Pluton emplacement

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The methods of pluton emplacement are the ways magma is accommodated in a host rock where the final result is a pluton. The methods of pluton emplacement are not yet fully understood, but there are many different proposed pluton emplacement mechanisms. Stoping, diapirism and ballooning are the widely accepted mechanisms. There is now evidence of incremental emplacement of plutons.

Contents

Stoping

Vertical migration of magma is driven by gravity. Stoping occurs when blocks of wall rock material are transferred downward through a pluton. [1] [2] Stoping is an important emplacement mechanism in a variety of tectonic settings and has been widely used to explain discordant pluton contacts. [2] The most common signatures of stoping are sharp discordant contacts between plutons and wall rocks and a lack of ductile deformation of the wall rocks. Other characteristics of stoping include the presence of xenoliths in the plutons, evidence for the rotation of xenoliths and geochemical evidence of magma contamination. [2]

Structural relations around stoped blocks

Igneous minerals within a pluton can record deformation history. Therefore, it is useful to understand magmatic fabrics for understanding pluton emplacement. Experimental work done on rocks has helped with establishing a relationship between the rheology and deformation mechanisms on magma. The setbacks encountered are foliation and lineation can be produced by a number of different processes, magmatic strains can be decoupled from the host rocks, and strains and timing the exact time of fabric formation with a particular pluton ascent mechanism is difficult. Magmatic foliations and mafic enclaves usually indicate radially increasing strains normal to the pluton contact and extensional strains parallel to it.

Magmatic fabrics will not record information of the stoping process as they are only formed near the end of the pluton emplacement. Furthermore, any magmatic fabrics that are recorded are likely to be affected by strain. Therefore, the causes of the magmatic fabrics may not be discernable, and at best can only give inferences to the mechanisms for emplacement of the pluton, or magma chamber internal mechanisms. [3]

Problems with stoping as an emplacement process

In order for a magma body of a certain volume (V) to ascend by stoping by a distance equal to its height (H), a volume of wall rocks equivalent to its volume (V) must sink through the magma. For that reason, for stoping to be an important magma ascent process, plutons should contain large volumes of xenoliths; The floors of plutons such as the Lookout Peak pluton, the Tinemaha pluton and a number of plutons around the world lack an abundance of xenoliths. [2] If stoping is a significant process there should be abundant xenoliths found.

Daly who proposed the theory of stoping argued that it is an efficient process because large blocks can sink rapidly because of the quadratic dependence on sinking velocity. [2] Given the size of the blocks sinking, there should be abundant small fragments produced by natural fragmentation, however there is a paucity of small fragments at pluton margins and this is inconsistent with stoping.

Another drawback of stoping is it cools too rapidly and occurs too slowly for low density crustal rocks. There is also not a lot of evidence for forceful lateral emplacement with sufficient strain to make room for the ascending pluton.

Incremental emplacement

There is growing evidence that large homogenous plutons grew incrementally, frequently as sills. Sheeted intrusions are recognizable worldwide. Evidence suggests that steeply dipping sheets at the margins of some plutons were emplaced sub horizontally and then tilted at the margin of a sagging floor. It is thought that plutons are fed by dikes and have grown by this process. This is evident in McDoogle pluton in the Sierra Nevada; this pluton is compositionally layered parallel to its contacts and contains numerous thin concordant panels of wall rock. [4] Ascent by stoping is less feasible with incremental emplacement because if the active magma body is below the top of a pluton, stoping rearranges material within the pluton and produces no overall ascent. To reach a position at the top of the older increments, an increment would have to stop its way upward through all previous increments. [2] The rheology of host rock plays a key role: hard rock will be able to stop magma ascent [5] [6] Magma emplacement occurs as pulses, with repose time. If intrusion rate is high enough, the different pulses may mix, with their individual contacts being lost. Pulses are grouped into batches, sub-units and units, forming a pluton. [7] [8]

Ballooning

Ballooning is an emplacement mechanism used to describe the in situ inflation of the magma chamber of roughly spherical plutons. [9] In this proposed model, the magma rises until it loses heat and its outermost margin crystallizes, the hotter tail of the magma continues to ascend and expand the already crystallized outer margin.

Diapirism

Diapirism occurs when a hot fluid mass of magma moves by softening a thin region of wall rock nearest to the body. [10] It is thought to be limited to the mantle and lower crust which have high temperatures and ductile rocks.

