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2 Plate Tectonics

Learning Objectives

By the end of this chapter, students should be able to:

  • Describe how the ideas behind plate tectonics started with Alfred Wegener’s hypothesis of continental drift.
  • Describe the physical and chemical layers of the Earth and how they affect plate movement.
  • Explain how movement at the three types of plate boundaries causes earthquakes, volcanoes, and mountain building.
  • Identify convergent boundaries, including subduction and collisions, as places where plates come together.
  • Identify divergent boundaries, including rifts and mid-ocean ridges, as places where plates separate.
  • Explain transform boundaries as places where adjacent plates shear past each other.
  • Describe the Wilson cycle, from continental rifting, ocean basin creation, and plate subduction to ocean basin closure.
  • Explain how the tracks of hotspots, places that have continually rising magma, are used to calculate plate motion.
Figure description available at the end of the chapter.
Figure 2.1: Detailed map of all known plates, their boundaries, and movements. Figure description available at the end of the chapter.

Revolution is a word usually reserved for significant political or social changes. Several revolutionary ideas forced scientists to re-examine their entire fields, triggering a paradigm shift that shook up their conventionally held knowledge. Charles Darwin’s book on evolution, On the Origin of Species, published in 1859; Gregor Mendel’s discovery of the genetic principles of inheritance in 1866; and James Watson, Francis Crick, and Rosalind Franklin’s model for the structure of DNA in 1953 did that for biology. Albert Einstein’s concepts of relativity and quantum mechanics in the early twentieth century did the same for Newtonian physics.

The concept of plate tectonics was just as revolutionary for geology. The theory of plate tectonics attributes the movement of massive sections of the Earth’s outer layers with creating earthquakes, mountains, and volcanoes. Many Earth processes make more sense when viewed through the lens of plate tectonics. Because it is so important in understanding how the world works, plate tectonics is the first topic of discussion in this textbook.

2.1 Alfred Wegener’s Continental Drift Hypothesis

Black and white headshot of a man in a suit and tie.
Figure 2.2: Wegener later in his life, ca. 1924–1930. Figure description available at the end of the chapter.

Alfred Wegener (1880–1930) was a German scientist who specialized in meteorology and climatology. His knack for questioning accepted ideas started in 1910, when he disagreed with the explanation that the Bering Land Bridge was formed by isostasy and that similar land bridges once connected the continents. After reviewing the scientific literature, he published a hypothesis stating the continents were originally connected and then drifted apart. While he did not have the precise mechanism worked out, his hypothesis was backed up by a long list of evidence.

2.1.1 Early Evidence for Continental Drift Hypothesis

Figure description available at the end of the chapter.
Figure 2.3: Snider-Pellegrini’s map showing the continental fit and separation, 1858. Figure description available at the end of the chapter.

Wegener’s first piece of evidence was that the coastlines of some continents fit together like pieces of a jigsaw puzzle. People noticed the similarities in the coastlines of South America and Africa on the first world maps, and some suggested the continents had been ripped apart. Antonio Snider-Pellegrini did preliminary work on continental separation and matching fossils in 1858.

Figure description available at the end of the chapter.
Figure 2.4: Map of world elevations. Note the light blue areas, which are continental shelves flooded by shallow ocean water. These show the true shapes of the continents. Figure description available at the end of the chapter.

What Wegener did differently was synthesize a large amount of data in one place. He used the true edges of the continents, based on the shapes of the continental shelves. This resulted in a better fit than previous efforts that traced the existing coastlines.

Figure description available at the end of the chapter.
Figure 2.5: Image showing fossils that connect the continents of Gondwana (the southern continents of Pangea). Figure description available at the end of the chapter.

Wegener also compiled evidence by comparing similar rocks, mountains, fossils, and glacial formations across oceans. For example, the fossils of the primitive aquatic reptile Mesosaurus were found on the coastlines of both Africa and South America. Fossils of another reptile, Lystrosaurus, were found on Africa, India, and Antarctica. He pointed out these were land-dwelling creatures could not have swum across an entire ocean.

Opponents of continental drift insisted transoceanic land bridges allowed animals and plants to move between continents. The land bridges eventually eroded away, leaving the continents permanently separated. The problem with this hypothesis is the improbability of a land bridge being tall and long enough to stretch across a broad, deep ocean.

More support for continental drift came from the puzzling evidence that glaciers once existed in normally very warm areas in southern Africa, India, Australia, and Arabia. These climate anomalies could not be explained by land bridges. Wegener found similar evidence when he discovered tropical plant fossils in the frozen region of the Arctic Circle. As Wegener collected more data, he realized the explanation that best fit all the climate, rock, and fossil observations involved moving continents.

2.1.2 Proposed Mechanism for Continental Drift

Figure description available at the end of the chapter.
Figure 2.6: Animation of the basic idea of convection: an uneven heat source in a fluid causes rising material next to the heat and sinking material far from the heat. Figure description available at the end of the chapter.

Wegener’s work was considered a fringe science theory for his entire life. One of the biggest flaws in his hypothesis was an inability to provide a mechanism for how the continents moved. Obviously, the continents did not appear to move, so changing the conservative minds of the scientific community would require exceptional evidence that supported a credible mechanism. Other followers of continental drift used expansion, contraction, or even the Moon’s origin to explain how the continents moved. Wegener used centrifugal forces and precession, but this model was proven wrong. He also speculated about seafloor spreading, with hints of convection, but could not substantiate these proposals. As it turns out, current scientific knowledge reveals convection is one the major forces in driving plate movements, along with gravity and density.

2.1.3 Development of Plate Tectonic Theory

Figure description available at the end of the chapter.
Figure 2.7: GPS measurements of plate motions. Figure description available at the end of the chapter.

Wegener died in 1930 on an expedition in Greenland. Poorly respected in his lifetime, Wegener and his ideas about moving continents seemed destined to be lost in history as fringe science. However, in the 1950s, evidence started to trickle in that made continental drift a more viable idea. By the 1960s, scientists had amassed enough evidence to support the missing mechanism—namely, sea-floor spreading—for Wegener’s hypothesis of continental drift to be accepted as the theory of plate tectonics. Ongoing GPS and earthquake data analyses continue to support this theory. The next section provides the pieces of evidence that helped transform one man’s wild notion into a scientific theory.

Mapping of the Ocean Floors

Figure description available at the end of the chapter.
Figure 2.8: The complex chemistry around mid-ocean ridges. Figure description available at the end of the chapter.

In 1947, researchers started using an adaptation of sonar to map a region in the middle of the Atlantic Ocean with poorly understood topographic and thermal properties. Using this information, Bruce Heezen and Marie Tharp created the first detailed map of the ocean floor to reveal the Mid-Atlantic Ridge, a basaltic mountain range that spanned the length of the Atlantic Ocean, with rock chemistry and dimensions unlike the mountains found on the continents. Initially, scientists thought the ridge was part of a mechanism that explained the expanding Earth or ocean-basin growth hypotheses. In 1959, Harry Hess proposed the hypothesis of seafloor spreading, which suggested that the mid-ocean ridges represented tectonic plate factories, where new oceanic plate was issuing from these long volcanic ridges. Scientists later included transform faults perpendicular to the ridges to better account for varying rates of movement between the newly formed plates. When earthquake epicenters were discovered along the ridges, the idea that earthquakes were linked to plate movement took hold.

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Video 2.1: Uncovering the secrets of the ocean floor

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Seafloor sediment, measured by dredging and drilling, provided another clue. Scientists once believed sediment accumulated on the ocean floors over a very long time in a static environment. When some studies showed less sediment than expected, these results were initially used to argue against continental movement. With more time, researchers discovered these thinner sediment layers were located close to mid-ocean ridges, indicating the ridges were younger than the surrounding ocean floor. This finding supported the idea that the seafloor was not fixed in one place.

Paleomagnetism

Figure description available at the end of the chapter.
Figure 2.9: The magnetic field of Earth, simplified as a bar magnet. Figure description available at the end of the chapter.

The seafloor was also mapped magnetically. Scientists had long known of strange magnetic anomalies that formed a striped pattern of symmetrical rows on both sides of mid-oceanic ridges. What made these features unusual was that the north and south magnetic poles within each stripe were reversed in alternating rows. By 1963, Harry Hess and other scientists used these magnetic reversal patterns to support their model for seafloor spreading (see also Lawrence W. Morley).

Figure description available at the end of the chapter.
Figure 2.10: This animation shows how the magnetic poles have moved over 400 years. Figure description available at the end of the chapter.

Paleomagnetism is the study of magnetic fields frozen within rocks—basically a fossilized compass. In fact, the first hard evidence to support plate motion came from paleomagnetism.

Igneous rocks containing magnetic minerals like magnetite typically provide the most useful data. In their liquid state as magma or lava, the magnetic poles of the minerals align themselves with the Earth’s magnetic field. When the rock cools and solidifies, this alignment is frozen into place, creating a permanent paleomagnetic record that includes magnetic inclination related to global latitude and declination related to magnetic north.

Figure description available at the end of the chapter.
Figure 2.11: The iron in the solidifying rock preserves the current magnetic polarity as new oceanic plates form at mid-ocean ridges. Figure description available at the end of the chapter.

Scientists had noticed for some time the alignment of magnetic north in many rocks was nowhere close to the Earth’s current magnetic north. Some explained this away are part of the normal movement of Earth’s magnetic north pole. Eventually, scientists realized adding the idea of continental movement explained the data better than pole movement alone.

Wadati–Benioff Zones

Figure description available at the end of the chapter.
Figure 2.12: The Wadati-Benioff zone, showing earthquakes following the subducting slab down. Figure description available at the end of the chapter.

Around the same time mid-ocean ridges were being investigated, other scientists linked the creation of ocean trenches and island arcs to seismic activity and tectonic plate movement. Several independent research groups recognized that earthquake epicenters traced the shapes of oceanic plates sinking into the mantle. These deep earthquake zones congregated in planes that started near the surface around ocean trenches and angled beneath the continents and island arcs. Today, these earthquake zones called Wadati-Benioff zones.

Headshot of an older man wearing a suit and tie.
Figure 2.13: J. Tuzo Wilson. Figure description available at the end of the chapter.

Based on the mounting evidence, the theory of plate tectonics continued to take shape. J. Tuzo Wilson was the first scientist to put the entire picture together by proposing the opening and closing of the ocean basins. Before long, scientists proposed other models showing plates moving with respect to each other, with clear boundaries between them. Others started piecing together complicated histories of tectonic plate movement. The Plate Tectonics Revolution had taken hold.

 

 

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2.2 Layers of the Earth

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Figure 2.14: The layers of the Earth. Physical layers include lithosphere and asthenosphere; chemical layers are crust, mantle, and core. Figure description available at the end of the chapter.

In order to understand the details of plate tectonics, it is essential to first understand the layers of the Earth. Firsthand information about what is below the surface is very limited; most of what we know is pieced together from hypothetical models and analysis of seismic wave data and meteorite materials. In general, the Earth can be divided into layers based on chemical composition and physical characteristics.

2.2.1 Chemical Layers

The Earth is composed of a countless combination of elements. Regardless of what elements are involved, two major factors—temperature and pressure—are responsible for creating three distinct chemical layers.

Crust

The outermost chemical layer, and the one on which we currently reside, is the crust. There are two types of crust. Continental crust has a relatively low density and composition similar to granite. Oceanic crust has a relatively high density, especially when cold and old, and its composition is similar to basalt. The surface levels of crust are relatively brittle. The deeper parts of the crust are subjected to higher temperatures and pressure, which makes them more ductile. Ductile materials are like soft plastics or putty, moving under force. Brittle materials are like solid glass or pottery; they break under force, especially when it is applied quickly. Earthquakes generally occur in the upper crust and are caused by the rapid movement of relatively brittle materials.

Figure description available at the end of the chapter.
Figure 2.15: The global map of the depth of the Moho. Figure description available at the end of the chapter.

The base of the crust is characterized by a large increase in seismic velocity, which measures how fast earthquake waves travel through solid matter. Called the Mohorovičić discontinuity, or Moho for short, this zone was discovered by Andrija Mohorovičić (pronounced mo-ho-ro-vee-cheech; audio pronunciation) in 1909 after studying earthquake wave paths in his native Croatia. The change in wave direction and speed is caused by dramatic chemical differences of the crust and mantle. Underneath the oceans, the Moho is found roughly 5 km below the ocean floor; under the continents, it is located about 30–40 km below the surface. Near some large mountain-building events known as orogenies, the continental Moho depth is doubled.

Mantle

Figure description available at the end of the chapter.
Figure 2.16: This mantle xenolith containing olivine (green) is chemically weathering by hydrolysis and oxidation into the pseudomineral iddingsite, which is a complex of water, clay, and iron oxides. The more altered side of the rock has been exposed to the environment longer. Figure description available at the end of the chapter.

The mantle sits below the crust and above the core. It is the largest chemical layer by volume, extending from the base of the crust to a depth of about 2,900 km. Most of what we know about the mantle comes from seismic wave analysis, though information is gathered by studying ophiolites and xenoliths. Ophiolites are pieces of mantle that have risen through the crust until they are exposed as part of the ocean floor. Xenoliths are carried within magma and brought to the Earth’s surface by volcanic eruptions. Most xenoliths are made of peridotite, an ultramafic class of igneous rock (see Section 4.2 for explanation). Because of this, scientists hypothesize most of the mantle is made of peridotite.

Core

Figure description available at the end of the chapter.
Figure 2.17: A polished fragment of iron-rich Toluca meteorite with octahedral Widmanstätten pattern. Figure description available at the end of the chapter.

The core of the Earth, which has both liquid and solid layers, consists mostly of iron, nickel, and possibly some oxygen. Scientists looking at seismic data first discovered this innermost chemical layer in 1906. Through a union of hypothetical modeling, astronomical insight, and hard seismic data, they concluded the core is mostly metallic iron. Scientists studying meteorites, which typically contain more iron than surface rocks, have proposed the Earth was formed from meteoric material. They believe the liquid component of the core was created as the iron and nickel sank into the center of the planet, where it was liquefied by intense pressure.

2.2.2 Physical Layers

The Earth can also be broken down into five distinct physical layers based on how each layer responds to stress. While there is some overlap in the chemical and physical designations of layers, specifically the core-mantle boundary, there are significant differences between the two systems.

Lithosphere

Figure description available at the end of the chapter.
Figure 2.18: Map of the major plates and their motions along boundaries. Figure description available at the end of the chapter.

The lithosphere (from Lithos, Greek for stone) is the outermost physical layer of the Earth. It is grouped into two types: oceanic and continental. Oceanic lithosphere is thin and relatively rigid. It ranges in thickness from nearly zero in new plates found around mid-ocean ridges to an average of 140 km in most other locations. Continental lithosphere is generally thicker and considerably more plastic, especially at the deeper levels. Its thickness ranges from 40 to 280 km. The lithosphere is not continuous. It is broken into segments called plates. A plate boundary is where two plates meet and move relative to each other. Plate boundaries are where we see plate tectonics in action—building mountains, triggering earthquakes, and generating volcanic activity.

Asthenosphere

Figure description available at the end of the chapter.
Figure 2.19: The lithosphere-asthenosphere boundary changes with certain tectonic situations. Figure description available at the end of the chapter.

The asthenosphere is the layer below the lithosphere. Astheno- means lacking strength, and the most distinctive property of the asthenosphere is movement. Because it is mechanically weak, this layer moves and flows due to convection currents created by heat coming from the Earth’s core. Unlike the lithosphere, which consists of multiple plates, the asthenosphere is relatively unbroken. Scientists have determined this by analyzing seismic waves that pass through the layer. The depth at which the asthenosphere is found is temperature-dependent. It tends to lie closer to the Earth’s surface around mid-ocean ridges and much deeper underneath mountains and the centers of lithospheric plates.

Mesosphere

Figure description available at the end of the chapter.
Figure 2.20: General perovskite structure. Perovskite silicates (i.e., bridgmenite, (Mg,Fe)SiO3) are thought to be the main component of the lower mantle, making it the most common mineral in or on Earth. Figure description available at the end of the chapter.

The mesosphere, sometimes known as the lower mantle, is more rigid and immobile than the asthenosphere. Located at a depth of approximately 410 to 660 km below the Earth’s surface, the mesosphere is subjected to very high pressures and temperatures. These extreme conditions create a transition zone in the upper mesosphere where minerals continuously change into various forms, or pseudomorphs. Scientists identify this zone by changes in seismic velocity and sometimes by physical barriers to movement. Below this transitional zone, the mesosphere is relatively uniform until it reaches the core.

Inner and Outer Core

Antique photo of young woman wearing a sweater.
Figure 2.21: Lehmann in 1932. Figure description available at the end of the chapter.

The outer core is the only entirely liquid layer within the Earth. It starts at a depth of 2,890 km and extends to 5,150 km, making it about 2,300 km thick. In 1936, the Danish geophysicist Inge Lehmann analyzed seismic data and was the first to prove a solid inner core existed within a liquid outer core. The solid inner core is about 1,220 km thick, and the outer core is about 2,300 km thick.

Figure description available at the end of the chapter.
Figure 2.22: The outer core’s spin causes our protective magnetic field. Figure description available at the end of the chapter.

It seems like a contradiction that the hottest part of the Earth is solid, as the minerals making up the core should be liquified or vaporized at this temperature. Immense pressure keeps the minerals of the inner core in a solid phase. The inner core grows slowly from the lower outer core, solidifying as heat escapes the interior of the Earth and is dispersed to the outer layers.

The Earth’s liquid outer core is critically important in maintaining a breathable atmosphere and other environmental conditions favorable for life. Scientists believe the Earth’s magnetic field is generated by the circulation of molten iron and nickel within the outer core. If the outer core were to stop circulating or become solid, the loss of the magnetic field would result in Earth being stripped of life-supporting gases and water. This is what happened, and continues to happen, on Mars.

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2.2.3 Plate Tectonic Boundaries

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Figure 2.23: Passive margin. Figure description available at the end of the chapter.

At passive margins, the plates don’t move; the continental lithosphere transitions into oceanic lithosphere and forms plates made of both types. A tectonic plate may be made of both oceanic and continental lithosphere connected by a passive margin. North and South America’s eastern coastlines are examples of passive margins. Active margins are places where the oceanic and continental lithospheric tectonic plates meet and move relative to each other, such as the western coasts of North and South America. This movement is caused by frictional drag created between the plates and differences in plate densities. The majority of mountain-building events, earthquake activity, and active volcanism on the Earth’s surface can be attributed to tectonic plate movement at active margins.

Figure description available at the end of the chapter.
Figure 2.24: Schematic of plate boundary types. Figure description available at the end of the chapter.

In a simplified model, there are three categories of tectonic plate boundaries. Convergent boundaries are places where plates move toward each other. At divergent boundaries, the plates move apart. At transform boundaries, the plates slide past each other.

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2.3 Convergent Boundaries

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Figure 2.25: Geologic provinces, with the shield (orange) and platform (pink) comprising the craton, the stable interior of continents. Figure description available at the end of the chapter.

Convergent boundaries, also called destructive boundaries, are places where two or more plates move toward each other. Convergent boundary movement is divided into two types, subduction and collision, depending on the density of the involved plates. Continental lithosphere is of lower density and thus more buoyant than the underlying asthenosphere. Oceanic lithosphere is more dense than continental lithosphere, and, when old and cold, may even be more dense than asthenosphere.

When plates of different densities converge, the higher-density plate is pushed beneath the more buoyant plate in a process called subduction. When continental plates converge without subduction occurring, this process is called collision.

2.3.1. Subduction

Subduction occurs when a dense oceanic plate meets a more buoyant plate, like a continental plate or a warmer/younger oceanic plate, and descends into the mantle. The worldwide average rate of oceanic plate subduction is 25 miles per million years—about a half-inch per year. As an oceanic plate descends, it pulls the ocean floor down into a trench. These trenches can be more than twice as deep as the average depth of the adjacent ocean basin, which is usually 3–4 km. The Mariana Trench, for example, approaches a staggering 11 km.

Figure description available at the end of the chapter.
Figure 2.26: Diagram of ocean-continent subduction. Figure description available at the end of the chapter.
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Figure 2.27: Microcontinents can become part of the accretionary prism of a subduction zone. Figure description available at the end of the chapter.

Within the trench, ocean-floor sediments are scraped together and compressed between the subducting and overriding plates. This feature is called the accretionary wedge, mélange, or accretionary prism. Fragments of continental material, including microcontinents, riding atop the subducting plate may become sutured to the accretionary wedge and accumulate into a large area of land called a terrane. Vast portions of California are comprised of accreted terranes.

Figure description available at the end of the chapter.
Figure 2.28: Accreted terranes of Western North America. Everything that is not the “ancient continental interior (craton)” has been smeared onto the side of the continent by accretion from subduction. Figure description available at the end of the chapter.

When the subducting oceanic plate, or slab, sinks into the mantle, the immense heat and pressure pushes volatile materials like water and carbon dioxide into an area below the continental plate and above the descending plate called the mantle wedge. The volatiles are released mostly by hydrated minerals that revert to nonhydrated minerals in these higher temperature and pressure conditions. When mixed with asthenospheric material above the plate, the volatile lower the melting point of the mantle wedge, and through a process called flux melting, it becomes liquid magma. The molten magma is more buoyant than the lithospheric plate above it, migrating to the Earth’s surface, where it emerges as volcanism. The resulting volcanoes frequently appear as curved mountain chains (known as volcanic arcs) due to the curvature of the Earth. Both oceanic and continental plates can contain volcanic arcs.

Figure description available at the end of the chapter.
Figure 2.29: Location of the large (Mw 8.5–9.0) 1755 Lisbon earthquake. Figure description available at the end of the chapter.

How subduction is initiated is still a matter of scientific debate. It is generally accepted that subduction zones start as passive margins, where oceanic and continental plates come together, and then gravity initiates subduction and converts to margin from passive to active. One hypothesis is that gravity pulls the denser oceanic plate down or that the plate can start to flow with ductility at a low angle. Scientists seeking to answer this question have collected evidence that suggests a new subduction zone is forming off the coast of Portugal. Some scientists have proposed that large earthquakes like the 1755 Lisbon earthquake may even have something to do with this process of creating a subduction zone, although the evidence is not definitive. Another hypothesis proposes that subduction happens at transform boundaries involving plates of different densities.

Some plate boundaries look like they should be active but show no evidence of subduction. For example, the oceanic lithospheric plates on either side of the Atlantic Ocean are denser than the underlying asthenosphere and are not subducting beneath the continental plates. One hypothesis is that the bond holding the oceanic and continental plates together is stronger than the downward force created by the difference in plate densities.

Figure description available at the end of the chapter.
Figure 2.30: Earthquakes along the Sunda megathrust subduction zone along the island of Sumatra, showing the 2006 Mw 9.1-9.3 Indian Ocean earthquake as a star. Figure description available at the end of the chapter.

Subduction zones are known for having the largest earthquakes and tsunamis; they are the only places with fault surfaces large enough to create magnitude 9 earthquakes. These subduction-zone earthquakes are not only very large but are also very deep. When a subducting slab becomes stuck and cannot descend, a massive amount of energy builds up between the stuck plates. If this energy is not gradually dispersed, it may force the plates to suddenly release along several hundred kilometers of the subduction zone. Because subduction-zone faults are located on the ocean floor, this massive amount of movement can generate giant tsunamis such as those that followed the 2004 Indian Ocean earthquake and 2011 Tōhoku earthquake in Japan.

Figure description available at the end of the chapter.
Figure 2.31: Various parts of a subduction zone. This subduction zone is ocean-ocean subduction, though the same features can apply to continent-ocean subduction. Figure description available at the end of the chapter.

All subduction zones have a forearc basin, a feature of the overriding plate found between the volcanic arc and oceanic trench. The forearc basin experiences a lot of faulting and deformation activity, particularly within the accretionary wedge.

In some subduction zones, tensional forces working on the continental plate create a back-arc basin on the interior side of the volcanic arc. Some scientists have proposed a subduction mechanism called oceanic slab rollback, which creates extension faults in the overriding plates. In this model, the descending oceanic slab does not slide directly under the overriding plate but instead rolls back, pulling the overlying plate seaward. The continental plate behind the volcanic arc gets stretched like pizza dough until the surface cracks and collapses to form a backarc basin. If the extension activity is extensive and deep enough, a backarc basin can develop into a continental rifting zone. These continental divergent boundaries may be less symmetrical than their mid-ocean ridge counterparts.

In places where numerous young buoyant oceanic plates converge and subduct at a relatively high velocity, they may force the overlying continental plate to buckle and crack. This is called back-arc faulting. Extensional back-arc faults pull rocks and chunks of plates apart. Compressional back-arc faults, also known as thrust faults, push them together.

The dual spines of the Andes mountain range include a example of compressional thrust faulting. The western spine is part of a volcanic arc. Thrust faults have deformed the nonvolcanic eastern spine, pushing rocks and pieces of continental plate on top of each other.

There are two styles of thrust fault deformation: thin-skinned faults that occur in superficial rocks lying on top of the continental plate and thick-skinned faults that reach deeper into the crust. The Sevier orogeny in the Western US is a notable thin-skinned type of deformation created during the Cretaceous Period. The Laramide orogeny, a thick-skinned type of deformation, occurred near the end of and slightly after the Sevier orogeny in the same region.

Figure description available at the end of the chapter.
Figure 2.32: Shallow subduction during the Laramide orogeny. Figure description available at the end of the chapter.

Flat-slab, or shallow, subduction caused the Laramide orogeny. When the descending slab subducts at a low angle, there is more contact between the slab and the overlying continental plate than in a typical subduction zone. The shallowly subducting slab pushes against the overriding plate and creates an area of deformation on the overriding plate many kilometers away from the subduction zone.

Oceanic-Continental Subduction

Figure description available at the end of the chapter.
Figure 2.33: Subduction of an oceanic plate beneath a continental plate, forming a trench and volcanic arc. Figure description available at the end of the chapter.

Oceanic-continental subduction occurs when an oceanic plate dives below a continental plate. This convergent boundary has a trench, mantle wedge, and frequently, a volcanic arc. Well-known examples of continental volcanic arcs are the Cascade Mountains in the Pacific Northwest and the western Andes Mountains in South America.

Oceanic-Oceanic Subduction

Figure description available at the end of the chapter.
Figure 2.34: Subduction of an oceanic plate beneath another oceanic plate, forming a trench and an island arc. Figure description available at the end of the chapter.

The boundaries of oceanic-oceanic subduction zones show very different activity from those involving oceanic-continental plates. Since both oceanic lithosphere, it is usually the older plate that subducts because it is colder and denser. The volcanism on the overlying oceanic plate may remain hidden underwater. If the volcanoes rise high enough to reach the ocean surface, the chain of volcanism forms an island arc. Examples of these island arcs include the Aleutian Islands in the northern Pacific Ocean, the Lesser Antilles in the Caribbean Sea, and numerous island chains scattered throughout the western Pacific Ocean.

2.3.2. Collisions

Figure description available at the end of the chapter.
Figure 2.35: Two continental plates colliding. Figure description available at the end of the chapter.

When continental plates converge—for example, during the closing of an ocean basin—subduction is not possible between the equally buoyant plates. Instead of one plate descending beneath another, the two masses of continental lithosphere slam together in a process known as collision. Without subduction, there is no magma formation and no volcanism. Collision zones are characterized by tall, nonvolcanic mountains; broad zones of frequent, large earthquakes; and very little volcanism.

When oceanic crust connected by a passive margin to continental crust completely subducts beneath a continent, an ocean basin closes and continental collision begins. Eventually, as ocean basins close, continents join together to form a massive accumulation of continents called a supercontinent, a process that takes place in ~500-million-year cycles over Earth’s history.

Figure description available at the end of the chapter.
Figure 2.36: A reconstruction of Pangea, showing approximate positions of modern continents. Figure description available at the end of the chapter.

The process of collision created Pangea, the supercontinent envisioned by Wegener as the key component of his continental drift hypothesis. Geologists now have evidence that continental plates have been continuously converging into supercontinents and splitting into smaller basin-separated continents throughout Earth’s existence in a process known as the supercontinent cycle, which takes approximately 500 million years. For example, Pangea is estimated to have begun separating 200 million years ago. Pangea was preceded by an earlier supercontinents, including Rodinia, which existed 1.1 billion years ago and started breaking apart 800 million to 600 million years ago.

Figure description available at the end of the chapter.
Figure 2.37: The tectonics of the Zagros Mountains. Note the Persian Gulf foreland basin. Figure description available at the end of the chapter.

A foreland basin is a feature that develops near mountain belts, as the combined mass of the mountains forms a depression in the lithospheric plate. While foreland basins may occur at subduction zones, they are most commonly found at collision boundaries. The Persian Gulf is possibly the best modern example, created entirely by the weight of the nearby Zagros Mountains.

An outcrop of medium-gray rocks that have bulbous texture which are old cooled pillow lavas.
Figure 2.38: Pillow lavas, which only form under water, from an ophiolite in the Apennine Mountains of Central Italy. Figure description available at the end of the chapter.

If continental and oceanic lithosphere are fused on the same plate, it can partially subduct, but its buoyancy prevents it from fully descending. In very rare cases, part of a continental plate may become trapped beneath a descending oceanic plate in a process called obduction. When a portion of the continental crust is driven down into the subduction zone, it returns to the surface relatively quickly due to its buoyancy.

As pieces of the continental lithosphere break loose and migrate upward through the obduction zone, they bring along bits of the mantle and ocean floor to the top of the continental plate. Rocks composed of this mantle and ocean-floor material are called ophiolites, and they provide valuable information about the composition of the mantle.

Figure description available at the end of the chapter.
Figure 2.39: Animation of India crashing into Asia. Figure description available at the end of the chapter.

The area of collision-zone deformation and seismic activity usually covers a broader area because continental lithosphere is plastic and malleable. Unlike subduction-zone earthquakes, which tend to be located along a narrow swath near the convergent boundary, collision-zone earthquakes may occur hundreds of kilometers from the boundary between the plates.

The Eurasian continent has many examples of collision-zone deformations covering vast areas. The Pyrenees Mountains begin in the Iberian Peninsula and cross into France. Additionally, the Alps stretch from Italy to Central Europe; the Zagros Mountains from Arabia to Iran; and the Himalayas from the Indian subcontinent to Central Asia.

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2.4 Divergent Boundaries

At divergent boundaries, sometimes called constructive boundaries, lithospheric plates move away from each other. There are two types of divergent boundaries, categorized by where they occur: continental rift zones and mid-ocean ridges. Continental rift zones occur in weak spots in the continental lithospheric plate. A mid-ocean ridge usually originates in a continental plate as a rift zone that expands to the point of splitting the plate apart, with seawater filling the gap. The separate pieces continue to drift apart and become individual continents. This process is known as rift-to-drift.

