assemblage, recording the
metamorphic conditions undergone but the subducting slab. Transitions
between facies cause hydrous minerals to dehydrate at certain
pressure-temperature conditions and can therefore be tracked to melting
events in the mantle beneath a volcanic arc.
Two kinds of arcs are generally observed on Earth: island arcs that form
on the oceanic lithosphere (for example, the Mariana and the Tonga
island arcs), and continental arcs such as the Cascade Volcanic Arc,
that form along the coast of continents. Island arcs (intraoceanic or
primitive arcs) are produced by the subduction of oceanic lithosphere
beneath another oceanic lithosphere (ocean-ocean subduction) while
continental arcs (Andean arcs) form during the subduction of oceanic
lithosphere beneath a continental lithosphere (ocean-continent
subduction).^\[65\]^ An example of a volcanic arc having both island and
continental arc sections is found behind the Aleutian Trench subduction
zone in Alaska.
Volcanoes that occur above subduction zones, such as Mount St. Helens,
Mount Etna, and Mount Fuji, lie approximately one hundred kilometers
from the trench in arcuate chains called volcanic arcs. Plutons, like
Half Dome in Yosemite National Park, generally form 10--50 km
(6--31 mi)^\[66\]^ below the volcanoes within the volcanic arcs and are
only visible on the surface once the volcanoes have weathered away. The
volcanism and plutonism occur as a consequence of the subducting oceanic
slab dehydrating as it reaches higher pressures and temperatures. Once
the oceanic slab reaches about 100 km (62 mi) in depth,^\[66\]^ hydrous
minerals become unstable and release fluids into the asthenosphere. The
fluids act as a flux for the rock within the asthenosphere and cause it
to partially melt. The partially melted material is more buoyant and as
a result will rise into the lithosphere, where it forms large magma
chambers called diapirs. Some of the magma will make it to the surface
of the crust where it will form volcanoes and, if eruptive on earth\'s
surface, will produce andesitic lava. Magma that remains in the
lithosphere long enough will cool and form plutonic rocks such as
diorite, granodiorite, and sometimes granite.
The arc magmatism occurs one hundred to two hundred kilometers from the
trench and approximately one hundred kilometers above the subducting
slab.^\[67\]^ Arcs produce about 10% of the total volume of magma
produced each year on Earth (approximately 0.75 cubic kilometers), much
less than the volume produced at mid-ocean ridges,^\[68\]^ but they have
formed most continental crust.^\[4\]^ Arc volcanism has the greatest
impact on humans because many arc volcanoes lie above sea level and
erupt violently. Aerosols injected into the stratosphere during violent
eruptions can cause rapid cooling of Earth\'s climate and affect air
travel.^\[69\]^
Arc-magmatism plays a role in Earth\'s carbon cycle by releasing
subducted carbon through volcanic processes. Older theory states that
the carbon from the subducting plate is made available in overlying
magmatic systems via decarbonation, where CO~2~ is released through
silicate-carbonate metamorphism.^\[70\]^ However, evidence from
thermodynamic modeling has shown that the pressures and temperatures
necessary for this type of metamorphism are much higher than what is
observed in most subduction zones.^\[70\]^ Frezzoti et al. (2011)
propose a different mechanism for carbon transport into the overriding
plate via dissolution (release of carbon from carbon-bearing minerals
into an aqueous solution) instead of decarbonation. Their evidence comes
from the close examination of mineral and fluid inclusions in
low-temperature (\<600 °C) diamonds and garnets found in an eclogite
facies in the Alps. The chemistry of the inclusions supports the
existence of a carbon-rich fluid in that environment, and additional
chemical measurements of lower pressure and temperature facies in the
same tectonic complex support a model for carbon dissolution (rather
than decarbonation) as a means of carbon transport.^\[70\]^
<div>
# # Earthquakes and tsunamis {#Earthquakes_and_tsunamis}
</div>
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Elastic strain caused by plate convergence in subduction zones produces
at least three types of earthquakes. These are deep earthquakes,
megathrust earthquakes, and outer rise earthquakes. Deep earthquakes
happen within the crust, megathrust earthquakes on the subduction
interface near the trench, and outer rise earthquakes on the subducting
lower plate as it bends near the trench.
Anomalously deep events are a characteristic of subduction zones, which
produce the deepest quakes on the planet. Earthquakes are generally
restricted to the shallow, brittle parts of the crust, generally at
depths of less than twenty kilometers. However, in subduction zones
quakes occur at depths as great as 700 km (430 mi). These quakes define
inclined zones of seismicity known as Wadati--Benioff zones which trace
the descending slab.^\[71\]^
Nine of the ten largest earthquakes of the last 100 years were
subduction zone megathrust earthquakes. These included the 1960 Great
Chilean earthquake which at M 9.5 was the largest earthquake ever
recorded, the 2004 Indian Ocean earthquake and tsunami, and the 2011
Tōhoku earthquake and tsunami. The subduction of cold oceanic
lithosphere into the mantle depresses the local geothermal gradient and
causes a larger portion of Earth\'s crust to deform in a more brittle
fashion than it would in a normal geothermal gradient setting. Because
earthquakes can occur only when a rock is deforming in a brittle
fashion, subduction zones can cause large earthquakes. If such a quake
causes rapid deformation of the sea floor, there is potential for
tsunamis. The largest tsunami ever recorded happened due to a
mega-thrust earthquake on December 26, 2004. The earthquake was caused
by subduction of the Indo-Australian plate under the Eurasian plate, but
the tsunami spread over most of the planet and devastated the areas
around the Indian Ocean. Small tremors which cause small, nondamaging
tsunamis, also occur frequently.^\[71\]^
A study published in 2016 suggested a new parameter to determine a
subduction zone\'s ability to generate mega-earthquakes.^\[72\]^ By
examining subduction zone geometry and comparing the degree of lower
plate curvature of the subducting plate in great historical earthquakes
such as the 2004 Sumatra-Andaman and the 2011 Tōhoku earthquake, it was
determined that the magnitude of earthquakes in subduction zones is
inversely proportional to the angle of subduction near the trench,
meaning that \"the flatter the contact between the two plates, the more
likely it is that mega-earthquakes will occur\".^\[73\]^
Outer rise earthquakes on the lower plate occur when normal faults
oceanward of the subduction zone are activated by flexure of the plate
as it bends into the subduction zone.^\[74\]^ The 2009 Samoa earthquake
is an example of this type of event. Displacement of the sea floor
caused by this event generated a six-meter tsunami in nearby Samoa.
Seismic tomography has helped detect subducted lithospheric slabs deep
in the mantle where no earthquakes occur.^\[29\]^ About one hundred
slabs have been described in terms of depth and their timing and
location of subduction.^\[75\]^ The great seismic discontinuities in the
mantle, at 410 km (250 mi) depth and 670 km (420 mi), are disrupted by
the descent of cold slabs in deep subduction zones. Some subducted slabs
seem to have difficulty penetrating the major discontinuity that marks
the boundary between the upper mantle and lower mantle at a depth of
about 670 km (420 mi). Other subducted oceanic plates have sunk to the
core--mantle boundary at 2,890 km (1,800 mi) depth. Generally, slabs
decelerate during their descent into the mantle, from typically several
cm/yr (up to \~10 cm/yr in some cases) at the subduction zone and in the
uppermost mantle, to \~1 cm/yr in the lower mantle.^\[75\]^ This leads
to either folding or stacking of slabs at those depths, visible as
thickened slabs in seismic tomography. Below \~1700 km, there might be a
limited acceleration of slabs due to lower viscosity as a result of
inferred mineral phase changes until they approach and finally stall at
the core--mantle boundary.^\[75\]^ Here the slabs are heated up by the
ambient heat and are not detected anymore \~300 Myr after
subduction.^\[75\]^
Orogeny is the process of mountain building. Subducting plates can lead
to orogeny by bringing oceanic islands, oceanic plateaus, sediments and
passive continental margins to convergent margins. The material often
does not subduct with the rest of the plate but instead is accreted to
(scraped off) the continent, resulting in exotic terranes. The collision
of this oceanic material causes crustal thickening and
mountain-building. The accreted material is often referred to as an
accretionary wedge or prism. These accretionary wedges can be associated
with ophiolites (uplifted ocean crust consisting of sediments, pillow
basalts, sheeted dykes, gabbro, and peridotite).^\[76\]^
Subduction may also cause orogeny without bringing in oceanic material
that accretes to the overriding continent. When the lower plate subducts
at a shallow angle underneath a continent (something called \"flat-slab
subduction\"), the subducting plate may have enough traction on the
bottom of the continental plate to cause the upper plate to contract by
folding, faulting, crustal thickening, and mountain building. Flat-slab
subduction causes mountain building and volcanism moving into the
continent, away from the trench, and has been described in western North
America (i.e. Laramide orogeny, and currently in Alaska, South America,
and East Asia.^\[75\]^
The processes described above allow subduction to continue while
mountain building happens concurrently, which is in contrast to
continent-continent collision orogeny, which often leads to the
termination of subduction.
