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Evolution of a Cooling Planet • Magma ocean • Thick buoyant crust • Melting at base • Heat pipes • Eclogite at base • Delamination • Plate instability *prior to all this is accretional zone refining & differentiation

Evolution of a Cooling Planet

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Evolution of a Cooling Planet. Magma ocean Thick buoyant crust Melting at base Heat pipes Eclogite at base Delamination Plate instability. *prior to all this is accretional zone refining & differentiation. The Earth started out HOT!. - PowerPoint PPT Presentation

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Page 1: Evolution of a Cooling Planet

Evolution of a Cooling Planet

• Magma ocean

• Thick buoyant crust

• Melting at base

• Heat pipes

• Eclogite at base

• Delamination

• Plate instability*prior to all this is accretional zone refining & differentiation

Page 2: Evolution of a Cooling Planet

The Earth started out HOT!• ‘Standard Models’ of geochemistry invoke a

volatile-rich lower mantle, with Helium & Water leaking into the Transition Region & Upper Mantle from below

• (Wasserburg, DePaolo, Allegre, O’Nions, Kellogg, Bercovici, Karato, Helffrich, Hart)

• The transition Zone may be a filter, but it filters downgoing material

• Volatiles were zone-refined up, and some came in as Late Veneer

• Deep mantle is the dense depleted residue

Page 3: Evolution of a Cooling Planet

STANDARD MODEL

Standard Assumptions: upper mantle is homogeneous, isothermal [‘the convecting mantle’] & subsolidus; anomalous magmatism requires hot deep thermal plumes from a deep Thermal Boundary Layer (TBL)

Page 4: Evolution of a Cooling Planet

HOT EARLY EARTH COLDER EARTH

BASALTBASALT, ECLOGITE

MELT

PERIDOTITE ECLOGITE

Basalt, eclogite, harzburgite & magmas are less dense than lower mantle; lower mantle is dense residue of differentiation

UPPER MANTLE (basalt, peridotite, eclogite, kimberlite)

Page 5: Evolution of a Cooling Planet

Rocks and minerals arranged by density: crust & upper mantle

• delaminates when crust > 50 km thick

• warmer than MORB

Page 6: Evolution of a Cooling Planet

Part of accretional differentiation is irreversible

• The buoyant and volatile products of early differentiation are excluded upwards (radial zone refining)

• The dense residues (restites) get trapped at depth as pressure increases and coefficient of thermal expansion decreases

• Layers that differ enough in intrinsic density & viscosity cannot be mixed back

Page 7: Evolution of a Cooling Planet

Fertile patches in upper mantle are subducted seamounts etc. & delaminated lower continetal crust=melting anomalies

Page 8: Evolution of a Cooling Planet

The transition zone is a crust-slab-water filter but it filters from above, not below. Most recycled material bottoms out above 650-km depth

Page 9: Evolution of a Cooling Planet

Densitycrossover

PREM isDenser than pyrolite

Ponding of eclogite

Page 10: Evolution of a Cooling Planet

ECLOGITE CAN BE BROUGHT BACK UP BY A VARIETY OF MECHANISMS

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Buoyancy, melting, entrainment, displacement

- - - - - -

- - -

___

These should NOT be called ‘plumes’, e.g.’splash plumes’!

Page 11: Evolution of a Cooling Planet
Page 12: Evolution of a Cooling Planet

There are many things in the mantle other than old slabs

• Delaminated lithosphere & crust• Cumulates• Trapped melts• Young plate, subducted ridges…• If these differ from ‘normal’ mantle by more

than ~3% and are large (~10 km) they will settle to various depths

• The ‘convecting mantle’ is stratified and blobby

• Some of these can cause non-plume melting anomalies

Page 13: Evolution of a Cooling Planet

3 4 5 6pyroxenite 3.23eclogite 3.24UMR AVERAGE 3.29

LID bronzite 3.29dunite 3.30PHN1569 3.31sp.perid. 3.35

Gt.Lhz. 3.35 UPPER melt 3.30

opx 3.37 MANTLEPHN1611 3.42 _________36%ol,17%gt 3.43

LMP eclogite 3.43LMP eclogite 3.46

melt 3.20gt.perid. 3.35 _______Hawaii Lhz. 3.47magma(16 Gpa) 3.50 MAGMAmajorite (mj) 3.52mj 3.53DRY MORB MAGMA (1600 C)DRY KOMATIITE MELT (1600 C)garnet 3.57 _____

