Plate tectonics - Wikipedia, the free encyclopedia
Plate tectonics - Wikipedia, the free encyclopedia
Plate tectonics
From Wikipedia, the free encyclopedia
Plate tectonics (from Greek , tektn "builder" or "mason") describes the large scale motions of Earth's lithosphere. The theory encompasses the older concepts of continental drift, developed during the first half of the 20th century, and seafloor spreading, understood during the 1960s.
The outermost part of the Earth's interior is
made up of two layers: above is the
lithosphere, comprising the crust and the
rigid uppermost part of the mantle. Below
the lithosphere lies the asthenosphere.
Although solid, the asthenosphere has
relatively low viscosity and shear strength and can flow like a liquid on geological time
The tectonic plates of the world were mapped in the second half of the 20th century.
scales. The deeper mantle below the
asthenosphere is more rigid again due to the higher pressure.
The lithosphere is broken up into what are called tectonic plates -- in the case of Earth, there are seven major and many minor plates (see list below). The lithospheric plates ride on the asthenosphere. These plates move in relation to one another at one of three types of plate boundaries: convergent or collision boundaries, divergent or spreading boundaries, and transform boundaries. Earthquakes, volcanic activity, mountain-building, and oceanic trench formation occur along plate boundaries. The lateral movement of the plates is typically at speeds of 50--100 mm/a.[1]
Contents
1 Synopsis of the development of the theory 2 Key principles 3 Types of plate boundaries
3.1 Transform (conservative) boundaries 3.2 Divergent (constructive) boundaries 3.3 Convergent (destructive) boundaries 4 Driving forces of plate motion 4.1 Friction 4.2 Gravitation
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4.3 External forces 4.4 Relative significance of each mechanism 5 Major plates 6 Historical development of the theory 6.1 Continental drift 6.2 Floating continents 6.3 Plate tectonic theory
6.3.1 Explanation of magnetic striping 6.3.2 Subduction discovered 6.3.3 Mapping with earthquakes 6.4 Geological paradigm shift 7 Biogeographic implications on biota 8 Plate tectonics on other planets 8.1 Venus 8.2 Mars 8.3 Galilean satellites 8.4 Titan 9 See also 10 References 11 Further reading 12 External links
Synopsis of the development of the theory
In the late 19th and early 20th centuries,
geologists assumed that the Earth's
major features were fixed, and that most
geologic features such as mountain
ranges could be explained by vertical
crustal movement, as explained by
geosynclinal theory. It was observed as
early as 1596 that the opposite coasts of
the Atlantic Ocean -- or, more precisely,
the edges of the continental shelves --
have similar shapes and seem once to have fitted together.[2] Since that time many theories were proposed to explain
Detailed map showing the tectonic plates with their movement vectors.
this apparent compatibility, but the
assumption of a solid earth made the various proposals difficult to explain.[3]
The discovery of radium and its associated heating properties in 1896 prompted a re-examination of the apparent age of the Earth,[4] since this had been estimated by its cooling rate and assumption the Earth's
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surface radiated like a black body.[5] Those calculations implied that, even if it started at red heat, the Earth would have dropped to its present temperature in a few tens of millions of years. Armed with the knowledge of a new heat source, scientists reasoned it was credible that the Earth was much older, and also that its core was still sufficiently hot to be liquid.
Plate tectonic theory arose out of the hypothesis of continental drift proposed by Alfred Wegener in 1912[6] and expanded in his 1915 book The Origin of Continents and Oceans. He suggested that the present continents once formed a single land mass that drifted apart, thus releasing the continents from the Earth's core and likening them to "icebergs" of low density granite floating on a sea of more dense basalt.[7][8] But without detailed evidence and a force sufficient to drive the movement, the theory was not generally accepted: the Earth might have a solid crust and a liquid core, but there seemed to be no way that portions of the crust could move around. Later science supported theories proposed by English geologist Arthur Holmes in 1920 that plate junctions might lie beneath the sea and Holmes' 1928 suggestion of convection currents within the mantle as the driving force.[9][10][3]
The first evidence that the lithospheric plates did move came with the discovery of variable magnetic field direction in rocks of differing ages, first revealed at a symposium in Tasmania in 1956. Initially theorized as an expansion of the global crust,[11] later collaborations developed the plate tectonics theory, which accounted for spreading as the consequence of new rock upwelling, but avoided the need for an expanding globe by recognizing subduction zones and conservative translation faults. It was at this point that Wegener's theory became generally accepted by the scientific community. Additional work on the association of seafloor spreading and magnetic field reversals by Harry Hess and Ron G. Mason[12][13][14][15] pinpointed the precise mechanism which accounted for new rock upwelling.
Following the recognition of magnetic anomalies defined by symmetric, parallel stripes of similar magnetization on the seafloor on either side of a mid-ocean ridge, plate tectonics quickly became broadly accepted. Simultaneous advances in early seismic imaging techniques in and around WadatiBenioff zones together with many other geologic observations soon made plate tectonics a theory with extraordinary explanatory and predictive power.
Study of the deep ocean floor was critical to development of the theory; the field of deep sea marine geology accelerated in the 1960s. Correspondingly, plate tectonic theory was developed during the late 1960s and has since been accepted by almost all scientists throughout all geoscientific disciplines. The theory revolutionized the Earth sciences, explaining a diverse range of geological phenomena and their implications in other studies such as paleogeography and paleobiology.
