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The macroscopic description of a defect-free, flat grain boundary in a pure material requires five degrees of freedom.
In this work, the computationally efficient model is a sharp interface solidification model of a pure material.
Stress variations along a perturbed planar growth front result in variations in interfacial mobility in a manner that is destabilizing under one sign of the stress state and stabilizing under the opposite sign, even for a pure material.
The simulation is performed on a two dimensional square grid for dendrites of a pure material growing into an undercooled liquid.
Algorithm performance is assessed for two benchmark problems of phase change convection of a pure material, one melting and one freezing.
It is shown that in alloy solidification with complete solute trapping the T−V relation is similar to that of a pure material with a hypothetical "melting point" given as the T0-temperature.
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PLD uses very high intensity pulses of UV laser to deposit subatomic layers from a target of pure material onto a substrate.
The phase angle, δ, is equal to 90° for a purely viscous material, 0° for a pure elastic material, and 0° < δ < 90° for viscoelastic materials [ 36].
Hence, the hyperspectral unmixing, which decomposes a mixed pixel into a combination of pure material spectra known as endmembers, weighted by their corresponding abundance coefficients, is a challenging task.
Cycling behavior at 0.245 mA cm−2 is characterized by high and stable (after the first few cycles) specific capacity, ie 0.28-0.24 A hg−1 of pure material.
It possesses a thick section of pure material (ice) that can be used as a cosmic particle detector.
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