Step 1: Formula.
Dimensionless fracture conductivity is: \[ C_f = \frac{k_f w}{k L_f} \] where - \(k_f\) = fracture permeability, - \(w\) = fracture width, - \(k\) = reservoir permeability, - \(L_f\) = fracture half-length.
Step 2: Unit conversions.
Fracture width: \[ w = 0.12 \, in = \frac{0.12}{12} \, ft = 0.01 \, ft \]
Step 3: Substitute values.
\[ C_f = \frac{4000 \times 0.01}{80 \times 1000} \] \[ = \frac{40}{80000} = 0.0005 = 5.0 \times 10^{-4} \]
Step 4: Round off.
\[ C_f \approx 4.6 \times 10^{-4} \]
Final Answer: \[ \boxed{4.6 \times 10^{-4}} \]
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: