Mantle
D layer
Lower Mantle
Transition Zone
Upper Mantle
Basics -- Earth'sInterior
Introduction
Tour through the layers of earth
Surface to core, chemically
Crust
Mantle
Core
Surface to core, physically
Lithosphere
Asthenosphere
Upper mesosphere
Lower mesosphere
Outer core
Inner core
Earth's magnetic field originates in the core
Beyond simple layers
How do we know?
Igneous rocks and fault blocks
Seismic waves
Gravity
Moment of inertia
Meteorites
Experiments
Introduction
If we could journey to the center of the earth we would have to travel about 6,400 km (4,000 miles). Along the way to earth's core we would pass layers of rock that can be classified in two different ways, either by their chemistry or their physical behavior.
According to the chemical composition of the rocks, earth's interior can be differentiated into three layers - crust, mantle, and core.
When considering the rocks of earth's interior in terms of their physical behavior, six layers can be differentiated from the surface to the core. The characteristics that distinguish these six different layers are based on the relative strength of a given layer in response to stress and whether it is solid or liquid.
Tour through the layers of earth
The chemical compositions and physical behaviors of the rocks of earth's interior converge in many ways but it is worthwhile to become familiar with the each of the different set of layers individually before exploring how they overlap.
The chemical composition and physical behavior of rock inside the earth relate to each other because the chemical composition of a rock is one of the factors that determines its physical behavior. However, the physical behavior of rock also depends on the pressure and temperature it is subjected to at its depth within the earth. As depth inside the earth increases, the pressure and temperature increase. Some layers in the earth are harder or softer than adjacent layers, even though they have the same composition, because they are at different pressures and temperatures.
Surface to core, chemically
Crust
The tour starts at the surface with earth's crust. Generally speaking, the crust is predominately silicon oxide and aluminum oxide. Continental crust is thicker and less dense than oceanic crust. Earth's crust varies in thickness from less than 5 km (under mid-ocean spreading ridges) to more than 70 km (beneath the highest mountain range).
Mantle
The next layer down chemically is the mantle. The mantle has an ultramafic composition - it contains more iron, magnesium, less aluminum and somewhat less silicon than the crust. The mantle is roughly 2,900 km thick. In terms of volume, the mantle is the largest of earth's three chemical layers.
Core
The final stop on the chemical tour is the core, which is mostly iron and nickel. The core is about 3,500 km thick.
The following table summarizes the chemical layers of the earth.
Chemical Layers of Earth
Crust
Mantle
Core
composition: high Si, Al, & O
composition: moderate Si, high Mg & Fe
composition: Fe & Ni
thickness: 5 to 70 km
thickness: 2,900 km
thickness: 3,500 km
Surface to core, physically
Lithosphere
Starting at the surface, the first layer is the lithosphere. We humans, and the other creatures that live on earth, occupy the surface of the lithosphere. The lithosphere is entirely solid except where there are zones of magma beneath volcanoes or in places undergoing magma intrusion. The volume of molten rock in the lithosphere is a tiny fraction, less than 0.1%, of the volume of the entire lithosphere.
The lithosphere itself has two parts. The top part is the crust. The bottom part is the lithospheric mantle. The two components of the lithosphere, in combination, form a relatively strong, rigid layer of rock that covers the earth. Earth's tectonic plates, all of which are in motion relative to each other, make up the lithosphere.
Asthenosphere
Beneath the lithosphere is a relatively weak and ductile layer of the mantle called the asthenosphere. Although the asthenosphere is solid, not liquid, it flows at geological rates, up to several cm (several inches) per year. In other words, the asthenosphere behaves much more plastically than the rigid lithosphere above it does.
The chemical composition of the asthenosphere is about the same as the chemical composition of the overlying lithospheric mantle. Why, then, is the asthenosphere soft and the lithosphere rigid? It is because at the depth of the asthenosphere, temperatures are very close to the melting point of the rock, weakening the rock. In fact, it is thought likely, from indirect evidence, that there is a small percentage of molten rock in the tiny spaces between the minerals of the asthenosphere, which contributes to the soft nature of the rock. However, the solid minerals of the asthenosphere are extensively in contact with each other, forming a material that is solid overall despite the possible presence of a small amount of partial melt.
The asthenosphere is the primary source of most magma. Because the asthenosphere is close to its melting point and may contain everywhere a small proportion of partly molten rock, it does not take much to cause magma to form and separate from the asthenosphere. As explained in the igneous rocks Basics page, melting of the asthenosphere can be caused by addition of fluid, particularly water, or by a decrease in pressure. In subduction zones, slabs of sinking lithosphere release water into the asthenosphere, causing the asthenosphere to melt and produce magma which rises into and through the crust, producing the volcanic arc that is found at every subduction zone. At divergent plate boundaries, the asthenosphere flows upward, or upwells, which reduces the lithostatic pressure enough to cause the rock of the asthenosphere to melt. That is why divergent plate boundaries are volcanic zones. The solidified lavas and intrusions at divergent plate boundaries produce new lithosphere, which fills in and replaces the plate material that spreads away on either side.
Upper mesosphere
Beneath the asthenosphere is the rest of the mantle, the mesosphere. The mesosphere makes up most of the volume of the mantle. The mesosphere is entirely solid. The temperature and pressure of the rock in the mesosphere keep it from breaking; therefore, no earthquakes originate from the mesosphere.
The upper mesosphere is a transition zone in which the rock rapidly becomes denser with depth in response to the increasing lithostatic pressure.
Lower mesosphere
The lower mesosphere starts at a depth of 660 km from earth's surface. At that depth there is an abrupt increase in density. This increase is caused by changes in the crystal structures of the most abundant minerals in the rock. These minerals change from less dense crystal structures above the boundary to more dense crystal structures below the boundary. The lower mesosphere undergoes little density change from its top boundary at 660 km to its base at 2900 km where it meets the outer core.
Outer core
The bottom of the mesosphere is the boundary with the earth's core. The core is about twice as dense as the crust, and about 1.5 times as dense as the mantle. The outer core is liquid, as was discovered when it was first observed that S-waves will not pass through it.
Inner core
The inner core is solid. The inner and outer cores are made of the same iron-rich, metallic composition. The temperature of the inner core is not very much greater than the temperature of the outer core. However, lithostatic pressure keeps increasing with depth and the inner core has the great weight of the rest of the earth pressing in on it. The pressure on the inner core is high enough to keep it in the solid state.
The following table summarizes the physical layers of the earth.
Physical Layers of Earth
Lithosphere
Asthenosphere
Upper Mesosphere
Lower Mesosphere
Outer Core
Inner Core
physical behavior:
rigid, brittle at shallow depths
physical behavior:
ductile
physical behavior:
rigid, not brittle, rapid increase in density with depth
physical behavior:
denser and more rigid than upper mesosphere
physical behavior:
liquid
physical behavior:
rigid, not brittle
thickness:
5 to 200 km
thickness:
100 to 300 km
thickness:
300 to 400 km
thickness:
2,300 km
thickness:
2,300 km
thickness:
1,200 km
Earth's magnetic field originates in the core
The liquid outer core is the source of the earth's magnetic field, as a result of its metallic nature, which means it contains electrons not attached to particular nuclei. Heat is transferred upward to the mantle from the inner core via convective cells, in which the liquid in the outer core flows in looping patterns. The combination of the loose electrons and looping convective flow with the rotation of the earth results in a geodynamo that produces a magnetic field. Because the magnetic field is generated by a dynamically convecting and rotating sphere of liquid, it is unstable. Every now and then, after several hundred thousand to several million years, the earth's magnetic field becomes unstable to the point that it temporarily shuts down. When it restarts, its north and south magnetic poles must inevitably be reversed, according to the physics of magnetic fields produced spontaneously from geodyamos. (For comparison, the magnetic field of the Sun, which is also produces by convecting electrical charges in a rotating sphere, becomes magnetically unstable and reverses its magnetic field on a more regular basis, every 11 years.)
Given that the inner core is a solid metallic sphere, made mostly of iron and nickel, surrounded entirely by liquid, it can be pictured as a giant ball bearing spinning in a pressurized fluid. Detailed studies of earthquake waves passing though the inner core have found evidence that it is spinning - rotating - just slightly faster than the rest of the earth.
Beyond simple layers
The interior of the earth is not simply layered. Some of the layers, particularly the crust and lithosphere, are highly variable in thickness. The boundaries between layers are rough and irregular. Some layers penetrate other layers at certain places. Variations in the thickness of the earth's layers, irregularities in layer boundaries, and interpenetrations of layers, reflect the dynamic nature of the earth.
For example, the lithosphere penetrates deep into the mesosphere at subduction zones. Although it is still a matter of research and debate, there is some evidence that subducted plates may penetrate all the way into the lower mesosphere. If so, plate tectonics is causing extensive mixing and exchange of matter in the earth, from the bottom of the mantle to the top of the crust.
As another example, hot spots may be places where gases and fluids rise from the core-mantle boundary, along with heat. Studies of helium isotopes in hot spot volcanic rocks find evidence that much of the helium comes from deep in the earth, probably from the lower mesosphere.
How do we know?
We humans have no hands-on access to samples of the earth's interior from deeper than the upper mantle. The earth's core is so dense and so deep, it is completely inaccessible. Contrary to a popular misconception, lava does not come from the earth's core. Magma and lava come from only the lithosphere and asthenosphere, the upper 200 km of earth's 6,400 km thickness. Attempts have been made to drill through the crust to reach the mantle, without success. Given the lack of actual pieces of the earth from deeper than the asthenosphere, how do we know about the internal layers of the earth, what they are made of, and what their properties and processes are?
Igneous rocks and fault blocks
There are two sources of rock samples from the lower lithosphere and asthenosphere, igneous rocks and fault blocks. Some igneous rocks contain xenoliths, pieces of solid rock that were adjacent to the body of magma, became incorporated into the magma, and were carried upward in the magma. From xenoliths in plutonic and volcanic igneous rocks, many samples of the lower crust and upper mantle have been identified and studied.
