Mineral physics
Mineral physics is the science of materials that compose the interior of planets, particularly the Earth. It overlaps with
Laboratory work in mineral physics require high pressure measurements. The most common tool is a diamond anvil cell, which uses diamonds to put a small sample under pressure that can approach the conditions in the Earth's interior.
Creating high pressures
Shock compression
Many of the pioneering studies in mineral physics involved explosions or projectiles that subject a sample to a shock. For a brief time interval, the sample is under pressure as the
Multi-anvil press
Multi-anvil presses involve an arrangement of anvils to concentrate pressure from a press onto a sample. Typically the apparatus uses an arrangement eight cube-shaped tungsten carbide anvils to compress a ceramic octahedron containing the sample and a ceramic or Re metal furnace. The anvils are typically placed in a large hydraulic press. The method was developed by Kawai and Endo in Japan.[2] Unlike shock compression, the pressure exerted is steady, and the sample can be heated using a furnace. Pressures of about 28 GPa (equivalent to depths of 840 km),[3] and temperatures above 2300 °C,[4] can be attained using WC anvils and a lanthanum chromite furnace. The apparatus is very bulky and cannot achieve pressures like those in the diamond anvil cell (below), but it can handle much larger samples that can be quenched and examined after the experiment.[5] Recently, sintered diamond anvils have been developed for this type of press that can reach pressures of 90 GPa (2700 km depth).[6]
Diamond anvil cell
The
Creating high temperatures
Achieving temperatures found within the interior of the earth is just as important to the study of mineral physics as creating high pressures. Several methods are used to reach these temperatures and measure them. Resistive heating is the most common and simplest to measure. The application of a voltage to a wire heats the wire and surrounding area. A large variety of heater designs are available including those that heat the entire diamond anvil cell (DAC) body and those that fit inside the body to heat the sample chamber. Temperatures below 700 °C can be reached in air due to the oxidation of diamond above this temperature. With an argon atmosphere, higher temperatures up to 1700 °C can be reached without damaging the diamonds. A tungsten resistive heater with Ar in a BX90 DAC was reported to achieve temperatures of 1400 °C.[8]
Properties of materials
Equations of state
To deduce the properties of minerals in the deep Earth, it is necessary to know how their density varies with pressure and temperature. Such a relation is called an equation of state (EOS). A simple example of an EOS that is predicted by the Debye model for harmonic lattice vibrations is the Mie-Grünheisen equation of state:
where is the heat capacity and is the Debye gamma. The latter is one of many Grünheisen parameters that play an important role in high-pressure physics. A more realistic EOS is the Birch–Murnaghan equation of state.[9]: 66–73
Interpreting seismic velocities
Inversion of seismic data give profiles of seismic velocity as a function of depth. These must still be interpreted in terms of the properties of the minerals. A very useful heuristic was discovered by
- .
This relationship became known as Birch's law. This makes it possible to extrapolate known velocities for minerals at the surface to predict velocities deeper in the Earth.
Other physical properties
- Viscosity
- Creep (deformation)
- Melting
- Electrical conductionand other transport properties
Methods of crystal interrogation
There are a number of experimental procedures designed to extract information from both single and powdered crystals. Some techniques can be used in a diamond anvil cell (DAC) or a multi anvil press (MAP). Some techniques are summarized in the following table.
Technique | Anvil Type | Sample Type | Information Extracted | Limitations |
---|---|---|---|---|
X-ray Diffraction(XRD)[12] |
DAC or MAP | Powder or Single Crystal | cell parameters | |
Electron Microscopoy | Neither | Powder or Single Crystal | Symmetry Group | Surface Measurements Only |
Neutron Diffraction | Neither | Powder | cell parameters | Large Sample needed |
Infrared spectroscopy[13] | DAC | Powder, Single Crystal or Solution | Chemical Composition | Not all materials are IR active |
Raman Spectroscopy[13] | DAC | Powder, Single Crystal or Solution | Chemical Composition | Not all materials are Raman active |
Brillouin Scattering[14] |
DAC | Single Crystal | Elastic Moduli | Need optically thin sample |
Ultrasonic Interferometry[15] | DAC or MAP | Single Crystal | Elastic Moduli |
First principles calculations
Using quantum mechanical numerical techniques, it is possible to achieve very accurate predictions of crystal's properties including structure, thermodynamic stability, elastic properties and transport properties. The limit of such calculations tends to be computing power, as computation run times of weeks or even months are not uncommon.[9]: 107–109
History
The field of mineral physics was not named until the 1960s, but its origins date back at least to the early 20th century and the recognition that the
A landmark in the history of mineral physics was the publication of Density of the Earth by Erskine Williamson, a mathematical physicist, and Leason Adams, an experimentalist. Working at the Geophysical Laboratory in the
The experimental work at the Geophysical Laboratory benefited from the pioneering work of
References
- S2CID 21791428.
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- ^ "Studying the Earth's formation: The multi-anvil press at work". Lawrence Livermore National Laboratory. Archived from the original on 28 May 2010. Retrieved 29 September 2010.
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- doi:10.1063/1.882374.
- ^ Yan, J., Doran, A., MacDowell, A.A. and Kalkan, B., 2021. A tungsten external heater for BX90 diamond anvil cells with a range up to 1700 K. Review of Scientific Instruments, 92(1), p.013903.
- ^ a b Poirier 2000
- .
- .
- ^ Burnley, Pamela. "Synchrotron X-Ray Diffraction". Science Education Resource Center. Carleton College. Retrieved 18 September 2015.
- ^ a b Thomas, Sylvia-Monique. "Infrared and Raman Spectroscopy". Science Education Resource Center. Carleton College. Retrieved 18 September 2015.
- ^ Thomas, Sylvia-Monique. "Brillouin Spectroscopy". Science Education Resource Center. Carleton College. Retrieved 18 September 2015.
- ^ Burnley, Pamela. "Ultrasonic Measurements". Science Education Resource Center. Carleton College. Retrieved 18 September 2015.
- ISBN 9780444535764. Retrieved 27 September 2017.
- ^ .
- .
- .
Further reading
- Kieffer, S. W.; Navrotsky, A. (1985). Microscopic to macroscopic : atomic environments to mineral thermodynamics. Washington, D.C.: Mineralogical Society of America. ISBN 978-0-939950-18-8.
- Poirier, Jean-Paul (2000). Introduction to the Physics of the Earth's Interior. Cambridge Topics in Mineral Physics & Chemistry. ISBN 0-521-66313-X.
External links
- "Teaching Mineral Physics Across the Curriculum". On the cutting edge - professional development for geoscience faculty. Retrieved 21 May 2012.