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Published byFerdinand Owens Modified over 9 years ago
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Specific heat
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Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO
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Thermal expansion
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Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO
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Once have F(V.T) -- can get everything
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Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO
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M-G EOS Parameters -- from Stixrude et al, 2005 with modifications
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High pressure experiments
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2) Anvil Devices: 2 broad types Static Measurements: i)Large volume multi-anvil press (MAP) ii) Symmetric opposed anvil design (many different designs e.g. DAC)
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Types of Large Volume Presses Piston-Cylinder- 4-6 Gpa Multi-Anvil- 25GPa Paris-Edinburgh- 12GPa
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A large-volume high-pressure and high-temperature apparatus for in situ X-ray observation, ‘SPEED-Mk.II’ By Katsura et al SPEED-Mk.II’ is a multi- anvil KAWAI-type press
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Large volume multi anvil cells: Large volume: House probes, synthesize larger specimens, some experiments require large V (e.g. ultrasonic interferometry) Hydrostatic Pressure: Closer, since squeezing from 8 directions, But, not easily used with gas pressure medium Pressures: Top of lower mantle at best with sintered diamonds and synchrotron radiation 3 orders of magnitude higher than DACs!
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P/T Measurement Pressure can be measured by calibrating the machine to a sample with well known diffraction patterns, such as NaCl. Since this is a large volume press, temperature can be measured directly with thermocouples.
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Diamond Anvil Cells: Why Diamonds? Can use: Steel, tungsten carbide, boron carbide, sapphire, cubic zirconia, sintered diamond, or single-crystal diamond Single crystal diamond: 1) Strongest material known 2) Transparent (IR, optical, UV, and X-ray) 3) Non-magnetic insulator: ,
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Creating Temperature: 3 ways: 1) External heating 2) Internal heating 3) IR Laser Heating
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unheated ruby chips Sample size Optics to enlarged image Pressure medium P-T gradient
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Laser heating - use black body radiation T: temperature I: intensity : wavelength Cs: constants : emissivity Perfect black body: = 1 Grey body: < 1 is wavelength dependent But dependence not known for many materials! (known for Fe)
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Advances in laser heating… - Double sided laser heating - split beam and heat from both ends - Or mix 2 lasers at different modes - flat T distribution - Can now get temps ~3000K (+/- 10K) at high P - Bottom line: use caution when trusting results from laser heating experiments prior to 1996-98
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Pressure media low shear strength Chemical inertness Low thermal conductivity Low emissivity Low absorption of laser light Ar 8GPa, Ne 20GPa, He >100GPa Draw back: high fluorescence, high compressibility
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Pressure gradients
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Synchrotron Radiation Bi-product of particle accelerators Transverse emission of EM radiation tangential to ring Advantages: 1)Focussing (on small samples) 2)Bandwidth 3)Strength to penetrate high pressure vessels 4)Polarized - elasticity, structure, density of states Now: ‘3rd generation’ synchrotron radiation
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Provides Crystal Structure, Density and melting points Synchrotron Radiation provides highly collimated x-ray source Braggs Law: 2q = angle of diffraction d = spacing of crystal planes = wavelength of X-ray In-Situ X-Ray Diffraction Measuring Material Parameters…
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X-Ray Spectrography Use polychromatic X-rays and Be gaskets Observe absorption freq. Absorption changes with phase Observe: –Atomic Coordination –Structures –Electronic/Magnetic Properties Measuring Material Parameters…
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X-ray detected lattice parameters during a phase transformation For X-ray studies: Know temp gradients Suitable pressure mediums Angular Diffraction method Monochromatic X-rays used Best for quantitative intensity Precision Lattice Parameter measurement Energy Diffraction method Fastest method Gasket Selection Be allows trans-gasket measurements at 4 keV+ Diamonds allow hard X-rays. 12 keV+
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Measurement of Pressure Ruby Chips Fluorescence Method –Freq. shift of ruby with increasing pressure –Linear to 30 GPa –Calibrated to 100 GPa by Raman Spec. –Calibrated to >200 GPa by Gold –Accurate to 15-20% at 200 GPa –Diffuses with temperature (>700K) –Ruby and Diamond Fluorescence overlap between 120-180 GPa –KEY: Allows sampling at multiple points in pressure medium Measuring Material Parameters…
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Need higher pressure
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Optical Probes Optical Absorption –High pressure melting, crystallization, phase transitions Infrared Spectroscopy –Detailed bonding properties Raman Spectroscopy (10-1000cm -1 ) –Most definitive diagnostic tool for the identification of specific molecules –Diagnostic evidence for phase transition in simple molecular compounds Brillouin Spectroscopy (<1cm -1 ) –Wave velocities and elasticity tensor –New primary pressure standard Fluorescence Spectroscopy –Electronic states
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Raman Spectroscopy Raman Techniques –Measures scattering of monochromatic light due to atomic vibrations. Provides vibration frequencies in a solid –Temperature = noise : most samples temperature quenched. –Synchrotron radiation: a powerful, narrow beam of highly collimated light source. Parameters Measured –Entropies –Specific Heats –Grüneisen Parameters –Phase Boundaries Measuring Material Parameters…
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Elastic Moduli: , , Vp, Vs 3 ways to get these: 1)Static compression (no info on shear properties) 2)Shock compression 3)Acoustic vibration (frequencies 10^13 Hz) (applicability?)
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Extending elastic observations to higher P-T: Brillouin Spectroscopy - Optical beam scattered by an acoustic wave Compression and dilatation by acoustic wave results in change in refractive index of material Look at Doppler shift of laser frequency - get wave velocity of the acoustic wave can get up to ~60GPa at ~2500K in DAC with laser (mid lower mantle)
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Some conclusions Early DAC measurements suspect because non-hydrostatic Still very hard to do simultaneous high T and P – very few elasticity measurements at high T Pressure calibrations improving and becoming more consistent – but take care when using older measurements!
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Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO
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Raman Spectroscopy
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