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Global earth structure lecture 2 EPS 122 –Spring 2017 03/14/2017 Instructor: Barbara Romanowicz Sharp density changes: 1) CMB: 5.57 103-à 9.90 103 kg/m3 2) At 410 and 660 km discontinuities (about 5%) 3) At the inner core boundary: about 4% Density profile -> gravity -> pressure inside the earth: r P(r) = − ∫ g(r)ρ (r)dr 0 1 GPa = 10 kbar or 1 atm =105 Pa 410 km: P= 13.3 GPa 660 km: P= 23.8 GPa CMB P = 136 GPa ICB P = 329 GPa Center P = 364 GPa Silicate mantle Mostly Mg Iron rich core Composition constrained from seismology+density+lab. experiments on behavior of earth materials at high P and T Composition • Constraints: extraterrestrial – Nucleosynthesis – Meteorites • Constraints: near surface – Xenoliths – Magma source • Constraints: Interior – Physical properties • Fractionation important – Earth-hydrosphere-space – Crust-mantle-core èPyrolite/Lherzolite/Peridotite/… A conceptual model of a high pressure device for experiments under various conditions of pressure and temperature. A diamond anvil cell Samples ~30µm in diameter Pressures > 500 GPa T -> 6000 K Multi-anvil presses and diamond cells generate pressures that cover full range of conditions in the mantle and even the core. Multi-anvil apparatus “DIA” 3 pairs of octohedral pistons; internal heating -> 20 Gpa Larger samples ~1 mm in diameter Heated internally – can be used to study deformation Elastic properties and changes in crystal structure can be recorded “in situ” when combined with monochromatic X-ray beam The silicate mantle • Main constituent: olivine – End members of olivine • Forsterite (Fo) Mg2SiO4 • Fayalite (Fa) Fe2SiO4 – “normal mantle”: very forsteritic : Fo91-Fo94 • Here 91= 91% of Mg in (Mg,Fe)2SiO4 • Other major mantle minerals: • Orthopyroxene (Opx) (Mg,Fe)SiO3 • Clinopyroxene (Cpx) Ca(Mg,Fe)Si2O6 • Garnet (Gt) (Mg,Fe)3Al2Si3O12 Pyrolite model: composition of upper mantle Pyrolite is a synthetic rock invented by Ringwood as a model for experimenting with constitution of the upper an lower mantle. This composition is generally accepted for the uppermost part of the mantle. As we go deeper, differences among various authors increase. In particular, it remains a matter of a hot debate whether composition is constant throughout the mantle. Phase changes in olivine • Olivine undergoes phase changes to denser structure at pressures equivalent to depths ~400km, ~520 km and ~670 km. – 400-670km: mantle “transition zone” • At 400 km: olivine phase change: – Olivine (α) to spinel (β) – Exothermic (releases heat) Clapeyron slope 2-3MPa/K – Density increases by about 5% At 400 km: olivine phase change: Olivine (α) to spinel (β) Exothermic Increase in density and seismic velocities ~5% At 520 km: (β)-> (γ) (wadsleite to ringwoodite) Less effect on seismic velocities Exothermic At 670 km: (γ)-> perovskite (Mg,Fe)SiO3+magnesiowüstite (Mg,Fe)O Endothermic (negative Clapeyron slope (-2-6 MPpa/K) Increase in density by ~10% Melting temperatures such that mantle is solid Phase diagrams Two different models for upper mantle composition Two different data types to investigate upper mantle discontinuities … * reflected waves * both continents and oceans * converted waves * only beneath stations Global Transverse Component Stacks Shearer, 1991 Receiver function concept Mantle Phases • Upper mantle – Olivine, orthopyroxene, clinopyroxene, plag→spinel→garnet • Transition Zone – Olivine→Wadsleyite→ Ringwoodite – Pyroxenes dissolve into garnet • Lower mantle – Two perovksites + oxide • What else? – Most of interior still relatively little explored – Discovery of post-perovskite phase (2004) Mineral sequence II Lower Mantle + + (Mg(1-x-z),Fex, Alz)(Si(1-y),Aly)O3 Mg/Fe perovskite (Mgx,Fe(1-x))O oxide CaSiO3 Ca- perovskite Minerals in Earth’s mantle (Mg,Fe,Al)-MgSiO3 perovskite post-perovskite? CaSiO3 - perovskite (Mg,Fe)O - ferropericlase (Mg,Fe,Al,Ca)silicates Courtesy of S. Sinogeikin Now called bridgmanite Heterogeneity in the D” region of the mantle Precursors to ScS S ScS The lowermost mantle Most of the lower mantle appears to have a constant composition and changes in the seismic velocities and density appear to correspond to those predicted accounting for the increasing pressure. There are, however, complications in the deepest 200-300 km of the mantle. The example on left is a collection of S-velocity models in the lowermost mantle. The origin of the discontinuity has recently been attributed to a newly discovered phase transition: perovskite-> post-perovskite Discovery of post-perovskite at T and P conditions of the base of the mantle (120 GPa, 2500oC) MgSiO3 perovskite MgSiO3 post-perovskite N= New phase M Murakami et al. Science 2004;304:855-858 Periclase: cubic structure (cf NaCl) Bridgmanite and post-perovskite: Orthorombic structure MgSiO3 phase diagram in the lower mantle based on LHDAC Experiments of Murakami et al. (2004) and ab inito computations of Tsuchiya et al. (2004) Irifune and Tsuchiya (2015)