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Reverse the Inverse problem to spatial superposition where pressure response 

LaTeX Math Inline
bodyp_m(t)
in 
LaTeX Math Inline
bodym
-well is decomposed into a sum of individual pressure responses from :

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anchorPCD
alignmentleft
p_m(t) = p_i + \sum_k \delta p_{mk}(t) = p_i +   \int_0^t p_{umk}(t-\tau) \, dq_k(\tau) = p_i + \int_0^t p_{umm}(t-\tau) \, dq_k(\tau) + \sum_{k \neq m}  \int_0^t p_{umk}(t-\tau) \, dq_k(\tau)

where

 with:


InputOutput

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body\{ q_k(t_j) \}_{k=1..N, \, j= 1..T}

flowrate variation history

LaTeX Math Inline
bodyp_{umm}(\tau)

Drawdown Transient Response (DTR)

LaTeX Math Inline
body\{ p_k(t_j) \}_{k=1..N, \, j= 1..T}

pressure variation history

LaTeX Math Inline
body\delta p_{mk}(t)

specific component of 

LaTeX Math Inline
bodym
-well pressure variation caused by 
LaTeX Math Inline
bodyk
-well flowrate history 
LaTeX Math Inline
bodyq_k(t)

LaTeX Math Inline
bodyp_{umm}(\tau)

DTR pressure response in 
LaTeX Math Inline
bodym
-well to unit-rate drawdown in the same well 

LaTeX Math Inline
bodyp_{

ukm

umk}(\tau)

CTR pressure response in 

LaTeX Math Inline
bodym
-well to unit-rate drawdown in 
LaTeX Math Inline
bodyk
-well 

...

LaTeX Math Inline
bodyp_{ukm}(\tau)

...