2.4.1. Continental Rifting

Figure description available at the end of the chapter.
Figure 2.40: Faulting that occurs in divergent boundaries. Figure description available at the end of the chapter.

In places where the continental plates are very thick, they reflect so much heat back into the mantle that it develops strong convection currents that push super-heated mantle material up against the overlying plate, softening it. Tensional forces created by this convective upwelling begin to pull the weakened plate apart. As it stretches, it becomes thinner and develops deep cracks called extension faults, or normal faults. Eventually plate sections located between large faults drop into deep depressions known as rift valleys, which often contain keystone-shaped blocks of down-dropped crust known as grabens. The shoulders of these grabens are called horsts. If only one side of a section drops, it is called a half-graben. Depending on the conditions, rifts can grow into very large lakes and even oceans.

Figure description available at the end of the chapter.
Figure 2.41: The Afar Triangle (center) has the Red Sea ridge (center to upper left), Gulf of Aden ridge (center to right), and East African Rift (center to lower left) form a triple junction that are about 120° apart. Figure description available at the end of the chapter.

While seemingly occurring at random, rifting is dictated by two factors. Rifting does not occur in continents with older and more stable interiors, known as cratons. When continental rifting does occur, the break-up pattern is called a truncated icosahedron, which resembles the seams of a soccer ball. This is the most common surface-fracture pattern to develop on an evenly expanding sphere because it uses the least amount of energy.

Using the soccer ball model, rifting tends to lengthen and expand along a particular seam while fizzling out in the other directions. These seams with little or no tectonic activity are called failed rift arms. A failed rift arm is still a weak spot in the continental plate; even without the presence of active extension faults, it may develop into what is known as an aulacogen. One example of a failed rift arm is the Mississippi Valley embayment, a depression through which the upper end of the Mississippi River flows. Occasionally, connected rift arms do develop concurrently, creating multiple boundaries of active rifting. In places where the rift arms do not fail, for example the Afar Triangle, three divergent boundaries can develop near each other, forming a triple junction.

Satellite photo of a tan landscape that has long ridges and valleys.
Figure 2.42: NASA image of the Basin and Range horsts and grabens across central Nevada. Figure description available at the end of the chapter.

Rifts come in two types: narrow and broad. Narrow rifts are characterized by a high density of highly active divergent boundaries. The East African rift zone, where the Horn of Africa is pulling away from the mainland, is an excellent example of an active narrow rift. Lake Baikal in Russia is another. Broad rifts also have numerous fault zones, but they are distributed over wide areas of deformation. The Basin and Range region located in the Western United States is a type of broad rift. The Wasatch fault, which also created the Wasatch mountain range in the state of Utah, forms the eastern divergent boundary of this broad rift (Animation 1 and Animation 2).

Figure description available at the end of the chapter.
Figure 2.43: India colliding into Eurasia to create the modern day Himalayas. Figure description available at the end of the chapter.

Rifts have earthquakes, although not of the magnitude and frequency of other boundaries. They may also exhibit volcanism. Unlike the flux-melted magma found in subduction zones, rift-zone magma is created by decompression melting. As the continental plates are pulled apart, they create a region of low pressure that melts the lithosphere and draws it upwards. When this molten magma reaches the weakened and fault-riddled rift zone, it migrates to the surface by breaking through the plate or escaping via an open fault. Examples of young rift volcanoes are scattered throughout the Basin and Range region in the United States. Rift-zone activity is responsible for generating some unique volcanism, such as the Ol Doinyo Lengai in Tanzania. This volcano erupts lava consisting largely of carbonatite, a relatively cold, liquid carbonate mineral.

2.4.2. Mid-Ocean Ridges

Figure description available at the end of the chapter.
Figure 2.44: Progression from rift to mid-ocean ridge. Figure description available at the end of the chapter.

As rifting and volcanic activity progress, the continental lithosphere becomes more mafic (see Chapter 4) and thinner, with the eventual result transforming the plate under the rifting area into oceanic lithosphere. This is the process that gives birth to a new ocean, much like the narrow Red Sea emerging with the movement of Arabia away from Africa. As the oceanic lithosphere continues to diverge, a mid-ocean ridge is formed.

Mid-ocean ridges, also known as spreading centers, have several distinctive features. They are the only places on Earth that create new oceanic lithosphere. Decompression melting in the rift zone changes asthenosphere material into new lithosphere, which oozes up through cracks in oceanic plate. The amount of new lithosphere being created at mid-ocean ridges is highly significant. These undersea rift volcanoes produce more lava than all other types of volcanism combined. Despite this, most mid-oceanic ridge volcanism remains unmapped because the volcanoes are located deep on the ocean floor.

In rare cases, such as a few locations in Iceland, rift zones display the type of volcanism, spreading, and ridge formation found on the ocean floor.

Figure description available at the end of the chapter.
Figure 2.45: Age of oceanic lithosphere, in millions of years. Notice the differences in the Atlantic Ocean along the coasts of the continents. Figure description available at the end of the chapter.

The ridge feature is created by the accumulation of hot lithosphere material, which is lighter than the dense underlying asthenosphere. This chunk of isostatically buoyant lithosphere sits partially submerged and partially exposed on the asthenosphere, like an ice cube floating in a glass of water.

As the ridge continues to spread, the lithosphere material is pulled away from the area of volcanism and becomes colder and denser. As it continues to spread and cool, the lithosphere settles into wide swaths of relatively featureless topography called abyssal plains with lower topography.

This model of ridge formation suggests the sections of lithosphere furthest away from the mid-ocean ridges will be the oldest. Scientists have tested this idea by comparing the ages of rocks located in various locations on the ocean floor. Rocks found near ridges are younger than those found far away from any ridges. Sediment-accumulation patterns also confirm the idea of seafloor spreading. Sediment layers tend to be thinner near mid-ocean ridges, indicating it has had less time to build up.

Figure description available at the end of the chapter.
Figure 2.46: A time progression (with “a” being youngest and “c” being oldest) showing a spreading center getting wider while recording changes in the magnetic field of the Earth. Figure description available at the end of the chapter.

As mentioned in the section on paleomagnetism and the development of plate tectonic theory, scientists noticed that mid-ocean ridges contained unique magnetic anomalies that show up as symmetrical striping on both sides of the ridge. The Vine-Matthews-Morley hypothesis proposes these alternating reversals are created by the Earth’s magnetic field being imprinted into magma after it emerges from the ridge. Very hot magma has no magnetic field. As the oceanic plates get pulled apart, the magma cools below the Curie point—the temperature below which a magnetic field gets locked into magnetic minerals. The alternating magnetic reversals in the rocks reflects the periodic swapping of Earth’s magnetic north and south poles. This paleomagnetic pattern provides a great historical record of ocean-floor movement and is used to reconstruct past tectonic activity and determine rates of ridge spreading.

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Video 2.2: Pangea breakup and formation of the northern Atlantic Ocean

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Figure description available at the end of the chapter.
Figure 2.47: Black smoker hydrothermal vent with a colony of giant (6’+) tube worms. Figure description available at the end of the chapter.

Thanks to their distinctive geology, mid-ocean ridges are home to some of the most unique ecosystems ever discovered. The ridges are often studded with hydrothermal vents, which are deep fissures that allow seawater to circulate through the upper portions of the oceanic plate and interact with hot rock. The super-heated seawater rises back up to the surface of the plate, carrying dissolved gases and minerals as well as small particulates. The hydrothermal water emitted as a result looks like black underwater smoke.

Scientists had known about these geothermal areas on the ocean floor for some time. However, it was not until 1977 that scientists piloting a deep submergence vehicle, the Alvin, discovered a thriving community of organisms clustered around these hydrothermal vents. These unique organisms, which include ten-foot-long tube worms taller than people, live in the complete darkness of the ocean floor, deprived of oxygen and sunlight. They use geothermal energy provided by the vents and a process called bacterial chemosynthesis to feed on sulfur compounds. Before this discovery, scientists believed life on Earth could not exist without photosynthesis, a process that requires sunlight. Some scientists suggest this type of environment could have been the origin of life on Earth and perhaps even extraterrestrial life elsewhere in the galaxy, such as on Jupiter’s moon Europa.

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2.5 Transform Boundaries

Figure description available at the end of the chapter.
Figure 2.48: The two types of transform/strike-slip faults. Figure description available at the end of the chapter.

A transform boundary, sometimes called a strike-slip or conservative boundary, is where the lithospheric plates slide past each other in the horizontal plane. This movement is described based on the perspective of an observer standing on one of the plates, looking across the boundary at the opposing plate. Dextral, also known as right-lateral, movement describes the opposing plate moving to the right. Sinistral, also known as left-lateral, movement describes the opposing plate moving to the left.

Most transform boundaries are found on the ocean floor around mid-ocean ridges. These boundaries form aseismic fracture zones filled with earthquake-free transform faults to accommodate different rates of spreading occurring at the ridge.

Figure description available at the end of the chapter.
Figure 2.49: Map of the San Andreas fault showing relative motion. Figure description available at the end of the chapter.

Some transform boundaries produce significant seismic activity, primarily as earthquakes, with very little mountain-building or volcanism. This type of transform boundary may contain a single fault or series of faults, which develop in places where plate tectonic stresses are transferred to the surface. As with other types of active boundaries, if the plates are unable to shear past each other, the tectonic forces will continue to build up. If the built-up energy between the plates is suddenly released, the result is an earthquake.

In the eyes of humanity, the most significant transform faults occur within continental plates and have a shearing motion that frequently produces moderate-to-large magnitude earthquakes. Notable examples include the San Andreas fault in California, Northern and Eastern Anatolian faults in Turkey, Altyn Tagh fault in Central Asia, and Alpine fault in New Zealand.

2.5.1 Transpression and Transtension

Figure description available at the end of the chapter.
Figure 2.50: A transpressional strike-slip fault, causing uplift called a restraining bend. Figure description available at the end of the chapter.

Bends along transform faults may create compressional or extensional forces that cause secondary faulting zones. Transpression occurs where there is a component of compression in addition to the shearing motion. These forces build up around the area of the bend, where the opposing plates are restricted from sliding past each other. As the forces continue to build up, they create mountains in the restraining bend around the fault. The Big Bend area, located in the southern part of the San Andreas fault, includes a large area of transpression where many mountains have been built, moved, and even rotated.

Figure description available at the end of the chapter.
Figure 2.51: A transtensional strike-slip fault, causing a restraining bend. In the center of the fault, a depression with extension would be found. Figure description available at the end of the chapter.

