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Astenosphere entrainment Astenosphere entrainment at a subduction zone:at a subduction zone:
numerical and laboratory numerical and laboratory experimentsexperiments
J. Hasenclever*, J. Phipps MorganJ. Hasenclever*, J. Phipps Morgan††, M. Hort*, M. Hort*, L. Rüpke, L. Rüpke‡‡
** Institut für Geophysik, Universität Hamburg Institut für Geophysik, Universität Hamburg† † Cornell University, Ithaca, New YorkCornell University, Ithaca, New York‡ ‡ Leibniz-Institut für Meereswissenschaften IFM-Leibniz-Institut für Meereswissenschaften IFM-Geomar, KielGeomar, Kiel
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Typical sketch of mantle flow at a Typical sketch of mantle flow at a subduction zonesubduction zone
Mantle flows in concert with the oceanic Mantle flows in concert with the oceanic lithospherelithosphere
In the mantle wedge a corner flow occursIn the mantle wedge a corner flow occurs
33
Typical sketch of mantle flow at a Typical sketch of mantle flow at a subduction zonesubduction zone
Mantle flows in concert with the oceanic Mantle flows in concert with the oceanic lithospherelithosphere
In the mantle wedge a corner flow occursIn the mantle wedge a corner flow occurs
? ?
44
OverviewOverview 1. Hints for an asthenosphere and its 1. Hints for an asthenosphere and its
propertiesproperties 2. Governing equations & numerical method2. Governing equations & numerical method 3. Simulating the “oceanic side“3. Simulating the “oceanic side“ 4. Simulating the “overriding plate side“4. Simulating the “overriding plate side“ 5. Setup and conduction of the laboratory 5. Setup and conduction of the laboratory
experiments experiments 6. Results and implications6. Results and implications
55
Hints for a weakHints for a weak(suboceanic) asthenosphere layer(suboceanic) asthenosphere layer
zone of low seismic velocity zone of low seismic velocity [[GutenbergGutenberg, , 1959; 1959; Dziewonski and AndersonDziewonski and Anderson, 1981], 1981]
and high attenuation and high attenuation [[Widmer et al.Widmer et al., 1991], 1991] postglacial rebound in Icelandpostglacial rebound in Iceland [ [Sigmundsson Sigmundsson
and Einarssonand Einarsson, 1992], 1992]
andand distribution of stresses in oceanic plates distribution of stresses in oceanic plates [[Richter and McKenzieRichter and McKenzie, 1978; , 1978; Wiens and Wiens and SteinStein, 1985], 1985] => 10=> 1018 18 – 10– 1019 19 Pa sPa s
enhanced electrical conductivity at ~100-enhanced electrical conductivity at ~100-300 km depth 300 km depth [[Oldenburg, Oldenburg, 19811981; Constable, ; Constable, 1992]1992]
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Scenario: plume-fed asthenosphere ?Scenario: plume-fed asthenosphere ?
[[Phipps Morgan et al.Phipps Morgan et al., 1995], 1995]
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Scenario: plume-fed asthenosphere ?Scenario: plume-fed asthenosphere ?
material originates from mantle plumesmaterial originates from mantle plumes
=> ~200°C hotter than “normal” => ~200°C hotter than “normal” mantlemantle
material might be compositionally material might be compositionally buoyant due to prior melting processesbuoyant due to prior melting processes
depletion and temperature lead to depletion and temperature lead to a ~1% reduced density anda ~1% reduced density anda 10 to 1000-fold reduced viscositya 10 to 1000-fold reduced viscosity
88
The 2-D numerical modelThe 2-D numerical model
Constitutive equation for Newtonian fluidsConstitutive equation for Newtonian fluids
0
uy
v
x
u
i
j
j
iij x
u
x
u
0
iij
ij gx
p
x
Force balance equationForce balance equation
Viscous (Stoke‘s) flow model in Boussinesq approx.Viscous (Stoke‘s) flow model in Boussinesq approx.
