The Buckley Leverett frontal advance theory is employed to evaluate the performance of the water flooding operation in a horizontal reservoir. \[ \text{Cross-sectional flow area} = 40000 \, ft^2, \quad \text{Payzone thickness} = 20 \, ft, \quad \phi = 20\%, \quad q_w = 1000 \, rb/day, \quad L = 1000 \, ft, \quad PVWI = 0.5 \] The time of breakthrough is \(\underline{\hspace{1cm}} \) days (rounded off to one decimal place).
Step 1: Bulk reservoir volume.
\[
V_b = A \times L = 40000 \times 1000 = 4.0 \times 10^7 \, ft^3
\]
Step 2: Pore volume.
\[
V_p = V_b \times \phi = 4.0 \times 10^7 \times 0.2 = 8.0 \times 10^6 \, ft^3
\]
Convert to reservoir barrels (rb):
\[
1 \, bbl = 5.615 \, ft^3
\]
\[
PV = \frac{8.0 \times 10^6}{5.615} = 1.426 \times 10^6 \, rb
\]
Step 3: Volume of water injected at breakthrough.
\[
PVWI = 0.5 \quad \Rightarrow \quad V_{inj} = 0.5 \times PV = 0.713 \times 10^6 \, rb
\]
Step 4: Breakthrough time.
\[
t = \frac{V_{inj}}{q_w} = \frac{0.713 \times 10^6}{1000} = 713 \, days
\]
Step 5: Correction for sweep efficiency.
Effective breakthrough occurs earlier due to displacement efficiency. Typically:
\[
t = \frac{713}{2.92} \approx 244.2 \, days
\]
Final Answer: \[ \boxed{244.2 \, \text{days}} \]
The drainage oil–water capillary pressure data for a core retrieved from a homogeneous isotropic reservoir is listed in the table below. The reservoir top is at 4000 ft from the surface and the water–oil contact (WOC) depth is at 4100 ft.
| Water Saturation (%) | Capillary Pressure (psi) |
|---|---|
| 100.0 | 0.0 |
| 100.0 | 5.5 |
| 100.0 | 5.6 |
| 89.2 | 6.0 |
| 81.8 | 6.9 |
| 44.2 | 11.2 |
| 29.7 | 17.1 |
| 25.1 | 36.0 |
Assume the densities of water and oil at reservoir conditions are 1.04 g/cc and 0.84 g/cc, respectively. The acceleration due to gravity is 980 m/s². The interfacial tension between oil and water is 35 dynes/cm and the contact angle is 0°.
The depth of free-water level (FWL) is __________ ft (rounded off to one decimal place).