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2Outline
- I. Summary of the inversion method for the 3-D
seismic temperature structure of the
oceanic lithosphere/upper mantle. - II. Temperature structure as evidence for
reheating in the Central Pacific. - Cause of reheating?
- (Simulation of thermal boundary layer
instabilities (TBI) by van Hunen, Zhong, and
Huang.)
3I. Inversion Method
- Data Rayleigh and Love wave group speeds. (20 -
150 sec). Phase speeds (40 -150 s) from Harvard
Utrecht Universities. - Surface wave tomography creation of maps of
surface wave speeds -- diffraction effects. - Monte-Carlo inversion
- Seismic parameterization
- Temperature parameterization based on a thermal
model
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6Surface Wave Speeds Relative to a Diffusively
Cooling Half Space (HSC Model)
7II. Inversion Procedure Thermal Model
Temperature Parameterization
Location In the C. Pacific
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9Shear Velocity Structure
10Temperature Structure
11Uniqueness of the Temperature Structure of the
Pacific
12III. Cause(s) of the Reheating of the Central
Pacific Lithosphere?
- Initial conditions.
- Small-scale, deep-seated processes plumes.
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Large-scale, deep-seated processes global
convection. Small-scale, shallow processes
lithospheric instabilities, small-scale
convection (Richter rolls).
Shijie Zhong Jeroen van Hunen Jinshui Huang
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14Comparison of Thermal Structure Observed and
from Simulated Thermal Boundary Layer
Instabilities (TBI).
- TBI
- Sets on at 70 Ma.
- (Rayleigh )
- 2. After on-set, reheats
- the deep lithosphere.
- After about 25 My, no
- longer effectively
- heats the lithosphere.
- 4. Duration strength of reheating
- depend on rheology.
- Right Newtonian,
- effective E 120 KJ/mol.)
15Historical Proximity to Known Active Hot Spots
Paleo-trajectories from Wessel Kroenke (1997)
Much of the W. Pacific at one time was near
known hotspots. Role of plumes in reheating C.
Pacific lithosphere ? direct thermo-mechanical
erosion, ? asthenospheric heating triggering
TBI.
16Summary Conclusions
Seismic Evidence Pacific lithosphere, on
average,has experienced a two-stage cooling
history cooling 0-70 Ma, 100 - 135
Ma. reheating 70 - 100 Ma Reheating
dominantly at depth between 70 150 km This
cooling history appears to be unique to the
Pacific. 3-D Simulations of Thermal Boundary
Layer Instabilities (TBI) Thermal structure
depends on rheology. Can approximately match
observed average cooling history of the
Pacific. TBI is an important dynamical agent at
work in the C. Pacific Interplay between plumes
and TBI and the joint effect on lithospheric
temperatures remain poorly understood
requires further work.
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18Effect of Problem Specification on Dispersion
Maps (e.g., Rayleigh Phase 50 sec)
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