TZ beta(.1FeO) 3.59

400 km mj 3.61gr garnet 3.60

LMP eclogite 3.60LMP eclogite 3.61 LVZ

melt 3.40

500 km gamma(.1FeO) 3.68py gt 3.71komatiite(18 Gpa) 3.80 KOMATIITE ___

LO-T il(.1FeO) 3.92jd-mj 4.00

magma

eclogite

Density VsSTABLE STRATIFICATION

3.2

3.3

3.4

3.5

3.6

3.7

density

Page 14: Evolution of a Cooling Planet

Is there any evidence for a blobby laminated mantle?

• Plenty!• reflections, conversions, scatterers, low-

velocity zones…

• Mafic blobs at depths of neutral buoyancy or trapped at phase changes have a chance to warm up and can be the source of melting anomalies

Page 15: Evolution of a Cooling Planet

Dueker

Page 16: Evolution of a Cooling Planet

Phase changes are flat and stack-up. Chemical boundaries & blobs are variable depth.

Phase changes V V V

Chemical boundaries Chemical discontinuities &

blobs

410 520 650

Page 17: Evolution of a Cooling Planet

Low-velocity zone atop the 410-kmseismic discontinuity in thenorthwestern United States

Teh-Ru Alex Song, Don. V. Helmberger & Stephen P. Grand

400-km

Page 18: Evolution of a Cooling Planet

MANTLE IS NOT SIMPLE

Page 19: Evolution of a Cooling Planet

Lower mantle (LM) is denser than pyrolite; therefore eclogite can be trapped in TZ

Lower mantle is chondritic minus {volatiles-crust-upper mantle}, e.g.SiO2-rich

LM is (depleted, refractory, residual; formed during accretion)

K.Lee et al.

Perovskite is too dense

Pyrolite & low-FeO is too light

Page 20: Evolution of a Cooling Planet

Figure 5-2: Rocks and minerals arranged by density

Rock type SHEAR VELOCITY (P=0) STP Vs (km/s)

density 3 4 5 6 km/s

(g/cc)granite 2.62

A' gabbro 2.87CRUST dolerite 2.93 usual max. crustal thickness

gneiss 2.98 50 km

A" eclogites & 3.45 unstablearc eclogites 3.46 root eclogite(arclogites,arcl) 3.48 " 3.62 Vp= 8.1 km/s

UPPER harzburgite 3.30MANTLE dunite 3.31 Vp= 8.4 km/s UPPER

pyrolite 3.38 Vp= 8.3 Km/s MANTLEperidotite 3.42

B arcl(highMgO) 3.45 stableeclogite 3.46 Vp=8.1 km/s eclogiteHawaii Lhz. 3.47arcl(highMgO) 3.48 8.1 km/s

3 4 5 6 km/s

β- (.1 )spinel FeO 3.59 X 410 kmTZ (.12 )FeO 3.60 9.3 /km s

(410 )pyrolite km "majorite "

Some eclogites equilibrate above 400-km depth

Page 21: Evolution of a Cooling Planet

THE ALTERNATE TO A TURBULENT WELL-STIRRED MANTLE IS ONE OF NEUTRAL

DENSITY GRAVITATIONAL STRATIFICATION OF THE MANTLE

BUOYANT CRUSTDENSE LOWER CRUST

HARZBURGITE

BASALT UNDERPLATE

PERISPHERE

PICLOGITE

PYROLITE

GARNETITE

PEROVSKITITE

DENSE DREGS

Page 22: Evolution of a Cooling Planet

Mantle stratification

• irregular chemical discontinuities expected

• difficult to see in tomography

• can be seen in receiver functions

Page 23: Evolution of a Cooling Planet

CHEMICAL STRATIFICATION OF CRUST AND MANTLE

MAGMA 1600 C

*δ ρ with respect to PREM

DENSITY ( =0)SHEAR VELOCITY P=LMP ( ρ )

low deficit VS

melting (δ ρ)*point KGVs3 4 5 6

basalt 2.59graniteplagioclase 2.64quartzgranodiorite 2.68 _______________

UPPER anorthositeCRUST gneiss 2.79

dioriteanorthosite 2.80 CRUSTALserpentinite &MINERALSgabbro 2.86 ROCKSmetabasaltdolerite 2.93gabbro _______________

