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

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Presentation on theme: "Plumes, hotspots and the CMB Lecture 6: Geodynamics Carolina Lithgow-Bertelloni."— Presentation transcript:

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

2 Earth’s temperature profile

3 Scales of Convection [from Geoff Davies]

4 Plumes and Hotspots  Hotspots  Island chains and age progression  Importance for plate motions, TPW  Fixity  Chemistry  Origin  Plumes  Difference with large-scale upwellings  Heads and tails  Effects of viscosity on morphology  Plume initiation and flood basalts  How much entrainment  Comparison to geochemistry  Effects of composition  Shape, 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

5 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 IA  Some hotspots have broad topographic swell ~ 1000 m [Steinberger et al., 2004]

6 43-48 Ma Hotspots and Plates 25-43 Ma

7 Hotspots, fixity and plate motions

8 Hotspot fixity and mantle wind [Steinberger et al., 2004]

9 Chemistry [Barfod et al., 1999]

10 Plumes and hotspots  Rayleigh-Taylor instability  Large head, thin tail  Rheology  Vigor of convection  Compositional vs thermal buoyancy  Ascent times  Rheology  Deflection, capture by mantle wind  Compositional vs thermal buoyancy [Griffiths and Campbell, 1990]

11 Rise time estimate Ratio of buoyancy force to viscous forces B = -4  r 3 g  /3  =  /r; R=  r  Forces on the sphere balanced velocity constant B+R=0V= -g  r 2 /3c  If viscosity of sphere and surrounding different c =   /   c ~ 1-1.5 v r  r = 500 km        V =80 km/My

12 Generating a mantle plume [from Geoff Davies]

13 Large-scale upwellings and plumes [Boschi and Dziewonski,1999] [Ni et al.,2002]

14 Plume morphology: effects of viscosity [Whitehead and Luther, 1975]

15 July 13, 2004CIDER-KITP Plumes heads and tails [Lithgow-Bertelloni et al., 2001]

16 Head & Tail Radii [Lithgow-Bertelloni et al., 2001]

17 Thermochemical Plumes [Farnetani, 2004]

18 Entrainment and mixing

19 Plumes and geochemical heterogeneity [Samuel and Farnetani, 2003]

20 Evolution of heterogeneity [LeBars and Davaille, 2004]

21 Plumes and large-scale upwellings [Davaille, 2000]

22 Thermochemical plumes and fixity [Jellinek and Manga, 2002]

23 Plume capture by large-scale flow V and  hot /  int No effect V<< 1 ~ 1 Suppression V> 10 > 100 Sweeping V intermediate f(  [Jellinek et al., 2002]  and Pe control BLT and Q   ~ (Pe ) 1/3  Q ~ (Pe) 1/2

24 Where do plumes originate? [Davaille, 2000]

25 The plume source region: CMB [Sidorin et al., 1999]

26 Plume Frequency 3 Different Experiments

27 Episodic Crustal Production? Condie, 1998


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