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The viscous properties of the surrounding medium are described by Riemann Liouville fractional derivative.
The base plate and the solid phase of the porous medium are described as an equivalent visco-elastic plate.
Water flow and solute transport in a fractured medium are described by the Channel Network model, CHAN3D.
The designs of tubular mills loaded with steel rods along its length as the grinding medium are described in this chapter.
The results of dissolution experiments for benzene, toluene, m-xylene and naphthalene (BTXN) from a relatively insoluble oil phase (tridecane), residually trapped in a non-sorbing porous medium, are described.
For the spherical source (S1), spherical crack source (S2), and Eshelby spherical source (S5), the displacement fields in an infinite medium are described by the following static equilibrium equation: ∂ 2 u r ∂ r 2 + 2 r ∂ u r ∂r - 2 r 2 u r = 0, (11).
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The flow in porous medium is described by employing the Darcy Forchheimer based model.
Viscoelastic medium is described as infinite parallel springs as well as shear and viscous layers.
Dispersion of the medium is described by kz and the shift −ω/v indicates that Eq. (4) is solved in the local frame of the scatterer.
The surrounding elastic medium is described as the Winkler and Pasternak models, defined by the kw and kp coefficients.
A model problem for two-phase fluid flow and heat transfer with phase change in a porous medium is described.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com