LOWER gneiss restite 2.98CRUST amphibolite

-granulite mafic 3.10amphibole

^ mafic melt (-0.68) buoyant ^ ultramafic melt (-0.40) magma

50 km jadeite 3.20pyroxenite 3.23 pyroxenites

LMP eclogite 3.24100 km mafic melt (-0.40) buoyant ^

ultramafic melt (-0.15) magma UMR AVERAGE 3.29

bronzitedunite 3.30

1569PHN. .sp perid 3.35

200 km . .Gt Lhz peridotites^ mafic melt (-0.18) rises

ultramafic melt(+0.00) stableopx 3.37

1611PHNPYROLITE 3.3836% ,17%ol gt 3.43

3 4 5 6LMP eclogite 3.43 ,eclogitesLMP eclogite 3.46 ,garnetites

300 km Hawaii Lherzolite 3.47 ultramaficLMP eclogite 3.48 &melts^ mafic melt (-0.1) rises - iron richv "ultramafic (+0.03) sinks lherzolites

( )majorite mj 3.52mjgarnet 3.57

400 km (.1 )beta FeO gr garnet 3.60

pyrolite 3.60 low MgOLMP eclogite 3.60 &eclogitesLMP eclogite 3.61 mafic magmas

mafic melt (+0.00) stablepyrolite 3.67

500 km (.1 )gamma FeO 3.68( + )eclogite mj coe MORB

py garnet 3.71 eclogites( + )eclogite mj st 3.75

- (.1 )Mg ilmenite FeO 3.92mj 4.00

650 km ( .8)mw Mg-Mg perovskite 4.10

In a petrologically realistic planet the products of differentiation are not mixed back in; the mantle becomes stratified (pink and red are mafic rocks & melts)

Page 24: Evolution of a Cooling Planet

Geochemical & geodynamic models are dominated by

simplistic 1 & 2 layer models• The idea of a homogeneous (‘the convecting’)

mantle is based on low resolution techniques (global tomography, sampling at ridges, 2D Boussinesq convection simulations)

• Higher resolution (receiver functions, reflections, xenoliths, inclusions, seamounts) methods paint a different picture

Page 25: Evolution of a Cooling Planet

NMORB,DMORB,EMORB,TMORB,OIB,AOB,DMM,EM,HIMU,DUPAL,

LONU,PHEM,FOZO…

• Kimberlites, carbonatites, abyssal peridotites, continental mantle…are underappreciated sources of enrichment

• Eclogites come in many flavors and densities

• The mantle is not just 1 or 2 reservoirs or components

Page 26: Evolution of a Cooling Planet

WHEN DID PLATE TECTONICS BEGIN?

When did water get into the mantle?

Page 27: Evolution of a Cooling Planet

Is Sea Ice Tectonics ‘Plate Tectonics’?

Sea ice has ‘plates’, collisions (pressure ridges), break-ups (leads), rifts, sutures, rapid motions, shallow

underthrusting when thin…but no subduction tectonics

Page 28: Evolution of a Cooling Planet

THERMAL HISTORY CONSIDERATIONS Observed heat loss from Earth is actually 33 TW not 44 TW Low concentration of heat-producing elements in MORB source (which is much smaller than “the convecting mantle” or “upper mantle”) SCLM & perisphere have high radioactivities Kimberlite has very high U, Th & K & cannot be ignored U-contents in MORB vary by more than an order of magnitude There is no need for a hidden heat reservoir There are numerous minor sources of energy (tidal, differentiation, shrinking) There are large (25 %) temporal variations in heat flow Hot mantle does not imply high heat flow, smaller plates, faster plates, or thinner lithosphere

