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24-Pet-B2 Oil and Gas Evaluation and Economics · May 2016

Question 6 of 7: Real-Gas Pseudopressure Drawdown

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams May 2016, 98-Pet-B2, Natural Gas Engineering — 3 hours, closed book (non-communicating calculator permitted), 7 questions of 20 marks each. NOTES item 5 states only the first five questions in the answer book are marked; all 7 are solved.

Reference texts: Katz et al., Handbook of Natural Gas Engineering; Lee & Wattenbarger, Gas Reservoir Engineering (SPE Textbook Series Vol. 5); Ahmed, Reservoir Engineering Handbook, 5th ed.; Mohitpour et al., Pipeline Design and Construction, 3rd ed. (ASME Press); McCain, The Properties of Petroleum Fluids, 3rd ed.

Question 6: Real-Gas Pseudopressure Drawdown (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Check: this question omits reservoir temperature entirely, and the required real-gas pseudopressure formula needs it.

Given.

QuantityValue
Flow rate, $q_{sc}$7,000 MSCFD (constant)
Initial pressure, $p_i$2,000 psia
Temperature, $T$580 °R (see the check note)
Thickness, $h$39 ft
Viscosity, $\mu$0.0158 cP
Porosity, $\phi$0.15
Permeability, $k$20 mD
Well radius, $r_w$0.4 ft
Compressibility, $c_t$0.00053 psi$^{-1}$
Time36 hr

Find. Flowing bottomhole pressure $p_{wf}$ after 36 hr.

Approach. Compute dimensionless time, check whether the semilog (Ei-function) approximation applies, get the dimensionless pressure, convert to a real-gas pseudopressure drop via the transient flow equation, then invert through the digitized $\psi(p)$-vs-$p$ chart to recover $p_{wf}$.

  1. Dimensionless time. Using the formula sheet's diffusivity grouping ($k$ in mD, $t$ in days): $$t_D=\frac{6.33\,k\,t}{\phi\mu c_t r_w^2}=\frac{6.33(20)(36/24)}{0.15(0.0158)(0.00053)(0.4)^2}$$ $$t_D=9.45\times10^5 \gg 100 \Rightarrow \text{semilog (log) approximation applies}$$
  2. Dimensionless pressure. $$p_D=\tfrac{1}{2}\left(\ln t_D+0.809\right)=\tfrac{1}{2}\left(\ln(9.45\times10^5)+0.809\right)$$ $$\boxed{p_D=7.284}$$
  3. Pseudopressure drop. $$\Delta\psi=\frac{1.422\,q_{sc}T}{kh}\,p_D=\frac{1.422(7000)(580)}{20(39)}(7.284)$$ $$\boxed{\Delta\psi=53{,}900\ \text{psia}^2/\text{cp}}$$
  4. Invert through the $\psi(p)$ chart. Reading $\psi_i$ at $p_i=2000$ psia off the digitized chart gives $\psi_i=3.400\times10^8$; subtracting the drawdown and reading back: $$\psi_{wf}=\psi_i-\Delta\psi=3.400\times10^8-5.39\times10^4=3.39946\times10^8$$ $$\boxed{p_{wf}\approx1999.8\ \text{psia}}$$ The pressure drop after only 36 hr is tiny (<1 psi) — consistent with this well's very high $\psi$-vs-$p$ sensitivity near $p_i$ (the chart's slope is steep there) combined with a moderate rate and only a day and a half of production.
0.005001,0001,5002,0002,50001e+082e+083e+084e+085e+08Pressure, p (psia)Pseudopressure, ψ (psia²/cp)ψi @ pi=2000ψwf @ 36 hr
Digitized $\psi(p)$-vs-$p$ chart used to convert the computed pseudopressure drop back to a flowing bottomhole pressure.
QuantityResult
$t_D$$9.45\times10^5$
$p_D$ (log approximation)7.284
Pseudopressure drop, $\Delta\psi$53,900 psia$^2$/cp
Flowing bottomhole pressure, $p_{wf}$1,999.8 psia