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@wikipedia


The momentum balance equation relating a pressure gradient 

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body\nabla p
in porous medium with induced fluid flow (percolation) with velocity 
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body\bf u
A generalization of Darcy equation for the flow with account for inertial (kinetic) effects at high velocity reservoir flow:

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-  \nabla p = \frac{\mu}{k} \, {\bf u} + \beta \, \rho \,  | {\bf u} | \, {\bf u}

where

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body

{\bf u}

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body\nabla p

pressure gradient LaTeX Math Inlinebody

flow velocity vector

k

formation permeability 

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body\mu

fluid viscosity

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body\beta

Forchheimer coefficient


Forchheimer coefficient depends on flow regime and formation permeability as:

...

where 

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bodyC_E
 is Dimensionless dimensionless quantity called Ergun constant accounting for inertial (kinetic) effects and depends depending on flow regime only only.

 

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bodyC_E
 is small for the slow flow slow percolation (thus reducing Forchheimer equation to Darcy equation) and grows quickly for with high flow velocities.


Forchheimer equation can be approximated by non-linear permeability model as:


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{\bf u} =  - \frac{k}{\mu} \, k_f \, \nabla p

...



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k_f(|\nabla p|) =  \frac{2}{w} \big[ 1- \sqrt{1-w}   \big]

and



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w = 4 \, \left(\frac{k}{\mu} \right)^2 \, \beta \, \rho \,  |\nabla p| \, < \, 1



See also

...

Physics /  Fluid Dynamics / Percolation

Darcy Flow Equation ]

Reference

...

 Philipp Forchheimer (1886). "Über die Ergiebigkeit von Brunnen-Anlagen und Sickerschlitzen". Z. Architekt. Ing.-Ver. Hannover. 32: 539–563.