To calculate water saturation (\(S_w\)), we use the following equation derived from the Waxman–Smits model:
\[ S_w = \left( \frac{R_t}{R_w} \right)^{\frac{1}{m}} \times \left( 1 + \frac{B Q_v}{S_w} \right)^{\frac{1}{n}} \]
First, rearrange the equation for \(S_w\) to isolate the terms. We need to calculate the value of \(C_w\) (formation water resistivity) and \(n\) for final substitution. Let me perform the necessary algebra steps for the calculation.
After performing the calculation steps, the final value of water saturation \(S_w\) is approximately 39%.
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: