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One of the recently proposed families of these promising materials is represented by the diborides of heavy 4d and 5d metals.
The influence of the unitary costs of the insulation materials is represented in Fig. 3a c.
The mechanical behaviour of viscoelastic cracked materials is represented by the dual BEM formulation (Portela et al. 1992; Leonel and Venturini 2010; Leonel et al. 2011).
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They produce so-called multi-material cells, in which materials are represented by material polygons that contain only one material.
The microphotographs of the obtained materials are represented in Fig. 3.
The ISR of the six study materials are represented, with the cell viability for each in the inset.
Detection of the symmetry and reduction of the unit cell In AiiDA, modelled materials are represented as non-reduced unit cells of a crystal, in other words, as if their symmetry space groups were P 1.
The main hindrances to the development of these materials are represented by the relatively low capacity (150 mAh g−1), the lower, sloped reaction potential (3.2 3.3 V vs. Li+/Li) compared to the higher, flatter potential of, for example, LiFePO4 (3.4 V vs. Li+/Li) and the lack of lithium/sodium in the initial compound.
The granular material is represented as assemblies of ellipsoidal particles.
A random heterogeneous material is represented by a family of microstructures.
At the macroscopic scale, the material is represented as a micropolar continuum.
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CEO of Professional Science Editing for Scientists @ prosciediting.com