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Normalised dimensionless difference between the sandface bottomhole pressure (BHP)  p_{wf}(t) and a model of a full-entry vertical well with homogeneous reservoir and non-damaged near-well reservoir zone  p^*_{wf}(t):

S = \frac{p_{wf}(t) - p(t, r_w)}{r_w \cdot \frac{\partial p}{\partial r} \Bigg|_{r=r_w} }

where

q_t

total sandface rate

\sigma

formation transmissibility outside the damaged reservoir zone  A_s


By definition the skin-factor is a pressure adjustment at the well-reservoir contact and does not affect pressure distribution in reservoir away from wellbore r > r_s.


The total skin is usually decomposed into a sum of two components:

S_T = S_G + \frac{A_w}{A_{wrc}} \cdot S_M

where

S_G

Geometrical skin, related to deviation of the well-reservoir contact from the simplest model

S_M

Mechanical skin, related to pressure drop caused by the near-reservoir zone formation damage

A_w

borehole flow area

A_{wrc}

well-reservoir contact area


Based on definition the wellbore pressure dynamics  p_{wf}(t) of the well with skin-factor can be writen as:

p_{wf}(t) = \frac{q_t}{2 \pi \sigma} \, S + p^*_{wf}(t)

where  p^*_{wf}(t) is a model of a full-entry vertical well with homogeneous reservoir and non-damaged near-reservoir zone.

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