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For the pressure diffusion with constant diffusion coefficients and homogeneous boundary conditions the pressure response  p(t) in one well to a complex flowrate history  q(t) in the same well honours the convolution equation:

(1) p(t) = p_0 + \int_0^t p_u(t-\tau) \, dq(\tau) = p_0 + \int_0^t p_u(t-\tau) \, \dot q(\tau) \, d\tau

where

p_0

initial formation pressure at zero time t=0

p_u(\tau)
Drawdown Transient Response

\dot q(\tau) = \frac{dq}{d\tau}


a pace of sandface flow rate variation per unit time



In case a well is interfering with the offset wells the pressure in a given well   n may respond to the offset wells  m \neq n and the multi-well form of convolution is going to be:

(2) p_n(t) = p_{n, 0} + \sum_{m=1}^N \int_0^t p_{u,nm}(t-\tau) \, dq_m(\tau) = p_{n, 0} + \sum_{m=1}^N \int_0^t p_{u,nm}(t-\tau) \, \dot q_m(\tau) \, d\tau = p_{n, 0} + \int_0^t p_{u,nn}(t-\tau) \, \dot q_n(\tau) \, d\tau + p_{n, 0} + \sum_{m \neq n}^N \int_0^t p_{u,nm}(t-\tau) \, \dot q_m(\tau) \, d\tau

where

p_{n, \, 0}

Initial formation pressure at zero time t=0 for the n-th well

p_{u,nm}(\tau)

Drawdown Transient Response in the n-th well to the unit-rate production


p_{u,nm}(\tau)



Cross-well Transient Response
in the n-th well to the unit-rate production in m-th well


\dot q_m(\tau) = \frac{dq_m}{d\tau}


A speed of n-th well total sandface flow rate variation

See Also


Petroleum Industry / Upstream / Subsurface E&P Disciplines / Well Testing / Pressure Testing

Well & Reservoir Surveillance ] [ Pressure Diffusion ] [ Pressure drawdown ]

Convolution @math ]

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