Another source of pieces of the lower crust and upper mantle is fault zones and exposed orogenic zones (root zones of mountains that have been exposed after much uplift and erosion). Some slabs of thrust-faulted rock contain lithospheric mantle rock. In ophiolites (see the ophiolite discussion on the exotic terranes Basics page), ultramafic rock from the mantle part of the lithosphere is a defining attribute. Most ophiolites and thrust-faulted slices of rock that contain pieces of the upper mantle are related to either subduction zones or transform plate boundaries.
Seismic waves
As discussed on the earthquakes Basics page, P-waves and S-waves move through different parts of the earth's interior in different ways. Analogous to how you can see what is in the room around you by interpreting the light that your eyes receive, light that has interacted with the things in the room around you to give it its characteristics, seismologists can interpret recordings of seismic waves to "see" inside the earth. Such imaging of the earth's interior is based on how the different layers of the earth have affected the seismic waves in different ways.
Where seismic waves speed up or slow down, they refract, changing the direction in which they are traveling. Where seismic waves encounter an abrupt boundary between two very different layers, some of the seismic wave energy is reflected, bouncing back at the same angle it struck. The reflections and refractions of seismic waves allow the layers and boundaries within the earth to be located and studied.
Here are some examples of what we have been able to distinguish in the earth's interior from the study of seismic waves and how they travel through the layers of the earth:
The thickness of the crust. This is a measure of the thickness of the crust based on the abrupt increase in speed of seismic waves that occurs when they enter the mantle. The boundary between the crust and mantle, as inferred from the change in the speed of P- and S-waves, is called the Mohorovicic discontinuity, named after the Croatian seismologist who first discerned it; usually it is referred to simply as the Moho. It is mainly from seismic waves that we know how thin oceanic crust is and how thick continental crust is.
The thickness of the lithosphere. Where seismic waves pass down from the lithosphere into the asthenosphere, they slow down. This is because of the lower rigidity and compressibility of the rocks in the layer below the lithosphere. The zone below the lithosphere where seismic waves travel more slowly is called the low velocity zone. The low velocity zone is probably coincident with the asthenosphere.
The boundary between the upper and lower mesosphere (upper and lower mantle). This shows up as an increase in seismic wave speed at a depth of 660 km.
The boundary between the mantle and the core. This is marked by S-waves coming to an abrupt stop, presumably because the outer core is liquid, and a sudden large reduction in the speed of P-waves, as they enter the liquid core where there is no rigidity to contribute to P-wave speed.
The inner core. This was first recognized by refraction of P-waves passing through this part of the core, due to an abrupt increase in their speed, which was not shown by P-waves traveling through only the outer part of the core.
Seismic tomography: imaging slabs and masses at various orientations in the earth, not just in layers. By combining data from many seismometers, three-dimensional images of zones in the earth that have higher or lower seismic wave speeds can be constructed. Seismic tomography shows that in some places there are masses of what may be subducted plates that have penetrated below the asthenosphere into the mesosphere and, in some cases, penetrated into the lower mesosphere, the deepest part of the mantle. In other places, subducted plates appear to have piled up at the base of the upper mesosphere without penetrating into the lower mesosphere.
Gravity
Isaac Newton was the first to calculate the total mass of the earth. This gives us an important constraint on what the earth is made of, because, by dividing the mass of the earth by the volume of the earth, we know the average density of the earth. Whatever the earth is made of, it must add up to the correct amount of mass. Gravity measurements, and the earth's mass, tell us that the interior of the earth must be denser than the crust, because the average density of earth is much higher than the density of the crust.
Because different parts of the crust, mantle, and core have different thicknesses and densities, the strength of gravity over particular points on earth varies slightly. These variations from the average strength of earth's gravity are called gravity anomalies. Mapping and analyzing gravity anomalies, in some cases by using satellites, and also be measuring the effect of gravity anomalies on the surface shape of the ocean, has given us much insight into subduction zones, mid-ocean spreading ridges, and mountain ranges, including constraints on the depths of their roots.
Moment of inertia
The earth's gravity tells us how much total mass the earth has, but does not tell us how the mass is distributed within the earth. A property known as moment of inertia, which is the resistance (inertia) of an object to changes in its spin (rotation), is determined by exactly how matter is distributed in a spinning object, from its core to its surface. The earth's moment of inertia is measured by its effect on other objects with which it interacts gravitationally, including the Moon, and satellites. Knowing the earth's moment of inertia provides a way of checking and refining our understanding of the mass and density of each of the earth's internal layers.
Meteorites
Studies of meteorites, which are pieces of asteroids that have landed on earth, along with astronomical studies of what the Sun, the other planets, and orbiting asteroids are made of, give us a model for the general chemical composition of objects in the inner solar system, which are made mainly of elements that form rocks and metals, as opposed to the outer planets such as Jupiter, which are made mostly of light, gas-forming elements. The general compositional model of the rocky and metallic part of the solar system has much higher percentages of iron, nickel, and magnesium than is found in the earth's crust.
If the earth's mantle is made of ultramafic rock, as is found in actual samples of the upper mantle in xenoliths and ophiolites, that would account for part of the missing iron, nickel, and magnesium. But much more iron and nickel would still be missing. If the core is made mostly of iron, and abundant nickel as well, it would give the earth an overall composition similar to the composition of other objects in the inner solar system, and similar to the proportions of rock and metal-forming elements measured in the Sun.
A mantle with an ultramafic composition, and a core made mostly of iron plus nickel, would make earth's composition match the composition of the rest of the solar system, and give those layers the right densities to account for the earth's moment of inertia and total mass.
Experiments
Geology, like other sciences, is based on experiment along with observation and theory. earth scientists and physicists have developed experimental methods to study how materials behave at the pressures and temperatures of the earth's interior, including core temperatures and pressures. They can measure such properties as the density, the state of matter (liquid or solid), the rigidity, the compressibility, and the speed at which seismic waves pass through these materials at high pressures and temperatures. These studies allow further refinement of our knowledge of what the interior of the earth is made of and how it behaves. These experiments support the theory that the mantle is ultramafic and the core is mostly iron and nickel, because they show that materials with those compositions have the same density and seismic wave speeds as have been observed in the earth.
The internal structure of Earth
Structure[edit]
Rheology[edit]
The Earth's mantle is divided into two major
rheological layers: the rigid
lithosphere comprising the uppermost mantle, and the more viscous
asthenosphere, separated by the
lithosphere-asthenosphere boundary. Lithosphere underlying ocean crust has a thickness of around 100 km, whereas lithosphere underlying continental crust generally has a thickness of 150-200 km.
[3] The lithosphere and overlying
crust make up
tectonic plates, which move over the asthenosphere.
The big 3[edit]
The Earth's mantle is divided into three major layers defined by sudden changes in
seismic velocity:
- the upper mantle (starting at the Moho, or base of the crust around 7 to 35 km (4.3 to 21.7 mi) downward to 410 km (250 mi))[4]
- the transition zone (approximately 410–660 km or 250–410 mi), in which wadsleyite (≈ 410–520 km or 250–320 mi) and ringwoodite (≈ 525–660 km or 326–410 mi) are stable
- the lower mantle (approximately 660–2,891 km or 410–1,796 mi), in which bridgmanite (≈ 660–2,685 km or 410–1,668 mi) and post-perovskite (≈ 2,685–2,891 km or 1,668–1,796 mi) are stable
The lower ~200 km of the lower mantle constitutes the D" (
D-double-prime) layer, a region with anomalous seismic properties. This region also contains
LLSVPs and
ULVZs.
Mineralogical structure[edit]
At the top of the transition zone, olivine undergoes isochemical phase transitions to wadsleyite and ringwoodite. Unlike nominally anhydrous olivine, these high-pressure olivine polymorphs have a large capacity to store water in their crystal structure. This has led to the hypothesis that the transition zone may host a large quantity of water.
[7] At the base of the transition zone, ringwoodite decomposes into bridgmanite (formerly called magnesium silicate perovskite), and ferropericlase. Garnet also becomes unstable at or slightly below the base of the transition zone.
The lower mantle is composed primarily of bridgmanite and
ferropericlase, with minor amounts of
calcium perovskite, calcium-ferrite structured oxide, and
stishovite. In the lowermost ~200 km of the mantle, bridgmanite isochemically transforms into post-perovskite.
Composition[edit]
The chemical composition of the mantle is difficult to determine with a high degree of certainty because it is largely inaccessible. Rare exposures of mantle rocks occur in
ophiolites, where sections of oceanic lithosphere have been
obducted onto a continent. Mantle rocks are also sampled as
xenoliths within
basalts or
kimberlites.
Most estimates of the mantle composition are based on rocks that sample only the uppermost mantle. There is debate as to whether the rest of the mantle, especially the lower mantle, has the same bulk composition.
[10] The mantle's composition has changed through the Earth's history due to the extraction of magma that solidified to form oceanic crust and continental crust.
Temperature and pressure[edit]
In the mantle, temperatures range from approximately 200 °C (392 °F) at the upper boundary with the crust to approximately 4,000 °C (7,230 °F) at the
core-mantle boundary.
[11] The
geothermal gradient of the mantle increases rapidly in the thermal
boundary layers at the top and bottom of the mantle, and increases gradually through the interior of the mantle.
[12]Although the higher temperatures far exceed the
melting points of the mantle rocks at the surface (about 1200 °C for representative peridotite), the mantle is almost exclusively solid.
[13] The enormous
lithostatic pressure exerted on the mantle prevents melting, because the temperature at which melting begins (the
solidus) increases with pressure.
The pressure in the mantle increases from a few kbar at the Moho to 1390 kbar (139 GPa) at the core-mantle boundary
[11].
Movement[edit]
This figure is a snapshot of one time-step in a model of mantle convection. Colors closer to red are hot areas and colors closer to blue are cold areas. In this figure, heat received at the
core–mantle boundary results in thermal expansion of the material at the bottom of the model, reducing its density and causing it to send plumes of hot material upwards. Likewise, cooling of material at the surface results in its sinking.
Because of the temperature difference between the Earth's surface and outer core and the ability of the crystalline rocks at high pressure and temperature to undergo slow, creeping, viscous-like deformation over millions of years, there is a
convective material circulation in the mantle.
[14] Hot material
upwells, while cooler (and heavier) material sinks downward. Downward motion of material occurs at
convergent plate boundaries called subduction zones. Locations on the surface that lie over plumes are predicted to have
high elevation (because of the buoyancy of the hotter, less-dense plume beneath) and to exhibit
hot spot volcanism. The volcanism often attributed to deep mantle plumes is alternatively explained by passive extension of the crust, permitting magma to leak to the surface (the "Plate" hypothesis).
[15]
The
convection of the Earth's mantle is a
chaotic process (in the sense of fluid dynamics), which is thought to be an integral part of the motion of plates. Plate motion should not be confused with
continental drift which applies purely to the movement of the crustal components of the continents. The movements of the lithosphere and the underlying mantle are coupled since descending lithosphere is an essential component of convection in the mantle. The observed continental drift is a complicated relationship between the forces causing oceanic lithosphere to sink and the movements within Earth's mantle.
Although there is a tendency to larger viscosity at greater depth, this relation is far from linear and shows layers with dramatically decreased viscosity, in particular in the upper mantle and at the boundary with the core.
[16] The mantle within about 200 km (120 mi) above the core–mantle boundary appears to have distinctly different seismic properties than the mantle at slightly shallower depths; this unusual mantle region just above the core is called
D″ ("D double-prime"), a nomenclature introduced over 50 years ago by the geophysicist
Keith Bullen.
[17]D″ may consist of material from subducted
slabs that descended and came to rest at the core–mantle boundary and/or from a new mineral polymorph discovered in perovskite called post-perovskite.
Earthquakes at shallow depths are a result of strike-slip faulting; however, below about 50 km (31 mi) the hot, high pressure conditions ought to inhibit further seismicity. The mantle is considered to be viscous and incapable of brittle faulting. However, in subduction zones, earthquakes are observed down to 670 km (420 mi). A number of mechanisms have been proposed to explain this phenomenon, including dehydration, thermal runaway, and phase change. The geothermal gradient can be lowered where cool material from the surface sinks downward, increasing the strength of the surrounding mantle, and allowing earthquakes to occur down to a depth of 400 km (250 mi) and 670 km (420 mi).
The pressure at the bottom of the mantle is ~136 G
Pa (1.4 million
atm).
[18] Pressure increases as depth increases, since the material beneath has to support the weight of all the material above it. The entire mantle, however, is thought to deform like a fluid on long timescales, with permanent plastic deformation accommodated by the movement of point, line, and/or planar defects through the solid crystals composing the mantle. Estimates for the viscosity of the upper mantle range between 10
19 and 10
24 Pa·s, depending on depth,
[16]temperature, composition, state of stress, and numerous other factors. Thus, the upper mantle can only flow very slowly. However, when large forces are applied to the uppermost mantle it can become weaker, and this effect is thought to be important in allowing the formation of tectonic plate boundaries.
Exploration[edit]
Exploration of the mantle is generally conducted at the seabed rather than on land because of the relative thinness of the oceanic crust as compared to the significantly thicker continental crust.
The first attempt at mantle exploration, known as
Project Mohole, was abandoned in 1966 after repeated failures and cost over-runs. The deepest penetration was approximately 180 m (590 ft). In 2005 an oceanic borehole reached 1,416 metres (4,646 ft) below the sea floor from the ocean drilling vessel
JOIDES Resolution.
On 5 March 2007, a team of scientists on board the
RRS James Cook embarked on a voyage to an area of the
Atlantic seafloor where the mantle lies exposed without any crust covering, midway between the
Cape Verde Islands and the
Caribbean Sea. The exposed site lies approximately three kilometres beneath the ocean surface and covers thousands of square kilometres.
[20][21] A relatively difficult attempt to retrieve samples from the Earth's mantle was scheduled for later in 2007.
[22] The Chikyu Hakken mission attempted to use the Japanese vessel
Chikyū to drill up to 7,000 m (23,000 ft) below the seabed. This is nearly three times as deep as preceding
oceanic drillings.
A novel method of exploring the uppermost few hundred kilometres of the Earth was proposed in 2005, consisting of a small, dense, heat-generating probe which melts its way down through the crust and mantle while its position and progress are tracked by acoustic signals generated in the rocks.
[23] The probe consists of an outer sphere of
tungsten about one metre in diameter with a
cobalt-60 interior acting as a radioactive heat source. It was calculated that such a probe will reach the oceanic
Moho in less than 6 months and attain minimum depths of well over 100 km (62 mi) in a few decades beneath both
oceanic and
continental lithosphere.
[24]
Exploration can also be aided through computer simulations of the evolution of the mantle. In 2009, a
supercomputer application provided new insight into the distribution of mineral deposits, especially
isotopes of iron, from when the mantle developed 4.5 billion years ago.
[
Like all the other
terrestrial planets, (Mercury, Venus, and Mars) the Earth is made up of many layers. This is the result of it undergoing planetary differentiation, where denser materials sink to the center to form the core while lighter materials form around the outside. Whereas the core is composed primarily of iron and nickel, Earth’s upper layer are composed of silicate rock and minerals.
This region is known as the mantle, and accounts for the vast majority of the Earth’s volume. Movement, or convection, in this layer is also responsible for all of Earth’s volcanic and seismic activity. Information about structure and composition of the mantle is either the result of geophysical investigation or from direct analysis of rocks derived from the mantle, or exposed mantle on the ocean floor.
Definition:
Composed of silicate rocky material with an average thickness of 2,886 kilometres (1,793 mi), the mantle sits between the Earth’s crust and its upper core. The mantle makes up 84% of the Earth by volume, compared to 15% in the core and the remainder being taken up by the crust. While it is predominantly solid, it behaves like a viscous fluid due to the fact that temperatures are close to the melting point in this layer.
Our knowledge of the upper mantle, including the tectonic plates, is derived from analyses of earthquake waves; heat flow, magnetic, and gravity studies; and laboratory experiments on rocks and minerals. Between 100 and 200 kilometers below the Earth’s surface, the temperature of the rock is near the melting point; molten rock erupted by some volcanoes originates in this region of the mantle.
Structure and Composition:
The mantle is divided into sections which are based upon results from seismology. These are the upper mantle, which extends from about 7 to 35 km (4.3 to 21.7 mi) from the surface down to a depth of 410 km (250 mi); the transition zone, which extends from 410 t0 660 km (250 – 410 mi); the lower mantle, which reaches from 660 km to a depth of 2,891 km (410 – 1,796 mi); and the the core-mantle boundary, which has a variable thickness (~200 km or 120 mi on average).
In the upper mantle two main zones are distinguished. The innermost of these is the inner asthenosphere, which is composed of plastic flowing rock of that averages about 200 km (120 mi) in thickness. The outer zone is the lowermost part of the lithosphere, which is composed of rigid rock and is about 50 to 120 km (31 to 75 mi) thick.
The upper part of the lithosphere is the Earth’s crust, a thin layer that is about 5 to 75 km (3.1 to 46.6 mi) thick, which is separated from the mantle by the Mohorovicic discontinuity (or “Moho”, which is defined by a sharp increase downward in the speed of earthquake waves).
In some places under the ocean, the mantle is actually exposed. There are also a few places on land where mantle rock has been pushed to the surface by tectonic activity, most notably the Tablelands region of Gros Morne National Park in Newfoundland and Labrador, Canada, St. John’s Island, Egypt, or the island of Zabargad in the Red Sea.
In terms of its constituent elements, the mantle is made up of 44.8% oxygen, 21.5% silicon, and 22.8% magnesium. There’s also iron, aluminum, calcium, sodium, and potassium. These elements are all bound together in the form of silicate rocks, all of which take the form of oxides. The most common is Silicon dioxide (SiO2) at 48%, followed by Magnesium Oxide (MgO) at 37.8%. Examples of rocks that you might find inside the mantle include: olivine, pyroxenes, spinel, and garnet.
Convection:
Because of the temperature difference between the Earth’s surface and outer core, there is a convective material circulation in the mantle. This consists of the slow, creeping motion of the Earth’s silicate mantle across the surface, carrying heat from the interior of the Earth to the surface. Whereas hot material rises to the surface, cooler, heavier material sinks beneath.
The lithosphere is divided into a number of plates that are continuously being created and consumed at their opposite plate boundaries. Downward motion of material occurs in subduction zones, locations at convergent plate boundaries where one mantle layer moves under another. Accretion occurs as material is added to the growing edges of a plate, associated with seafloor spreading.
This chaotic process is believed to be an integral part of the motion of plates, which in turn gives rise to continental drift. Subducted oceanic crust is also what gives rise to volcanism, as demonstrated by the
Pacific Ring of Fire.
Exploration:
Scientific investigations and exploration of the mantle is generally conducted on the seabed due to the relative thickness of the oceanic crust compared to the continental crust. The first attempt at mantle exploration (known as Project Mohole) achieved a deepest penetration of approximately 180 meters (590 feet). It was abandoned in 1966 after repeated failures and cost over-runs.
In 2005, the ocean drilling vessel JOIDES Resolution achieved a borehole that was 1,416 meters (4,646 ft) in depth below the sea floor. In 2007, a team of scientists aboard the UK research ship RRS James Cook conducted a study on an exposed section of mantle located between the Cape Verdr Islands and the Caribbean Sea.
In recent years, a method of exploring the Earth’s layers was proposed using a small, dense, heat-generating probe. This would melt its way through the crust and mantle and communicate via acoustic signals generated by its penetration of the rocks. The probe would consist of an outer shell of tungsten with a core of cobalt-60, which acts as a radioactive heat source.
It was calculated that such a probe will reach the oceanic Moho in less than 6 months and attain minimum depths of well over 100 km (62 mi) in a few decades beneath both oceanic and continental lithosphere. In 2009, a supercomputer application created a simulation that provided new insight into the distribution of mineral deposits from when the mantle developed 4.5 billion years ago.
While the Earth’s mantle has yet to be explored at any significant depth, much has been learned from indirect studies over the past few centuries. As human exploration of the Solar System continues, we are sure to learn more about terrestrial planets, their geological behavior, and their formation.
Is the Earth’s mantle made of liquid magma?
The Earth’s mantle, on which the crust is lying on, is not made of liquid magma. It is not even made of
magma. The Earth’s mantle is mostly made of solid rock. The misconception of a liquid mantle arises from expressions like “a subducted tectonic plate sinks into the mantle” or “continental drift”, expressions that implicitly refer to the liquid element.
The Earth’s mantle is mostly solid from the liquid outer core to the crust, but it can creep on the long-term, which surely strengthens the misconception of a liquid mantle.
What is Earth made of?
The Earth is made out of many things. Deep inside Earth, near its center, lies Earth's core which is mostly made up of nickel and iron. Above the core is Earth's mantle, which is made up of rock containing silicon, iron, magnesium, aluminum, oxygen and other minerals. The rocky surface layer of Earth, called the crust, is made up of mostly oxygen, silicon, aluminum, iron, calcium, sodium, potassium and magnesium. Earth's surface is mainly covered with liquid water and its atmosphere is is mainly nitrogen and oxygen, with smaller amounts of carbon dioxide, water vapor and other gases.
The internal structure of Earth
Mantle convection
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The Earth's surface
lithosphere rides atop the
asthenosphere and the two form the components of the
upper mantle. The lithosphere is divided into a number of
plates that are continuously being created and consumed at their opposite
plate boundaries. Accretion occurs as mantle is added to the growing edges of a plate, associated with
seafloor spreading. This hot added material cools down by
conduction and
convection of heat. At the consumption edges of the plate, the material has thermally contracted to become dense, and it sinks under its own weight in the process of
subduction usually at an
ocean trench.
[3]
The subducted oceanic crust triggers
volcanism, although the basic mechanisms are varied. Volcanism may occur due to processes that add buoyancy to partially melted mantle, which would cause upward flow of the partial melt due to decrease in its density. Secondary convection may cause surface volcanism as a consequence of intraplate extension
[6] and
mantle plumes.
[7]
Types of convection[edit]
Earth cross-section showing location of upper (3) and lower (5) mantle
Earth's temperature vs depth. Dashed curve: layered mantle convection. Solid curve: whole-mantle convection.
[7]
During the late 20th century, there was significant debate within the geophysics community as to whether convection is likely to be "layered" or "whole".
[10][11] Although elements of this debate still continue, results from
seismic tomography, numerical simulations of mantle convection and examination of Earth's gravitational field are all beginning to suggest the existence of 'whole' mantle convection, at least at the present time. In this model, cold, subducting oceanic lithosphere descends all the way from the surface to the core–mantle boundary (CMB) and hot plumes rise from the CMB all the way to the surface.
[12] This picture is strongly based on the results of global seismic tomography models, which typically show slab and plume-like anomalies crossing the mantle transition zone.
Although it is now well accepted that subducting slabs cross the mantle transition zone and descend into the lower mantle, debate about the existence and continuity of
plumes persists, with important implications for the style of mantle convection. This debate is linked to the controversy regarding whether intraplate volcanism is caused by shallow,
upper-mantle processes or by
plumes from the lower mantle.
[6]Many geochemistry studies have argued that the lavas erupted in intraplate areas are different in composition from shallow-derived
mid-ocean ridge basalts (MORB). Specifically, they typically have elevated Helium-3 – Helium-4 ratios. Being a primordial nuclide, Helium-3 is not naturally produced on earth. It also quickly escapes from earth's atmosphere when erupted. The elevated He-3/He-4 ratio of Ocean Island Basalts (OIBs) suggest that they must be sources from a part of the earth that has not previously been melted and reprocessed in the same way as MORB source has been. This has been interpreted as their originating from a different, less well-mixed, region, suggested to be the lower mantle. Others, however, have pointed out that geochemical differences could indicate the inclusion of a small component of near-surface material from the lithosphere.
Planform and vigour of convection[edit]
On Earth, the
Rayleigh number for convection within Earth's mantle is estimated to be of order 10
7, which indicates vigorous convection. This value corresponds to whole mantle convection (i.e. convection extending from the Earth's surface to the border with the
core). On a global scale, surface expression of this convection is the tectonic plate motions, and therefore has speeds of a few cm/a.
[13][14][15] Speeds can be faster for small-scale convection occurring in low-viscosity regions beneath the lithosphere, and slower in the lowermost mantle where viscosities are larger. A single shallow convection cycle takes on the order of 50 million years, though deeper convection can be closer to 200 million years.
[16]
Currently, whole mantle convection is thought to include broad-scale downwelling beneath the Americas and the Western Pacific, both regions with a long history of subduction, and upwelling flow beneath the central Pacific and Africa, both of which exhibit
dynamic topographyconsistent with upwelling.
[17] This broad-scale pattern of flow is also consistent with the tectonic plate motions, which are the surface expression of convection in the Earth's mantle and currently indicate degree-2 convergence toward the western Pacific and the Americas, and divergence away from the central Pacific and Africa.
[18] The persistence of net tectonic divergence away from Africa and the Pacific for the past 250 Myr indicates the long-term stability of this general mantle flow pattern,
[18] and is consistent with other studies
[19][20][21] that suggest long-term stability of the
LLSVP regions of the lowermost mantle that form the base of these upwellings.
Creep in the mantle[edit]
Since the mantle is primarily composed of olivine ((Mg,Fe)2SiO4), the rheological characteristics of the mantle are largely those of olivine. Additionally, due to the varying temperatures and pressures between the lower and upper mantle, a variety of creep processes can occur with dislocation creep dominating in the lower mantle and diffusional creep occasionally dominating in the upper mantle. However, there is a large transition region in creep processes between the upper and lower mantle and even within each section, creep properties can change strongly with location and thus temperature and pressure. In the power law creep regions, the creep equation fitted to data with n = 3–4 is standard.
[22]
The strength of olivine not only scales with its melting temperature, but also is very sensitive to water and silica content. The solidus depression by impurities, primarily Ca, Al, and Na, and pressure affects creep behavior and thus contributes to the change in creep mechanisms with location. While creep behavior is generally plotted as homologous temperature versus stress, in the case of the mantle it is often more useful to look at the pressure dependence of stress. Though stress is simple force over area, defining the area is difficult in geology. Equation 1 demonstrates the pressure dependence of stress. Since it is very difficult to simulate the high pressures in the mantle (1MPa at 300–400 km), the low pressure laboratory data is usually extrapolated to high pressures by applying creep concepts from metallurgy.
[23]
Most of the mantle has homologous temperatures of 0.65–0.75 and experiences strain rates of
per second. Stresses in mantle are dependent on density, gravity, thermal expansion coefficients, temperature differences driving convection, and distance convection occurs over, all of which give stresses around a fraction of 3-30MPa. Due to the large grain sizes (at low stresses as high as several mm), it is unlikely that Nabarro-Herring (NH) creep truly dominates. Given the large grain sizes, dislocation creep tends to dominate. 14 MPa is the stress below which diffusional creep dominates and above which power law creep dominates at 0.5Tm of olivine. Thus, even for relatively low temperatures, the stress diffusional creep would operate at is too low for realistic conditions. Though the power law creep rate increases with increasing water content due to weakening, reducing activation energy of diffusion and thus increasing the NH creep rate, NH is generally still not large enough to dominate. Nevertheless, diffusional creep can dominate in very cold or deep parts of the upper mantle. Additional deformation in the mantle can be attributed to transformation enhanced ductility. Below 400 km, the olivine undergoes a pressure induced phase transformation into spinel and can cause more deformation due to the increased ductility.
[23] Further evidence for the dominance of power law creep comes from preferred lattice orientations as a result of deformation. Under dislocation creep, crystal structures reorient into lower stress orientations. This does not happen under diffusional creep, thus observation of preferred orientations in samples lends credence to the dominance of dislocation creep.
[24]
Mantle convection in other celestial bodies[edit]
A similar process of slow convection probably occurs (or occurred) in the interiors of other planets (e.g.,
Venus,
Mars) and some satellites (e.g.,
Europa, Enceladus).
There are three great categories of rocks: igneous, sedimentary, and metamorphic. Most of the time, they're simple to tell apart. They are all connected in the endless rock cycle, moving from one form to another and changing shape, texture, and even chemical composition along the way. Igneous rocks form from the
cooling of magmaor lava and compose much of the Earth's continental crust and nearly all of the oceanic crust.
Identifying Igneous Rocks
The key concept about all igneous rocks is that they were once hot enough to melt. The following traits are all related to that.
- Because their mineral grains grew together tightly as the melt cooled, they are relatively strong rocks.
- They're made of primary minerals that are mostly black, white, or gray. Any other colors they may have are pale in shade.
- Their textures generally look like something that was baked in an oven. The even texture of coarse-grained granite is familiar from building stones or kitchen counters. Fine-grained lava may look like black bread (including gas bubbles) or dark peanut brittle (including larger crystals).
Origin
Igneous rocks (derived from the Latin word for fire,
ignis) can have very different mineral backgrounds, but they all share one thing in common: they formed by the cooling and crystallization of a melt. This material may have been lava erupted at the Earth's surface, or
magma (unerupted lava) at depths of up to a few kilometers, known as magma in deeper bodies.
Those three different settings create three main types of igneous rocks. Rock formed of lava is called extrusive, rock from shallow magma is called intrusive, and rock from deep magma is called plutonic. The deeper the magma, the slower it cools, and it forms larger mineral crystals.
Where They Form
Igneous rocks form at four main places on Earth:
- At divergent boundaries, like mid-ocean ridges, plates drift apart and form gaps that are filled by magma.
- Subduction zones occur whenever a dense oceanic plate is subducted underneath another oceanic or continental plate. Water from the descending oceanic crust lowers the melting point of the above mantle, forming magma that rises to the surface and forms volcanoes.
- At continental-continental convergent boundaries, large landmasses collide, thickening and heating the crust to melting.
- Hot spots, like Hawaii, form as the crust moves over a thermal plume rising from deep in the Earth. Hot spots form extrusive igneous rocks.
