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2:57 PM, Dec. 8, 2012 CIDER Post-AGU 2012 “Snowfall” in F Layer Jie (Jackie) Li University of Michigan Advanced Photon Source.

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Presentation on theme: "2:57 PM, Dec. 8, 2012 CIDER Post-AGU 2012 “Snowfall” in F Layer Jie (Jackie) Li University of Michigan Advanced Photon Source."— Presentation transcript:

1 2:57 PM, Dec. 8, 2012 CIDER Post-AGU 2012 “Snowfall” in F Layer Jie (Jackie) Li University of Michigan Advanced Photon Source

2 Collaborators Advanced Photon Source Jeffrey Pigott – Mineral Physics (Ohio State) Jie (Jackie) Li – Mineral Physics (U of Michigan) Bin Chen – Mineral Physics (U of Michigan) Matt Armentrout – Mineral Physics (UCLA) Antonio Buono – Mineral Physics (MIT) John Hernlund – Geodynamics (UC- Berkeley) Jodi Gaeman – Geodynamics (U of Maryland) Lauren Waszek – Seismology (Cambridge) Louis Kellogg, Barbara Romanowicz, Jeroen Tromp, Vernon Cormier

3 Seismic features of the F-layer Outer Core Inner Core F-layer PRE M AK13 5 PREM2 Zou et al. 08 Krasnoshchekov et al. 05 Cao et al. 07 Sun and Song 08 Gubbins et al. 08,

4 “Snowing” cores in Solar System Williams 09Hauck et al. 06 JGRChen et al. 08 GRL Stewart et al. 07 Science

5 Occurrence of “snowfall” in Earth’s core ? Case 1Case 2 Case 1 Melting gradient decreases Case 2 Adiabatic gradient increases

6 Integrative approach MP - Adiabat, melting curve for snow criterion - Density for dynamic modeling - Velocity for seismic comparison Seismo - Compare PKIKP-PKiKP differential travel time with PREM - Compare PKIKP-PKiKP differential travel time b/w east-west hemispheres Dynamics - Evolution of thermal, compositional, and structural profiles with time - Origin of stratified layer - Stability of F-layer

7 Adiabatic temperature gradient Core adiabat (dT/dP) S =  thT/K liq  th: 1.65 K liq: 1343 T: geotherm Perturbation to geotherm Dziewonski and Anderson 81 Anderson O. 98 Greff-Lefftz and Legros 99,

8 Melting curve Lindemann’s Law for fixed composition dT m /dP = 2(  SL – 1/3)T m /K sol 2(  SL – 1/3) = K’ -1, K’ = 1.7 to 3.6 K sol: 1500 T m : melting temperature Binary solution Dziewonski and Anderson 81 Seagle et al. 09

9 Grüneisen parameters

10 Case 1a: Wide “Snowing zone” Parameter space for “snowing”

11 Case 1b: Narrow “snowing” zone Chen et al. 08

12 Case 2: Greff-Lefftz and Legros 99, Temperature near ICB increases due to resonant period and viscomagnetic friction power

13 Looking back  2010 July-Aug: CIDER Boundary Layer, KITP  2010 Nov: MP Mini-Meeting Umich  2010 Dec: AGU presentation, meeting  2011 Nov: MP Mini-Meeting Umich  2011 Dec: AGU presentation, Post-AGU CIDER Workshop  2012 Sep: MP Mini-Meeting Umich

14 Tips and Traps Accomplishments - Cross-discipline exchange - MP collaboration that otherwise would not have occurred - AGU presentations (Li, Hernlund) - SEDI grant (Hernlund and Cormier) - Thesis project (Piggot) Obstacles - Define leadership role - Follow up - Generate a concrete product For discussion - Group, ungroup, regroup

15 Looking forward 2012 has been an eventful year for the group new-year resolution Arron and Cynthia Chen Jeff and his bride

16 Looking forward 2012 has been an eventful year for the group new-year resolution Arron and Cynthia Chen Jeff and his bride

17 PKP Cdiff – PKP DF differential travel time (Zou et al., 2008)

18 A thermochemical F-layer Gubbins et al. 2008, GJI A slurry F-layer Inner core freezing must occur above the solid boundary (Loper and Roberts, 1981 PEPI) CMB ICB Slurry zone

19 A thermochemical F-layer Gubbins et al. 2008, GJI A slurry F-layer Inner core freezing must occur above the solid boundary (Loper and Roberts, 1981 PEPI) CMB ICB

20 Geodynamics

21 Origin of Vp gradient  Can solid/liquid fraction account for Vp gradient?


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