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Double Diffusion in the Core David Gubbins SEE, University of Leeds CIDER Community Workshop Marconi Center 2009 David Gubbins SEE, University of Leeds.

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Presentation on theme: "Double Diffusion in the Core David Gubbins SEE, University of Leeds CIDER Community Workshop Marconi Center 2009 David Gubbins SEE, University of Leeds."— Presentation transcript:

1 Double Diffusion in the Core David Gubbins SEE, University of Leeds CIDER Community Workshop Marconi Center 2009 David Gubbins SEE, University of Leeds CIDER Community Workshop Marconi Center 2009

2 Double Diffusion in the Oceans  In the oceans, solar heating warms the top producing hot (light), salty (heavy) water  Heat diffuses faster than salt  This leads to an instability, loss of heat increases the density and carries salty water downwards, producing an instability (salt fountain)  This process can produce “fingering” (salt fingers)  …and establish layering, stratified layers separated by thin zones of turbulent mixing  In the oceans, solar heating warms the top producing hot (light), salty (heavy) water  Heat diffuses faster than salt  This leads to an instability, loss of heat increases the density and carries salty water downwards, producing an instability (salt fountain)  This process can produce “fingering” (salt fingers)  …and establish layering, stratified layers separated by thin zones of turbulent mixing

3 Double Diffusion in the Core  If both heat and composition are unstable, they combine  If a layer is compositionally stratified (e.g. at top or bottom of the core) we have the opposite situation to the oceans  The top is cold (heavy) and high in light elements (light)  This produces an overstability  This can also produce a layered structure  The time scale is about 100 Myr  If both heat and composition are unstable, they combine  If a layer is compositionally stratified (e.g. at top or bottom of the core) we have the opposite situation to the oceans  The top is cold (heavy) and high in light elements (light)  This produces an overstability  This can also produce a layered structure  The time scale is about 100 Myr

4 Possible Stratified Layers  1991: Souriau & Poupinet find decrease in Vp of 0.1% in bottom 150 km of inner core, deduce density stratification  1992, 1995: Song & Helmberger find similar anomalous structure from amplitudes and waveforms -> PREM2  1995: Similar structure incorporated into model AK135…  …confirmed by others, eg Zou, Koper & Cormier (2008)  At the top: slow diffusion of light elements from the mantle may produce ~100km light layer (Asahara et al, 2007; Hernlund)  1991: Souriau & Poupinet find decrease in Vp of 0.1% in bottom 150 km of inner core, deduce density stratification  1992, 1995: Song & Helmberger find similar anomalous structure from amplitudes and waveforms -> PREM2  1995: Similar structure incorporated into model AK135…  …confirmed by others, eg Zou, Koper & Cormier (2008)  At the top: slow diffusion of light elements from the mantle may produce ~100km light layer (Asahara et al, 2007; Hernlund)

5 In the oceans, evaporation at the surface leads to hot salty water above cold fresh water, leading to a “perpetual salt fountain”. In the core the solute is light and the gradients are opposite, as on the right, leading to overstable oscillations. DOUBLY-DIFFUSIVE CONVECTION

6 Parameters for the Core Two Rayleigh numbers: Ra, Rs Ra=g  T  Td 3 /  Ratio Ra/Rs =  T  T/  c  x For compositional stratification  x = 0.02 For a layer on the liquidus  T = 500 K Then Ra/Rs = 0.02 Two Rayleigh numbers: Ra, Rs Ra=g  T  Td 3 /  Ratio Ra/Rs =  T  T/  c  x For compositional stratification  x = 0.02 For a layer on the liquidus  T = 500 K Then Ra/Rs = 0.02

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8 In the oceans double diffusion leads to a stack of stably stratified layers separated by thin, turbulent zones After J. S. Turner, “Buoyancy in Fluids”, 1979

9 CONCLUSIONS: DYNAMICAL STABILITY  A partially stratified layer may be subject to doubly-diffusive instabilities  This may lead to layering within the stable zone, as in oceanic double diffusion  Layering could explain the discrepancy between seismic travel times and amplitudes  Worth a look!  A partially stratified layer may be subject to doubly-diffusive instabilities  This may lead to layering within the stable zone, as in oceanic double diffusion  Layering could explain the discrepancy between seismic travel times and amplitudes  Worth a look!


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