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The dynamic holographic method based on light-induced refractive index change during the interaction of beams in a material occupies a special place because it allows to potentially implement almost all currently known functions of manipulation of light [11,12].
These soft tissue fillers provide correction by two basic mechanisms: (1) the filler material occupies a void space, or (2) the filler material stimulates processes that produce volume.
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In particular, an incompressible, viscous, electrically conducting liquid material occupying a given domain Ω is considered.
Determination of the chemical components of the material occupying a region of space greatly enhances the identification of threats such as explosives, fissile materials, toxic materials and weapons of mass destruction.
Since the magnitude of optical gain is the practically most limiting factor, the modulation space for PT-symmetric materials occupies a relatively small region in the index modulation diagram, while plasmonic and metallo-dielectric metamaterials occupy the widest region in the vs. modulation space.
These assumptions are related to the modeling of reaction diffusion processes in composite materials occupying a bounded domain Ω, which at some points behave as perfect insulators.
We assume that a ferromagnetic material occupies the domain Ω.
In present days nano material occupies the major area in engineering field.
Foams are modelled as two-phase composites consisting of a solid material and voids; the elasto-plastic and damage response of the parent material is deduced from its measured mechanical responses in tension and compression, while the material occupying the voids is assigned a plastically compressible constitutive response, to mimic the effects of pore collapse and subsequent self-contact.
The material bed only occupies a small fraction of the volume of the kiln and has a negligible limited impact of temperature distribution.
The effect of three factors on constituent release were examined: (1) volume fraction of material occupied by the aggregates compared to a homogeneous porous material, (2) aggregate size and, (3) differences in mass transfer rates between the binder and the aggregates.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com