Question:

Consider the following diffusivity equation for the radial flow of a fluid in an infinite and homogeneous reservoir. \[ \frac{1}{r} \frac{\partial}{\partial r} \left( r \frac{\partial P}{\partial r} \right) = \frac{1}{\eta} \frac{\partial P}{\partial t} \] where, \( P \) denotes pressure, \( r \) is the radial distance from the center of the wellbore, \( t \) denotes time, and \( \eta \) is the diffusivity constant. The initial pressure of the reservoir is \( P_i \). The condition(s) used in the derivation of analytical solution of the above equation for pressure transient analysis in an infinite acting reservoir is/are:

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When solving for pressure transient analysis in reservoirs, remember the importance of initial conditions and boundary conditions, such as uniform pressure at the initial time and pressure approaching the initial value at infinity.
Updated On: May 1, 2025
  • At time \( t = 0 \), \( P = P_i \) for all \( r \).
  • Wellbore is treated as a line source.
  • As \( r \to \infty \), \( P \to P_i \) for all \( t \).
  • At any radius \( r \) and time \( t \), the pressure gradient \( \frac{\partial P}{\partial r} \) is constant.
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The Correct Option is A, B, C

Solution and Explanation

The diffusivity equation describes the radial pressure distribution in a reservoir due to fluid flow. The analytical solution of this equation requires certain assumptions and conditions, which include: 
- Option (A) is correct. At the initial time \( t = 0 \), the pressure is assumed to be uniform across the reservoir, and the pressure everywhere is equal to the initial pressure \( P_i \). This is a typical initial condition in pressure transient analysis. 
- Option (B) is correct. In the derivation of analytical solutions for pressure transient analysis, the wellbore is often modeled as a line source, which simplifies the mathematical treatment of radial flow. 
- Option (C) is correct. As the radial distance \( r \) becomes very large (i.e., far from the well), the pressure approaches the initial reservoir pressure \( P_i \) for all times, assuming no significant reservoir depletion in the far field. 
- Option (D) is incorrect because the pressure gradient \( \frac{\partial P}{\partial r} \) is not constant at all times and locations. The pressure gradient changes with time and position within the reservoir. 
Thus, the correct answers are options (A), (B), and (C).

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