M1_-_Geomorphology_-_Tectonic_Geomorphology
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Transcript of M1_-_Geomorphology_-_Tectonic_Geomorphology
TECTONIC GEOMORPHOLOGYBenjamin Guillaume
GEOMORPHOLOGY
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[from greek gê, Earth and morphê, shape and logos, speech] «the branch of geology that is concerned with the
structure, origin, and development of the topographical features of the Earth's surface»
TECTONICS
[from greek tektonikos, relating to building] «the branch of geology relating to the structure of the Earth’s
crust and the large-scale processes which take place within it»
TOPOGRAPHY
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Topography (ETOPO1)
-10.9 km <elevation< 8.9 kmMariannes trench Everest
PLATE TECTONICS
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Chamot-Rooke et Rabote (2006)
Morgan, McKenzie et Le Pichon (1967)Wegener (1912)
• diverging plate boundaries (spreading ridges)• transform plate boundaries (transform faults)• converging plate boundaries (subduction-collision)
PLATE TECTONICS
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Chamot-Rooke et Rabote (2006)
Morgan, McKenzie et Le Pichon (1967)Wegener (1912)
~1 cm/yr <convergence velocity< ~25 cm/yr
PLATE TECTONICS
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John Nelson, IDV Solutions
maximum released energy and deformation at convergent plate boundaries
“Pacific ring of fire“
The shape of the EARTH is controlled at first-order by plate tectonics and modulated by surface processes
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60˚S 60˚S
30˚S 30˚S
0˚ 0˚
30˚N 30˚N
60˚N 60˚N
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Tectonics act at different time-scales
sec
10’s of Myr
earthquakes
mountain building
Burbank and Anderson (2012)
SHORT-TERM DEFORMATION
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Some theory
ß = 45° + Ω/2Ω : internal friction angle
ß = 45° - Ω/2
π = 45° - Ω/2
SHORT-TERM DEFORMATION
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Some theory
right-lateralstrike-slip fault
2-stages process
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Example : Nankaido (Japan) December 1946 Mw : 8.1
after Hyndman and Wang (1995)opposite vertical motions during coseismic and interseismic stages
subduction thrust fault
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Models for earthquake recurrence
after Shimaki and Nakata (1980) and Friedrich et al. (2003)
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Earthquake nucleation
after Zielke and Arrowsmith (2008)
controlled by the difference between coefficients of dynamic and static friction= maximum slip where Δt is largest
Slip propagates toward the surface : a few 10’s mm to 10’s cm
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Length-displacement ratios on faults
after Scholz (1990), Schlische et al. (1996), and Davis et al. (2005)
Maximum displacement ranges from 0.3% to 30% of fault length
GEOMORPHIC EXPRESSION OF FAULTS
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Strike-slip fault zones(maximum compressive stress is horizontal + horizontal deviatoric tensile stress)
Garlock fault (California)
• Offset drainage channel• Beheaded stream• Linear valley
➜ Location of fault trace and direction of relative motion
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Strike-slip fault zones
Right-lateral / left-lateral?
San Andreas fault (California)
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Right-lateral strike-slip fault!
San Andreas fault (California)
Strike-slip fault zones
Normal faults(maximum compressive stress is vertical + horizontal deviatoric tensile stress)
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2D
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3D
East African rift system
after Morley (1989)
Transfer of displacement between adjacent major faults
Normal faults(maximum compressive stress is vertical + horizontal deviatoric tensile stress)
2D
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after Stein et al. (1988)
Example : Lost River Range (Idaho) 1983 - M = 7.0
Asymmetry during coseismic phase
Persists during interseismic phase
Thrust faults : the most destructive earthquakes
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Since 1960’s : • Great Chilean (1960 ; Mw = 9.5)• Alaska (1964 ; Mw = 9.2)• Sumatra-Andaman (2004 ; Mw = 9.1)• Tohoku-Oki (2011 ; Mw = 9.0)
Thrust faults(maximum compressive stress is horizontal + vertical deviatoric tensile stress)
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short-term
long-termafter Stein et al. (1988)
Example : Kern County (California) 1952 - M = 7.3
Thrust faults : model of deformation during earthquake cycle
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after Davis et al. (2005)
Different models of folds (see your textbooks...)
