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. LaTeX Math Block |
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| J = \frac{q}{p_{\rm frm} - p_{wf}} = \frac{2 \pi \sigma}{ \ln \frac{r_e}{r_w} - \epsilon + S} = \frac{2 \pi \cdot \frac{k \, h}{\mu} }{ \ln \frac{r_e}{r_w} - \epsilon + S} |
where |
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definition and boundary type ( LaTeX Math Inline |
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body | \epsilon =\{ 0, \, 0.5, \, 0.75 \} |
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In case of homogeneous reservoir with only one vertical well producing the Dupuit PI @model is the exact analytical solution of Reservoir Flow Model (RFM).
Table 1. Variations to Dupuit PI @model depending on the reservoir flow regime and the definition/application of Productivity Index. |
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| J_e = \frac{2 \pi \sigma}{ \ln \frac{r_e}{r_w} + S} |
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| LaTeX Math Block |
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| J_e = \frac{2 \pi \sigma}{ \ln \frac{r_e}{r_w} |
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For the fractured vertical well the geometrical skin-factor is related to Fracture half-length as: LaTeX Math Block |
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| S_G = -\ln \left(\frac{X_f}{2\, r_w} \right) |
LaTeX Math Block |
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| J = \frac{q}{p_{\rm frm} - p_{wf}} = \frac{2 \pi \sigma}{ \ln \frac{r_e}{r_w} - \epsilon + S} = \frac{2 \pi M \cdot h}{ \ln \frac{r_e}{r_w} - \epsilon + S} = \frac{2 \pi k_{abs} \cdot h}{ \ln \frac{r_e}{r_w} - \epsilon + S} \cdot M_r = T \cdot M_r(s_w, s_g) |
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See also
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Petroleum Industry / Upstream / Subsurface E&P Disciplines / Well Testing / Pressure Testing
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