Earth’s Core-Mantle Boundary: Results of Experiments at High Pressures and Temperatures Knittle& Jeanloz, Science, Vol. 251 (5000), 1991.

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Presentation transcript:

Earth’s Core-Mantle Boundary: Results of Experiments at High Pressures and Temperatures Knittle& Jeanloz, Science, Vol. 251 (5000), 1991

Observations Previous interpretation The Core-Mantle boundary and the lowermost mantle exhibit radial and lateral heterogeneities in seismic velocities, velocity gradients, discontinuities and scattering. over 1000K The CMB is a thermal boundary layer which support a thermal gradient of over 1000K over ~200 Km.

Suggested model D” is also a chemical boundary layer between the silicate mantle and the iron core May support the 1000K gradient, by allowing density variations to counteract the thermal buoyancy forces Can also explain lateral heterogeneities

Lab Experiments Objective : Tools : Recreate the CMB in miniature, within a 200μm sample in a laser heated diamond-cell – Iron foils embedded in a silicate matrix (x4) – Laser heating melted the iron (not the silicates) – Pressure resemble CMB’s( ≥70 GPa) – Two comparison samples: one not heated and under pressure ; one heated and under low pressure.

Experiment Results All 4 samples had reaction zones between iron and silicates

Experiment Results –Contd. Resolution of microprobereadings ≤2μm (determined using the pressure-only sample). Observed composition gradients: –Diffusion of O, Mg, Si: 4-7μm –Diffusion of Fe: at least 12 μm Migration of elements much stronger under higher pressures

Chemical gradient across the interface Compositional profiles (Variations from the unreacted sample) Average Weight percent Distance (µm) Weight percent Distance (µm) Weight percent Distance (µm) OxygenSiliconMagnesium

Note – penetration of Fe into unmelted silicate matrix: – migration along grain boundaries? – Soretdiffusion of heaviest component?

Thermodynamics Proposed balanced equation: By assuming amount of FeSi equal to SiO 2 Sign of thermodynamic driving force: – By calculating the volume change – By experiments with higher Fe content Result: the reaction is favored under high pressure and higher Fe content (See Fig 8-9)

Lower mantle Outer core Liquid Fe alloy Reaction Zone Boundary layer Mixed(?)thermal and chemical D”layer perovskitemagnesiowustite Metalic alloys Implications on the CMB The proposed reaction inevitablytakes place in D’’ Can cause strong heterogeneity in density, elastic properties and electrical conductivity Implications on the magnetic field –due to lateral variations in electric conductivity (Secular variations?) See Buffet,1996; Busse&Witch, 1992 Implications on mantle dynamics due to variations in thermal conductivity (Manga&Jeanloz, 1996)

Length and time scales Short time/length scale: Long time/length scales: – Mantle rocks in direct contact with core iron react rapidly. – The reaction zone will penetrate upwards on order of meters, based on capillary rise along grain boundaries – The reaction zone will be swept upwards by slow mantle convection. Will expose fresh rock to reaction. – Reacted material is denser – cannot rise very high  will form the D”layer

Implications on outer core Reaction products, mainly Oxygen, swept into the core by the rapid outer convection. May explain why the density is lower by 10% of pure liquid iron

Conclusions Lower mantle Outer core Liquid Fe alloy Reaction Zone Boundary layer Mixed(?)thermal and chemical D”layer perovskitemagnesiowustite Metalic alloys Preferred model – – Vigorous chemical reaction between liquid iron of the outer core and the crystalline silicates of the lower mantle. – Dissolving of mantle O, Mg and Siinto the core – Dissolving of core Fe into the mantle.