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GEOMORPHIC EXPRESSION OF FOLDS
after Hubert-Ferrari et al. (2007)
Surface expression of slip gradients
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Displacement variations in the subsurface fault are directly related to the magnitude of rock uplift at the surface.
Lateral fold growth
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Example : Wheeler Ridge anticline
after Burbank et al. (1996)
Lateral fold growth
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Example : Wheeler Ridge anticline
• Intense dissection on the steeply dipping flank of the fold
• Deflection of streams toward the east by the growing fold
after Burbank et al. (1996)
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EARTHQUAKE-TRIGGERED EROSION : LANDSLIDES
Papua - New Guinea (courtesy of N. Hovius)
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EARTHQUAKE-TRIGGERED EROSION : LANDSLIDES
Landslides triggered by earthquakes develop preferentially close to crests and channels
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EARTHQUAKE-TRIGGERED EROSION : LANDSLIDES
Landslides triggered by earthquakes develop preferentially close to crests and channels
Amplification of seismic shaking near crests
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EARTHQUAKE-TRIGGERED EROSION : LANDSLIDES
Landslides triggered by earthquakes develop preferentially close to crests and channels
Amplification of seismic shaking near crests
Higher pore pressures + local steepening of hillslopes by river incision near channels
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METHODS FOR MEASURING SHORT-TERM DEFORMATION AND TOPOGRAPHY
• Trilateration arrays (horizontal)• Tide gauges (vertical)• Tropical corals (vertical)• GPS (horizontal + vertical)• Radar interferometry (horizontal)• Lidar imaging (vertical)• ASTER imagery (vertical)• ....
See Burbank and Anderson, Tectonic geomorphology, 2012
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
Intermediate time-scales?
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
Intermediate time-scales?
Holocene-Pleistocene boundary (11.6 ky) ➜ 300-400 ky
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
Intermediate time-scales?
Holocene-Pleistocene boundary (11.6 ky) ➜ 300-400 ky
Landscape = episodic + continuous tectonic and geomorphic processes
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
Intermediate time-scales?
Holocene-Pleistocene boundary (11.6 ky) ➜ 300-400 ky
Landscape = episodic + continuous tectonic and geomorphic processes
• Allows determining long-term mean rate of deformation• Needed to compare with shorter-term record
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
Intermediate time-scales?
Holocene-Pleistocene boundary (11.6 ky) ➜ 300-400 ky
Landscape = episodic + continuous tectonic and geomorphic processes
• Allows determining long-term mean rate of deformation• Needed to compare with shorter-term record
Mean vertical uplift of 1 mm/yr and horizontal deformation of 1 cm/yr gives 400 m of vertical motion and 4 km of horizontal motion
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DEFORMATION AND GEOMORPHOLOGY AT INTERMEDIATE TIME-SCALES
At these time-scales : • Pristine tectonic forms become degraded by erosion• Major glacial-interglacial cycles : specific geomorphic markers (marine terraces, fluvial terraces)
after Porter (1989) and Lisiecki and Raymo (2005)
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CALIBRATING RATES OF DEFORMATION
Marine terraces : formation
Terraces form during highstand sea-level and are abandoned during lowstand sea-level
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CALIBRATING RATES OF DEFORMATION
Marine terraces : formation
Regard et al. (2010)
Uplift rate from age-elevation relationship
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Marine terraces : extracting uplift rates
Steady Uplift rate = Elevation / Age
after Lajoie (1986)
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Marine terraces : extracting uplift rates
Unsteady Uplift rate = Elevation / Age
after Merritts and Bull (1989)
northern California
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Marine terraces : extracting uplift rates
UpliftRateΔi0 = (ShAi −Ei)/ Agei
