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In many practical cases the Radial Flow Pressure Diffusion is evolving towards pressure stabilization and can be efficiently analyzed using the pseudo-steady state flow model.


Inputs & Outputs

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InputsOutputs

LaTeX Math Inline
bodyq_t

total sandface rate

LaTeX Math Inline
bodyp(t,r)

reservoir pressure

LaTeX Math Inline
body{p_i}

initial formation pressure

LaTeX Math Inline
bodyp_{wf}(t)

well bottomhole pressure

LaTeX Math Inline
body\sigma

transmissibility,

LaTeX Math Inline
body\sigma = \frac{k \, h}{\mu}



LaTeX Math Inline
body\chi

pressure diffusivity,

LaTeX Math Inline
body\chi = \frac{k}{\mu} \, \frac{1}{\phi \, c_t}



LaTeX Math Inline
bodyS

skin-factor

LaTeX Math Inline
bodyr_w

wellbore radius

LaTeX Math Inline
bodyr_e

drainage radius


Expand
titleDetailing


LaTeX Math Inline
bodyk

absolute permeability

LaTeX Math Inline
bodyc_t

total compressibility,

LaTeX Math Inline
bodyc_t = c_r + c

LaTeX Math Inline
bodyh

effective thickness

LaTeX Math Inline
body{c_r}

pore compressibility

LaTeX Math Inline
body\mu

dynamic fluid viscosity

LaTeX Math Inline
bodyc

fluid compressibility

LaTeX Math Inline
body{\phi}

porosity


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Radial fluid flowHomogenous reservoirFinite reservoir flow boundarySlightly compressible fluid flowConstant rateConstant skin

LaTeX Math Inline
bodyp(t, {\bf r}) \rightarrow p(r)

LaTeX Math Inline
body{\bf r} \in ℝ^2 = \{ x, y\}

LaTeX Math Inline
bodyM(r, p)=M =\rm const

LaTeX Math Inline
body\phi(r, p)=\phi =\rm const

LaTeX Math Inline
bodyh(r)=h =\rm const

LaTeX Math Inline
bodyc_r(r)=c_r =\rm const

LaTeX Math Inline
bodyr_w \leq r \leq r_e < \infty

LaTeX Math Inline
bodyc_t(r,p) = \rm const

LaTeX Math Inline
bodyq_t = \rm const

LaTeX Math Inline
bodyS = \rm const

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Expand
titleDefinition


3MUX9p(t, r ) = p(r) \Leftrightarrow 0


LaTeX Math Block
anchor3MUX9
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r_{wf} < r \leq r_e




LaTeX Math Block
anchor
52112
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\frac{\partial p}{\partial t}
= 
LaTeX Math Block
anchor52112
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\chi \left[ \frac{\partial^2 p}{\partial r^2} + \frac{1}{r} \frac{\partial p}{\partial r} =0\right]



LaTeX Math Block
anchor3MUX9
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\left[ \frac{\partial p}{\partial r} \right]_{r=r_e} = 0



LaTeX Math Block
anchorEM415
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\left[ r\frac{\partial p(r )}{\partial r} \right]_{r \rightarrow r_w} = \frac{q_t}{2 \pi \sigma}



LaTeX Math Block
anchor3MUX9
alignmentleft
p_{wf}= p(r_w ) - S \cdot r_w \, \frac{\partial p}{\partial r} \Bigg|_{r=r_w}



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