In order for plutons to ascend, room must be made for them, but the general mechanisms are uncertain. A question that is most commonly asked is what happened to the rock occupying the space now occupied by the pluton? A viable method proposed to make room from ascending magma is a zone of lateral extension which can be found at mid ocean ridges, strike slip faults and dilational jogs (areas of tension along a fault offset). A problem with this method is that the extension rates are too slow and the slip magnitudes are too small to allow a magma chamber to form by intrusion of magma by the extension rate. [11]

Related Research Articles

Granite Common type of intrusive, felsic, igneous rock with granular structure

Granite is a coarse-grained (phaneritic) intrusive igneous rock composed mostly of quartz, alkali feldspar, and plagioclase. It forms from magma with a high content of silica and alkali metal oxides that slowly cools and solidifies underground. It is common in the continental crust of Earth, where it is found in igneous intrusions. These range in size from dikes only a few centimeters across to batholiths exposed over hundreds of square kilometers.

Gabbro Coarse-grained mafic intrusive rock

Gabbro is a phaneritic (coarse-grained), mafic intrusive igneous rock formed from the slow cooling of magnesium-rich and iron-rich magma into a holocrystalline mass deep beneath the Earth's surface. Slow-cooling, coarse-grained gabbro is chemically equivalent to rapid-cooling, fine-grained basalt. Much of the Earth's oceanic crust is made of gabbro, formed at mid-ocean ridges. Gabbro is also found as plutons associated with continental volcanism. Due to its variant nature, the term gabbro may be applied loosely to a wide range of intrusive rocks, many of which are merely "gabbroic". By rough analogy, gabbro is to basalt as granite is to rhyolite.

Batholith Large igneous rock intrusion

A batholith is a large mass of intrusive igneous rock, larger than 100 km2 (40 sq mi) in area, that forms from cooled magma deep in Earth's crust. Batholiths are almost always made mostly of felsic or intermediate rock types, such as granite, quartz monzonite, or diorite.

Anorthosite Mafic intrusive igneous rock composed predominantly of plagioclase

Anorthosite is a phaneritic, intrusive igneous rock characterized by its composition: mostly plagioclase feldspar (90–100%), with a minimal mafic component (0–10%). Pyroxene, ilmenite, magnetite, and olivine are the mafic minerals most commonly present.

Magma chamber Accumulation of molten rock within the Earths crust

A magma chamber is a large pool of liquid rock beneath the surface of the Earth. The molten rock, or magma, in such a chamber is less dense than the surrounding country rock, which produces buoyant forces on the magma that tend to drive it upwards. If the magma finds a path to the surface, then the result will be a volcanic eruption; consequently, many volcanoes are situated over magma chambers. These chambers are hard to detect deep within the Earth, and therefore most of those known are close to the surface, commonly between 1 km and 10 km down.

Xenolith

A xenolith is a rock fragment that becomes enveloped in a larger rock during the latter's development and solidification. In geology, the term xenolith is almost exclusively used to describe inclusions in igneous rock entrained during magma ascent, emplacement and eruption. Xenoliths may be engulfed along the margins of a magma chamber, torn loose from the walls of an erupting lava conduit or explosive diatreme or picked up along the base of a flowing body of lava on the Earth's surface. A xenocryst is an individual foreign crystal included within an igneous body. Examples of xenocrysts are quartz crystals in a silica-deficient lava and diamonds within kimberlite diatremes. Xenoliths can be non-uniform within individual locations, even in areas which are spatially limited, e.g. rhyolite-dominated lava of Niijima volcano (Japan) contains two types of gabbroic xenoliths which are of different origin - they were formed in different temperature and pressure conditions.

Dike (geology) A sheet of rock that is formed in a fracture of a pre-existing rock body

A dike or dyke, in geological usage, is a sheet of rock that is formed in a fracture of a pre-existing rock body. Dikes can be either magmatic or sedimentary in origin. Magmatic dikes form when magma flows into a crack then solidifies as a sheet intrusion, either cutting across layers of rock or through a contiguous mass of rock. Clastic dikes are formed when sediment fills a pre-existing crack.

Laccolith Mass of igneous rock formed from magma

A laccolith is a large blister or igneous mound with a dome-shaped upper surface and a level base fed by a pipe like conduit from below. They form after an initial sheet-like intrusion has been injected within or between layers of sedimentary rock. The pressure of the magma is high enough that the overlying strata are forced upward and folded, giving the laccolith a dome or mushroom-like form with a generally planar base. Over time, erosion can form small hills and even mountains around a central peak since the magma rock is likely more resistant to weathering than the host rock. The growth of laccoliths can take as little as a few months when associated with a single magma injection event, or up to hundreds or thousands of years by multiple magmatic pulses stacking sills on top of each other and deforming the host rock incrementally.

