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Normalised dimensionless difference between the sandface bottomhole pressure (BHP)  p_{wf}(t) and the sandface reservoir pressure  \displaystyle p({\bf r}, t) |_{{\bf r} \in \Gamma_s} at the boundary \Gamma_s of damaged reservoir zone A_s

S = \frac{2 \pi \sigma}{q_t} \cdot \left[ p_{wf}(t) - p({\bf r}, t) |_{{\bf r} \in \Gamma_s} \right]

where

q_t

total sandface rate

\sigma

formation transmissibility at the boundary \Gamma_s of the damaged reservoir zone  A_s

A_s

damaged reservoir zone

\Gamma_s


It quantitatively characterises permeability change in a thin layer around the well or fracture plane caused by stimulation or deterioration during production, injection or well intervention.

It contributes to the total skin estimated in transient well testing


For the radial-symmetric permeability change around the well it can be estimated from Hawkins equation:

(1) S_M = \left ( \frac{k}{k_s} - 1 \right ) \ \ln \left ( \frac{r_s}{r_w} \right )

where 

r_w

well radius from drilling

r_s

damaged reservoir ( k_s \neq k) radius: r_s > r_w ( the most typical range is: r_w < r_s < 1 m )

k

absolute formation permeability in the undamaged reservoir zone away from well location

k_s

absolute formation permeability in the damaged near-well reservoir zone


The definition 

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suggests that
 

  • deteriorated near-well reservoir zone  k_s < k is characterized by a positive skin-factor  S>0,
     
  • improved near-well reservoir zone   k_s > k is characterized by a negative skin-factor  S<0.


The most popular practical range of skin-factor variation is  -5 < S < 8.


Formula 

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 provides a good example how mechanical skin-factor affects pressure dynamics.


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