Mean uplift rate over a time interval ti–t0 (Δi0) between each marine terrace (i) and present sea level (0)
If age of the surface is known directly (cosmogenic datation, U-Th,...) or indirectly (relative to Marine
Isotopic Stage)
ShAi : present-day elevation of the shoreline angle of the marine terrace (time ti)Ei : sea-level elevation at ti compared to the present sea level
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UpliftRateΔij = [(ShAi - Ei) - (ShAj - Ej)]/ [Agei - Agej]
Incremental uplift rate over a time interval ti–tj (Δij) between two successives marine terraces
ShAi : present-day elevation of the shoreline angle of the marine terrace (time ti)Ei : sea-level elevation at ti compared to the present sea level
Marine terraces : extracting uplift rates
If age of the surface is known directly (cosmogenic datation, U-Th,...) or indirectly (relative to Marine
Isotopic Stage)
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A CASE STUDY : SOUTH AMERICA
Tectonic framework
Espurt et al. (2008)
• Subduction of the Nazca plate beneath the South American plate for 10’s of Myr
• Present-day convergence velocity = 8 cm/yr
• Subduction of ridges (topographic anomalies = thickenned crust produced by hot spot volcanism)
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A CASE STUDY : SOUTH AMERICA
Tectonic framework
Espurt et al. (2008)
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Shore morphology
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Methodology : example of Punta Choros (Chile)
• DEM from aerial stereophotos• Identification of terraces = break-in-slope on cross-sections
• Sampling for cosmogenic dating (10Be)
> 400 ky
> 400 ky
➜ Uplift rate J. Maison (M1, 2013)
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Rasa age evaluation - lower level (~110 m)
Regard et al. (2010)
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Main results
The Central Andes coast morphology (rasa) seems to indicate that uplift is:• Recent (Quaternary, with evidences of preexisting subsidence)• Wide (most probably due to subduction)• MIS 11 (~400 kyrs BP) appears to have been particularly marked: variation in uplift rate or greater efficiency in erosion?
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MIS 5e uplift rates (~100 ky)
after Pedoja et al. (2011) ��Ý:
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Taux de soulèvement(MIS 5e)
Ride de Carnegie
Ride d
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ca5LGH�G·,TXLTXH
5LGH�-XDQ�)HUQDQGH]
Higher uplift rates related to topographic anomalies within the subducting plate
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Marine terraces : determining slip rates on faults
San Juan (Chile)
Saillard et al. (2011)
Loma Fault
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Saillard et al. (2011)
SlipRateΔij = (ShACEHi −ShACTHi) - (ShACEHj −ShACTHj) / (Agei −Agej)
Marine terraces : determining slip rates on faults
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Marine terraces : folding and shortening rates
Melnick et al. (2009)
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CALIBRATING RATES OF DEFORMATION
Fluvial terraces : formation
Unlike marine terraces, fluvial terraces are not necessarily horizontal
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CALIBRATING RATES OF DEFORMATION
Fluvial terraces : are diachronous
Terrace T6 at Cajon Creek (California)
after Weldon (1986)
4 ky
7 ky
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Fluvial terraces : displacement across faults
Wellington Fault (New-Zealand)
after Van Dissen et al. (1992)
Increase of the amount of offset with age
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Fluvial terraces : displacement across faults
Ventura River (California)
• Asymmetry in faulting rate• Maximum faulting rate at the core of the fold• Increase of the amount of offset with terrace age• Variable faulting rate on single fault
after Rockwell et al. (1984)
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CALIBRATING RATES OF DEFORMATION
Stream gradient : principle
For a uniform lithology, anomalously steep or gentle profile may be interpreted in term of ongoing tectonism
after Duvall et al. (2004)
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Stream gradient : physical modeling
Adaptation of the river profile to a change in tectonic uplift rate : knickpoint
