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Property closures delineate the complete set of theoretically feasible combinations of macroscale (homogenized) properties in a given material system.
If the spins of neighboring electrons in a given material are opposite one another, these magnetic fields cancel each other out.
Because a fast electron will travel perhaps 100 times as far in a given material as a heavy charged particle with the same initial energy, its energy is much less densely deposited along its track.
Ferroelectricity ceases in a given material above a characteristic temperature, called its Curie temperature, because the heat agitates the dipoles sufficiently to overcome the forces that spontaneously align them.
Property closures are an important outcome of the MSD methodology, and delineate the complete set of theoretically feasible effective (homogenized) anisotropic property combinations in a given material system for a selected homogenization theory.
The theory of plurality of forms is instead the theory that there is a plurality of substantial forms in a given material substance.
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In addition, for a given material, changes in the trajectory paths occur because of changing crack growth mechanisms.
In fact for a given material, loading and mechanical boundary conditions the former parameter depends only on the applied stress amplitude and load ratio in a constant amplitude fatigue test, while the latter depends also on the specimen geometry, test frequency and the thermal boundary conditions that determine the rate of heat transfer from the material to the surroundings.
A robust method is suggested for the classification of the porous samples of a given material in terms of permeability heterogeneities.
Engineers can calculate the maximum stiffness of a given material in a given shape; for instance, they know how to give airplane wings their maximum strength using a given alloy.
According to the current theoretical understanding, the two electron-phonon coupling parameters βBG and βint are expected to be independent of disorder for a given material in the weakly disordered regime [7].
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