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LaTeX Math Inline
bodyt

time since the water injection rate has changed by the 

LaTeX Math Inline
body\delta q_2
value.

LaTeX Math Inline
bodyp_{u,\rm 21}(t)

cross-well pressure transient response in producer W1 to the unit-rate production in injector W2


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titleDerivation


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Consider a pressure convolution equation for the BHP in producer Wwith constant flowrate production at producer W1 

LaTeX Math Inline
bodyq_1 = \rm const
 and varying injection rate at injector W2 
LaTeX Math Inline
bodyq_2(t)
:

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anchorCase2_PSS_p11
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p_1(t) = p_i - \int_0^t p_{u,\rm 11}(t-\tau) dq_1(\tau) - \int_0^t p_{u,\rm 21}(t-\tau) dq_2(\tau) = p_i - \int_0^t p_{u,\rm 21}(t-\tau) dq_2(\tau)

Consider a step-change in injector's W2 flowrate 

LaTeX Math Inline
body \delta q_2
 at zero time 
LaTeX Math Inline
body\tau = 0
, which can be written as: 
LaTeX Math Inline
bodydq_2(\tau) = \delta q_2 \cdot \delta(\tau) \, d\tau
.

The responding pressure variation 

LaTeX Math Inline
body\delta p_1
in producer Wwill be:

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anchorCase2_PSS_p11
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\delta p_1(t) = p_1(t)-p_i = - \int_0^t p_{u,\rm 21}(t-\tau)  \delta q_2 \cdot \delta(\tau) \,  d\tau = - p_{u,\rm 21}(t) \cdot  \delta q_2




Case #2 – Constant BHP
LaTeX Math Inline
bodyp_1 = \rm const

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