Page tree

Versions Compared

Key

  • This line was added.
  • This line was removed.
  • Formatting was changed.

...

Although the actual flow may not have an axial symmetry around the well-reservoir contact or reservoir inhomogeneities (like boundary and faults and composite areas) but still:

...



  • in most practical cases the long-term correlation between the flowrate and  bottom-hole pressure response can be approximated by a radial flow 


Inputs & Outputs

...


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
body{p_{wf}(t)}

well bottomhole pressure

LaTeX Math Inline
body\sigma

transmissibility

LaTeX Math Inline
body\chi

pressure diffusivity

...

Expand
titleDefinition



LaTeX Math Block
anchor52112
alignmentleft
\frac{\partial p}{\partial t}  = \chi \, \left( \frac{\partial^2 p}{\partial r^2} + \frac{1}{r} \frac{\partial p}{\partial r} \right)



LaTeX Math Block
anchor88AEG
alignmentleft
p(t = 0, {\bf r}) = p_i



LaTeX Math Block
anchor3MUX9
alignmentleft
p(t, r \rightarrow \infty ) = p_i



LaTeX Math Block
anchorEM415
alignmentleft
\left[ r\frac{\partial p(t, r )}{\partial r} \bigg|right]_{r \rightarrow 0r_w} = \frac{q_t}{2 \sigmapi \, dsigma}




Expand
titleSolution



LaTeX Math Block
anchorp_F
alignmentleft
p(t,r) = p_i + \frac{q_t}{4 \pi \sigma} \,  F \bigg( - \frac{r^2}{4 \chi t} \bigg)



LaTeX Math Block
anchorpwf
alignmentleft
p_{wf}(t) = p_i + \frac{q_t}{4 \pi \sigma} \, \bigg[ - 2S +   F \bigg( - \frac{r_w^2}{4 \chi t} \bigg) \bigg]


where

LaTeX Math Inline
bodyF(\xi)
a single-argument function describing the peculiarities of the diffusion model (well geometry, penetration geometry, formation inhomogeneities, hydraulic fractures, boundary conditions, etc.)


...