Page 29: Evolution of a Cooling Planet

Low seismic velocities can be partial melts, eclogite, CO2

Page 30: Evolution of a Cooling Planet

Eclogite 70% molten beforeperidotite starts to melt

• eclogite 70%molten atperidotite solidus

• eclogite sinkerswarmed byconduction

• rise before T hasrisen to that ofambient mantle

Cold eclogite can be negatively buoyant but it can have low shear wave velocities & low melting point

(Gpa)

Page 31: Evolution of a Cooling Planet

Old oceanic plate is likely to sink deeper than subducted seamount chains & younger plates

Page 32: Evolution of a Cooling Planet

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Eclogite,arclogite,garnet pyroxenite(GtPx)…can be trapped

Page 33: Evolution of a Cooling Planet

Slide 2

Page 34: Evolution of a Cooling Planet

QUANTATIVE & STATISTICAL TOMOGRAPHIC INTERPRETATIONS DO NOT SUPPORT WHOLE

MANTLE CONVECTION • Decorrelation of past subduction

reconstructions and tomography(Scrivner,Ray, Wen,Anderson,Becker,Boschi)

• Change in spatial patterns (Tanimoto)• Change in spectral characteristics

(Gu,Dziewonski)• Flat slabs (Zhou,Fukao)

Page 35: Evolution of a Cooling Planet

Sinking & rising blobsDYNAMIC

DYNAMIC

ISOLATED

SLUGGISH

Tri-partite mantle Density variability

Page 36: Evolution of a Cooling Planet
Page 37: Evolution of a Cooling Planet

The large “megaplumes” under s.Africa and Pacific are cold & dense!

Page 38: Evolution of a Cooling Planet

Dense but low velocity

Buoyant & high velocity

Page 39: Evolution of a Cooling Planet

Dense DomesNot Megaplumes

Page 40: Evolution of a Cooling Planet

The pyrolite model has problems; A transition zone that is slower than dry pyrolite & unacceptably low temperatures in deep mantle.A denser lower mantle where velocities increase with depth less fast than pyrolite would alleviate the problems.This would require (1) a change in transition zone composition (eclogite) (2) a gradual change in physical state of the lower mantle, e.g., a superadiabatic temperature gradient (3) more SiO2,FeO than upper

mantle (chondritic Mg/Si minus crust and upper mantle)

Page 41: Evolution of a Cooling Planet

SUBDUCTION?WATER INTO MANTLE?

ECLOGITE FORMATION?THIN OCEANIC CRUST?

KIMBERLITES?DELAMINATION?

Page 42: Evolution of a Cooling Planet

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 43: Evolution of a Cooling Planet

Complications in lower mantle

• Post-perovskite phases of pyroxenes

• Low-spin transitions

• Iron partitioning into isolated phases

• Pressure lowers expansivity & raises conductivity

• Radiative transfer

• Chemical layers and megablobs

Page 44: Evolution of a Cooling Planet
Page 45: Evolution of a Cooling Planet

Dry peridotite can only melt in shallow mantle

Page 46: Evolution of a Cooling Planet

Asthenospheric return flow vectors, with entrained mafic blobs, explain ‘hotspot’ tracks and relative motions between ‘hotspots’

Page 47: Evolution of a Cooling Planet

The fate of eclogite depends on composition.MORB is SiO2-rich and becomes stishovite-rich & dense

MORB-eclogite at high pressure

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Page 51: Evolution of a Cooling Planet

NORMAL TEMPERATURE FLUCTUATIONS ARE ~25 %

Page 52: Evolution of a Cooling Planet
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THE END GAME OF PLATE TECTONICS

Page 55: Evolution of a Cooling Planet

MANTLE IS A TOP-DOWN SYSTEM

Page 56: Evolution of a Cooling Planet

Archean Catastrophe?

Not if plates & volatiles rather than mantle viscosity are the control parameters

Page 57: Evolution of a Cooling Planet

Bottom Lines

Temperature is not the only or even the main parameter in controlling;

Seismic velocity

Melting

Viscosity

Density

(geologists know this but seismologists, geochemists &

geodynamicists do not!)