People commonly think of lava and magma as a liquid, like molten metal, but geologists find that magma is usually a mush — a partially-melted fluid loaded with mineral crystals. As it cools, magma crystallizes into a series of minerals, some of which crystallize sooner than others. As the minerals crystallize, they leave the remaining magma with a changed chemical composition. Thus, a body of magma evolves as it cools and also as it moves through the crust, interacting with other rocks.
Once magma erupts as lava, it freezes quickly and preserves a record of its history underground that geologists can decipher. Igneous petrology is a very complex field, and this article is only a bare outline.
Textures
The three types of igneous rocks differ in their
textures, starting with the size of their mineral grains.
- Extrusive rocks cool quickly (over periods of seconds to months) and have invisible or microscopic grains or an aphanitic texture.
- Intrusive rocks cool more slowly (over thousands of years) and have visible grains of small to medium-size, or phaneritic texture.
- Plutonic rocks cool over millions of years and can have grains as large as pebbles — even meters across.
Because they solidified from a fluid state, igneous rocks tend to have a uniform fabric without layers, and the mineral grains are packed together tightly. Think of the texture of something you would bake in the oven.
In many igneous rocks, large mineral crystals "float" in a fine-grained groundmass. The large grains are called phenocrysts, and rock with phenocrysts is called a porphyry — that is, it has a porphyritic texture. Phenocrysts are minerals that solidified earlier than the rest of the rock, and they are important clues to the rock's history.
Some extrusive rocks have distinctive textures.
- Obsidian, formed when lava hardens quickly, has a glassy texture.
- Pumice and scoria are volcanic froth, puffed up by millions of gas bubbles that give them a vesicular texture.
- Tuff is a rock made entirely of volcanic ash, fallen from the air or avalanched down a volcano's sides. It has a pyroclastic texture.
- Pillow lava is a lumpy formation created by extruding lava underwater.
Basalt, Granite, and More
Igneous rocks are classified by the minerals they contain. The main minerals in igneous rocks are hard, primary ones: feldspar, quartz, amphiboles, and pyroxenes (together called "dark minerals" by geologists), as well as olivine, along with the softer mineral mica. The two best-known igneous rock types are basalt and granite, which have distinctly different compositions and textures.
Basalt is the dark, fine-grained stuff of many lava flows and magma intrusions. Its dark minerals are rich in magnesium (Mg) and iron (Fe), hence basalt is called a "mafic" rock. It can be either extrusive or intrusive.
Granite is the light, coarse-grained rock formed at a depth that is exposed after deep erosion. It is rich in feldspar and quartz (silica) and hence is called a "felsic" rock. Therefore, granite is felsic and plutonic.
Basalt and granite account for the great majority of igneous rocks. Ordinary people, even ordinary geologists, use the names freely. Stone dealers call any plutonic rock "granite." But igneous petrologists use many more names. They generally talk about
basaltic and
granitic or
granitoid rocks among themselves and out in the field, because it takes laboratory work to determine an exact rock type according to the official
classifications. True granite and true basalt are narrow subsets of these categories.
A few of the less common igneous rock types can be recognized by non-specialists. For instance, a dark-colored plutonic mafic rock, the deep version of basalt, is called gabbro. A light-colored intrusive or extrusive felsic rock, the shallow version of granite, is called felsite or rhyolite. And there is a suite of ultramafic rocks with even more dark minerals and even less silica than basalt. Peridotite is the foremost of those.
Where Igneous Rocks Are Found
The deep seafloor (the oceanic crust) is made almost entirely of basaltic rocks, with peridotite underneath in the
mantle. Basalts are also erupted above the Earth's great subduction zones, either in volcanic island arcs or along the edges of continents. However, continental magmas tend to be less basaltic and more granitic.
The continents are the exclusive home of granitic rocks. Nearly everywhere on the continents, no matter what rocks are on the surface, you can drill down and reach granitoid eventually. In general, granitic rocks are less dense than basaltic rocks, and thus the continents float higher than the oceanic crust on top of the ultramafic rocks of the Earth's mantle. The behavior and histories of granitic rock bodies are among geology's deepest and most intricate mysteries.
The Mantle
The Mantle is the second layer of the Earth. It is the biggest and takes up 84 percent of the Earth. In this section you will learn and more about how hot the mantle is, what it is made of, and someinteresting facts about the Mantle.
Sections
The mantle is divided into two sections. The Asthenosphere, the bottom layer of the mantle made of plastic like fluid and The Lithosphere the top part of the mantle made of a cold dense rock.
Temperature
The average temperature of the mantle is 3000° Celsius. The temperature of the mantle will become much hotter as you get closer to the Inner Core
The mantle is composed of silicates of iron and magnesium, sulphides and oxides of silicon and magnesium.
Thickness
The mantle is about 2900 km thick. It is the largest layer of the Earth, taking up 84% of the Earth.
Convection Currents
Convection currents happen inside the mantle and are caused by the continuous circular motion of rocks in the lithosphere being pushed down by hot molasses liquid from the asthenosphere. The rocks then melt and float up as molasses liquid because it is less dense and the rocks float down because it is more dense.
Crust
The Crust is our home, yet it is also not our home. The very top of the crust is where we live on but deeper down it is all dense rock and metal ores. In this section you will learn about what the Crust is made of, the temperature, the thickness and a few interesting facts about the crust.
The Crust is composed of mainly granite, basalt, and diorite rocks
Thickness
The Crust's thickness can vary from wherever you are. From a continent to the edge of the crust is about 60 km. From the bottom of the ocean to the edge of the crust is about 10 km.
Temperature
The Crust's temperature is different throughout the entire crust. The temperatures start at about 200° Celsius and can rise up to 400° Celsius.
The Always Moving Layer
In the Mantle there are Convection Currents which will be defined more in The Mantle section. These huge currents are causing the crust to constantly move. These movements will cause earthquakes and volcanoes to erupt. The moving of the crust is also known as The Theory Of Plate Tectonics.
The Lithosphere
The Lithosphere is the top half of the mantle. It is a cold dense rock. This rock will be forced into the liquid in the asthenosphere causing it to melt and be pushed back up again causing the melted rock to cool off and return to normal rock. This is called
Convection Currents.
The Asthenosphere is the bottom half of the mantle. It is a hot plastic liquid that is a liquid molasses like substance. This hot molasses substance will be forced into the
lithosphere causing the liquid to cool off into rock, only to be forced back into the asthenosphere causing the rock to melt. This is called
Convection Currents.
The Outer Core
The Outer Core is the second to last layer of the Earth. It is a magma like liquid layer that surrounds the Inner Core and creates Earth's magnetic field. In this section you will learn about how Earth's magnetic field is created, how hot it is, how thick the Outer Core is and a few interesting facts about the Outer Core.
Temperature
The Outer Core is about 4000-5000 degrees Celsius. The Inner Core is so hot it causes all the metal in the Outer Core to melt into liquid magma.
The Outer Core is composed of iron and some nickel. There is very few rocks and iron and nickel ore left in the Outer Core because of the Inner Core melting all the metal into liquid magma
Thickness
The Outer Core is about 2200 km thick. It is the second largest layer and made entirely out of liquid magma.
Magnetism
Because the outer core moves around the inner core, Earth's magnetism is created.
The Inner Core
The Inner Core is the final layer of the Earth. It is a solid ball made of metal. To learn about what metal the Inner Core is made of, read this section about the Inner Core. You can also learn how hot the Inner Core is, how thick it is and some interesting facts about the Inner Core.
Thickness
The Inner Core is about 1250 km thick and is the second smallest layer of the Earth. Although it is one of the smallest, the Inner Core is also the hottest layer.
The Inner Core is a solid ball composed of an element named NiFe. Ni for Nickel and Fe for Ferrum also known as Iron.
Temperature
The Inner Core is about 5000-6000 degrees Celsius. It melts all metal ores in the Outer Core causing it to turn into liquid magma.
Theory Of Continental Drift
Alfred Wegner, A German Scientist, one day called his girlfriend and told her that the East edge of Africa looks like the Southwest/West edge of South America. He then let everyone know about his discovery, starting the Theory of Continental Drift.
Pangaea
Alfred Wegner was determined to prove to the world that the world was once a super continent called Pangea. He estimated that Pangaea existed around 245 million years ago around the Triassic Period. He believed that all continents fit together like puzzle pieces but eventually drifted apart creating today's continent formation.
Evidence Of Continental Drift
As the years went by, some scientists said that Pangaea could not have happened. The thought that every continent was at one time together is insane! Alfred knew he was right, he just had to prove it.
Plant And Animal Fossils
Plant fossils and animal fossils were a big part of Alfred's evidence. He found plant fossils that could only be found on land, in the middle of the ocean. He also discovered that there were the same animal fossils in North America and in Russia that could not swim, in both parts of the world.
Rock Formations
Alfred found that the rock in the Appalachian Mountains in North America is the same kind of rock found in a mountain range in Britain and Norway.
Earthquakes
Believe it or not, the ground is moving under you right this second!
Every day the crust's Tectonic Plates are moving in all different directions, causing them to force one another under them, rip apart, or rip off chunks as they move past each other. This section is on earthquakes, everything you will need to know about how they work.
Seismology
Seismology is the study of earthquakes. Seism, the Romanian word for earthquake and ology meaning the study of.
Seismographs
The word seismograph derives from the greek words seismós meaning shaking, or in other words, earthquakes and gráphō, meaning draw.
Seismographs measure and record the movement of the crust. After measuring and recording from at least 3 seismographs the epicentre of the earthquake can be found. The Richter Scale though, measures the Magnitude of an earthquake. Magnitude is the power of the earthquake.
Seismic Wave
Seismic waves are the waves released by a rock or plate after they break. When a rock or seismic wave plate breaks, it releases energy called seismic waves. There are three types of Seismic Waves each with is own unique characteristics.
Primary Waves
Primary waves are the fastest and least felt of all earthquakes. Although they are the least felt they can make dishes rattle, and make a warning sign as to the bigger waves to come. These waves can also travel through any state of matter on earth.
Secondary Waves
Secondary waves are slower then Primary waves and again is used as a warning sign. Unlike Primary waves, Secondary waves can not travel through solids or liquids.