Sill (geology) Tabular intrusion between older layers of rock

In geology, a sill is a tabular sheet intrusion that has intruded between older layers of sedimentary rock, beds of volcanic lava or tuff, or along the direction of foliation in metamorphic rock. A sill is a concordant intrusive sheet, meaning that a sill does not cut across preexisting rock beds. Stacking of sills builds a sill complex and a large magma chamber at high magma flux. In contrast, a dike is a discordant intrusive sheet, which does cut across older rocks. Sills are fed by dikes, except in unusual locations where they form in nearly vertical beds attached directly to a magma source. The rocks must be brittle and fracture to create the planes along which the magma intrudes the parent rock bodies, whether this occurs along preexisting planes between sedimentary or volcanic beds or weakened planes related to foliation in metamorphic rock. These planes or weakened areas allow the intrusion of a thin sheet-like body of magma paralleling the existing bedding planes, concordant fracture zone, or foliations.

Anatexis is the partial melting of rocks. Traditionally, anatexis is used specifically to discuss the partial melting of crustal rocks, while the generic term "partial melting" refers to the partial melting of all rocks, in both the crust and mantle.

Layered intrusion

A layered intrusion is a large sill-like body of igneous rock which exhibits vertical layering or differences in composition and texture. These intrusions can be many kilometres in area covering from around 100 km2 (39 sq mi) to over 50,000 km2 (19,000 sq mi) and several hundred metres to over one kilometre (3,300 ft) in thickness. While most layered intrusions are Archean to Proterozoic in age, they may be any age such as the Cenozoic Skaergaard intrusion of east Greenland or the Rum layered intrusion in Scotland. Although most are ultramafic to mafic in composition, the Ilimaussaq intrusive complex of Greenland is an alkalic intrusion.

In geology, igneous differentiation, or magmatic differentiation, is an umbrella term for the various processes by which magmas undergo bulk chemical change during the partial melting process, cooling, emplacement, or eruption. The sequence of magmas produced by igneous differentiation is known as a magma series.

Barberton Greenstone Belt Ancient granite-greenstone terrane on the eastern edge of the Kaapvaal craton in South Africa

The Barberton Greenstone Belt, also known as the Makhonjwa Mountains, is situated on the eastern edge of Kaapvaal Craton in South Africa. It is known for its gold mineralisation and for its komatiites, an unusual type of ultramafic volcanic rock named after the Komati River that flows through the belt. Some of the oldest exposed rocks on Earth are located in the Barberton Greenstone Belt of the Swaziland–Barberton areas and these contain some of the oldest traces of life on Earth. Only the rocks found in the Isua Greenstone Belt of Western Greenland are older.

Igneous intrusion Body of intrusive igneous rocks

In geology, an igneous intrusion is a body of intrusive igneous rock that forms by crystallization of magma slowly cooling below the surface of the Earth. Intrusions have a wide variety of forms and compositions, illustrated by examples like the Palisades Sill of New York and New Jersey; the Henry Mountains of Utah; the Bushveld Igneous Complex of South Africa; Shiprock in New Mexico; the Ardnamurchan intrusion in Scotland; and the Sierra Nevada Batholith of California.

Cathedral Peak Granodiorite

The Cathedral Peak Granodiorite (CPG) was named after its type locality, Cathedral Peak in Yosemite National Park, California. The granodiorite forms part of the Tuolumne Intrusive Suite, one of the four major intrusive suites within the Sierra Nevada. It has been assigned radiometric ages between 88 and 87 million years and therefore reached its cooling stage in the Coniacian.

Magmatic underplating Trapping of basaltic magmas within the crust

Magmatic underplating occurs when basaltic magmas are trapped during their rise to the surface at the Mohorovičić discontinuity or within the crust. Entrapment of magmas within the crust occurs due to the difference in relative densities between the rising magma and the surrounding rock. Magmatic underplating can be responsible for thickening of the crust when the magma cools. Geophysical seismic studies utilize the differences in densities to identify underplating that occurs at depth.

Okavango Dyke Swarm

The Okavango Dyke Swarm is a giant dyke swarm of the Karoo Large Igneous Province in northeast Botswana, southern Africa. It consists of a group of Proterozoic and Jurassic dykes, trending east-southeast across Botswana, spanning a region nearly 2,000 kilometres (1,200 mi) long and 110 kilometres (68 mi) wide. The Jurassic dykes were formed approximately 179 million years ago, composed of mainly tholeiitic mafic rocks. The formation is related to the magmatism at the Karoo triple junction, induced by the plate tectonic break up of the Gondwana supercontinent in the early Jurassic.

Kuna Crest Granodiorite, is found, in Yosemite National Park, United States. The granodiorite forms part of the Tuolumne Intrusive Suite, one of the four major intrusive suites within the Sierra Nevada. Of the Tuolumne Intrusive Suite, it is the oldest and darkest rock.

