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(1) \phi \cdot \partial_\tau \Psi - \nabla \cdot \left( k \cdot \vec \nabla \Psi \right) = 0
(2) -\frac{k}{\mu} \int_{\Sigma} \, \frac{\partial p}{ d n} \, d \sigma = q(t)

where

p(t, {\bf r})

reservoir pressure

t

time

\phi({\bf r})

effective porosity 

{\bf r }

position vector


c_t(p)
total compressibility 

{\bf r }_k

position vector of the k-th source


k
formation permeability to a given fluid

\nabla

gradient operator


\mu(p)

dynamic viscosity of a given  fluid

\displaystyle \Psi(p) =2 \, \int_0^p \frac{p \, dp}{\mu(p) \, Z(p)}

Pseudo-Pressure


Z(p)
fluid compressibility factor

\displaystyle \tau(t) = \int_0^t \frac{dt}{\mu(p) \, c_t(p)}

Pseudo-Time



q_k(t)




See also


Physics / Mechanics / Continuum mechanics / Fluid Mechanics / Fluid Dynamics / Pressure Diffusion / Pressure Diffusion @model






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