Surface Waves
Surface waves are the slowest out of all three waves but they are also the strongest. These huge waves travel in a rolling motion ripping up the ground a causing buildings to crumble.
Ring Of Fire
The Ring Of Fire is where a lot of the plate boundaries are. Because of this there are many earthquakes going on and lots of volcanoes being formed.
Normal Fault
Normal faults occur at
divergent boundaries. When this type of fault happens one of the two plates moving apart will suddenly slide under the earth causing an earthquake.
Reverse Fault
Reverse faults occur at
convergent boundaries. This type of fault causes the rock/plate above the fault line to be forced up causing more earthquakes.
Strike Slip Fault
Strike Slip Faults occur at transform boundaries and is caused by edges of a plate sticking out as the plates slide past each other. When the plates get caught on one another they push and pull until eventually the excess rock breaks off causing mass amount of pressure to be released making earthquakes.
Volcanoes
Volcanoes are mountains with craters at the top formed on Hot Spots or Divergent and Subduction Zones. Below that crater is a tube. Within that tube is hot magma flowing through to the top of the volcano. Gases within the volcano heat up, expand and finally cause the volcano to erupt. In this section you will learn about volcanoes, different types and some information about each of them.
Volcanology
Volcanology is the scientific study of volcanoes. Volcan is a word that comes from the Spanish language meaning "Volcano". Ology means "The study of".
Inside Volcano
From the outside a volcano may look like a simple mountain but the inside of a volcano is much different. Inside a volcano is a long tube leading up towards the top filled with lava. This is called a vent. The area in which the magma is held is called a magma reservoir. There are really only two parts to a volcano, the vent and magma reservoir. Although there are only two parts, there are different volcanoes to.
Shield Volcano
A shield volcano is a volcano that is huge in size, but not height. Take the Hawaiian islands for example, the islands are Shield Volcanoes. These volcanoes are mostly produced on plates with Hot Spots below them. Shield Volcanoes are made of lava flows that create a smooth sloped surface. Unlike the other volcanoes, shield volcanoes ooze magma rather than erupt violently.
Cinder Cone Volcanoes
Cinder cone volcanoes are the simplest type of volcano. The cinder cone has a bowl shaped crater and rarely rises more than 1 thousand feet. It is a steep sided volcano made of layers of ash and cinder that is crushed during eruption causing the tiny pieces to fall rapidly towards the ground, therefore creating more steep and rough ground. Unlike other volcanoes the cinder cone has only one vent leading towards the top of the volcano and has a very violent eruption that shoots out ash and lava.
Composite Volcano
Composite volcanoes are made of alternating layers of ash and lava. These volcanoes are a mix of the other two types of volcanoes, therefore it shoots out both lava and ash, along with oozing out magma. Composite volcanoes can have a very violent eruption or a calm ooze of magma. These volcanoes are the biggest in the world. Unlike other volcanoes, the composite has many vents rather than one.
Tsunamis
Earthquakes, believe it or not, can be even more destructive than they already are. When an earthquake appears out at sea the force of the tectonic waves is so powerful it will create a gigantic wave in the water. Not one of those waves that a surfer rides on, this wave is one that floods entire towns and causes many deaths. Tsunamis move towards the shore and slow down as they hit the shore causing water to flood a city and drag many people out to sea.
Tectonic Plate Boundaries
Tectonic plates are the plates beneath us in the mantle that are constantly moving. There are 3 types of tectonic plate boundaries. Divergent, Convergent, and Transform. These plate movements are caused by convection currents in the Mantle.
The Theory Of Plate Tectonics
German Scientist, Alfred Wegner, came up with The Theory Of Continental Drift. This theory soon became the Theory Of Plate Tectonics. The word Tectonic came from the Greek word tektonikos, basically meaning "construction". The word tectonics is talking about the general structure of the Earth.
Convergent Boundaries
A convergent boundary is a type of boundary where two plates meet together and start to push against one another. There are three types of convergent boundaries each with its own consequences.
Oceanic-Continental Convergence
The first type of convergent boundary is Oceanic-Continetal Convergence. This type of convergent boundary happens where an oceanic plate and a continental plate push together causing the oceanic plate to be forced under the continental plate into the mantle because the oceanic plate is thinner. This is called a subduction. When the oceanic plate is pushed under, it melts and turns into hot magma which burns its way through the continental plate, creating a volcano and causing many earthquakes.
Oceanic-Oceanic Convergence
The next type is Oceanic-Oceanic Convergence. This type of convergent boundary happens where two oceanic plates push against one another, causing the colder, denser, older plate to buckle up and sink into the mantle. Hot magma comes from where the plate sank, creating new crust.
Continental-Continental Convergence
The final type of convergent boundary is Continental-Continental Convergence. This type of boundary happens where two continental plates collide and push up creating mountain ranges. Like colliding icebergs resist downward motion, the same thing happens with colliding continental plates, instead of moving down, they move up.
Divergent Boundaries
Divergent boundaries are plates that move away from one another causing underwater volcanoes and the spreading of the seafloor.
The Spreading Seafloor
When divergent plates move they move away from each other. When two oceanic plates move away from each other the seafloor starts to spread apart making more and more and more ground at the bottom of the sea.
Why do they move apart?
Deep in the mantle are huge convection currents. When they move up the plates start to move apart because of the rising convection currents pushing on the bottom of the asthenosphere.
Transform Boundary
A Transform Boundary is a type of boundary that slides past one another instead of colliding or moving apart.
Transform Faults
Transform faults are found on the seafloor and are caused by surges of magma rising to make a ridge that is discontinued after its formed. While this happens the plates move in different directions sliding against each other making earthquakes, big and small. The most famous fault is the San Andreas fault
Minerals
Minerals are chemical elements or compounds that form a rock. There are many minerals in the world. There are so many that some minerals end up looking like each other! Geologists, Scientists who study rocks and minerals, use different tests to identify each mineral. These tests are: Hardness, Crystal Structure, Lustre, Colour, Streak, and Cleavage/Fracture.
Hardenss
Hardness is a mineral test involving Moh's Hardness Scale. The hardness scale measures a minerals resistance to scratching from 1-10, 1 being the softest and 10 being the hardest. Talc is one of the softest materials in the world, its so soft you can scratch it with your fingernail. Diamond is the hardest, only able to be scratched by diamond itself.
Crystal Structure
There are 7 Major Crystal Systems in the world. Crystal systems tell us about the shape of a mineral. The 7 systems are: Cubic, Tetragonal, Orthorhombic, Monoclinic, Triclinic, Hexagonal, and Trigonal. Cubic is in the shape of a cube, Tetragonal is a rectangle, Orthorhombic is a smaller type of rectangle, Monoclinic is even smaller, Triclinic is the smallest rectangle, Hexagonal is in the shape of a hexagon and Trigonal is a mix between a cubic and hexagonal shape.
Lustre
Lustre is a minerals shine. A minerals shine is put into to groups of lustre. Metallic lustre is where a mineral shines like polished metal and Non Metallic lustre is where a mineral does not shine like polished metal. Some examples of non metallic lustre are Waxy: where the mineral feels like wax, Pearly: where the mineral looks like pearl, Silky: where the mineral has a shine like silk, Greasy: it looks as if its covered in oil, Glassy: it has a reflection like glass, and Adamantine: the mineral shines like a diamond.
Color
Color is probably one of the least important mineral tests because there are so many minerals they all look the same! Color, although not very useful, tells us a minerals colour.
Streak
The streak of a mineral is the mark it will leave on an unglazed porcelain tile. The streak will help us identify different minerals because some minerals leave no streak, some leave a white streak and some will leave a coloured streak.
Cleavage And Fracture
Cleavage and Fracture is the test that tells us how a mineral breaks. If a mineral has cleavage it will break in nice smooth edges. If it has fracture then the mineral will break in rough jagged edges. An example of a mineral with cleavage is Mica (My-KA). This mineral breaks in smooth flat planes. An example of fracture is quartz. This mineral breaks in rough jagged edges.
Depends which part of the mantle you are talking about. The outer mantle consists of olivine and pyroxene (both coarse dark green crystalls) with flecs of black chromite. Deeper into the mantle the pressure and temperature conditions cause the minerals to recrystallize to perovskite and spinel. Most probably dark brown or greyish, possibly with red garnet. Deeper still, is so deep that nobody has ever sampled it, and we cannot be sure what the minerals will be. So the short answer is deep green or brownish crystalline rock.
Incidentally, you can visit the Sultanate of Oman where an anomalous raft of mantle material is exposed at the ground surface in what is known as the Semail ophiolite.
- The mantle is the mostly-solid bulk of Earth’s interior. The mantle lies between Earth’s dense, super-heated core and its thin outer layer, the crust. The mantle is about 2,900 kilometers (1,802 miles) thick, and makes up a whopping 84% of Earth’s total volume. As Earth began to take shape about 4.5 billion years ago, iron and nickel quickly separated from otherrocks and minerals to form the core of the new planet. The moltenmaterial that surrounded the core was the early mantle. Over millions of years, the mantle cooled. Water trapped inside minerals erupted with lava, a process called “outgassing.” As more water was outgassed, the mantle solidified. The rocks that make up Earth’s mantle are mostly silicates—a wide variety of compounds that share a silicon and oxygen structure. Common silicates found in the mantle include olivine, garnet, and pyroxene. The other major type of rock found in the mantle is magnesium oxide. Other mantle elements include iron, aluminum, calcium, sodium, and potassium. The temperature of the mantle varies greatly, from 1000° Celsius (1832° Fahrenheit) near itsboundary with the crust, to 3700° Celsius (6692° Fahrenheit) near its boundary with the core. In the mantle, heat and pressuregenerally increase with depth. Thegeothermal gradient is a measurement of this increase. In most places, the geothermal gradient is about 25° Celsius per kilometer of depth (1° Fahrenheit per 70 feet of depth). The viscosity of the mantle also varies greatly. It is mostly solid rock, but more viscous at tectonic plate boundaries and mantle plumes. Mantle rocks there are soft and able to move plastically (over the course of millions of years) at great depth and pressure. The transfer of heat and material in the mantle helps determine the landscape of Earth. Activity in the mantle drives plate tectonics, contributing to volcanoes, seafloor spreading, earthquakes, andorogeny (mountain-building). The mantle is divided into several layers: the upper mantle, the transition zone, the lower mantle, and D” (D double-prime), the strange region where the mantle meets the outer core.
