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Numerical Study of Bottom Water Draw-Off of Stratified Oil-Water Pipe Flow

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Title: Numerical Study of Bottom Water Draw-Off of Stratified Oil-Water Pipe Flow


1
Numerical Study of Bottom Water Draw-Off of
Stratified Oil-Water Pipe Flow
Yousef Zurigat Bssam Jubran Lyes Khezzar Salam
Al-Far
  • Department of Mechanical and Industrial
    Engineering
  • College of Engineering
  • Sultan Qaboos University, Oman

2
Plan
  • Introduction Objectives
  • Oil-water Transport dehydration issues
  • Simulation Model
  • Results
  • Conclusions

3
Water issues in Oil-Production
  • Well life extension results in increased water
    Production (98)
  • Need to separate water from oil (dehydration
    facilities cost money)
  • Pre-separation may take place in transport
    pipelines
  • Can we take advantage of it?

4
Concept of Bottom Water Draw Off
  • Depending upon prevailing conditions a water
    layer may form at the bottom of the pipe.
  • It can then be selectively removed.

5
Design Challenge of BWDO Concept
  • What is the maximum water flow rate that can be
    drawn off (With Acceptable quality)?
  • How can disturbance of the water/oil-in-water-disp
    ersion interface be avoided?
  • If several draw-off points are used, how will the
    interface and flow regimes in between draw points
    be affected?

6
Objectives
  • For a single draw-off pipe, investigate the
    variation of oil concentration in the draw-off
    pipe as a function of draw-off flow rate and
    interface position.(Interface location not known
    a priori!!)
  • Investigate the maximum possible water flow
    rates with acceptable quality (oil concentration)
    for two consecutive draw-off pipes.

7
Flow Regimes of Oil-Water Mixtures
  • Depending upon the oil superficial velocity
    several regimes are possible for horizontal water
    dominated flows

8
Geometry and Flow Parameters
  • Main pipe Diameter 0.68 m
  • Draw-Off Pipe Diameter 0.240 m
  • Oil-flow rate 8049 m3/day
  • Water flow rate 43614 m3/day
  • Interface Location 25 cm from bottom of main
    pipe.
  • Simulation conducted with one and two draw-off
    pipes

9
Modelling challenges
  • Flow is complex and two-phase (dispersions
    present)
  • Two Approaches
  • 1. Single-Phase Flow Modeling If negligible
  • slip between the phases and hold-up take
  • place--?In the present regime!! (water-
  • cut85, water superficial velocity1.3
  • m/s)!
  • 2. Two-Fluid Flow Modeling Actual Flow

10
Mathematical Model
  • SINGLE-PHASE FLOW MODEL
  • Steady, Single-phase, incompressible and
    turbulent flow.
  • Pressure drop approaches that of single phase
    flow
  • Flow dynamics very similar to single phase flow
  • Full three-D simulation

11
Quantitative analysis of draw-off water
quality-Single Phase Flow Model
  • Initial oil concentrations in the pipe regions
    above and below the interface are based on
    experimental data. The concentration of oil in
    free water assumed equal to 600 ppm in accordance
    with field data.
  • The amounts of oil in the areas above- and
    below-the-interface streams which make up the
    draw-off flow are calculated based on the flow
    rates and the concentrations calculated in the
    first step above.

12
Cut-off flow rates with water quality lt2000 ppm
from two tappings
13
Two-Fluid Modeling
  • In the PHOENICS, the concept of thermo- dynamic
    phase is used, i.e., the water and oil are
    treated as two different phases in the mixture.
    These two phases are in motion relative to each
    other due to the buoyancy effect, which leads to
    inter-phase momentum transfer.
  • The Inter-Phase Slip Algorithm (IPSA) is adopted
    to predict the phenomenon in this work.

14
Phase equations
  • Each phase is regarded as having its own distinct
    velocity components.
  • Phase velocities are linked by interphase
    momentum transfer - droplet drag, film surface
    friction etc.
  • Each phase may have its own temperature,
    enthalpy, and mass fraction of chemical species.
  • Phase concentrations are linked by interphase
    mass transfer.

15
Phase equations (Cont.)
t time Ri volume fraction of phase i ri density
of phase i fi any conserved property of phase i
velocity vector of phase i Gf,i exchange
coefficient of the entity f in phase
i Sf,i source rate of fi
16
Results
17
Results (Cont.)
18
Results (Cont.)
19
Results (Cont.)

20
Results (Cont.)

21
Results (Cont.)
22
Results (Cont.)

23
Results (Cont.)

24
AcknowledgementsPDOs FUNDING OF THIS WORK IS
GRATEFULLY ACKNOWLEDGED
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