Plate Tectonics: Boundaries, Motions, Magnetic Records, Plumes and Numericals

This chapter answers the Part A heading “Plate Tectonics” of the Geology and Geophysics (GG) paper: “Type of plate boundaries; Plate motions and driving mechanisms; Processes at plate boundaries - volcanism, seismicity, orogenesis, sea-floor spreading and magnetic anomalies and paleomagnetism, formation of back-arc basins; Continental rifting, mantle plumes, hotspots; Numerical problems related to plate motions”. It teaches the three boundary types, Euler-pole motion and the driving forces, the magnetic record of sea-floor spreading and paleomagnetism, the processes at ridges, subduction zones and collisions, back-arc basins, rifts, plumes and hotspot tracks. The numericals are spreading rates from anomaly ages and distances, relative velocity about an Euler pole, paleolatitude from inclination (tan I = 2 tan λ), the age of a seamount chain, and subduction time and trench distance.

1. Plates and the types of plate boundary

The lithosphere is broken into rigid plates that move over the weak asthenosphere: usually counted as seven major ones (Pacific, North American, South American, Eurasian, African, Indo-Australian and Antarctic) and several minor ones such as Nazca, Cocos, Caribbean, Philippine Sea, Arabian and Juan de Fuca. Plate interiors are stable; almost all earthquakes, volcanoes and mountain building are concentrated at the boundaries. There are three types, distinguished by relative motion.

The three types of plate boundary
TypeRelative motion and resultExamples
DivergentPlates move apart; new lithosphere forms; ridge or rift with shallow normal-fault earthquakes and basaltMid-Atlantic Ridge, East Pacific Rise, East African Rift
Convergent: ocean–ocean and ocean–continentDenser oceanic plate subducts; trench, volcanic arc, Benioff zone and great thrust earthquakesMariana, Aleutian, Andes, Andaman–Sumatra
Convergent: continent–continentBuoyant continental lithosphere does not subduct; collision thickens the crust to form an orogen and a sutureHimalaya, Alps
TransformPlates slide past each other; lithosphere is neither created nor destroyed; strike-slip faultingSan Andreas Fault, Alpine Fault of New Zealand

A transform fault joins two ridge segments, or a ridge and a trench; it is active only between the offset ridge crests, and its inactive prolongation is a fracture zone. A triple junction is a point where three plates meet, as at Afar, where the Red Sea, the Gulf of Aden and the Main Ethiopian Rift meet. India shows two convergent types: the Himalaya is the collision of India with Eurasia, and the Andaman–Nicobar–Sumatra margin is a subduction zone where the Indian plate descends beneath the Burma–Sunda side (the 2004 Sumatra–Andaman earthquake, magnitude about 9.1, ruptured it).

2. Plate motions and Euler poles

By Euler’s theorem the motion of one rigid plate relative to another on a sphere is a rotation about an axis through the centre of the Earth. Its surface end is the Euler pole and the rate is the angular velocity ω. At angular distance θ from the pole the linear speed is v = ω R sin θ, with ω in radians per unit time: zero at the pole and greatest 90° from it. Along a ridge the spreading rate therefore changes with distance from the pole, and transform faults lie along small circles about it. With R = 6,371 km, 1° of arc is 111.2 km, and 1 cm/yr = 10 mm/yr = 10 km/Myr.

The full spreading rate is the rate at which the two plates separate; the half rate is the rate of each away from the axis, and with symmetric spreading the full rate is twice the half rate. Typical full rates are about 2 to 4 cm/yr on the Mid-Atlantic Ridge and up to about 15 cm/yr on the East Pacific Rise; plate speeds are 1 to 10 cm/yr. India now moves north-north-east at about 5 cm/yr, but moved at 15 to 20 cm/yr before the collision. Relative velocities come from magnetic anomalies, transform azimuths and GPS, and add as vectors: two plates moving directly toward each other at 4 and 3 cm/yr in some fixed frame converge at 7 cm/yr. Absolute motion needs a frame such as the hotspot frame.

3. Driving mechanisms

The plates are the cold, strong upper boundary layer of mantle convection, and the forces that move them are part of that convection. Slab pull is the pull on a plate by the cold, dense subducting slab that is attached to it, and is generally the largest force. Ridge push is the gravitational push from the elevated ridge, and from the lithosphere sliding down the thickening lithosphere–asthenosphere boundary as it ages; it is several times smaller. Mantle drag at the base can drive or resist, depending on the mantle flow, and trench suction draws the overriding plate toward the trench. Resisting forces are friction on the subduction interface, collision and the viscous resistance of the mantle to the sinking slab.

The evidence is in the speeds. Plates attached to long subducting slabs, such as the Pacific, Nazca and Indo-Australian plates, move fastest, while plates with little subducting margin, such as the African, North American and Antarctic plates, move slowest; speed follows the length of subducting margin rather than the area of the plate. Oceanic lithosphere cools as it ages and after some tens of millions of years is denser than the asthenosphere below, so it can sink.

⚠️ Plates are not rafts on convection cells
The old picture of plates carried passively like a conveyor belt on convection cells is not the accepted one. Plates are the cold boundary layer of the convection, and slab pull and ridge push are the way that convection acts on them. Mantle drag matters less than slab pull.

4. Sea-floor spreading, magnetic anomalies and paleomagnetism

Hess (1960–62) proposed that new crust forms at ridges, moves sideways and is consumed at trenches. The evidence is that sea-floor age rises symmetrically away from ridge axes and in the main ocean basins nowhere exceeds about 200 Ma, sediment is thin near the ridge and thickens away, and the floor deepens as it ages. Basalt acquires a thermoremanent magnetisation as it cools through the Curie temperature (about 580 °C for magnetite) in the direction of the field of that moment. The field reverses at irregular intervals; the last reversal, Brunhes–Matuyama, was about 0.78 Ma.

A ship-towed magnetometer measures the total field and subtracts a regional model. A positive anomaly marks crust magnetised in the present (normal) direction, whose field adds to the present field; a negative anomaly marks reversed crust. The result is a pattern of stripes parallel to the ridge and symmetric about it (Vine and Matthews, and Morley, 1963). Matching the stripes with the dated polarity time scale gives the age of the floor and the spreading rate: half rate = x/t, full rate = 2x/t, where x is the distance of an anomaly of age t from the axis. A distance of 1 km in 1 Myr is 1 mm/yr.

Paleomagnetism reads the field direction frozen into rocks. Averaged over many thousands of years, the field behaves as a geocentric axial dipole, so the inclination I and the latitude λ at which the rock formed are related by tan I = 2 tan λ: I is 0° at the equator and 90° at the pole. For normal polarity I is positive (downward) in the northern hemisphere and negative in the southern; reversed polarity flips both signs. The declination points toward the paleopole. Inclination gives paleolatitude but not paleolongitude, because the axial dipole field is the same at all longitudes. Apparent polar wander paths of different continents merge when the continents are reconstructed together. For example, a normal-polarity basalt now at 10° N with I = 45° has tan λ = 0.5, so λ = 26.6° N: its plate has moved 16.6°, about 1,840 km, southward since it formed.

5. Processes at plate boundaries

Ridges. Upwelling peridotite melts by decompression, giving tholeiitic basalt (MORB), and the crust is pierced by shallow, small, normal-fault earthquakes. Subduction zones have a trench, a forearc, a volcanic arc and often a back-arc. The slab descends along a dipping Benioff–Wadati zone of earthquakes reaching about 700 km, the deepest earthquakes on Earth. Water released from the slab at about 100 km depth lowers the melting point of the mantle wedge (flux melting), and the calc-alkaline, andesitic arc volcanoes stand where the slab is about 100 to 120 km deep. The locked plate interface, the megathrust, generates the largest earthquakes.

Orogenesis is of two kinds. At ocean–continent margins the Andean (cordilleran) type combines a magmatic arc with a fold-and-thrust belt. In collision orogens, after the ocean has closed, buoyant continental lithosphere is thickened (crust about 70 km), thrust sheets stack up, and a suture marks the join: in the Himalaya the Main Frontal, Main Boundary and Main Central Thrusts and the Indus–Tsangpo Suture. The India–Eurasia collision began about 50 Ma and continues.

Back-arc basins form by extension of the overriding plate behind an island arc. The cause is slab rollback: when an old, steep slab sinks faster than the plates converge, the trench retreats toward the ocean and stretches the plate behind the arc, until new oceanic crust forms by back-arc spreading, as in the Mariana Trough, Lau Basin, Sea of Japan and Andaman Sea. Uyeda and Kanamori’s two end types summarise it: Mariana type (old, steep slab, rollback, extensional back-arc) and Chilean type (young, buoyant, shallow slab, strong coupling, compression, great earthquakes, no back-arc basin).

6. Continental rifting, mantle plumes and hotspots

Rifting thins and breaks continental lithosphere. In active rifting a hot mantle upwelling first domes the crust and then drives the extension; in passive rifting far-field extensional stress thins the lithosphere and volcanism follows. The stages are thinning, normal faulting that makes grabens, bimodal and alkaline volcanism, and, if extension continues, breakup with new oceanic crust and passive margins. Examples are the East African Rift, Baikal, Rio Grande and Rhine, and the Red Sea and Gulf of Aden are young oceans formed this way.

A mantle plume is a narrow, hot, buoyant upwelling from deep in the mantle, possibly from the core–mantle boundary, with a large head and a thin tail. The head melts by decompression and erupts flood basalts, such as the Deccan Traps of about 66 Ma. As a plate moves over the nearly fixed tail, it leaves a hotspot track, a chain of volcanoes that age away from the active one: the Hawaiian–Emperor chain has its bend at about 47 Ma, and the Deccan–Réunion track runs through the Chagos–Laccadive Ridge and Mascarene Plateau to the active volcano at Réunion. Evidence for plumes includes age-progressive chains, large swells, high ³He/⁴He ratios and low-velocity columns in tomography.

⚠️ A hotspot is not a plate boundary, but it can sit on one
Hawaii lies within the Pacific plate, Yellowstone within a continent, and Iceland sits on the Mid-Atlantic Ridge, where a plume and a ridge coincide. The track gives the direction and speed of the plate over the plume, not the speed of the plume. Not every hotspot is proved to be a deep plume.

7. Numerical problems on plate motions

Relations for plate-motion numericals
ProblemRelationCare needed
Spreading rateHalf rate = x/t; full rate = 2x/tState which rate; 1 km/Myr = 1 mm/yr
Velocity about an Euler polev = ω R sin θUse radians, or 1° = 111.2 km
Paleolatitudetan λ = ½ tan I; distance = Δλ × 111.2 km/°Sign of I depends on polarity and hemisphere
Hotspot chainAge t = d/vv is the plate speed over the plume
SubductionSlab length = depth/sin(dip); time = length/rate; horizontal distance = depth/tan(dip)Slab assumed to move along its dip at the convergence rate

Spreading. An anomaly of age 20 Ma lies 480 km from the axis on one side: half rate 480/20 = 24 km/Myr = 24 mm/yr, full rate 48 mm/yr. Euler pole. For ω = 0.6°/Myr and a point 40° from the pole, v = 0.6 × 111.2 × sin 40° = 42.9 km/Myr = 4.3 cm/yr. Hotspot chain. A seamount 1,500 km from the active volcano is 25 Myr old, so the plate speed is 60 km/Myr = 6 cm/yr, and a seamount 2,100 km away is 2,100/60 = 35 Myr old.

Subduction. A slab dips at 30° and plunges at 6 cm/yr = 60 km/Myr. To reach 300 km depth it travels 300/sin 30° = 600 km, which takes 600/60 = 10 Myr, and a volcano above that depth stands 300/tan 30° = 520 km horizontally from the trench. At a more typical arc depth of 120 km and the same dip the distance is 208 km. Always check the units of the angle and of the rate before computing.

⚠️ Common slips
Quoting the half rate when the question asks for the full rate (a factor of 2); using degrees where radians are needed in ω R sin θ; using the sign of the inclination without checking the polarity; and dividing the depth, not the slab length, by the convergence rate.

Key takeaways

  • There are three boundary types: divergent (new lithosphere), convergent (ocean–ocean, ocean–continent, continent–continent) and transform (neither created nor destroyed). Transforms lie along small circles about the Euler pole, and triple junctions join three plates.
  • Plate motion is rotation about an Euler pole, v = ω R sin θ, with 1° = 111.2 km and 1 cm/yr = 10 km/Myr. Slab pull is the largest driving force, ridge push is smaller, and plates are the cold boundary layer of mantle convection.
  • Magnetic stripes are symmetric about ridges: positive anomalies are normally magnetised crust. Half rate = x/t and full rate = 2x/t. Paleomagnetism uses tan I = 2 tan λ to give paleolatitude, not paleolongitude, and reverses signs with polarity.
  • Ridges melt by decompression to MORB; arcs melt by water released from the slab, above a Benioff zone to about 700 km. Collision orogens thicken crust to about 70 km, as in the Himalaya. Back-arc basins form by slab rollback in Mariana-type subduction.
  • Rifts are active (plume doming first) or passive (far-field stress), ending in breakup if extension continues. A mantle plume has a head that erupts flood basalts (Deccan) and a tail that makes an age-progressive hotspot track (Réunion to the Chagos–Laccadive Ridge).
  • Numericals: t = d/v for seamount chains, slab length = depth/sin(dip) and time = length/rate, trench distance = depth/tan(dip). Check the half or full rate, the units and the polarity before computing.