- Upper Mantle The upper mantle extends from the crust to a depth of about 410 kilometers (255 miles). The upper mantle is mostly solid, but its moremalleable regions contribute totectonic activity. Two parts of the upper mantle are often recognized as distinctregions in Earth’s interior: the lithosphere and the asthenosphere. LithosphereThe lithosphere is the solid, outer part of the Earth, extending to a depth of about 100 kilometers (62 miles). The lithosphere includes both the crust and the brittle upper portion of the mantle. The lithosphere is both the coolest and the most rigid of Earth’s layers. The most well-known feature associated with Earth’s lithosphere is tectonic activity. Tectonic activity describes the interaction of the huge slabs of lithosphere calledtectonic plates. The lithosphere is divided into 15 major tectonic plates: the North American, Caribbean, South American, Scotia, Antarctic, Eurasian, Arabian, African, Indian, Philippine, Australian, Pacific, Juan de Fuca, Cocos, and Nazca. The division in the lithosphere between the crust and the mantle is called the Mohorovicic discontinuity, or simply the Moho. The Moho does not exist at a uniform depth, because not all regions of Earth are equally balanced in isostatic equilibrium.Isostasy describes the physical, chemical, and mechanical differences that allow the crust to “float” on the sometimes more malleable mantle. The Moho is found at about 8 kilometers (5 miles) beneath the ocean and about 32 kilometers (20 miles) beneath continents. Different types of rocks distinguishlithospheric crust and mantle. Lithospheric crust is characterized by gneiss (continental crust) and gabbro (oceanic crust). Below the Moho, the mantle is characterized by peridotite, a rock mostly made up of the minerals olivine and pyroxene. AsthenosphereThe asthenosphere is the denser, weaker layer beneath the lithospheric mantle. It lies between about 100 kilometers (62 miles) and 410 kilometers (255 miles) beneath Earth’s surface. The temperature and pressure of the asthenosphere are so high that rocks soften and partly melt, becoming semi-molten. The asthenosphere is much moreductile than either the lithosphere or lower mantle. Ductility measures a solid material’s ability to deform or stretch under stress. The asthenosphere is generally more viscous than the lithosphere, and the lithosphere-asthenosphere boundary (LAB) is the point wheregeologists and rheologists—scientists who study the flow of matter—mark the difference in ductility between the two layers of the upper mantle. The very slow motion of lithospheric plates “floating” on the asthenosphere is the cause of plate tectonics, a process associated with continental drift, earthquakes, the formation of mountains, and volcanoes. In fact, the lava that erupts from volcanicfissures is actually the asthenosphere itself, melted intomagma. Of course, tectonic plates are not really floating, because the asthenosphere is not liquid. Tectonic plates are only unstable at their boundaries and hot spots.
- Transition Zone From about 410 kilometers (255 miles) to 660 kilometers (410 miles) beneath Earth’s surface, rocks undergo radicaltransformations. This is the mantle’s transition zone. In the transition zone, rocks do not melt or disintegrate. Instead, theircrystalline structure changes in important ways. Rocks become much, much more dense. The transition zone prevents large exchanges of material between the upper and lower mantle. Some geologists think that the increased density of rocks in the transition zone prevents subducted slabs from the lithosphere from falling further into the mantle. These huge pieces of tectonic plates stall in the transition zone for millions of years before mixing with other mantle rock and eventually returning to the upper mantle as part of the asthenosphere, erupting as lava, becoming part of the lithosphere, or emerging as new oceanic crust at sites of seafloor spreading. Some geologists and rheologists, however, think subducted slabs can slip beneath the transition zone to the lower mantle. Other evidence suggests that the transition layer ispermeable, and the upper and lower mantle exchange some amount of material. WaterPerhaps the most important aspectof the mantle’s transition zone is itsabundance of water. Crystals in the transition zone hold as much water as all the oceans on Earth’s surface. Water in the transition zone is not “water” as we know it. It is not liquid, vapor, solid, or even plasma. Instead, water exists as hydroxide.Hydroxide is an ion of hydrogen and oxygen with a negative charge. In the transition zone, hydroxide ions are trapped in the crystalline structure of rocks such as ringwoodite and wadsleyite. These minerals are formed from olivine at very high temperatures and pressure. Near the bottom of the transition zone, increasing temperature and pressure transform ringwoodite and wadsleyite. Their crystal structures are broken and hydroxide escapes as “melt.” Melt particles flow upwards, toward minerals that can hold water. This allows the transition zone to maintain a consistent reservoir of water. Geologists and rheologists think that water entered the mantle from Earth’s surface during subduction.Subduction is the process in which a dense tectonic plate slips or melts beneath a more buoyant one. Most subduction happens as an oceanic plate slips beneath a less-dense plate. Along with the rocks and minerals of the lithosphere, tons of water and carbon are also transported to the mantle. Hydroxide and water are returned to the upper mantle, crust, and even atmosphere through mantle convection, volcanic eruptions, and seafloor spreading.
- Lower Mantle The lower mantle extends from about 660 kilometers (410 miles) to about 2,700 kilometers (1,678 miles) beneath Earth’s surface. The lower mantle is hotter and denser than the upper mantle and transition zone. The lower mantle is much less ductile than the upper mantle and transition zone. Although heat usually corresponds to softening rocks, intense pressure keeps the lower mantle solid. Geologists do not agree about the structure of the lower mantle. Some geologists think that subducted slabs of lithosphere have settled there. Other geologists think that the lower mantle is entirely unmoving and does not even transfer heat by convection.
- D Double-Prime (D’’) Beneath the lower mantle is a shallow region called D'', or “d double-prime.” In some areas, D’’ is a nearly razor-thin boundary with the outer core. In other areas, D’’ has thick accumulations of iron and silicates. In still other areas, geologists and seismologists have detected areas of huge melt. The unpredictable movement of materials in D’’ is influenced by the lower mantle and outer core. The iron of the outer core influences the formation of a diapir, a dome-shaped geologic feature (igneous intrusion) where more fluidmaterial is forced into brittle overlying rock. The iron diapir emits heat and may release a huge, bulging pulse of either material or energy—just like a Lava Lamp. This energy blooms upward, transferring heat to the lower mantle and transition zone, and maybe even erupting as a mantle plume. At the base of the mantle, about 2,900 kilometers (1,802 miles) below the surface, is the core-mantle boundary, or CMB. This point, called the Gutenberg discontinuity, marks the end of the mantle and the beginning of Earth’s liquid outer core.
- Mantle Convection Mantle convection describes the movement of the mantle as it transfers heat from the white-hot core to the brittle lithosphere. The mantle is heated from below, cooled from above, and its overall temperature decreases over long periods of time. All these elements contribute to mantle convection. Convection currents transfer hot, buoyant magma to the lithosphere at plate boundaries and hot spots.Convection currents also transfer denser, cooler material from the crust to Earth’s interior through the process of subduction. Earth's heat budget, which measures the flow of thermalenergy from the core to the atmosphere, is dominated by mantle convection. Earth’s heat budget drives most geologic processes on Earth, although its energy output is dwarfed by solar radiation at the surface. Geologists debate whether mantle convection is “whole” or “layered.”Whole-mantle convectiondescribes a long, long recycling process involving the upper mantle, transition zone, lower mantle, and even D’’. In this model, the mantle convects in a single process. A subducted slab of lithosphere may slowly slip into the upper mantle and fall to the transition zone due to its relative density and coolness. Over millions of years, it may sink further into the lower mantle. Convection currents may then transport the hot, buoyant material in D’’ back through the other layers of the mantle. Some of that material may even emerge as lithosphere again, as it is spilled onto the crust through volcanic eruptions or seafloor spreading. Layered-mantle convectiondescribes two processes. Plumes of superheated mantle material may bubble up from the lower mantle and heat a region in the transition zone before falling back. Above the transition zone, convection may be influenced by heat transferred from the lower mantle as well as discreteconvection currents in the upper mantle driven by subduction and seafloor spreading. Mantle plumes emanating from the upper mantle may gush up through the lithosphere as hot spots. Mantle PlumesA mantle plume is an upwelling of superheated rock from the mantle. Mantle plumes are the likely cause of “hot spots,” volcanic regions not created by plate tectonics. As a mantle plume reaches the upper mantle, it melts into a diapir. This molten material heats the asthenosphere and lithosphere, triggering volcanic eruptions. These volcanic eruptions make a minor contribution to heat loss from Earth’s interior, although tectonic activity at plate boundaries is the leading cause of such heat loss. The Hawaiian hot spot, in the middle of the North Pacific Ocean, sits above a likely mantle plume. As the Pacific plate moves in a generally northwestern motion, the Hawaiian hot spot remains relatively fixed. Geologists think this has allowed the Hawaiian hot spot to create a series of volcanoes, from the 85-million-year-old Meiji Seamount near Russia’s Kamchatka Peninsula, to the Loihi Seamount, a submarine volcano southeast of the “Big Island” of Hawaii. Loihi, a mere 400,000 years old, will eventually become the newest Hawaiian island. Geologists have identified two so-called “superplumes.” These superplumes, or large low shear velocity provinces (LLSVPs), have their origins in the melt material of D’’. The Pacific LLSVP influences geology throughout most of the southern Pacific Ocean (including the Hawaiian hot spot). The African LLSVP influences the geology throughout most of southern and western Africa. Geologists think mantle plumes may be influenced by many different factors. Some may pulse, while others may be heated continually. Some may have a single diapir, while others may have multiple “stems.” Some mantle plumes may arise in the middle of a tectonic plate, while others may be “captured” by seafloor spreading zones. Some geologists have identified more than a thousand mantle plumes. Some geologists think mantle plumes don’t exist at all. Until tools and technology allow geologists to more thoroughly explore the mantle, the debate will continue.
