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@wikipedia\backslash frac\{\backslash partial\; s\}\{\backslash partial\; t\}\; +\; q\; \backslash cdot\; \backslash frac\{\backslash partial\; \}\{\backslash partial\; x\}\; \backslash left(\; \backslash frac\{f\}\{\backslash phi\; \backslash ,\; A\; \}\; \backslash right)\; =\; 0s(t=0,x)\; =\; 0s(t,0)\; =\; 1@wikipedia


Ideally balanced water + dead oil 1D waterflood model without gravity and capillary effects. 

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\frac{\partial s}{\partial t} + q \,cdot \frac{\partial }{\partial x} \left( \frac{f}{\phi \, A \Sigma} \right) = 0
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s(t=0,x) = 0
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s(t,0) = 1

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body--uriencoded--\displaystyle s= E_D = \frac%7Bs_w - s_%7Bwi%7D%7D%7B1-s_%7Bwi%7D-s_%7Bor%7D%7D

water → oil displacement efficiency

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bodyq

sandface injection rate, assumed equal to sandface liquid production rate

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body\phi(x)

reservoir porosity

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bodyA\Sigma(x) = h \, L_ D

cross-section area available for flow

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bodyh(x)

reservoir thickness

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bodyL_D(x)

rerservoir reservoir width = reservoir length transversal to flow

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body--uriencoded--\displaystyle f = \frac%7B1%7D%7B1+M_%7Bro%7D/M_%7Brw%7D%7D

in-situ fractional flow function


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body--uriencoded--M_%7Bro%7D= k_%7Bro%7D(s_o)/\mu_o
relative oil mobility

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body--uriencoded--M_%7Bwo%7D = k_%7Brw%7D(s_w)/\mu_w

relative water mobility


Approximations

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In many practical applications (for example, laboratory SCAL tests and reservoir proxy-modeling) one can assume constant porosity and reservoir width: 

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\frac{\partial s}{\partial t_D} +\frac{\partial f}{\partial x_D} = 0
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s(t=0,x) = 0
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s(t,0) = 1

where

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body--uriencoded--\displaystyle t_D = \frac%7BV_\phi \, t%7D%7Bq%7D

dimensionless time

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body--uriencoded--\displaystyle x_D = \frac%7Bx%7D%7BL%7D

dimensionless distance

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bodyL

reservoir length along

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bodyx
-axis

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bodyV_\phi= \phi \cdot h \cdot D \cdot L

reservoir pore volume

See Also

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Petroleum Industry / Upstream / Subsurface E&P Disciplines / Dynamic Flow Model / Reservoir Flow Model (RFM)

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