Practice questions (17)

Attempt each one before opening the answer. Every explanation names the tempting wrong option as well as the right one, because that is where marks are lost.

  1. At which type of plate boundary is lithosphere neither created nor destroyed, the plates sliding past each other?

    1. A divergent boundary such as the Mid-Atlantic Ridge
    2. A convergent boundary such as the Andean trench
    3. A transform boundary such as the San Andreas Fault
    4. A collisional boundary such as the Himalaya
    Show answer

    Answer: C — A transform boundary such as the San Andreas Fault

    At a transform boundary the plates slide horizontally past each other along a strike-slip fault, so no lithosphere is made or consumed. Ridges make it, and subduction and collision consume or thicken it.
  2. Which pairing of a feature with its plate-boundary setting is correct?

    1. The Himalaya: ocean–ocean convergence producing an island arc
    2. The East African Rift: an incipient divergent boundary within a continent
    3. The Mid-Atlantic Ridge: a transform boundary along which plates slide past
    4. The Andes: continent–continent collision with no subduction
    Show answer

    Answer: B — The East African Rift: an incipient divergent boundary within a continent

    The East African Rift is continental extension that may lead to a new ocean. The Himalaya is a continent–continent collision, the Mid-Atlantic Ridge is divergent (offset by transforms), and the Andes are an ocean–continent subduction margin.
  3. Plates attached to long subducting slabs (Pacific, Nazca, Indo-Australian) move fastest, while plates with little subducting margin (African, Antarctic) move slowest. Which driving force does this pattern most strongly support?

    1. Ridge push, since the plates with the longest ridge margins are the ones that move fastest
    2. Basal drag proportional to plate area, since the largest plates are the ones that move fastest
    3. Tidal drag from the Moon, which pushes every plate steadily westward at much the same speed
    4. Slab pull, the negative buoyancy of the cold, dense slab pulling the plate along
    Show answer

    Answer: D — Slab pull, the negative buoyancy of the cold, dense slab pulling the plate along

    Fast plates are those with a long subducted slab, which points to slab pull. Plates with long ridge margins, such as the African and Antarctic plates, are slow, which contradicts ridge push as the main force. Basal drag proportional to area would make the large African, Eurasian and Antarctic plates fast, but they are slow, and a Moon-driven westward push would not distinguish between plates.
  4. Which of the following statements about the forces that drive plate motion are correct?

    1. Plate motion is driven mainly by the Coriolis force that arises from the rotation of the Earth
    2. Slab pull is the force exerted on a plate by the cold, dense subducting slab attached to it
    3. A subducting slab sinks because it is hotter, and therefore denser, than the surrounding mantle
    4. Ridge push arises from the raised ridge and the plate sliding down the thickening base of the lithosphere
    Show answer

    Answer: B — Slab pull is the force exerted on a plate by the cold, dense subducting slab attached to it; D — Ridge push arises from the raised ridge and the plate sliding down the thickening base of the lithosphere

    Slab pull and ridge push are both real driving forces, with slab pull the larger. The Coriolis force is far too weak and is not the driver. A slab sinks because it is colder, and therefore denser, than the mantle around it, since a hotter body would be less dense.
  5. A magnetometer towed over the sea floor records a positive magnetic anomaly over a stripe of oceanic crust. What does this indicate?

    1. The crust there was magnetised during a reversed interval, and its field reinforces the present field of the Earth
    2. The crust there is magnetised in the present field’s direction, so its field adds to the present field
    3. The crust there is the youngest crust at the ridge crest, whatever direction it happened to be magnetised in
    4. The crust there has lost its magnetisation, because it was later heated above the Curie temperature of its minerals
    Show answer

    Answer: B — The crust there is magnetised in the present field’s direction, so its field adds to the present field

    A positive anomaly is the sum of the field of the crust and the regional field, which is larger where the crust is magnetised in the same (normal) direction as the present field. Reversed crust subtracts and gives a negative anomaly. The age of the crust does not fix the sign, and crust that had lost its magnetisation would give no anomaly.
  6. A magnetic anomaly of age 20 Ma lies 480 km from the ridge axis on one flank, and spreading is symmetric. The full spreading rate, in mm/yr, is ____.

    Numerical answer — type the value.

    Show answer

    Answer: 48

    Half rate = 480 km/20 Myr = 24 km/Myr = 24 mm/yr, because 1 km/Myr is 1 mm/yr. The full rate is twice the half rate, 48 mm/yr. Quoting 24 gives the half rate.
  7. A basalt formed under a geocentric axial dipole field has a well-determined mean inclination and declination. Which statement about what it constrains is correct?

    1. Inclination gives paleolatitude, but paleolongitude is not constrained, as the dipole field is the same at every longitude
    2. The declination gives the paleolatitude of the site, while the inclination gives its paleolongitude once the polarity is known
    3. Both the paleolatitude and the paleolongitude follow from the inclination alone, since the field differs between longitudes
    4. The inclination fixes the absolute speed of the plate over the deep mantle, independent of any reference frame
    Show answer

    Answer: A — Inclination gives paleolatitude, but paleolongitude is not constrained, as the dipole field is the same at every longitude

    Under an axial dipole the field depends only on latitude, so inclination (tan I = 2 tan λ) gives latitude, while longitude leaves no trace. Declination records the rotation of the site about a vertical axis, not latitude, and a single inclination says nothing about the plate’s absolute speed, which needs a reference frame.
  8. A lava flow 60 Myr old now lies at 20° N. It carries a stable magnetisation of normal polarity with inclination −30°, and the field was a geocentric axial dipole. Take the Earth’s radius as 6,371 km and assume steady northward motion only. The mean northward plate speed since the flow formed, in cm/yr, to one decimal place, is ____.

    Numerical answer — type the value.

    Show answer

    Answer: 6.7

    tan λ = ½ tan(−30°) = −0.2887, so λ = −16.1°, which is southern because the polarity is normal and I is negative. The flow moved from 16.1° S to 20° N, 36.1° of latitude = 36.1 × 111.19 = 4,014 km. Speed = 4,014 km/60 Myr = 66.9 km/Myr = 6.7 cm/yr. Taking λ as +16.1° gives only 3.9° of motion, a wrong result.
  9. The relative motion of two plates is a rotation about an Euler pole with angular velocity 0.6°/Myr. Take the Earth’s radius as 6,371 km. The relative speed at a point on the plate boundary that is 40° of arc from the pole, in cm/yr, to one decimal place, is ____.

    Numerical answer — type the value.

    Show answer

    Answer: 4.3

    v = ω R sin θ with ω = 0.6° = 0.6 × π/180 = 0.010472 rad/Myr: v = 0.010472 × 6,371 × sin 40° = 66.71 × 0.6428 = 42.9 km/Myr = 4.3 cm/yr. Using sin 90°, the maximum, would give 6.7 cm/yr.
  10. A seamount 1,200 km from an active hotspot volcano is 15 Myr old. Assume the plate has moved at a constant speed over a fixed plume along the line of the chain. The age of a seamount 3,000 km from the active volcano, in Myr, to one decimal place, is ____.

    Numerical answer — type the value.

    Show answer

    Answer: 37.5

    Speed = 1,200 km/15 Myr = 80 km/Myr (8 cm/yr). Age = 3,000/80 = 37.5 Myr. Scaling the age by 3,000/1,200 gives the same result, whereas adding the distances is a slip.
  11. A slab dips at 45° and descends along its dip at the convergence rate of 8 cm/yr. The time for a point on the slab to travel from the trench to a depth of 660 km, in Myr, to one decimal place, is ____.

    Numerical answer — type the value.

    Show answer

    Answer: 11.7

    Distance along the slab = 660/sin 45° = 933.4 km. Rate = 8 cm/yr = 80 km/Myr. Time = 933.4/80 = 11.67 Myr, which is 11.7 Myr. Dividing the depth 660 km by 80 gives 8.25 Myr, which ignores the dip.
  12. Which process best explains the formation of an extensional back-arc basin such as the Mariana Trough?

    1. Collision of two continents, which thickens and uplifts the crust in the region behind the volcanic arc
    2. Strong compression from ridge push, which buckles the plate behind the volcanic arc downward into a basin
    3. Slab rollback, in which an old, steep slab sinks faster than the plates converge, so the trench retreats
    4. Flat subduction of a young, buoyant slab that locks the two plates together and compresses the overriding plate
    Show answer

    Answer: C — Slab rollback, in which an old, steep slab sinks faster than the plates converge, so the trench retreats

    When the slab sinks faster than the plates converge, the trench retreats toward the ocean and the overriding plate is stretched, so back-arc crust forms by spreading. Collision and flat, coupled subduction produce compression and uplift, not extension, and ridge push is too weak to buckle a plate into a basin.
  13. A volcanic chain on the Pacific plate shows ages that rise steadily with distance from one active volcano. What is the most direct inference?

    1. The plate has moved over a fixed hot source in the mantle, and the chain trends along the plate’s motion
    2. The chain lies on a transform fault, and each volcano erupted in turn when the fault last slipped at that point
    3. A subduction zone beneath the chain has fed each volcano in turn, as the slab rolled back beneath the plate
    4. The chain follows a divergent boundary that has propagated slowly in one direction along the plate
    Show answer

    Answer: A — The plate has moved over a fixed hot source in the mantle, and the chain trends along the plate’s motion

    Age progression along a line is the signature of a plate moving over a fixed melting anomaly, as in the Hawaiian chain, and the line records the direction of motion. Transform faults, subduction rollback and propagating ridges do not give a steady age increase along a chain away from a single active volcano in the middle of a plate.
  14. The Deccan Traps of India are generally attributed to which hotspot, whose later track includes the Chagos–Laccadive Ridge?

    1. Hawaii
    2. Iceland
    3. Yellowstone
    4. Réunion
    Show answer

    Answer: D — Réunion

    The Deccan flood basalts are linked to the Réunion plume. As India moved north the plume left the Chagos–Laccadive Ridge and the Mascarene Plateau, ending at the active volcano on Réunion. Hawaii, Iceland and Yellowstone lie far from India’s track.
  15. Which statement about earthquakes at a subduction zone is correct?

    1. Earthquakes occur only in the shallow crust, above about 100 km, because the slab is too warm below that
    2. Hypocentres define a Benioff–Wadati zone dipping beneath the overriding plate to about 700 km
    3. Hypocentres deepen toward the ocean, away from the volcanic arc, following the dip of the trench wall
    4. Earthquakes are common throughout the lower mantle, all the way down to the core–mantle boundary
    Show answer

    Answer: B — Hypocentres define a Benioff–Wadati zone dipping beneath the overriding plate to about 700 km

    Earthquakes in the cold slab trace a plane dipping from the trench beneath the arc, and the deepest are about 700 km. They deepen toward the continent or arc side, not toward the ocean, they are not confined to the shallow crust, and none occur in the deep lower mantle.
  16. Which of the following statements about magma generation at plate boundaries are correct?

    1. Arc volcanoes stand directly above the trench axis, where the slab first bends down
    2. Basalt at mid-ocean ridges forms by decompression melting of upwelling mantle peridotite
    3. Arc magmas form where water released from the slab lowers the melting point of the mantle wedge
    4. Melting at mid-ocean ridges is triggered mainly by water added from a subducting slab
    Show answer

    Answer: B — Basalt at mid-ocean ridges forms by decompression melting of upwelling mantle peridotite; C — Arc magmas form where water released from the slab lowers the melting point of the mantle wedge

    Ridges melt by decompression as the mantle rises, and arcs melt by flux melting, since slab-derived water lowers the solidus of the wedge. Arc volcanoes lie where the slab is about 100 to 120 km deep, inland of the trench, and ridges have no subducting slab to supply water.
  17. Which of the following statements about continental rifting are correct?

    1. Passive rifting is driven by far-field tension, with volcanism following lithospheric thinning
    2. Rift valleys are bounded by steep reverse faults that shorten and thicken the crust
    3. Rift volcanism is always andesitic and calc-alkaline, as it is in volcanic island arcs
    4. Active rifting begins with doming of the crust over a hot, buoyant mantle upwelling
    Show answer

    Answer: A — Passive rifting is driven by far-field tension, with volcanism following lithospheric thinning; D — Active rifting begins with doming of the crust over a hot, buoyant mantle upwelling

    Passive rifting is stress-driven and active rifting starts with plume-related doming. Rift valleys are bounded by normal faults because the crust is extending, and rift magmas are bimodal and often alkaline, not arc-like andesites.