- Exploring the Mantle The mantle has never been directly explored. Even the mostsophisticated drilling equipmenthas not reached beyond the crust. Drilling all the way down to the Moho (the division between the Earth's crust and mantle) is an important scientific milestone, but despite decades of effort, nobody has yet succeeded. In 2005, scientists with the Integrated Ocean Drilling Project drilled 1,416 meters (4,644 feet) below the North Atlantic seafloor and claimed to have come within just 305 meters (1,000 feet) of the Moho. XenolithsMany geologists study the mantle by analyzing xenoliths. Xenoliths are a type of intrusion—a rock trapped inside another rock. The xenoliths that provide the most information about the mantle are diamonds. Diamonds form under very unique conditions: in the upper mantle, at least 150 kilometers (93 miles) beneath the surface. Above depth and pressure, the carbon crystallizes as graphite, not diamond. Diamonds are brought to the surface in explosive volcanic eruptions, forming “diamond pipes” of rocks called kimberlites and lamprolites. The diamonds themselves are of less interest to geologists than the xenoliths some contain. These intrusions are minerals from the mantle, trapped inside the rock-hard diamond. Diamond intrusions have allowed scientists to glimpse as far as 700 kilometers (435 miles) beneath Earth’s surface—the lower mantle. Xenolith studies have revealed that rocks in the deep mantle are most likely 3-billion-year old slabs of subducted seafloor. The diamond intrusions include water, oceansediments, and even carbon. Seismic WavesMost mantle studies are conducted by measuring the spread of shock waves from earthquakes, calledseismic waves. The seismic waves measured in mantle studies are called body waves, because these waves travel through the body of the Earth. The velocity of body waves differs with density, temperature, and type of rock. There are two types of body waves: primary waves, or P-waves, and secondary waves, or S-waves. P-waves, also called pressure waves, are formed by compressions. Sound waves are P-waves—seismic P-waves are just far too low a frequency for people to hear.S-waves, also called shear waves, measure motion perpendicular to the energy transfer. S-waves are unable to transmit through fluids or gases. Instruments placed around the world measure these waves as they arrive at different points on the Earth’s surface after an earthquake. P-waves (primary waves) usually arrive first, while s-waves arrive soon after. Both body waves “reflect” off different types of rocks in different ways. This allows seismologists to identify different rocks present in Earth’s crust and mantle far beneath the surface. Seismic reflections, for instance, are used to identify hidden oil deposits deep below the surface. Sudden, predictable changes in the velocities of body waves are called “seismic discontinuities.” The Moho is a discontinuity marking the boundary of the crust and upper mantle. The so-called “410-kilometer discontinuity” marks the boundary of the transition zone. The Gutenberg discontinuity is more popularly known as the core-mantle boundary (CMB). At the CMB, S-waves, which can’t continue in liquid, suddenly disappear, and P-waves are strongly refracted, or bent. This alerts seismologists that the solid and molten structure of the mantle has given way to the fiery liquid of the outer core. Mantle MapsCutting-edge technology has allowed modern geologists and seismologists to produce mantle maps. Most mantle maps display seismic velocities, revealing patterns deep below Earth’s surface. Geoscientists hope that sophisticated mantle maps can plot the body waves of as many as 6,000 earthquakes withmagnitudes of at least 5.5. These mantle maps may be able to identify ancient slabs of subducted material and the precise position and movement of tectonic plates. Many geologists think mantle maps may even provide evidence for mantle plumes and their structure.
Whole-mantle convection
The Earth's surface
lithosphere rides atop the
asthenosphere and the two form the components of the
upper mantle. The lithosphere is divided into a number of
plates that are continuously being created and consumed at their opposite
plate boundaries. Accretion occurs as mantle is added to the growing edges of a plate, associated with
seafloor spreading. This hot added material cools down by
conduction and
convection of heat. At the consumption edges of the plate, the material has thermally contracted to become dense, and it sinks under its own weight in the process of
subduction usually at an
ocean trench.
[3]
The subducted oceanic crust triggers
volcanism, although the basic mechanisms are varied. Volcanism may occur due to processes that add buoyancy to partially melted mantle, which would cause upward flow of the partial melt due to decrease in its density. Secondary convection may cause surface volcanism as a consequence of intraplate extension
[6] and
mantle plumes.
[7]
Types of convectionEdit
Earth cross-section showing location of upper (3) and lower (5) mantle
Earth's temperature vs depth. Dashed curve: layered mantle convection. Solid curve: whole-mantle convection.
[7]
During the late 20th century, there was significant debate within the geophysics community as to whether convection is likely to be "layered" or "whole".
[10][11] Although elements of this debate still continue, results from
seismic tomography, numerical simulations of mantle convection and examination of Earth's gravitational field are all beginning to suggest the existence of 'whole' mantle convection, at least at the present time. In this model, cold, subducting oceanic lithosphere descends all the way from the surface to the core–mantle boundary (CMB) and hot plumes rise from the CMB all the way to the surface.
[12] This picture is strongly based on the results of global seismic tomography models, which typically show slab and plume-like anomalies crossing the mantle transition zone.
Although it is now well accepted that subducting slabs cross the mantle transition zone and descend into the lower mantle, debate about the existence and continuity of
plumes persists, with important implications for the style of mantle convection. This debate is linked to the controversy regarding whether intraplate volcanism is caused by shallow,
upper-mantle processes or by
plumes from the lower mantle.
[6]Many geochemistry studies have argued that the lavas erupted in intraplate areas are different in composition from shallow-derived
mid-ocean ridge basalts (MORB). Specifically, they typically have elevated Helium-3 – Helium-4 ratios. Being a primordial nuclide, Helium-3 is not naturally produced on earth. It also quickly escapes from earth's atmosphere when erupted. The elevated He-3/He-4 ratio of Ocean Island Basalts (OIBs) suggest that they must be sources from a part of the earth that has not previously been melted and reprocessed in the same way as MORB source has been. This has been interpreted as their originating from a different, less well-mixed, region, suggested to be the lower mantle. Others, however, have pointed out that geochemical differences could indicate the inclusion of a small component of near-surface material from the lithosphere.
Planform and vigour of convectionEdit
On Earth, the
Rayleigh number for convection within Earth's mantle is estimated to be of order 10
7, which indicates vigorous convection. This value corresponds to whole mantle convection (i.e. convection extending from the Earth's surface to the border with the
core). On a global scale, surface expression of this convection is the tectonic plate motions, and therefore has speeds of a few cm/a.
[13][14][15] Speeds can be faster for small-scale convection occurring in low-viscosity regions beneath the lithosphere, and slower in the lowermost mantle where viscosities are larger. A single shallow convection cycle takes on the order of 50 million years, though deeper convection can be closer to 200 million years.
[16]
Currently, whole mantle convection is thought to include broad-scale downwelling beneath the Americas and the Western Pacific, both regions with a long history of subduction, and upwelling flow beneath the central Pacific and Africa, both of which exhibit
dynamic topography consistent with upwelling.
[17] This broad-scale pattern of flow is also consistent with the tectonic plate motions, which are the surface expression of convection in the Earth's mantle and currently indicate degree-2 convergence toward the western Pacific and the Americas, and divergence away from the central Pacific and Africa.
[18] The persistence of net tectonic divergence away from Africa and the Pacific for the past 250 Myr indicates the long-term stability of this general mantle flow pattern,
[18] and is consistent with other studies
[19][20][21] that suggest long-term stability of the
LLSVP regions of the lowermost mantle that form the base of these upwellings.
Creep in the mantleEdit
Since the mantle is primarily composed of olivine ((Mg,Fe)2SiO4), the rheological characteristics of the mantle are largely those of olivine. Additionally, due to the varying temperatures and pressures between the lower and upper mantle, a variety of creep processes can occur with dislocation creep dominating in the lower mantle and diffusional creep occasionally dominating in the upper mantle. However, there is a large transition region in creep processes between the upper and lower mantle and even within each section, creep properties can change strongly with location and thus temperature and pressure. In the power law creep regions, the creep equation fitted to data with n = 3–4 is standard.
[22]
The strength of olivine not only scales with its melting temperature, but also is very sensitive to water and silica content. The solidus depression by impurities, primarily Ca, Al, and Na, and pressure affects creep behavior and thus contributes to the change in creep mechanisms with location. While creep behavior is generally plotted as homologous temperature versus stress, in the case of the mantle it is often more useful to look at the pressure dependence of stress. Though stress is simple force over area, defining the area is difficult in geology. Equation 1 demonstrates the pressure dependence of stress. Since it is very difficult to simulate the high pressures in the mantle (1MPa at 300–400 km), the low pressure laboratory data is usually extrapolated to high pressures by applying creep concepts from metallurgy.
[23]
Most of the mantle has homologous temperatures of 0.65–0.75 and experiences strain rates of
per second. Stresses in mantle are dependent on density, gravity, thermal expansion coefficients, temperature differences driving convection, and distance convection occurs over, all of which give stresses around a fraction of 3-30MPa. Due to the large grain sizes (at low stresses as high as several mm), it is unlikely that Nabarro-Herring (NH) creep truly dominates. Given the large grain sizes, dislocation creep tends to dominate. 14 MPa is the stress below which diffusional creep dominates and above which power law creep dominates at 0.5Tm of olivine. Thus, even for relatively low temperatures, the stress diffusional creep would operate at is too low for realistic conditions. Though the power law creep rate increases with increasing water content due to weakening, reducing activation energy of diffusion and thus increasing the NH creep rate, NH is generally still not large enough to dominate. Nevertheless, diffusional creep can dominate in very cold or deep parts of the upper mantle. Additional deformation in the mantle can be attributed to transformation enhanced ductility. Below 400 km, the olivine undergoes a pressure induced phase transformation into spinel and can cause more deformation due to the increased ductility.
[23] Further evidence for the dominance of power law creep comes from preferred lattice orientations as a result of deformation. Under dislocation creep, crystal structures reorient into lower stress orientations. This does not happen under diffusional creep, thus observation of preferred orientations in samples lends credence to the dominance of dislocation creep.
[24]