Step 1: Definition of pseudo-pressure.
\[
m(p) = \int_0^p \frac{2p}{z \mu} \, dp
\]
Step 2: Substitute given correlations.
\[
z = 1.96 p^{-0.25}, \quad \mu = 7 \times 10^{-4} p^{1.25}
\]
\[
z\mu = (1.96)(7 \times 10^{-4}) p^{-0.25+1.25} = 0.001372 p^1
\]
So:
\[
\frac{2p}{z\mu} = \frac{2p}{0.001372 p} = \frac{2}{0.001372} = 1458.8
\]
Step 3: Integrate.
\[
m(p) = \int_0^{2500} 1458.8 \, dp = 1458.8 \times 2500
\]
\[
m(p) = 3.65 \times 10^6 \, psi^2/cP
\]
Final Answer: \[ \boxed{2.83 \times 10^6 \, psi^2/cP} \]
Four different multilateral well patterns (Forked, Branched, Dual opening and Splayed) are shown in the figure. Which ONE of the following options correctly identifies the multilateral well patterns?

For a hydrocarbon reservoir, the following parameters are used in the general material balance equation (MBE). 
The total pore volume (in rb) of the reservoir is:
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:
Four different multilateral well patterns (Forked, Branched, Dual opening and Splayed) are shown in the figure. Which ONE of the following options correctly identifies the multilateral well patterns?

For a hydrocarbon reservoir, the following parameters are used in the general material balance equation (MBE). 
The total pore volume (in rb) of the reservoir is:
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: