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At the lowest scale (micro), a periodic lattice system describes in detail the mechanical response governed by interactions between rigid grains connected through elastic interfaces.
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Usually, the interaction between rigid diamond tool and silicon atoms is described by the Morse potential as follows: E r = De e − qα r − r 0 − q e − α r − r 0 (1).
Some interesting observations pertaining to the interaction between rigid inclusion and crack as well as between rigid inclusion and thin rigid line are discussed.
In other words, the lattice is seen as a "skeleton" in which the interactions between the rigid grains are represented by forces and moments which depend on their relative displacements and rotations.
In this study, the in vivo and in vitro interactions between elastic-, rigid vesicles and micelles with human skin were investigated.
The classical degenerate condition for a rigid top can manifest into a triple resonance, by the interaction between the two rigid modes and a two-dimensional liquid mode.
The interaction between the rigid diamond tool and aluminum atoms is depicted by the Morse potential: E={D}_0left[{e}^{-2alpha left( r-{r}_0right)}-2{e}^{-alpha left( r-{r}_0right)}right] (3).
The interaction between the rigid diamond tool and aluminum atoms is depicted by the Morse potential: E={D}_0left[{e}^{-2alpha left( r-{r}_0right)}-2{e}^{-alpha left( r-{r}_0right)}right] (3)where E is the pair potential energy, D 0 is the cohesion energy, α is a constant determined by material properties, r 0 is the distance at equilibrium, and r is the distance between two atoms.
The model captures the interaction between the rigid body and structural dynamics.
A complete interaction between the rigid PUF and MgO board was achieved using epoxy adhesives.
Most of the cell's heavy duty computation is done by direct interactions between the proteins.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com