Plate Tectonics: Boundaries, Motions, Magnetic Records, Plumes and Numericals
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.
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.
7. Numerical problems on plate motions
| Problem | Relation | Care needed |
|---|---|---|
| Spreading rate | Half rate = x/t; full rate = 2x/t | State which rate; 1 km/Myr = 1 mm/yr |
| Velocity about an Euler pole | v = ω R sin θ | Use radians, or 1° = 111.2 km |
| Paleolatitude | tan λ = ½ tan I; distance = Δλ × 111.2 km/° | Sign of I depends on polarity and hemisphere |
| Hotspot chain | Age t = d/v | v is the plate speed over the plume |
| Subduction | Slab 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.
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.
At which type of plate boundary is lithosphere neither created nor destroyed, the plates sliding past each other?
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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.Which pairing of a feature with its plate-boundary setting is correct?
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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.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?
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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.Which of the following statements about the forces that drive plate motion are correct?
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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.A magnetometer towed over the sea floor records a positive magnetic anomaly over a stripe of oceanic crust. What does this indicate?
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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.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.
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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.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?
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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.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.
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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.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.
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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.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.
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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.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.
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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.Which process best explains the formation of an extensional back-arc basin such as the Mariana Trough?
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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.A volcanic chain on the Pacific plate shows ages that rise steadily with distance from one active volcano. What is the most direct inference?
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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.The Deccan Traps of India are generally attributed to which hotspot, whose later track includes the Chagos–Laccadive Ridge?
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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.Which statement about earthquakes at a subduction zone is correct?
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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.Which of the following statements about magma generation at plate boundaries are correct?
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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.Which of the following statements about continental rifting are correct?
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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.