knickpoint sweeps upstream
courtesy of D. Lague
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Stream gradient : knickpoints
Uplift rate x2
after Whipple and Tucker (1999)
Formation of a knickpoint that sweeps upstream- lower channel steepens - upper channel retains its initial gradient
Same concavity but different steepness
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Stream gradient : extracting uplift history from river profiles
Rate of change of elevation ∂z/∂t along a river profile :
∂z/∂t = U(x,t) + E(x,t)
x : distance along river profileU : rate of rock upliftE : rate of erosion
E(x,t) = -vAm (∂z/∂x)n + k (∂2z/∂x2)
n and m : constants affecting the concavity of a river profile (n generally taken = 1)Am : related to average discharge along a riverv and m : control the value of the advective term, which governs the transient form of a river profile and the knickpoint retreat velocitiesk : erosional diffusivity (10-107 m2 Ma-1)
➜ U(x,t)
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Stream gradient : extracting uplift history from river profiles
Inverse modeling testing plausible parameters values (2x102 <k< 7x102 ; 200<v<210 ; 0.19 <m< 0.21; 1<n<1.05)
Roberts et al. (2012)
In gray : observed profileIn black : best-fitting profile
Colorado catchment
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Stream gradient : extracting uplift history from river profiles
Roberts et al. (2012) Colorado catchment
Getting uplift rate history for different parameters
best-fit to river profile
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Stream gradient : extracting uplift history from river profiles
Roberts et al. (2012) Madagascar
Applying to a large number of rivers to get spatial uplift history
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Stream gradient : extracting uplift history from river profiles
Madagascar
Maps of cumulative uplift
Roberts et al. (2012)
Drawback : only works for uplifted areas
TECTONIC GEOMORPHOLOGY AT LARGER TIME-SCALES
Larger time-scales?
TECTONIC GEOMORPHOLOGY AT LARGER TIME-SCALES
Larger time-scales?
Time required for the growth and decay of a mountain chain = 10’s of Myr
TECTONIC GEOMORPHOLOGY AT LARGER TIME-SCALES
Larger time-scales?
Time required for the growth and decay of a mountain chain = 10’s of Myr
Currently observable deformation patterns, climate and erosion rates may have only tangential relevance to a range’s overall evolution
TECTONIC GEOMORPHOLOGY AT LARGER TIME-SCALES
Larger time-scales?
Time required for the growth and decay of a mountain chain = 10’s of Myr
Currently observable deformation patterns, climate and erosion rates may have only tangential relevance to a range’s overall evolution
At these time-scales, detailed interactions of short-term deformation and surface processes are often obscured
TECTONIC GEOMORPHOLOGY AT LARGER TIME-SCALES
Larger time-scales?
Time required for the growth and decay of a mountain chain = 10’s of Myr
Currently observable deformation patterns, climate and erosion rates may have only tangential relevance to a range’s overall evolution
At these time-scales, detailed interactions of short-term deformation and surface processes are often obscured
Larger spatial framework: 100’s to 1000’s of km
Climate and tectonics
Climate(through erosion)
Tectonics
Climate and tectonics
Climate(through erosion)
Tectonics
Erosion-controlled isostatic uplift (Molnar and England, 1990)
Climate and tectonics
Climate(through erosion)
Tectonics
Erosion-controlled isostatic uplift (Molnar and England, 1990)
Widening/narrowing of orogens in response to erosion (e.g., Whipple and
Meade, 2006)
Climate and tectonics
Climate(through erosion)
Tectonics
Erosion-controlled isostatic uplift (Molnar and England, 1990)
Widening/narrowing of orogens in response to erosion (e.g., Whipple and
Meade, 2006)
Enhanced deformation where rainfall is high (e.g., Willett, 1999)
...
Climate and tectonics
Climate(through erosion)
Tectonics
Erosion-controlled isostatic uplift (Molnar and England, 1990)
Widening/narrowing of orogens in response to erosion (e.g., Whipple and
Meade, 2006)
Problems of dataset (often use of proxy, e.g. cooling and not erosion rate) and time-frame of correlations
Enhanced deformation where rainfall is high (e.g., Willett, 1999)
...