<div>
# # Subduction of continental lithosphere {#Subduction_of_continental_lithosphere}
</div>
Continents are pulled into subduction zones by the sinking oceanic plate
they are attached to. Where continents are attached to oceanic plates
with no subduction, there is a deep basin that accumulates thick suites
of sedimentary and volcanic rocks known as a passive margin. Some
passive margins have up to 10 km (6.2 mi) of sedimentary and volcanic
rocks covering the continental crust. As a passive margin is pulled into
a subduction zone by the attached and negatively buoyant oceanic
lithosphere, the sedimentary and volcanic cover is mostly scraped off to
form an orogenic wedge. An orogenic wedge is larger than most
accretionary wedges due to the volume of material there is to accrete.
The continental basement rocks beneath the weak cover suites are strong
and mostly cold, and can be underlain by a \>200 km thick layer of dense
mantle. After shedding the low density cover units, the continental
plate, especially if it is old, goes down the subduction zone. As this
happens, metamorphic reactions increase the density of the continental
crustal rocks, which leads to less buoyancy.
One study of the active Banda arc-continent collision claims that by
unstacking the layers of rock that once covered the continental
basement, but are now thrust over one another in the orogenic wedge, and
measuring how long they are, can provide a minimum estimate of how far
the continent has subducted.^\[77\]^ The results show at least a minimum
of 229 km (142 mi) of subduction of the northern Australian continental
plate. Another example may be the continued northward motion of India,
which is subducting beneath Asia. The collision between the two
continents initiated around 50 my ago, but is still active.
<div>
# # []{#Intra-oceanic:_ocean.2Focean_plate_subduction}Intra-oceanic: ocean/ocean plate subduction {#Intra-oceanic:_ocean/ocean_plate_subduction}
</div>
Oceanic-Oceanic plate subduction zones comprise roughly 40% of all
subduction zone margins on the planet. The ocean-ocean plate
relationship can lead to subduction zones between oceanic and
continental plates, therefore highlighting how important it is to
understand this subduction setting. Although it is not fully understood
what causes the initiation of subduction of an oceanic plate under
another oceanic plate, there are three main models put forth by
Baitsch-Ghirardello et al. that explain the different regimes present in
this setting.^\[78\]^
The models are as follows:
1. *retreating subduction:* caused by weak coupling between the lower
and upper plate which leads to the opening of a back arc basin and
the subduction zone being moved by slab rollback.
2. *stable subduction:* caused by intermediate coupling between the
lower and upper plate. The subduction zone generally stays in the
same place and the subduction plate subducts at a consistent angle.
3. *advancing subduction:* caused by strong coupling between the upper
and lower plate. The subducting sediments thicken causing partially
molten plumes to be on top of subducting plate.
<div>
# # Arc-continent collision and global climate {#Arc-continent_collision_and_global_climate}
</div>
In their 2019 study, Macdonald et al. proposed that arc-continent
collision zones and the subsequent obduction of oceanic lithosphere was
at least partially responsible for controlling global climate. Their
model relies on arc-continent collision in tropical zones, where exposed
ophiolites composed mainly of mafic material increase \"global
weatherability\" and result in the storage of carbon through silicate
weathering processes. This storage represents a carbon sink, removing
carbon from the atmosphere and resulting in global cooling. Their study
correlates several Phanerozoic ophiolite complexes, including active
arc-continent subduction, with known global cooling and glaciation
periods.^\[79\]^ This study does not discuss Milankovitch cycles as a
driver of global climate cyclicity.
