Finite element modeling of melting and fluid flow in the laser-heated diamond-anvil cell

被引:9
|
作者
Gomez-Perez, N. [1 ,2 ,3 ]
Rodriguez, J. F. [4 ]
McWilliams, R. S. [2 ,3 ,5 ]
机构
[1] Univ Los Andes, Dept Geociencias, Bogota, Colombia
[2] Univ Edinburgh, Sch Phys & Astron, Edinburgh EH9 3FD, Midlothian, Scotland
[3] Univ Edinburgh, Ctr Sci Extreme Condit, Edinburgh EH9 3FD, Midlothian, Scotland
[4] Univ Los Andes, Dept Fis, Bogota, Colombia
[5] Carnegie Inst Sci, Geophys Lab, 5251 Broad Branch Rd NW, Washington, DC 20015 USA
基金
英国工程与自然科学研究理事会;
关键词
HIGH-PRESSURE; LOWER MANTLE; TEMPERATURE DISTRIBUTION; THERMAL-CONDUCTIVITY; MOLECULAR-DYNAMICS; PHASE-TRANSITIONS; EARTHS CORE; IRON; GRADIENTS; PLANETARY;
D O I
10.1063/1.4979313
中图分类号
O59 [应用物理学];
学科分类号
摘要
The laser-heated diamond anvil cell is widely used in the laboratory study of materials behavior at high-pressure and high-temperature, including melting curves and liquid properties at extreme conditions. Laser heating in the diamond cell has long been associated with fluid-like motion in samples, which is routinely used to determine melting points and is often described as convective in appearance. However, the flow behavior of this system is poorly understood. A quantitative treatment of melting and flow in the laser-heated diamond anvil cell is developed here to physically relate experimental motion to properties of interest, including melting points and viscosity. Numerical finite-element models are used to characterize the temperature distribution, melting, buoyancy, and resulting natural convection in samples. We find that continuous fluid motion in experiments can be explained most readily by natural convection. Fluid velocities, peaking near values of microns per second for plausible viscosities, are sufficiently fast to be detected experimentally, lending support to the use of convective motion as a criterion for melting. Convection depends on the physical properties of the melt and the sample geometry and is too sluggish to detect for viscosities significantly above that of water at ambient conditions, implying an upper bound on the melt viscosity of about 1 mPa s when convective motion is detected. A simple analytical relationship between melt viscosity and velocity suggests that direct viscosity measurements can be made from flow speeds, given the basic thermodynamic and geometric parameters of samples are known. Published by AIP Publishing.
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页数:13
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