Climate and tectonics
Cooling age = Age at which a rock crosses the closure temperature of a
specific thermochronometer
Zr FT : 220°CAp FT : 110°CAp He : 60°C
Proxy for erosion rate : younger age = faster erosion
Climate and tectonics
Climate and tectonics
Two possible scenari :
Acceleration of erosion rates into a increasingly narrow zone over the last 5 My (B)
vs. Spatially focused erosion pattern persisting for Myr (C)
Climate and tectonics
TectonicsClimate(through erosion)
Climate and tectonics
Tectonics
Orographic rainfall (Burbank et al., 2003)
Loci of high rainfall develop on the upwind side of a range vs rain shadow develop on the downwind side
Climate(through erosion)
Climate and tectonics
Example : summer monsoon in the Himalayas
Bookhagen and Burbank (2010)
Climate and tectonics
Example : summer monsoon in the Himalayas
Bookhagen and Burbank (2010)
Monsoon rainfall produces a peak associated with each topographic step
Latitudinal gradients in climate and tectonics
Elongate N-S oriented ranges can span latitudinal bands with contrasting climate regimes
Latitudinal gradients in climate and tectonics
Elongate N-S oriented ranges can span latitudinal bands with contrasting climate regimes
Montgomery et al. (2001)
Example : the Andes
the Andes : latitudinal gradients in climate and tectonics
Montgomery et al. (2001)
the Andes : latitudinal gradients in climate and tectonics
Montgomery et al. (2001)
Variable amount of sediments provided to the trench
the Andes : latitudinal gradients in climate and tectonics
Lamb and Davies (2003)
Central Andes : - low precipitation- low trench fill thickness (deep trench)- high interplate coupling- high topography
Northern and Southern Andes : the opposite
It’s a model...
Dynamic topography
WHEN MANTLE FLOW IS INVOLVED...
«Surface deformation associated with density driven convection in the sub-lithospheric mantle»
Dynamic topography
WHEN MANTLE FLOW IS INVOLVED...
«Surface deformation associated with density driven convection in the sub-lithospheric mantle»
Large-scale signal (100’s of km) and moderate amplitude (~100‘s of m)
Dynamic topography
Well expressed in areas with no recent tectonic activity (e.g., Africa)
Present-day topography
F. Guillocheau
Moucha and Forte (2011)
Signature of a plume
Tomography
Dynamic topography
Well expressed in areas with no recent tectonic activity (e.g., Africa)
Present-day topography
F. Guillocheau
∆ Dynamic topo (10 Ma-0 Ma)
Moucha and Forte (2011)
Dynamic topography
Inverse signal of equal amplitude above high density anomalies (subduction zones)
Steinberger (2007)
Dynamic topography
Inverse signal of equal amplitude above high density anomalies (subduction zones)
but signal convoluted with isostatic response of the lithosphere to convergence (generally of higher amplitude)
Steinberger (2007)
Dynamic topography
Control the fraction of inundated continents
60˚S 60˚S
30˚S 30˚S
0˚ 0˚
30˚N 30˚N
60˚N 60˚N
−10000 −8000 −6000 −4000 −2000 0 2000 4000 6000 8000
m
Present-day elevation
Dynamic topography
Control the fraction of inundated continents
60˚S 60˚S
30˚S 30˚S
0˚ 0˚
30˚N 30˚N
60˚N 60˚N
−10000 −8000 −6000 −4000 −2000 0 2000 4000 6000 8000
m
Present-day elevation -200m
Dynamic topography : tilting of the Australian continent
Sandiford (2007)
Subduction to the North : downward deflection
Mid-ocean ridge to the South : upward deflection
Dynamic topography : tilting of the Australian continent
Sandiford (2007)
Subduction to the North : downward deflection
Mid-ocean ridge to the South : upward deflection
Down to the north tilt of the continent!
(as recorded by shoreline migration for the last 15 Myr)