Reservoir Performance

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    Semester January 2015, Credit hour 3Duration 14 weeks Lecture + 2 Weeks Study & Exam

    Lecture 30 hours + Lab/Tutorial 24 hours

    InstructorDr. Mohammed MahbuburRahman

    1. Beggs H.(2003), Production Optimization Using NODAL Analysis, Second Edition, OGCI2. Economides M. et al. (1994), Petroleum Production Systems, Prentice-Hall Inc.3. Michael Golan and Curtis H. Whitson (1991), Well Performance, 2nd Edition, Prentice-Hall

    Course Content Reservoir Performance

     Well Performance Equations, Darcy’s Law  Factors affecting productivity index IPR for oil and gas wells Back pressure equations  Well Completion effects

    Flow in Pipes and Restrictions Energy equation, single and multi-phase flows Fluid Property calculations  Well flow correlations:

    Hagedorn and Brown Poettmann and Carpenter Duns and Ros Orkiszewski  Aziz, Govier and Fogarasi

    Pipe flow correlations Pressure drop through restrictions

    Total System Analysis Tubing and Flow line size selection System analysis for wells with restrictions Evaluating Completion effects Nodal analysis of injection wells Effect of depletion Relating performance to time  Analyzing multiwell systems

     Artificial Lift Design Continuous Flow Gas lift Electrical Submersible Pump (ESP) selection Sucker rod / beam pumping Hydraulic pumping

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    Course Learning Outcome

     At the end of the course, students should be able to:

    1.  Apply fundamentals of production optimization usingcommercial software.

    2.  Analyze the performance of the petroleum productionsystem.

    3. Understand the interaction of the reservoir system and

    its effect on the overall production system.4. Design optimum petroleum production systems.

    • Major segments of theproduction system

    • Reservoir (InflowPerformance Relationship)

    •  Wellbore (Completions,Tubing etc)

    • Surface Facilities (Flowlines, Separator, Pipelines

    etc)

    •  Any one of these canadversely affect our target – to’maximize oil rate’

    Let us look at the simplified production system

    The 1st component is the Reservoir. So lets begin with the Reservoir >>>

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    Lecture Outline

    Reservoir Performance

    Reservoir flow equations

    Darcy equation for different fluid types and f low patterns

    Reservoir – well system performance

    Productivity Index

    The Reservoir Most important component in the production system Relationship between flowrate and pressure drop in the reservoir can be very

    complex Flow is through “porous medium”, so its formulation is very different from

    other fluid f low problem, such as flow through pipes, channels, etc. Therefore, flow in the reservoir is handled differently than flow in the wellbore Parameters involved:

    Rock properties (k, φ, ct, etc.) Fluid properties (PVT, µ, etc) Flow regime (Transient, Stabilized, etc) Fluid saturation (Sw, So, Sg) Formation damage/improvement (+s, -s) Drive mechanism (WDI, DDI, etc)

    So lets begin with the flow in the Reservoir >>> We will learn about flow in the wellbore later in the course.

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    Fluid Flow though Porous Medium (Reservoir Flow) Depending on time dependency, flow in the reservoir can be

    Transient flow(pressure, f low rate etc., varying with time) Stabilized Flow (pressure, f low rate etc., NOT varying with time, or

     varying at a fixed rate) Pseudo-Steady State (varying at a fixed rate)- requires NO-FLOW boundary Steady State (not varying) – requires CONSTANT PRESSURE boundary, such as

    large aquifer support Both type of flows are also called “Boundary Dominated” f low 

    Transient flow is more relevant for Pressure Transient Analysis (WellTesting)

    Stabilized flow is more relevant for Production Engineering

    Therefore, we proceed with the Stabilized flow in the Reservoir >>>

    Stabilized flow in the Reservoir:Linear Flow: Liquids

    Basic equation to describe stabilizedflow in reservoir is the DarcyEquation.

    Can be written in different forms suchas differential form, Integral form

    Can be modified for different flowpattern (linear, radial, spherical, etc.)

