The STOIIP is related to reservoir oil volume as: LaTeX Math Block |
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| V_O = V_o/B_o |
and while the latter is related to the reservoir pore volume as: LaTeX Math Block |
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| V_o = s_o \, V_\phi = (1-s_{wi}) \, V_\phi |
so that LaTeX Math Block |
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| V_o = B_o \, V_O = (1-s_{wi}) \, V_\phi \quad \Rightarrow \quad V_\phi = \frac{B_o \, V_O}{(1-s_{wi})} |
The pore volume reduction due to offtakes is:
LaTeX Math Block |
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| \delta V_\phi = Q_O \, B_o |
thus leading to LaTeX Math Block |
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| c_t = \frac{1}{V_{\phi}} \frac{\partial V_{\phi}}{\partial p} =
\frac{1-s_{wi}}{B_o \, V_O} \frac{B_o \, Q_O}{\delta p} =\frac{1-s_{wi}}{\delta p} \frac{Q_O}{V_O} = \frac{1-s_{wi}}{\delta p} \cdot {\rm EUR_O} |
where LaTeX Math Block |
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| c_t = c_r + s_{wi} c_w + (1-s_{wi})c_o |
is total compressibility of oil saturated formation and
LaTeX Math Block |
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| \delta p = p_i - p_{wf} |
pressure reduction due to pore volume reduction caused by offtakes. For low compressible oil, the total compressibility can be assumed constant and LaTeX Math Block Reference |
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| becomes: LaTeX Math Block |
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| \frac{1-s_{wi}}{(p_i - p_{wf \, min})} \cdot {\rm EUR_O} = c_t = \rm const |
and LaTeX Math Block |
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| {\rm EUR}_O = \frac{ (p_i - p_{wf \, min}) \, c_t}{(1-s_{wi})} |
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