<div>
# Beginnings of subduction on Earth {#Beginnings_of_subduction_on_Earth}
</div>
Modern-style subduction is characterized by low geothermal gradients and
the associated formation of high-pressure low-temperature rocks such as
eclogite and blueschist.^\[80\]\[81\]^ Likewise, rock assemblages called
ophiolites, associated with modern-style subduction, also indicate such
conditions.^\[80\]^ Eclogite xenoliths found in the North China Craton
provide evidence that modern-style subduction occurred at least as early
as 1.8 Ga ago in the Paleoproterozoic Era.^\[80\]^ The eclogite itself
was produced by oceanic subduction during the assembly of
supercontinents at about 1.9--2.0 Ga.
Blueschist is a rock typical for present-day subduction settings. The
absence of blueschist older than Neoproterozoic reflects more
magnesium-rich compositions of Earth\'s oceanic crust during that
period.^\[82\]^ These more magnesium-rich rocks metamorphose into
greenschist at conditions when modern oceanic crust rocks metamorphose
into blueschist.^\[82\]^ The ancient magnesium-rich rocks mean that
Earth\'s mantle was once hotter, but not that subduction conditions were
hotter. Previously, the lack of pre-Neoproterozoic blueschist was
thought to indicate a different type of subduction.^\[82\]^ Both lines
of evidence refute previous conceptions of modern-style subduction
having been initiated in the Neoproterozoic Era 1.0 Ga
ago.^\[80\]\[82\]^
<div>
# History of investigation {#History_of_investigation}
</div>
Harry Hammond Hess, who during World War II served in the United States
Navy Reserve and became fascinated with the ocean floor, studied the
Mid-Atlantic Ridge, and proposed that hot molten rock was added to the
crust at the ridge and expanded the seafloor outward. This theory was to
become known as seafloor spreading. Since the Earth\'s circumference has
not changed over geologic time, Hess concluded that older seafloor has
to be consumed somewhere else, and suggested that this process takes
place at oceanic trenches, where the crust would be melted and recycled
into the Earth\'s mantle.^\[83\]^
In 1964, George Plafker researched the Good Friday earthquake in Alaska.
He concluded that the cause of the earthquake was a megathrust reaction
in the Aleutian Trench, a result of the Alaskan continental crust
overlapping the Pacific oceanic crust. This meant that the Pacific crust
was being forced downward, or *subducted*, beneath the Alaskan crust.
The concept of subduction would play a role in the development of the
plate tectonics theory.^\[84\]^
First geologic attestations of the \"subduct\" words date to
1970,^\[85\]^ In ordinary English *to subduct*, or *to subduce* (from
Latin [*subducere*]{title="Latin-language text"}, \"to lead
away\")^\[86\]^ are transitive verbs requiring a subject to perform an
action on an object not itself, here the lower plate, which has then
been *subducted* (\"removed\"). The geological term is \"consumed\",
which happens the geological moment the lower plate slips under, even
though it may persist for some time until its remelting and dissipation.
In this conceptual model, plate is continually being used up.^\[87\]^
The identity of the subject, the consumer, or agent of consumption, is
left unstated. Some sources accept this subject-object construct.
