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Mathematical Model

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titleDefinition


3MUX9


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r_{wf} < r \leq r_e



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\frac{\partial p}{\partial t}  = \chi \, \left( \frac{\partial^2 p}{\partial r^2} + \frac{1}{r} \frac{\partial p}{\partial r} \right)



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p(t = 0, {\bf r}) = p_i



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\left[ a \cdot ( p(t, r ) - p_i) + b \cdot \frac{\partial p}{\partial r} \right]_{r \rightarrow \infty )} = p_i0



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\left[ r\frac{\partial p(t, r )}{\partial r} \right]_{r \rightarrow r_w} = \frac{q_t}{2 \pi \sigma}



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




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titleSolution

There is no universal analytical solution to the above problem

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LaTeX Math Block Reference
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but it can be always presented as below:


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p(t,r) = p_i - \frac{q_t}{4 \pi \sigma} \,  F \bigg( - \frac{r^2}{4 \chi t} \bigg)



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p_{wf}(t) = p_i - \frac{q_t}{4 \pi \sigma} \, \bigg[2S +   F \bigg( - \frac{r_w^2}{4 \chi t} \bigg) \bigg]


where

LaTeX Math Inline
bodyF(\xi)
a single-argument function describing the peculiarities of the diffusion model (well geometry, penetration geometry, formation inhomogeneities, hydraulic fractures, boundary conditions, etc.).

The fact that solution of equations

LaTeX Math Block Reference
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LaTeX Math Block Reference
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can be represented as
LaTeX Math Block Reference
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finds a lot of practical applications in Well Testing.



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titleDerivation



Applications

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