    Can be modified for different f luids(incompressible, slightlycompressible, compressible)

    In the simplest form:

      = =

    q = flow rate

     v = fluid velocity 

     A = area open to flow

    µ = viscosity of the f luid

    dp/dx = pressure gradient

    It is the “differential” form of Darcy equationThere is NO variable to represent TIME- (Steady State) Valid only for LAMINAR flow Valid for incompressible/slightly compressible fluids (water, oil etc)NOT valid for GAS, or for TURBULENT flow

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    Stabilized flow in the Reservoir:Linear Flow: Gas

    For compressible fluid (gas), theequation can take the form:

    Due to the nature of pressuredependency of gas, the pressure termsin the equation are usually expressedin 3 different forms:  Average pressure Pressure quared

    Pseudo-pressure This is the «pressure squared» form Notice the new terms: z, T

    P = pressure, psia T = Temperature, oR  µ = viscosity, cp L = length, ft K = permeability, md  A = area open to flow, ft2

    qsc = flow rate, SCF/D

    Stabilized flow in the Reservoir:Radial Flow: Oil

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    Stabilized flow in the Reservoir:Radial Flow: Oil

    Fluid converging radially into the well Area open to flow is not constsnt

     Area is given by: A = 2πrh

    Darcy equation for radial flow, slightly compressiblefluid (oil):

       =

      0.00708 ℎ (−)

     ln( )

    qo =

    Stabilized flow in the Reservoir:Radial Flow: Gas For compressible fluid (gas), and steady state flow, the equation can take the form:

      2

    2 =   ln(

    )

     ℎ

    It is the «pressure squared form»

    Let psc = 14.7 psia & Tsc = 520 oR, and pseudo-steady state flow

     

     =703 106 ℎ (

    − )

    ln(0.472 

    )

    notice in addition to the conversion factor, the multiplier 0.472 in the ln argument for Gas, flow rate qsc is always reported/calculated/expressed in terms of standard

    condition

      , are evaluated at average pressure, i.e., at T and p = ½(     + )

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    Stabilized flow in the Reservoir:Radial Flow: Pressure Profile

    The behavior of the pressure in the reservoir as a function of radius canbe analyzed by plotting pressure vs radius.

     Assuming a fixed average reservoir pressure, pR at r = 0.472 re andsolving for pressure:

    Stabilized flow in the Reservoir:Radial Flow: Pressure Profile

    Figure shows that large increase inpressure gradient near the wellboreas the fluid velocity increases

     Approx. one half of the pressuredrawdown occurs within 15ft radiusfrom the well.

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    Stabilized flow in the Reservoir:Radial Flow: Pressure Profile

    From the previous equation, a plot of p- vs- ln(r)  will result in a straight lineof constant slope m, where

    Notice the change of ’m’ withchange in ’q’Larger ’q’ results in steeper slope,assuming other variables remain thesame

    Flow in the Reservoir: Recap

    So far we concentrated on stabilized flow only 

    Become familiar with the equations for:

    Steady state & pseudo-steady state flow

    Linear & radial flow patterns

    Liquids and gas

    Pressure profile in the reservoir as a function of radial distance from the wellbore

    But, how good is the reservoir? How much can be extracted from it with a given well? Where is the reservoir energy being spent??

    To answer these questions, we need to learn about the performance indicator ofthe reservoir & well system>>>

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    Productivity Index

    Strong indicator of performance of the reservoir-well system

    Defined by:

    Higher values of J indicate good performance, where more oil is produced perunit draw down

     Alternate definition:

    Notice the impact of each variable.

     Which one would you/can you change to increase J? What factors affect J?

    Productivity Index...

    Solving for p wf  in terms of qo reveals thata plot of p wf  vs qo on a Cartesiancoordinates results in a straight linehaving a slope of -1/J and an intercept ofpR at qo= 0.

     J can be obtained from production test orcalculated from equation

    This line is known as the InflowPerformance Relation (IPR) line

    Later we will see IPR curves, not straightlines

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    Sample exercise

    Calculate:

    The Productivity Index, J

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    Lecture Summary 

    The reservoir is the 1st and foremost component in the production system

    Fluid flow in the reservoir is described by Darcy equation, which applies forlaminar f low, and stabilized (steady and pseudo-steady) conditions

    Darcy equation is expressed for linear and radial flow

    It can be modified for compressible fluids such as gas

    Productivity Index is the most important indicator for reservoir-wellperformance

    From PI, we can derive the IPR 

    For production operations, and production optimization, obtaining the IPR,and studying the behavior of IPR, comprise the main part from the reservoirside.