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Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow- Bertelloni

Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

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Page 1: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plumes, hotspots and the CMB

Lecture 6: GeodynamicsCarolina Lithgow-Bertelloni

Page 2: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Earth’s temperature profile

3000

2500

2000

1500

1000

500

0

DEPTH (KM)

50004000300020001000

TEMPERATURE (K)

Page 3: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Scales of Convection

[from Geoff Davies]

Page 4: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plumes and Hotspots Hotspots

Island chains and age progressionImportance for plate motions, TPWFixityChemistryOrigin

PlumesDifference with large-scale upwellingsHeads and tails

Effects of viscosity on morphologyPlume initiation and flood basaltsHow much entrainmentComparison to geochemistry

Effects of compositionShape, heterogeneity, hotspot fixity

Relationship between large-scale upwellings and plumes?Capture by plate-scale flow

Consequences for heat flow

Where do they come from? Relationship to CMB structure

Page 5: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Hotspots

Concentrated volcanic activity. Linear volcanic chains in the interiors of the plates.Age progression along chain Chemistry of erupted lavas is significantly different than MOR or IASome hotspots have broad topographic swell ~ 1000 m

[Steinberger et al., 2004]

Page 6: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

43-48 Ma

Hotspots and Plates

25-43 Ma

Page 7: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Hotspots, fixity and plate motions

Page 8: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Hotspot fixity and mantle wind

[Steinberger et al., 2004]

Page 9: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Chemistry

[Barfod et al., 1999]

Page 10: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plumes and hotspots

Rayleigh-Taylor instabilityLarge head, thin tail

RheologyVigor of convectionCompositional vs thermal buoyancy

Ascent timesRheologyDeflection, capture by mantle windCompositional vs thermal buoyancy

[Griffiths and Campbell, 1990]

Page 11: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Rise time estimate

Ratio of buoyancy force to viscous forcesB = -4r3g/3=/r; R=r

Forces on the sphere balanced velocity constantB+R=0 V= -gr2/3c

If viscosity of sphere and surrounding differentc = /

c ~ 1-1.5

v

r

r = 500 km

V =80 km/My

Page 12: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Generating a mantle plume

QuickTime™ and aMotion JPEG A decompressor

are needed to see this picture.

[from Geoff Davies]

Page 13: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Large-scale upwellings and plumes

[Boschi and Dziewonski,1999]

[Ni et al.,2002]

Page 14: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plume morphology: effects of viscosity

[Whitehead and Luther, 1975]

Page 15: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

July 13, 2004 CIDER-KITP

Plumes heads and tails

0.3 m B C D

E

OUTLET

INLET

A

7.5

15.0

22.5

20

20

1 m

F-H

1 m

Screen N

Screen E

N

S

[Lithgow-Bertelloni et al., 2001]

Page 16: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Head & Tail Radii

0.0

1.0

2.0

3.0

4.0

5.0

6.0

7.0

10 5 10 6 10 7 10 8

Rao

[Lithgow-Bertelloni et al., 2001]

Page 17: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Thermochemical Plumes

QuickTime™ and aVideo decompressor

are needed to see this picture.

[Farnetani, 2004]

Page 18: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Entrainment and mixing

QuickTime™ and aVideo decompressor

are needed to see this picture.

Page 19: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plumes and geochemical heterogeneity

[Samuel and Farnetani, 2003]

Page 20: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Evolution of heterogeneity

[LeBars and Davaille, 2004]

Page 21: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plumes and large-scale upwellings

[Davaille, 2000]

Page 22: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Thermochemical plumes and fixity

[Jellinek and Manga, 2002]

Page 23: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plume capture by large-scale flow

V and hot/int

No effect V<< 1 ~ 1Suppression V> 10 > 100Sweeping V intermediate f(

[Jellinek et al., 2002]

and Pe control BLT and Q ~ (Pe)1/3

Q ~ (Pe)1/2

Page 24: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Where do plumes originate?

[Davaille, 2000]

Page 25: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

The plume source region: CMB

[Sidorin et al., 1999]

Page 26: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Plume Frequency3 Different Experiments

Page 27: Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni

Episodic Crustal Production?

Condie, 1998