Transtension zones require a fault that includes a releasing bend, where the plates are pulled apart by extensional forces. Depressions and sometimes volcanism develop in the releasing bend along the fault. The Dead Sea between Israel and Jordan and the Salton Sea of California are examples of basins formed by transtensional forces.

2.5.2 Piercing Points

Figure description available at the end of the chapter.
Figure 2.52: Wallace Creek (dry) on the Cariso Plain, California. Note that, as the creek flows from the northern mountainous part of the image, it takes a sharp right (as viewed from the flow of water), then a sharp left. This is caused by the San Andreas Fault cutting roughly perpendicular to the creek and shifting the location of the creek over time. The fault can be seen about halfway down, trending left to right, as a change in the topography. Figure description available at the end of the chapter.

When a geological feature is cut by a fault, it is called a piercing point. Piercing points are very useful for recreating past fault movement, especially along transform boundaries. Transform faults are unique because their horizontal motion keeps a geological feature relatively intact, preserving the record of what happened. Other types of faults—normal and reverse—tend to be more destructive, obscuring or destroying these features. The best type of piercing point includes unique patterns, which are used to match the parts of a geological feature separated by fault movement. Detailed studies of piercing points show the San Andreas fault has experienced over 225 km of movement in the last 20 million years, and this movement occurred at three different fault traces.

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Video 2.3: Video of the origin of the San Andreas fault. As the mid-ocean ridge subducts, the relative motion between the remaining plates become transform, forming the fault system. Note that, because the motion of the plates is not exactly parallel to the fault, it causes divergent motion in the interior of North America.

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2.6 The Wilson Cycle

Figure description available at the end of the chapter.
Figure 2.53: Diagram of the Wilson cycle, showing rifting and collision phases. Figure description available at the end of the chapter.

The Wilson cycle is named for J. Tuzo Wilson, who first described it in 1966, and it outlines the ongoing origin and breakup of supercontinents, such as Pangea and Rodinia. Scientists have determined this cycle has been operating for at least three billion years and possibly longer.

There are a number of hypotheses about how the Wilson cycle works. One mechanism proposes that rifting happens because continental plates reflect the heat much better than oceanic plates. When continents congregate together, they reflect more of the Earth’s heat back into the mantle, generating more vigorous convection currents that then start the continental rifting process. Some geologists believe mantle plumes are remnants of these periods of increased mantle temperature and convection upwelling, studying them for clues about the origin of continental rifting.

The mechanism behind how supercontinents are created is still largely a mystery. There are three schools of thought about what continues to drive the continents further apart and eventually bring them together. The ridge-push hypothesis suggests after the initial rifting event, plates continue to be pushed apart by mid-ocean spreading centers and their underlying convection currents. The slab-pull hypothesis proposes the plates are pulled apart by descending slabs in the subduction zones of the oceanic-continental margins. A third idea, gravitational sliding, attributes the movement to gravitational forces pulling the lithospheric plates down from the elevated mid-ocean ridges and across the underlying asthenosphere. Current evidence seems to support slab pull more than ridge push or gravitational sliding.

2.7 Hotspots

Figure description available at the end of the chapter.
Figure 2.54: Diagram showing a nonmoving source of magma (mantle plume) and a moving overriding plate. Figure description available at the end of the chapter.

The Wilson cycle provides a broad overview of tectonic plate movement. To analyze plate movement more precisely, scientists study hotspots. First postulated by J. Tuzo Wilson in 1963, a hotspot is an area in the lithospheric plate where molten magma breaks through and creates a volcanic center—islands in the ocean and mountains on land. As the plate moves across the hotspot, the volcano center becomes extinct because it is no longer over an active magma source. Instead, the magma emerges through another area in the plate to create a new active volcano. Over time, the combination of moving plate and stationary hotspot creates a chain of islands or mountains. Conventionally, hotspots were thought not to move, although recent evidence suggests that there may be exceptions.

Figure description available at the end of the chapter.
Figure 2.55: Map of world hotspots. Larger circles indicate more active hotspots. Figure description available at the end of the chapter.

Hotspots are the only types of volcanism not associated with subduction or rifting zones at plate boundaries; they seem totally disconnected from any plate tectonics processes, such as earthquakes. However, there are relationships between hotspots and plate tectonics. There are several hotspots, current and former, that are believed to have begun at the time of rifting. In addition, scientists use the age of volcanic eruptions and shape of the chain to quantify the rate and direction of plate movement relative to the hotspot.

Scientists are divided over how magma is generated in hotspots. Some suggest that hotspots originate from super-heated material that originates from as deep as the core and that reaches the Earth’s crust as a mantle plume. Others argue the molten material that feeds hotspots is sourced from the mantle. Of course, it is difficult to collect data from these deep-Earth features due to the extremely high pressure and temperature.

The initiation of hotspots is another highly debated subject. The prevailing mechanism considers hotspots as starting in divergent boundaries during supercontinent rifting. Scientists have identified a number of current and past hotspots believed to have begun this way. Subducting slabs have also been named as causing mantle plumes and hotspot volcanism. Some geologists have suggested another geological process not involving plate tectonics may be involved, such as large space objects crashing into Earth. Regardless of how they are formed, there are dozens on the Earth. Some well-known examples include the Tahiti Islands, Afar Triangle, Easter Island, Iceland, Galapagos Islands, and Samoan Islands. The United States is home to two of the largest and best-studied hotspots: Hawai’i and Yellowstone.

2.7.1 Hawaiian Hotspot

Figure description available at the end of the chapter.
Figure 2.56: The Hawaiian–Emperor seamount and island chain. Figure description available at the end of the chapter.

The active volcanoes in Hawai’i represent one of the most active hotspot sites on Earth. Scientific evidence indicates the Hawaiian hotspot is at least 80 million years old. Geologists believe it is actually much older; however any rocks capable of proving this have been subducted under the ocean floor. The big island of Hawai’i sits atop a large mantle plume that marks the active hotspot. The Kilauea volcano is the main vent for this hotspot and has been actively erupting since 1983.

This enormous volcanic island chain, much of which is underwater, stretches across the Pacific for almost 6,000 km. The seamount chain’s most striking feature is a sharp 60-degree bend located at the midpoint, which marks a significant change in plate movement direction that occurred 50 million years ago. The change in direction has commonly been linked to a plate reconfiguration but also to other things like plume migration.

Figure description available at the end of the chapter.
Figure 2.57: Diagram of the Hawaiian hotspot and islands that it formed. Figure description available at the end of the chapter.

In an attempt to map the Hawaiian mantle plume as far down as the lower mantle, scientists have used tomography, a type of three-dimensional seismic imaging. This information—along with other evidence gathered from rock ages, vegetation types, and island size—indicate the oldest islands in the chain are located the furthest away from the active hotspot.

2.7.2 Yellowstone Hotspot

Figure description available at the end of the chapter.
Figure 2.58: The track of the Yellowstone hotspot, which shows the age of different eruptions in millions of years ago. Figure description available at the end of the chapter.

Like the Hawaiian version, the Yellowstone hotspot is formed by magma rising through the lithosphere. What makes this hotspot different, however, is its location under a thick continental plate. Hawai’i sits on a thin oceanic plate, which is easily breached by magma coming to the surface. At Yellowstone, the thick continental plate presents a much more difficult barrier for magma to penetrate. When it does emerge, the eruptions are generally much more violent. Thankfully, they are also less frequent.

More than 15 million years of eruptions by this hotspot have carved a curved path across the Western United States. It has been suggested the Yellowstone hotspot is connected to the much older Columbia River flood basalts and even to 70-million-year-old volcanism found in the Yukon region of Canada.

Figure description available at the end of the chapter.
Figure 2.59: Several prominent ash beds found in North America, including three Yellowstone eruptions shaded pink (Mesa Falls, Huckleberry Ridge, and Lava Creek), the Bisho Tuff ash bed (brown dashed line), and the modern May 18th, 1980, ash fall (yellow). Figure description available at the end of the chapter.

The most recent major eruption of this hotspot created the Yellowstone Caldera and Lava Creek tuff formation approximately 631,000 years ago. The eruption threw 1,000 cubic kilometers of ash and magma into the atmosphere, some of which was found as far away as Mississippi. Should the hotspot erupt again, scientists predict it will be another massive event. This would be a calamity, reaching far beyond the Western United States. These supervolcanic eruptions fill the Earth’s atmosphere with so much gas and ash that they block sunlight from reaching the Earth. Not only would this drastically alter climates and environments around the globe, it could affect worldwide food production.

 

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Summary

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Video 2.4: Plate tectonics

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Plate tectonics is a unifying theory; it explains nearly all of the major geologic processes on Earth. Since its early inception in the 1950s and 1960s, geologists have been guided by this revolutionary perception of the world. The theory of plate tectonics states that the surface layer of the Earth is broken into a network of solid, relatively brittle plates. Underneath the plates is a much hotter and more ductile layer that contains zones of convective upwelling generated by the interior heat of Earth. These convection currents move the surface plates around—bringing them together, pulling them apart, and shearing them side-by-side. Earthquakes and volcanoes form at the boundaries where the ]plates interact, with the exception of volcanic hotspots, which are not caused by plate movement.

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Figure References

Figure 2.1: Detailed map of all known plates, their boundaries, and movements. Eric Gaba. 2006-10, updated 2015-09. CC BY-SA 2.5. https://commons.wikimedia.org/wiki/File:Tectonic_plates_boundaries_detailed-en.svg

Figure 2.2: Wegener later in his life, ca. 1924–1930. Author unknown. ca. 1924 and 1930. Public domain. https://commons.wikimedia.org/wiki/File:Alfred_Wegener_ca.1924-30.jpg

Figure 2.3: Snider-Pellegrini’s map showing the continental fit and separation, 1858. Antonio Snider-Pellegrini. 1858. Public domain. https://commons.wikimedia.org/wiki/File:Antonio_Snider-Pellegrini_Opening_of_the_Atlantic.jpg

Figure 2.4: Map of world elevations. Tahaisik. 2013. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Tahacik.jpg

Figure 2.5: Image showing fossils that connect the continents of Gondwana (the southern continents of Pangea). Osvaldocangaspadilla. 2010. Public domain. https://commons.wikimedia.org/wiki/File:Snider-Pellegrini_Wegener_fossil_map.svg

Figure 2.6: Animation of the basic idea of convection: an uneven heat source in a fluid causes rising material next to the heat and sinking material far from the heat. Oni Lukos. 2006. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Convection.gif

Figure 2.7: GPS measurements of plate motions. NASA. Public domain. https://cddis.nasa.gov/docs/2009/HTS_0910.pdf

Figure 2.8: The complex chemistry around mid-ocean ridges. National Oceanic and Atmospheric Administration (NOAA). https://oceanexplorer.noaa.gov/explorations/04fire/background/chemistry/media/chemistry_600.html

Figure 2.9: The magnetic field of Earth, simplified as a bar magnet. Zureks. 2012. Public domain. https://commons.wikimedia.org/wiki/File:Earth%27s_magnetic_field,_schematic.png

Figure 2.10: This animation shows how the magnetic poles have moved over 400 years. United States Geological Survey (USGS). 2010. Public domain. https://commons.wikimedia.org/wiki/File:Earth_Magnetic_Field_Declination_from_1590_to_1990.gif

Figure 2.11: The iron in the solidifying rock preserves the current magnetic polarity as new oceanic plates form at mid-ocean ridges. USGS. 2011. Public domain. https://commons.wikimedia.org/wiki/File:Mid-ocean_ridge_topography.gif

Figure 2.12: The Wadati-Benioff zone, showing earthquakes following the subducting slab down. USGS. 2013. Public domain. https://commons.wikimedia.org/wiki/File:Benioff_zone_earthquake_focus.jpg

Figure 2.13: J. Tuzo Wilson. Stephen Morris. 1992. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:John_Tuzo_Wilson_in_1992.jpg

Figure 2.14: The layers of the Earth. Drlauraguertin. 2015. CC BY-SA 3.0. https://wiki.seg.org/wiki/File:Earthlayers.png#file

Figure 2.15: The global map of the depth of the Moho. AllenMcC. 2013. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Mohomap.png

Figure 2.16: This mantle xenolith containing olivine (green) is chemically weathering by hydrolysis and oxidation into the pseudomineral iddingsite, which is a complex of water, clay, and iron oxides. Matt Affolter. 2010. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Iddingsite.JPG

Figure 2.17: A polished fragment of iron-rich Toluca meteorite with octahedral Widmanstätten pattern. H. Raab. 2005. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:TolucaMeteorite.jpg

Figure 2.18: Map of the major plates and their motions along boundaries. Scott Nash via USGS. 1996. Public domain. https://commons.wikimedia.org/wiki/File:Plates_tect2_en.svg

Figure 2.19: The lithosphere–asthenosphere boundary changes with certain tectonic situations. Nealey Sims. 2015. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Earth%27s_Inner_Layers_denoting_the_LAB.png

Figure 2.20: General perovskite structure. Perovskite silicates (i.e., bridgmenite, (Mg,Fe)SiO3) are thought to be the main component of the lower mantle, making it the most common mineral in or on Earth. Cadmium. 2006. Public domain. https://en.wikipedia.org/wiki/File:Perovskite.jpg

Figure 2.21: Lehmann in 1932. Even Neuhaus. 1932. Public domain. https://commons.wikimedia.org/wiki/File:Inge_Lehman.jpg

Figure 2.22: The outer core’s spin causes our protective magnetic field. NASA. 2017. Public domain. https://www.nasa.gov/mission_pages/sunearth/news/gallery/earths-dynamiccore.html

Figure 2.23: Passive margin. Joshua Doubek. 2013. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Passive_Contiental_Margin.jpg

Figure 2.24: Schematic of plate boundary types. NOAA via USGS. Public domain. https://oceanexplorer.noaa.gov/facts/plate-boundaries.html

Figure 2.25: Geologic provinces, with the shield (orange) and platform (pink) comprising the craton, the stable interior of continents. USGS. 2005. Public domain. https://commons.wikimedia.org/wiki/File:World_geologic_provinces.jpg

Figure 2.26: Diagram of ocean-continent subduction. K. D. Schroeder. 2016. CC-BY-SA 4.0. https://commons.wikimedia.org/wiki/File:Subduction-en.svg

Figure 2.27: Microcontinents can become part of the accretionary prism of a subduction zone. MagentaGreen. 2014. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Volcanic_Arc_System_SVG_en.svg

Figure 2.28: Accreted terranes of Western North America. Modified from illustration provided by Oceanus Magazine; original figure by Jack Cook, Woods Hole Oceanographic Institution; adapted by USGS. Used under fair use.

Figure 2.29: Location of the large (Mw 8.5-9.0) 1755 Lisbon earthquake. USGS. 2014. Public domain. https://commons.wikimedia.org/wiki/File:1755_Lisbon_Earthquake_Location.png

Figure 2.30: Earthquakes along the Sunda megathrust subduction zone along the island of Sumatra, showing the 2006 Mw 9.1-9.3 Indian Ocean earthquake as a star. USGS. 2007. Public domain. https://commons.wikimedia.org/wiki/File:SundaMegathrustSeismicity.PNG

Figure 2.31: Various parts of a subduction zone. USGS. 2006. Public domain. https://commons.wikimedia.org/wiki/File:Volcanic_Arc_System.png

Figure 2.32: Shallow subduction during the Laramide orogeny. Melanie Moreno. 2006. Public domain. https://commons.wikimedia.org/wiki/File:Shallow_subduction_Laramide_orogeny.png

Figure 2.33: Subduction of an oceanic plate beneath a continental plate, forming a trench and volcanic arc. USGS. 1999. Public domain. https://commons.wikimedia.org/wiki/File:Oceanic-continental_convergence_Fig21oceancont.gif

Figure 2.34: Subduction of an oceanic plate beneath another oceanic plate, forming a trench and an island arc. USGS. 2005. Public domain. https://commons.wikimedia.org/wiki/File:Oceanic-oceanic_convergence_Fig21oceanocean.gif

Figure 2.35: Two continental plates colliding. USGS. 2005. Public domain. https://commons.wikimedia.org/wiki/File:Continental-continental_convergence_Fig21contcont.gif

Figure 2.36: A reconstruction of Pangea, showing approximate positions of modern continents. Kieff. 2009. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Pangaea_continents.svg

Figure 2.37: The tectonics of the Zagros Mountains. Mikenorton. 2010. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:ZagrosFTB.png

Figure 2.38: Pillow lavas, which only form under water, from an ophiolite in the Apennine Mountains of Central Italy. Matt Affolter (Qfl247). 2010. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:ItalyPillowBasalt.jpg

Figure 2.39: Animation of India crashing into Asia. Raynaldi rji. 2015. CC BY-SA 4.0. https://en.wikipedia.org/wiki/File:India-Eurasia_collision.gif

Figure 2.40: Faulting that occurs in divergent boundaries. USGS; adapted by Gregors. 2011. Public domain. https://commons.wikimedia.org/wiki/File:Fault-Horst-Graben.svg

Figure 2.41: The Afar Triangle (center) has the Red Sea ridge (center to upper left), Gulf of Aden ridge (center to right), and East African Rift (center to lower left) form a triple junction that are about 120° apart. Koba-chan. 2005. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Topographic30deg_N0E30.png

Figure 2.42: NASA image of the Basin and Range horsts and grabens across central Nevada. NASA. 2005. Public domain. https://commons.wikimedia.org/wiki/File:Basin_range_province.jpg

Figure 2.43: India colliding into Eurasia to create the modern day Himalayas. USGS. 2007. Public domain. https://commons.wikimedia.org/wiki/File:Himalaya-formation.gif

Figure 2.44: Progression from rift to mid-ocean ridge. Hannes Grobe, Alfred Wegener Institute for Polar and Marine Research; adapted by Lichtspiel. 2011. CC BY-SA 2.5. https://commons.wikimedia.org/wiki/File:Ocean-birth.svg

Figure 2.45: Age of oceanic lithosphere, in millions of years. Muller, R.D., Sdrolias, M., Gaina, C., and Roest W.R. (2008). Age, spreading rates and spreading symmetry of the world’s ocean crust. Geochem. Geophys. Geosyst, 9(Q04006). doi:10.1029/2007GC001743. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Age_of_oceanic_lithosphere.jpg

Figure 2.46: A time progression (with “a” being youngest and “c” being oldest) showing a spreading center getting wider while recording changes in the magnetic field of the Earth. Chmee2. 2012. Public domain. https://commons.wikimedia.org/wiki/File:Oceanic.Stripe.Magnetic.Anomalies.Scheme.svg

Figure 2.47: Black smoker hydrothermal vent with a colony of giant (6’+) tube worms. NOAA. 2006. Public domain. https://commons.wikimedia.org/wiki/File:Main_Endeavour_black_smoker.jpg

Figure 2.48: The two types of transform/strike-slip faults. Cferrero. 2003. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Strike_slip_fault.png

Figure 2.49: Map of the San Andreas fault showing relative motion. Kate Barton, David Howell, and Joe Vigil via USGS. 2006. Public domain. https://commons.wikimedia.org/wiki/File:Sanandreas.jpg

Figure 2.50: A transpressional strike-slip fault, causing uplift called a restraining bend. GeoAsh. 2015. CC BY-SA 4.0. https://commons.wikimedia.org/wiki/File:Restraining_Bend.png

Figure 2.51: A transtensional strike-slip fault, causing a restraining bend. In the center of the fault, a depression with extension would be found. K. Martin. 2013. CC BY-SA 3.0. https://commons.wikimedia.org/wiki/File:Releasing_bend.png

Figure 2.52: Wallace Creek (dry) on the Cariso Plain, California. Robert E. Wallace via USGS. 2014. Public domain. https://commons.wikimedia.org/wiki/File:Wallace_Creek_offset_across_the_San_Andreas_Fault.png

Figure 2.53: Diagram of the Wilson cycle, showing rifting and collision phases. Hannes Grobe. 2007. CC BY-SA 2.5. https://commons.wikimedia.org/wiki/File:Wilson-cycle_hg.png

Figure 2.54: Diagram showing a nonmoving source of magma (mantle plume) and a moving overriding plate. Los688. 2008. Public domain. https://commons.wikimedia.org/wiki/File:Hotspot(geology)-1.svg

Figure 2.55: Map of world hotspots. Foulger. 2011. Public domain. https://commons.wikimedia.org/wiki/File:CourtHotspots.png

Figure 2.56: The Hawaii–Emperor seamount and island chain. Ingo Wölbern. 2008. Public domain. https://commons.wikimedia.org/wiki/File:Hawaii-Emperor_engl.png

Figure 2.57: Diagram of the Hawaiian hotspot and islands that it formed. Joel E. Robinson via USGS. 2006. Public domain. https://commons.wikimedia.org/wiki/File:Hawaii_hotspot_cross-sectional_diagram.jpg

Figure 2.58: The track of the Yellowstone hotspot, which shows the age of different eruptions in millions of years ago. Kelvin Case. 2013. CC BY 3.0. https://commons.wikimedia.org/wiki/File:HotspotsSRP_update2013.JPG

Figure 2.59: Several prominent ash beds found in North America, including three Yellowstone eruptions shaded pink (Mesa Falls, Huckleberry Ridge, and Lava Creek), the Bisho Tuff ash bed (brown dashed line), and the modern May 18th, 1980, ash fall (yellow). USGS. 2005. Public domain. https://commons.wikimedia.org/wiki/File:Yellowstone_volcano_-_ash_beds.svg

Figure Descriptions

Figure 2.1: World map with Pacific Ocean centered in the middle. Numerous tectonic plates are color-coded by outline: lavender outlines convergent boundaries, red outlines divergent boundaries, green outlines transform boundaries, and blue with triangles outlines subduction zones. The cardinal direction of plate movements are shown by small black arrows that are labeled with a number in millimeters per year.

Figure 2.2: Black and white headshot of a man in a suit and tie.

Figure 2.3: Two black and white illustrations side-by-side: the left illustration shows the world globe with eastern South America and western Africa connected, labeled as “Avant la separation.” The right illustration shows the world globe with South America and Africa separated by an ocean, labeled as “Apres la separation.”

Figure 2.4: World map color-coded by elevation. The ocean basins are dark blue except for the mid-ocean ridges and ocean margins which are light blue. The continents are green at low elevations and red to brown at higher elevations.

Figure 2.5: Illustration showing five continents connected. From the left to right, there are South America, Africa, India above Antarctica, and Australia. Overlain on the continents are color-coded tracks of various fossil evidence: a tan band across South America and Africa shows the extent of fossil evidence for Cynognathus, a Triassic therapsid approximately 3 meters long. A gray band across southern Africa, India, and Antarctica shows the extent of fossil evidence for the Triassic therapsid Lystrosaurus. A green band across southern South America, southern Africa, India, Antarctica, and Australia (all of the southern continents) shows the extent of fossil evidence for the fern Glossopteris. A blue band across southern South America and southern Africa shows the extent of fossil evidence for the freshwater reptile Mesosaurus.

Figure 2.6: An animation showing two circles rotating next to each other. The left circle is rotating counterclockwise while the right circle is rotating clockwise. At the bottom center of the animation is an animated flame that represents a heat source from below.

Figure 2.7: World map that has many red dots in various places around the world. Each dot is connected to a black arrow of variable length that represents the plate motion measured at the dot in centimeters per year.

Figure 2.8: Diagram showing a cross section of a mid-ocean ridge underwater. Volcanic heat is coming out of the mid-ocean ridge which is drawn like a cloud. Inside the cloud are many different chemicals. There are also arrows going from the water into the ridge, labeled “seawater” where it enters the ground and labeled “evolved seawater” as it reaches the mid- ocean ridge axis. The arrows are also labeled with many different chemicals. Deeper below the ridge is a red oval shape labeled “Magma 1200 degrees C.”

Figure 2.9: World globe with a dipole bar magnet superimposed on it, aligned roughly with Earth’s axis of rotation. The north end of the magnet points toward the South Pole while the south end of the magnet points toward the North Pole. There are also black curved lines coming out of the Earth’s axis, forming magnetic loops.

Figure 2.10: Animation of magnetic field lines superimposed on a world map. The lines move on the map as the animation goes from the year 1590 to 1990.

Figure 2.11: Animated gif depicting a mid-ocean ridge with two oceanic plates moving away from the center of the ridge. As the movement progresses, symmetrical magnetic stripes appear on each side of the ridge.

Figure 2.12: Cross section of an oceanic tectonic plate colliding with a continental tectonic plate. There’s a diagonal zone of red X’s that descend from the trench at the surface, labeled “Benioff Zone.” Each X represents an earthquake focus.

Figure 2.13: Headshot of an older man wearing a suit and tie.

Figure 2.14: From core to surface: Inner core (solid), outer core (liquid), mantle (including asthenosphere), crust (including lithosphere)

Figure 2.15: World map with the Moho depth color coded on the map: red is the deepest while blue is the shallowest. The Moho is deepest under central Asia and western South America, and the Moho is shallowest under the world ocean basins.

Figure 2.16: Photograph of a piece of basalt with a xenolith on top, sitting on a black and white scale with inches on the left and centimeters on the right. The xenolith consists of olive-green crystals and the basalt is gray-black. The entire sample is approximately 1.5 inches long.

Figure 2.17: Photograph of a cut and polished face of a silvery gray meteorite. There is a distinct pattern of criss-crossing lines on the polished surface.

Figure 2.18: World map with the largest tectonic plates outlined and filled in with a different color for each plate: the Eurasian Plate is colored green, the North American Plate is gray, the Australian Plate is orange, the Filipino Plate is red, the Pacific Plate is yellow, the Juan de Fuca and Cocos Plates are blueish purple, the Nazca Plate is light blue, the Antarctic Plate is dark blue, the Scotia Plate is medium blue, the Caribbean plate is pinkish orange, the South American Plate is purple, the African Plate is dark orange, the Arabian Plate is yellow, and the Indian Plate is dark red.

Figure 2.19: From core to surface: Inner core, outer core, asthenosphere (part of ductile mantle), LAB, upper solid mantle, lithosphere, oceanic crust, continental crust. Mid ocean ridges form from the asthenosphere.

Figure 2.20: Array of atoms in a cubic three-dimensional framework of an imaginary perovskite. The red atoms are oxygen anions which are connected to the blue central atoms, which designate smaller cations. There are also green atoms organized in rows in the blank space which represent the larger cations.

Figure 2.21: Antique photo of young woman wearing a sweater.

Figure 2.22: Diagram of Earth as a globe with a pie-shaped piece cut out of the crust to act as a window to view the interior. The mantle is inside of the crust, the liquid outer core is inside of the mantle, and the solid inner core is inside the innermost part of the globe. The diagram also shows the solid inner core rotating in a counterclockwise direction as viewed from the North Pole. There are black lines extending from the inner core toward the North Pole and they are fanned out, each showing the yearly locations of the magnetic North Pole from 1990 to 1996.

Figure 2.23: Cross section of a passive margin under water. Continental crust is in pink on the left-hand side with a line labeled “Paleozoic DFW” pointing to the continental crust. Connected to the right of the continental crust is transitional crust in orange, and connected to that is oceanic crust in brown. A yellow wedge of passive margin sediments lays on top of the crust and a double-sided arrow is above the passive margin sediments that’s labeled “Hinge Zone.” An arrow points to the passive margin sediments that says “Thickest section of sediments are deposited adjacent to the continents, above the transitional crust, in the region that becomes the hinge zone. Can be up to 20 km thick.”

Figure 2.24: 3D diagram showing a cross section into Earth’s crust. On the left-hand side is a convergent plate boundary, with a plate of oceanic crust colliding into another plate of oceanic crust. The oceanic crust on the right-hand side subducts toward the left and a line of volcanoes forms on the overriding oceanic plate as a volcanic island arc. To the right of that, there is a shield volcano on the lithosphere beneath the ocean with a hot spot feeding the volcano from below. To the right of the shield volcano, there is a divergent plate boundary where two oceanic plates move away from each other. There is a transform plate boundary labeled to the left of the divergent boundary. To the right of the divergent boundary, oceanic crust moves toward the right, colliding with continental crust. The oceanic crust subducts beneath the continental crust, forming a chain of continental volcanoes on top of the continental crust. To the farthest right of the diagram, there is a continental rift zone where the continental crust is splitting apart.

Figure 2.25: World map with geologic provinces color-coded: Shield are colored orange and are seen on northern North America, eastern South America, northwestern Europe, northern and southern Asia, northwestern Australia, and sub-Saharan and southern Africa. Platform are colored pink and are seen near the same locations as shield with the exception of large platforms covering most of northern Asia and Europe. Orogen are colored cyan and are seen along western North America, western South America, the northwestern edge of Africa, southern Europe, southeastern Australia, and southern, central, and northeastern Asia. Basin are colored blue and are seen as thin strips in central-west North America, central-west South America, southern and northeastern Asia, and small spots in central and northwestern Africa. Large igneous province is colored purple and are seen as small blobs in western North America, eastern South America, Iceland, eastern Africa, central India, and northern Asia. Extended Crust are colored yellow and are seen on the margins of all of the continents.

Figure 2.26: 3D diagram showing oceanic crust moving toward the right where it collides with continental crust and subducts down beneath it. Above the contact between the two plates, there is an ocean trench and accretionary prism to the right of the trench. There is a volcanic arc on top of the continental plate, above where the oceanic crust has subducted beneath it. Rising diapirs are labeled below the volcanic arc. The Moho discontinuity is marked by a green line at the base of the crust in both tectonic plates, above the solid uppermost mantle.

Figure 2.27: Cross section schematic showing oceanic crust subducting beneath another tectonic plate. Above the contact between the two plates, there is an ocean trench and accretionary prism. There is a volcanic front on top of the overriding plate which makes up a microcontinent, above where the oceanic crust has subducted beneath it. Ascending diapirs are labeled below the volcanic front. There are ocean basins on either side of the microcontinent.

Figure 2.28: Color-coded tectonic map of western North America and the eastern Pacific Ocean, showing accreted terranes and plate tectonic motion. The color coding is as follows: continental interior of North America is tan, attached fragments of land are green, ancient ocean floor that accreted is blue, submarine deposits that accreted are yellow, and island arcs that accreted are pink.

Figure 2.29: Map of the western coast of Portugal, Spain, and Morocco, showing an east-west trending fault that goes through the Strait of Gibraltar. A red star labels the location of the epicenter of the 1755 earthquake, located just south of the fault line in the North Atlantic Ocean.

Figure 2.30: Color-coded tectonic map centered on the island of Sumatra with numerous dots showing the locations of earthquakes along a northwest- southeast-trending subduction zone. The color coding is as follows: shallow earthquakes are orange and yellow dots, and deep earthquakes are blue, purple, and red dots. Generally, shallow earthquakes are toward the southwest while deep earthquakes are toward the northeast. An orange star marks the location of the 2006 Indian Ocean earthquake.

Figure 2.31: Cross sectional diagram showing a mid-ocean ridge on the left-hand side. On the right-hand side is oceanic floor moving toward the left which subducts when it collides with the other oceanic crustal plate. Above the subduction zone in the center of the diagram, a volcanic front forms, which are volcanic islands on oceanic crust. At the top of the diagram are the following labels from left to right: ocean basin, backarc, volcanic front, forearc, ocean basin.

Figure 2.32: Block diagram showing oceanic crust moving toward the right where it collides with continental crust and subducts down beneath it. Because the angle of subduction is shallow, the ocean crust travels inland before creating a volcanic arc on top of the continental plate, above where the oceanic crust has subducted beneath it–these are the Rocky Mountains.

Figure 2.33: Block diagram showing oceanic crust moving toward the right where it collides with continental crust and subducts down beneath it. Above the contact between the two plates, there is an ocean trench. There is a volcanic arc on top of the continental plate, above where the oceanic crust has subducted beneath it.

Figure 2.34: Block diagram showing an oceanic plate moving toward the right where it collides with another oceanic plate and subducts down beneath it. Above the contact between the two plates, there is an ocean trench. There is a volcanic island arc on top of the overriding oceanic plate, above where the oceanic crust has subducted beneath it.

Figure 2.35: Block diagram showing a continental plate moving toward the right where it collides with another continental plate and collides with it. Above the contact between the two plates, there is a mountain range with a high plateau. There is no subduction or volcanism occurring.

Figure 2.36: Map of crescent-shaped Pangaea with all of the modern continents placed together: Eurasia is located at the top of the map, followed by North America to the lower left of Eurasia, South America below North America, Africa to the right of South America, India to the right of Africa, Antarctica below India and Africa, and Australia to the lower right of Antarctica and India.

Figure 2.37: Annotated satellite image of the Arabian Plate next to the Eurasian Plate with the Persian Gulf Basin and Mesopotamian Basin between the two plates. Tectonic faults run northwest-to-southeast on the image and are labeled and colored as follows: the Main Zagros Reverse Fault in yellow on the Eurasian Plate, the Main Recent Fault in orange on the Eurasian plate, and the High Zagros Fault in lavender on the Eurasian Plate.

Figure 2.38: An outcrop of medium-gray rocks that have bulbous texture which are old cooled pillow lavas.

Figure 2.39: Animation of India crashing into Asia. The animation begins at 60 million years ago, progressing every 5 million years until present day. Throughout the animation, the Indian plate travels toward the rest of the Asian plate until it begins colliding around 45 million years ago. After colliding, a collision zone between the Indian Plate and Asia Plate grows a mountain range which is the present-day Himalayas.

Figure 2.40: Block diagram showing flat-lying layers being pulled apart, forming normal faults throughout the diagram that allow some blocks to drop down called grabens between high blocks called horsts.

Figure 2.41: Topographic map showing the Afar Triangle, a low area bordering on the Red Sea. It is part of the Great Rift Valley in East Africa. The area overlaps the borders of Eritrea, Djibouti and the entire Afar region of Ethiopia. The connecting three arms form a triple junction. The northernmost branching arm extends north through the Red Sea and into the Dead Sea, while the eastern arm extends through the Gulf of Aden and connects to the Mid-Indian Ocean ridge further to the east. Both of these rifting arms are below sea level and are similar to a mid-ocean ridge. The third rifting arm runs south through the countries of Kenya, Uganda, the Democratic Republic of Congo, Rwanda, Burundi, Tanzania, Zambia, Malawi and Mozambique.

Figure 2.42: Satellite photo of a tan landscape that has long ridges and valleys.

Figure 2.43: Drawing of a map showing the northward path that the India land mass and Sri Lanka took from 71 million years ago to today. The path shows the India land mass moving closer and closer to the Eurasian plate until it collides. Sri Lanka is located just south of the India land mass and also travels in the same path, but has not collided with the Eurasian plate.

Figure 2.44: Three cross sectional diagrams showing the progression from a rift valley to a mid-ocean ridge. In the first diagram, the cross section shows a rift that’s splitting apart a land mass with the analogy of the present-day African rift valley. In the second diagram, the cross section shows a new ocean basin after the rift has spread enough that sea water fills it in, with the analogy of the present-day Red Sea. In the third and final diagram, the cross section shows a mature ocean basin after the rift has spread so far that the spreading center has now become a mid-ocean ridge, with the analogy of the present-day Atlantic Ocean.

Figure 2.45: Color-coded world map that shows the various ages of oceanic lithosphere. Continents are in gray. The color-coding and locations are as follows: the youngest oceanic lithosphere is 0 million years old and runs along the centers of the ocean basins where there are mid-ocean ridges, colored in red. Oceanic lithosphere ages get older away from the mid- ocean ridges, and the oldest oceanic lithosphere is 280 million years old near continental margins, colored purple.

Figure 2.46: A series of 3 block diagrams showing a time progression of a spreading center getting wider and wider while the magnetic field of the Earth flips back and forth, being recorded in the currently-forming igneous rocks at the mid-ocean ridge.

Figure 2.47: A black smoker hydrothermal vent at the bottom of the sea floor. There is a plume of black smoke coming from a cone-shaped extrusion of rock and a colony of tube worms are attached to the cone-shaped rock.

Figure 2.48: Sinistral (left-lateral) strike-slip fault: top block moves left and overhangs bottom block that is moving right. Dextraal (right-lateral) strike-slip fault: top block moves right and overhangs bottom block that is moving left.

Figure 2.49: Map of western North America annotated with the location of the main San Andreas fault which runs from northwest of the Canadian coast, through western California, and southeast through Mexico. There are arrows on either side of the fault line showing relative movement: on the east side of the fault, movement is toward the lower right and on the west side of the fault, movement is toward the upper left.

Figure 2.50: Line drawing of an overhead view of a transpressional strike-slip fault. The fault has a bend in it, causing separation of the line with an uplift inside. The left-hand side of the drawing shows the plate moving to the upper left while the right-hand side of the drawing shows the plate moving to the lower right.

Figure 2.51: Line drawing of an overhead view of a transtensional strike-slip fault. The fault has a bend in it. The left-hand side of the drawing shows the plate moving to the upper left while the right-hand side of the drawing shows the plate moving to the lower right.

Figure 2.52: Aerial photo of a landscape in California. A dry creek flows from the northern mountainous part of the image, then takes a sharp right as viewed from the flow of water, then a sharp left, caused by the San Andreas Fault cutting roughly perpendicular to the creek. The fault can be seen about halfway down, trending left to right, as a change in the topography.

Figure 2.53: Rectangular diagram with a scale bar along the bottom labeled “million years.” On the left end of the scale is the number 1,000 and on the right end is the number 0 (present day). Starting at the left-hand side, the following labels are on the diagram: “inner ocean” around 950 million years, “mountain forming” around 800 million years, “Rodinia” around 660 million years, “Iapetus Ocean” around 500 million years, “Mountain forming” around 300 million years, “Pangaea” around 180 million years, and “Atlantic Ocean” around 50 million years.

Figure 2.54: Two cross sectional diagrams: the top diagram shows horizontal layers with a magma plume rising vertically through them and a volcano on top of the layers. The second diagram shows horizontal layers with the top layer moving toward the left; a magma plume rises vertically through them and a chain of volcanoes is formed on the top layer which is moving toward the left as the magma plume creates volcanoes on top.

Figure 2.55: World map showing locations of hot spots with various sizes according to how active they are. The largest circles are located in the following places on the map: there are five large circles in the Pacific Ocean including Hawaii, there are two large circles in the Atlantic Ocean including Iceland, and there are two large circles in/near the Indian Ocean including the Afar Triangle. Smaller dots are scattered throughout the world ocean basins with some on continental interiors such as Yellowstone.

Figure 2.56: Map of the Hawaii-Emperor seamount chain and seafloor topography. The Aleutian trench and islands run approximately east-to-west along the top of the map, the Emperor seamount chain runs approximately north-to- south near the left-hand side of the map, and the Hawaiian seamount chain runs approximately west-northwest-to-east-southeast near the bottom of the map.

Figure 2.57: Cross sectional diagram showing the Pacific plate moving toward the left of the diagram with the labels “NW” at the far left and “SE” at the far right. At the right-hand side of the diagram, a vertical mantle plume rises up from deep down, through the asthenosphere, and spreads laterally outward when it reaches the base of the lithosphere. Smaller vertical magma intrusions rise through the lithosphere, creating three volcanoes labeled Mauna Loa, Kilauea, and Lo’ihi. Arrows on the lithosphere point toward the left, indicating the direction that the Pacific Plate is traveling over the mantle plume. Along the top of the diagram is the label “Volcanoes are progressively older” with arrows to the left. There is a chain of volcanic islands on top of the Pacific Plate: from left to right or oldest to youngest, they are Ni’hau and Kaua’i which are labeled 5.6-4.9 Ma, O’ahu labeled 3.4 Ma, Moloka’i labeled 1.8 Ma, Maui labeled 1.3 Ma, and Hawai’i labeled 0.7-0 Ma.

Figure 2.58: Shaded relief map centered on Idaho, with small portions of the surrounding states shown too. The track of a hot spot is annotated on the map and color-coded at each past location. The hotspot started near the Idaho-Oregon-Nevada border with the label 16.1 which indicates it was there 16.1 million years ago, then moved relatively east-northeastward toward its present location near the Wyoming-Idaho-Montana border which is labeled 0.6-2.1 which indicates it has been there 2.1 to 0.6 million years ago. Note that the North American plate was moving over the hot spot, not that the hot spot was moving under North America.

Figure 2.59: Map of the United States with state borders outlined. Prominent ash beds are outlined and color-coded, including three Yellowstone eruptions shaded pink. One of the pink outlines is labeled Mesa Falls ash bed and encircles most of the states of Wyoming, Colorado, Kansas, and Nebraska, and partially encircles the states Montana, South Dakota, Oklahoma, and Texas. Another pink outline is labeled Huckleberry Ridge ash bed and encircles the a large western portion of the United States. The third pink outline is labeled Lava Creek ash bed and encircles most of the western half of the United States. There is also a brown dashed outline labeled “Bishop ash bed” which encircles the entire southwest portion of the United States. There is a yellow elongated outline labeled “Mount St. Helens ash 1980” which covers a east-west-trending portion of southern Washington state.

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Introduction to Earth Science, Second Edition Copyright © 2025 by Laura Neser is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License, except where otherwise noted.

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