Incompressibility constraintIncompressibility constraint
99
Newtonian viscosity lawNewtonian viscosity law
02
2
2
2
z
T
x
T
z
Tv
x
Tu
t
T
M
aD TTR
EDT
11exp,
*
Solved by high precision finite-Solved by high precision finite-difference algorithm (MPDATA)difference algorithm (MPDATA)
Heat advection-diffusion equation Heat advection-diffusion equation
Flow field solved by finite-element algorithmFlow field solved by finite-element algorithm
Buoyancy termBuoyancy term
DTTDT Mo 1,
1010
Simulating the “oceanic side“Simulating the “oceanic side“
oceanic sideoceanic side
1111
1212
1313
1414
Simulating the “overriding plate side“Simulating the “overriding plate side“
OverridingOverridingplate sideplate side
1515
asthenosphereasthenosphere : 10: 102020 Pa s Pa s 1 % less dense1 % less densemesospheremesosphere : 10: 102121 Pa s Pa s age of oceanic lithosphere: 160 age of oceanic lithosphere: 160 MaMa
1616
ResultsResults Entrainment rate increases with plate speed Entrainment rate increases with plate speed
and asthenosphere viscosityand asthenosphere viscosity Age of the slab is important: enhanced Age of the slab is important: enhanced
asthenosphere “freezing“ on top of old slabsasthenosphere “freezing“ on top of old slabs Thickness of entrainend layer amounts to 15 Thickness of entrainend layer amounts to 15
to 35 km and 25 to 75 km at the slab‘s to 35 km and 25 to 75 km at the slab‘s bottom and top side, respectivelybottom and top side, respectively
Suboceanic asthenosphere counterflow Suboceanic asthenosphere counterflow Decoupling of plate motion and deeper Decoupling of plate motion and deeper
mantle flowmantle flow Tilt of the asthenosphere mesosphere Tilt of the asthenosphere mesosphere
interfaceinterface Circulation / stagnation in the mantle wedgeCirculation / stagnation in the mantle wedge
1818
Laboratory experimentsLaboratory experiments
Plexiglas reservoir (50 x 30 x 10cm) Plexiglas reservoir (50 x 30 x 10cm) filled with two unequal layers of filled with two unequal layers of Glucose-syrupGlucose-syrup
Additional water reduces viscosity Additional water reduces viscosity and density of the upper layerand density of the upper layer
Highlighted glass beads visualize Highlighted glass beads visualize flow patternsflow patterns
Plate motion induced by a pulled Plate motion induced by a pulled plastic filmplastic film
1919
Setup of lab experimentsSetup of lab experiments Plastic film (red) is pulled along the upper Plastic film (red) is pulled along the upper
and inclined boundaryand inclined boundary Film is driven by DC motor and reduction Film is driven by DC motor and reduction
gear (0,5 up to 5 cm/min)gear (0,5 up to 5 cm/min)
2020
2121
Results of the lab experimentsResults of the lab experiments
Laboratory experiments support the Laboratory experiments support the results of the numerical simulationsresults of the numerical simulations
Asthenosphere entrainment, Asthenosphere entrainment, counterflow, and interface tilt are counterflow, and interface tilt are observedobserved
Numerical simulations of the laboratory Numerical simulations of the laboratory experiments agree with the measured experiments agree with the measured data in the laboratory (code verified)data in the laboratory (code verified)
On the oceanic side no 3D character of On the oceanic side no 3D character of the subduction process is observedthe subduction process is observed
(2D numerical approximation valid)(2D numerical approximation valid)
2222
Summary & implicationsSummary & implications Simplified model: e.g. dewatering, phase Simplified model: e.g. dewatering, phase
transitions, meltingtransitions, melting Low viscous asthenosphere decouples Low viscous asthenosphere decouples
plate motion and deeper mantle flowplate motion and deeper mantle flow Circulation and stagnation in the mantle Circulation and stagnation in the mantle
wedge may have impact on magma wedge may have impact on magma genesisgenesis
Entrained asthenosphere may be Entrained asthenosphere may be important for the evolution of the mantleimportant for the evolution of the mantle
Laboratory experiments are useful tools Laboratory experiments are useful tools to verify numerical resolution and the to verify numerical resolution and the “dimensionality“ of geodynamic “dimensionality“ of geodynamic processesprocesses
2323
Refined mantle flow and Refined mantle flow and entrainment processes at a entrainment processes at a
subduction zone in the presence of subduction zone in the presence of a buoyant, hot, and weak a buoyant, hot, and weak
asthenosphere layerasthenosphere layer