Crystal mush

A crystal mush is magma that contains a significant amount of crystals suspended in the liquid phase (melt). As the crystal fraction makes up less than half of the volume, there is no rigid large-scale three-dimensional network as in solids. As such, their rheological behavior mirrors that of absolute liquids. Within a single crystal mush, there is grading to a higher solid fraction towards the margins of the pluton while the liquid fraction increases towards the uppermost portions, forming a liquid lens at the top. Furthermore, depending on depth of placement crystal mushes are likely to contain a larger portion of crystals at greater depth in the crust than at shallower depth, as melting occurs from the adiabatic decompression of the magma as it rises, this is particularly the case for mid-oceanic ridges.

Volcanic and igneous plumbing systems Magma chambers

Volcanic and igneous plumbing systems (VIPS) consist of interconnected magma channels and chambers which are responsible for the production, storage and transportation of magma in Earth's crust. Volcanic plumbing systems can be found in all active tectonic settings, such as mid-oceanic ridges, subduction zones, and mantle plumes, when magmas generated in continental lithosphere, oceanic lithosphere, and in the sub-lithospheric mantle are transported. Magma is first generated by partial melting, followed by segregation and extraction from the source rock to separate the melt from the solid. As magma propagates upwards, a self-organised network of magma channels develops, transporting the melt from lower crust to upper regions. Channelled ascent mechanisms include the formation of dykes and ductile fractures that transport the melt in conduits. For bulk transportation, diapirs carry a large volume of melt and ascent through the crust. When magma stops ascending, or when magma supply stops, magma emplacement occurs. Different mechanisms of emplacement result in different structures, including plutons, sills, laccoliths and lopoliths.

References

  1. Daly, Reginald A. (1903). "The Mechanics of Igneous Intrusion". American Journal of Science. 15. Issue. 88: 269–298.
  2. 1 2 3 4 5 6 Glazner, A.; Bartley, J. (2006). "Is stoping a volumetrically significant pluton emplacement process?". GSA Bulletin. 118: 1185–1195. doi:10.1130/b25738.1.
  3. Fowler, T. Kenneth (1997). "Timing and the nature of magmatic fabrics from structural relations around stoped blocks". Journal of Structural Geology. 19. No. 2.: 209–224.
  4. Glazner, A. F.; Bartley, J.; Coleman, S. (2004). "Are plutons assembled over millions of years by amalgamation from small magma chambers?". GSA Today. 14: 114–121.
  5. Kavanagh, J. L.; Menand, T.; Sparks, R.S.J. (2006). "An experimental investigation of sill formation and propagation in layered elastic media. Earth Planet". Sci. Lett. 245: 799–813. doi:10.1016/j.epsl.2006.03.025.
  6. Leuthold, Julien; Müntener, Othmar; Baumgartner, Lukas; Putlitz, Benita; Ovtcharova, Maria; Schaltegger, Urs (2012). "Time resolved construction of a bimodal laccolith (Torres del Paine, Patagonia)". Earth and Planetary Science Letters. 325–326: 85–92. doi:10.1016/j.epsl.2012.01.032.
  7. Saint-Blanquat, M. de; Horsman, E.; Habert, G.; Morgan, S.S.; Vanderhaeghe, O.; Law, R.; Tikoff, B. (2011). "Multiscale magmatic cyclicity, duration of pluton construction, and the paradoxical relationship between tectonism and plutonism in continental arcs". Tectonophysics. 500 (1–4): 20–33. doi:10.1016/j.tecto.2009.12.009.
  8. Leuthold, Julien; Müntener, Othmar; Baumgartner, Lukas; Putlitz, Benita (2014). "Petrological constraints on the recycling of mafic crystal mushes and intrusion of braided sills in the Torres del Paine Mafic Complex (Patagonia)" (PDF). Journal of Petrology. 55 (5): 917–949. doi:10.1093/petrology/egu011. hdl: 20.500.11850/103136 .
  9. Vernon, R.; Paterson, S. (1995). "Bursting the bubble of ballooning plutons: A return to nested diapirs emplaced by multiple processes". GSA Bulletin. 107: 1356–1380.
  10. Marsh, D. B. 1984, On the mechanics of Igneous Diapirism, Stoping and Zone melting, American Journal of Science v. 282 p 808 – 855
  11. Hanson, R.B.; Glazner, A.F. (1995). "Thermal requirements for extensional emplacement of granitoids". Geology. 23: 213–216. doi:10.1130/0091-7613(1995)023<0213:trfeeo>2.3.co;2.