Geology makes *to subduct* into an intransitive verb and a reflexive
verb. The lower plate itself is the subject. It subducts, in the sense
of retreat, or removes itself, and while doing so, is the \"subducting
plate\". Moreover, the word slab is specifically attached to the
\"subducting plate\", even though in English the upper plate is just as
much of a slab.^\[88\]^ The upper plate is left hanging, so to speak. To
express it geology must switch to a different verb, typically *to
override*. The upper plate, the subject, performs the action of
overriding the object, the lower plate, which is overridden.^\[89\]^
Subduction zones are important for several reasons:
- Subduction zone physics: Sinking of the oceanic lithosphere
(sediments, crust, mantle), by the contrast of density between the
cold and old lithosphere and the hot asthenospheric mantle wedge, is
the strongest force (but not the only one) needed to drive plate
motion and is the dominant mode of mantle
convection.^\[*[citation\ needed]{title="This claim needs references to reliable sources. (January 2023)"}*\]^
- Subduction zone chemistry: The subducted sediments and crust dehydrate
and release water-rich (aqueous) fluids into the overlying mantle,
causing mantle melting and fractionation of elements between the
surface and deep mantle reservoirs, producing island arcs and
continental crust. Hot fluids in subduction zones also alter the
mineral compositions of the subducting sediments and potentially the
habitability of the sediments for microorganisms.^\[90\]^
- Subduction zones drag down subducted oceanic sediments, oceanic crust,
and mantle lithosphere that interact with the hot asthenospheric
mantle from the over-riding plate to produce calc-alkaline series
melts, ore deposits, and continental crust.
- Subduction zones pose significant threats to lives, property, economic
vitality, cultural and natural resources, and quality of life. The
tremendous magnitudes of earthquakes and volcanic eruptions can also
have knock-on effects with global impact.^\[91\]^
Subduction zones have also been considered as possible disposal sites
for nuclear waste in which the action of subduction itself would carry
the material into the planetary mantle, safely away from any possible
influence on humanity or the surface environment. However, that method
of disposal is currently banned by international
agreement.^\[92\]\[93\]\[94\]\[95\]^ Furthermore, plate subduction zones
are associated with very large megathrust earthquakes, making the
effects of using any specific site for disposal unpredictable and
possibly adverse to the safety of long-term disposal.^\[93\]^
- Compaction simulation
- Divergent boundary -- Linear feature between two tectonic plates
- Divergent double subduction -- Type of plate tectonic process
- List of tectonic plate interactions#Convergent boundaries (subduction
zones) -- Types of plate boundaries
- Obduction -- Geological process at tectonic plate boundaries
- Paired metamorphic belts -- Parallel linear rock units
- Ring of Fire -- Tectonic belt of earthquakes and volcanoes
- Slab window -- Type of gap in a subducted oceanic plate
- Wilson Cycle -- Geophysical model of the opening and closing of rifts
<!-- -->
- Stern, R.J. (1998). \"A Subduction Primer for Instructors of
Introductory Geology Courses and Authors of Introductory Geology
Textbooks\". *Journal of Geoscience Education*. '46' (3): 221--228.
Bibcode:1998JGeEd..46..221S.
doi:10.5408/1089-9995-46.3.221.[]{title="ctx_ver=Z39.88-2004&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&rft.genre=article&rft.jtitle=Journal+of+Geoscience+Education&rft.atitle=A+Subduction+Primer+for+Instructors+of+Introductory+Geology+Courses+and+Authors+of+Introductory+Geology+Textbooks&rft.volume=46&rft.issue=3&rft.pages=221-228&rft.date=1998&rft_id=info%3Adoi%2F10.5408%2F1089-9995-46.3.221&rft_id=info%3Abibcode%2F1998JGeEd..46..221S&rft.aulast=Stern&rft.aufirst=R.J.&rfr_id=info%3Asid%2Fen.wikipedia.org%3ASubduction"}
- Tatsumi, Y. (2005). \"The Subduction Factory: How it operates on
Earth\". *GSA Today*. '15' (7): 4--10.
doi:[10.1130/1052-5173(2005)015\[4:TSFHIO\]2.0.CO;2]{title="Freely accessible"}.[]{title="ctx_ver=Z39.88-2004&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&rft.genre=article&rft.jtitle=GSA+Today&rft.atitle=The+Subduction+Factory%3A+How+it+operates+on+Earth&rft.volume=15&rft.issue=7&rft.pages=4-10&rft.date=2005&rft_id=info%3Adoi%2F10.1130%2F1052-5173%282005%29015%5B4%3ATSFHIO%5D2.0.CO%3B2&rft.aulast=Tatsumi&rft.aufirst=Y.&rft_id=https%3A%2F%2Fdoi.org%2F10.1130%252F1052-5173%25282005%2529015%255B4%253ATSFHIO%255D2.0.CO%253B2&rfr_id=info%3Asid%2Fen.wikipedia.org%3ASubduction"}
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