By Tarek Ahmed PhD PE, Nathan Meehan
, Pages i,iii
, Page iv
, Page ix
Chapter 1 - good checking out Analysis
, Pages 1-226
Chapter 2 - Water Influx
, Pages 227-279
Chapter three - Unconventional fuel Reservoirs
, Pages 281-432
Chapter four - functionality of Oil Reservoirs
, Pages 433-483
Chapter five - Predicting Oil Reservoir Performance
, Pages 485-539
Chapter 6 - advent to more desirable Oil Recovery
, Pages 541-585
Chapter 7 - financial Analysis
, Pages 587-649
Chapter eight - monetary Analysis
, Pages 651-660
Chapter nine - Professionalism and Ethics
, Pages 661-682
, Pages 683-688
, Pages 689-702
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Additional resources for Advanced Reservoir Management and Engineering
Results of step 4 indicate that Darcy’s equation satisfies Eq. 76) and is indeed the solution to Laplace’s equation. To obtain a solution to the diffusivity equation (Eq. 75), it is necessary to specify an initial condition and impose two boundary conditions. The initial condition simply states that the reservoir is at a uniform pressure pi when production begins. , re 5 N. Based on the boundary conditions imposed on Eq. 75), there are two generalized solutions to the diffusivity equation. These are: (1) the constant-terminal-pressure solution; (2) the constant-terminal-rate solution.
During the infinite-acting behavior, is summarized in the following steps: Step 1. Calculate the dimensionless time tD by applying Eq. 86a): tD 5 0:0002637kt φμct rw2 Step 2. Determine the dimensionless radius reD. Note that for an infinite-acting reservoir, the dimensionless radius reD 5 N. CHAPTER 1 38 Well Testing Analysis Step 3. , Eq. 95): • For an infinite-acting reservoir: pD 5 0:5½lnðtD Þ 1 0:80907 • For a finite-acting reservoir: Step 4. Solve for the pressure by applying Eq. 12 A well is producing at a constant flow rate of 300 STB/day under unsteady-state flow conditions.
Thus, the authors’ wellbore radius rw was in this case the external radius of the reservoir and re was essentially the external boundary radius of the aquifer. 3 are practical for this application. Consider the Ei function solution to the diffusivity equations as given by Eq. 77): ! 70:6QBμ 2 948φμct r 2 pðr; tÞ 5 pi 1 Ei kt kh CHAPTER 1 36 TA B L E 1. 3 pD vs. 614 Notes: For tD smaller than values listed in this table for a given reD reservoir is infinite acting. 2. , 1982. Well Testing, SPE Textbook Series, Permission to Publish by the SPE, Copyright SPE, 1982.