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LaTeX Math Block
anchorCK
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k = 1014.24 \cdot FZI^2 \cdot \frac{\phi^3}{( 1 - \phi )^2}

where

LaTeX Math Inline
body\phi

effective porosity

LaTeX Math Inline
bodyFZI

Flow Zone Indicator



with Flow Zone Indicator having a complex dependance on porosity and shaliness:

LaTeX Math Block
anchorCK12
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FZI(V_{sh},\phi_r) = {\rm w}_1(V_{sh}) \, \phi_r^{m_1} + {\rm w}_2(V_{sh}) \, \phi_r^{m_2}

for each lithofacies individually.


Usually, the first component  

LaTeX Math Inline
body{\rm w}_1(V_{sh}) \, \phi_r^{m_1}
 dictates Flow Zone Indicator values at low porosities while second component 
LaTeX Math Inline
body{\rm w}_2(V_{sh}) \, \phi_r^{m_2}
 takes over at high porosities.


This allows to cover a wider range of porosity variations comparing to single-component Cozeny-Karman permeability @model.


The dependance of weight coefficients on shaliness can be often approximated as:

LaTeX Math Block
anchor1
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{\rm w}_1(V_{sh})  = {\rm w}_{01} \, (1- V_{sh}/V_{sh1})^{g_1}


LaTeX Math Block
anchor1
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{\rm w}_2(V_{sh}) = {\rm w}_{02} \, (1- V_{sh}/V_{sh2})^{g_2}

where

LaTeX Math Inline
body\{ {\rm w}_{01}, \, {\rm w}_{02} \}

the highest values of weights for shale-free rock matrix

LaTeX Math Inline
body\{ V_{sh1}, \, V_{sh2} \}

critical values of shaliness at which the corresponding component of Flow Zone Indicator vanishes

LaTeX Math Inline
body\{ g_1, \, g_2 \}

cementing factors, when low they diminish dependance on shaliness


This model is very flexible and covers a wide range of practical cases.


When 

LaTeX Math Inline
body\{ m_1, \, m_2 \}
and 
LaTeX Math Inline
body\{ g_1, \, g_2 \}
 are small (
LaTeX Math Inline
body\sim 0
) the Flow Zone Indicator becomes independent on porosity and shaliness and the model degrades to conventional Cozeny-Karman permeability @model with
LaTeX Math Inline
bodyFZI = \rm const
.


See also


Petroleum Industry / Upstream / Subsurface E&P Disciplines / Petrophysics / Absolute permeability / Absolute permeability @model