Key principles
The outer layers of the Earth are divided into lithosphere and asthenosphere. This is based on differences in mechanical properties and in the method for the transfer of heat. Mechanically, the lithosphere is cooler and more rigid, while the asthenosphere is hotter and flows more easily. In terms of heat transfer, the lithosphere loses heat by conduction whereas the asthenosphere also transfers heat by convection and has a nearly adiabatic temperature gradient. This division should not be confused with the chemical subdivision of these same layers into the mantle (comprising both the asthenosphere and the mantle portion of the lithosphere) and the crust: a given piece of mantle may be part of the lithosphere or the
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asthenosphere at different times, depending on its temperature and pressure.
The key principle of plate tectonics is that the lithosphere exists as separate and distinct tectonic plates, which ride on the fluid-like (visco-elastic solid) asthenosphere. Plate motions range up to a typical 10-40 mm/a (Mid-Atlantic Ridge; about as fast as fingernails grow), to about 160 mm/a (Nazca Plate; about as fast as hair grows).[16][17]
The plates are around 100 km (60 miles) thick and consist of lithospheric mantle overlain by either of two types of crustal material: oceanic crust (in older texts called sima from silicon and magnesium) and continental crust (sial from silicon and aluminium). The two types of crust differ in thickness, with continental crust considerably thicker than oceanic (50 km vs 5 km).
One plate meets another along a plate boundary, and plate boundaries are commonly associated with geological events such as earthquakes and the creation of topographic features like mountains, volcanoes and oceanic trenches. The majority of the world's active volcanoes occur along plate boundaries, with the Pacific Plate's Ring of Fire being most active and most widely known. These boundaries are discussed in further detail below.
Tectonic plates can include continental crust or oceanic crust, and a single plate typically carries both. For example, the African Plate includes the continent and parts of the floor of the Atlantic and Indian Oceans. The distinction between continental crust and oceanic crust is based on the density of constituent materials; oceanic crust is denser than continental crust owing to their different proportions of various elements, particularly silicon. Oceanic crust is denser because it has less silicon and more heavier elements ("mafic") than continental crust ("felsic").[18] As a result, oceanic crust generally lies below sea level (for example most of the Pacific Plate), while the continental crust projects above sea level (see isostasy for explanation of this principle).
Types of plate boundaries
Three types of plate boundaries exist, characterized by the way the plates move relative to each other. They are associated with different types of surface phenomena. The different types of plate boundaries are:
1. Transform boundaries occur where
plates slide or, perhaps more
accurately, grind past each other along
transform faults. The relative motion
of the two plates is either sinistral (left
side toward the observer) or dextral
Three types of plate boundary.
(right side toward the observer). The
San Andreas Fault in California is one
example.
2. Divergent boundaries occur where two plates slide apart from each other. Mid-ocean ridges (e.g.,
Mid-Atlantic Ridge) and active zones of rifting (such as Africa's Great Rift Valley) are both
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examples of divergent boundaries. 3. Convergent boundaries (or active margins) occur where two plates slide towards each other
commonly forming either a subduction zone (if one plate moves underneath the other) or a continental collision (if the two plates contain continental crust). Deep marine trenches are typically associated with subduction zones. The subducting slab contains many hydrous minerals, which release their water on heating; this water then causes the mantle to melt, producing volcanism. Examples of this are the Andes mountain range in South America and the Japanese island arc.
Transform (conservative) boundaries
John Tuzo Wilson recognized that because of friction, the plates cannot simply glide past each other. Rather, stress builds up in both plates and when it reaches a level that exceeds the strain threshold of rocks on either side of the fault the accumulated potential energy is released as strain. Strain is both accumulative and/or instantaneous depending on the rheology of the rock; the ductile lower crust and mantle accumulates deformation gradually via shearing whereas the brittle upper crust reacts by fracture, or instantaneous stress release to cause motion along the fault. The ductile surface of the fault can also release instantaneously when the strain rate is too great. The energy released by instantaneous strain release is the cause of earthquakes, a common phenomenon along transform boundaries.
A good example of this type of plate boundary is the San Andreas Fault which is found in the western coast of North America and is one part of a highly complex system of faults in this area. At this location, the Pacific and North American plates move relative to each other such that the Pacific plate is moving northwest with respect to North America. Other examples of transform faults include the Alpine Fault in New Zealand and the North Anatolian Fault in Turkey. Transform faults are also found offsetting the crests of mid-ocean ridges (for example, the Mendocino Fracture Zone offshore northern California).
Divergent (constructive) boundaries
At divergent boundaries, two plates move apart from each
other and the space that this creates is filled with new crustal
material sourced from molten magma that forms below. The
origin of new divergent boundaries at triple junctions is
sometimes thought to be associated with the phenomenon
known as hotspots. Here, exceedingly large convective cells
bring very large quantities of hot asthenospheric material
near the surface and the kinetic energy is thought to be
sufficient to break apart the lithosphere. The hot spot which
may have initiated the Mid-Atlantic Ridge system currently
underlies Iceland which is widening at a rate of a few centimeters per year.
Divergent boundaries are typified in the oceanic lithosphere
Bridge across the ?lfagj? rift valley in southwest Iceland, the boundary between
the Eurasian and North American continental tectonic plates.
by the rifts of the oceanic ridge system, including the
Mid-Atlantic Ridge and the East Pacific Rise, and in the continental lithosphere by rift valleys such as
the famous East African Great Rift Valley. Divergent boundaries can create massive fault zones in the
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