24-Pet-A3 Fundamental Reservoir Engineering · May 2018
Question 5 of 7: Drive-Mechanism Indices for a Combination-Drive Oil Reservoir
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
17-Pet-A3 — Fundamental Reservoir Engineering · National Exams, May 2018 · 3 hours, closed book, approved Casio/Sharp calculator only · five (5) questions constitute a complete exam paper (the first five as they appear in the answer book are marked), all questions equal value, all parts of a multipart question equal weight.
Reference texts: Craft, B.C. & Hawkins, M.F., Applied Petroleum Reservoir Engineering, 3rd ed. (material balance, well testing, relative permeability, Darcy flow); Ahmed, T., Reservoir Engineering Handbook, 5th ed. (material balance, transient well testing, gas PVT, decline-curve analysis); Lyons, W.C. (ed.), Standard Handbook of Petroleum and Natural Gas Engineering, 3rd ed.; McCain, W.D., The Properties of Petroleum Fluids, 3rd ed. (PVT properties, Z-factor correlations).
Question 5: Drive-Mechanism Indices for a Combination-Drive Oil Reservoir (20 marks)
Given. $N=67$ MMSTB (initial oil in place); gas cap $G_{fgi}=38$ MMMSCF at discovery; $c_f=c_w=0$; no water production ($W_p=0$); PVT/production table above (4100 psia = initial condition, 3950 psia = current condition).
Find. Depletion drive index (DDI), gas-cap drive index (SDI/GCDI), and water drive index (WDI) at 3950 psia.
Approach. Compute the two-phase FVF $B_t$ at both conditions, the gas-cap size ratio $m$, and the total underground withdrawal $F$; get DDI and SDI directly from their standard material-balance terms, then use the fact that the three indices must sum to 1 (and $c_f=c_w=0$ removes the rock/water-expansion term entirely) to obtain WDI by difference, since no water-influx volume $W_e$ is given directly.
Two-phase FVF, $B_t$. At $p_i=4100$ psia (bubble point/initial, $R_{so}=R_{soi}$): $B_{ti}=B_{oi}=1.41$ bbl/STB. At $p=3950$: $B_t=B_o+B_g(R_{soi}-R_{so})=1.34+0.000602(950-800)$, so $\boxed{B_t=1.4303\ \text{bbl/STB}}$.
Underground withdrawal, $F$. Cumulative GOR $R_p=G_p/N_p=1140/1.314=867.6$ SCF/STB. $F=N_p\left[B_t+B_g(R_p-R_{soi})\right]=1.314\times10^{6}\left[1.4303+0.000602(867.6-950)\right]$, so $\boxed{F=1.814\times10^{6}\ \text{bbl}}$.
Depletion drive index. $\text{DDI}=\dfrac{N(B_t-B_{ti})}{F}=\dfrac{67\times10^{6}(1.4303-1.41)}{1.814\times10^{6}}$, so $\boxed{\text{DDI}=0.750\ (75.0\%)}$.
Gas-cap drive index. $\text{SDI}=\dfrac{Nm\frac{B_{ti}}{B_{gi}}(B_g-B_{gi})}{F}=\dfrac{67\times10^{6}(0.2377)\frac{1.41}{0.000591}(0.000602-0.000591)}{1.814\times10^{6}}$, so $\boxed{\text{SDI}=0.230\ (23.0\%)}$.
Water drive index, by difference. With $c_f=c_w=0$, the rock-and-water expansion term vanishes and, since no $W_e$ (water influx volume) is given, the three drive indices are found to sum to 1: $\text{WDI}=1-\text{DDI}-\text{SDI}=1-0.750-0.230$, so $\boxed{\text{WDI}=0.020\ (2.0\%)}$.
Check: WDI is obtained as the residual $1-\text{DDI}-\text{SDI}$ rather than from a separately computed water-influx volume $W_e$, because $W_e$ is not among the data given for this reservoir; by definition the three drive indices always sum to unity, so this is the standard approach when $W_e$ cannot be evaluated directly.