+ All Categories
Home > Documents > PERFORATING DYNAMICS AND MODELING · Carlos Vega, University of Utah John McLennan, University of...

PERFORATING DYNAMICS AND MODELING · Carlos Vega, University of Utah John McLennan, University of...

Date post: 22-Oct-2020
Category:
Upload: others
View: 2 times
Download: 0 times
Share this document with a friend
21
PERFORATING DYNAMICS AND MODELING Numerical simulation for near borehole fluid dynamics at perforation tunnel 2019-NAPS-XX AUTHORS: Carlos Vega, University of Utah John McLennan, University of Utah Ian Walton, Energy and Geoscience Institute DALLAS - FORT WORTH. AUGUST 5-6, 2019.
Transcript
  • PERFORATING DYNAMICS AND MODELING

    Numerical simulation for near borehole fluid dynamics

    at perforation tunnel

    2019-NAPS-XXAUTHORS: Carlos Vega, University of UtahJohn McLennan, University of UtahIan Walton, Energy and Geoscience Institute

    DALLAS - FORT WORTH. AUGUST 5-6, 2019.

  • OBJECTIVE

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    The proposed numerical simulation is a mathematical solution and visualization tool that can be implemented for the analysis of real case scenarios of fluid dynamics in perforations

  • AGENDA

    Outline

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Wellbore perforations Formation and perforation simulator Mass Balance Equation Numerical Method Description Fluid mechanics at perforation tunnel Results Conclusions

  • 1. WELLBORE PERFORATIONSTunnel Description

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    • Hydraulic communication between borehole and formation

    • Industry standards as per API 19B

    Schematics of the perforating geometry:

    1. Perforating Charge2. Perforating Gun3. Perforation jet4. Casing5. Cement6. Reservoir rock 7. Perforation tunnel length 8. Entrance Hole Diameter 9. Crushed zone 10. Crushed Zone Thickness

    (Grove, et al. 2012)

  • 2. FORMATION SIMULATION

    Petrophysical properties of the rock

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Each cell with unique properties simulating rock texture:

    PorosityPermeability

    Grid block size: 70x70 cellsGrid block dimensions: 16 x 16 in

    Assumptions:

    - All processes are isothermal

    - Fluids are incompressible and non-reactive.

    - No gravity effects on fluid segregation

    - Perforation tunnel is considered as high permeability packed bed with spherical particles.

    - Crushed zone permeability and porosity are reduced by a fraction of original values.

    - Grid block and dimensions kept at low figures for low computational load.

    - Convergence analysis to be done

  • 3. PERFORATION SIMULATION

    Petrophysical properties in the perforation tunnel

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Perforation properties:Gun type: 2” HSD, 6 spfPenetration: 11.5 inEntrance Hole: 0.25 inCrushed Zone Thickness: 0.5 inCrushed zone ratios:

    K: 0.3f: 0.3Sw: 0.3

  • 4. Material Balance Equations

    At every grid cell (control volume)

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Mass Balance:

    𝑚𝑖𝑛 − 𝑚𝑜𝑢𝑡 + 𝑚𝑠𝑖𝑛𝑘/𝑠𝑜𝑢𝑟𝑐𝑒 = 𝑚𝑎𝑐𝑐

    −𝜕

    𝜕𝑖𝜌𝑢𝑖𝐴𝑖 𝛥𝑖 +

    𝑞𝑚𝑎𝑐

    =𝑉𝑏𝑎𝑐

    𝜕

    𝜕𝑡𝜙𝜌

    Differential equation form:

    i= cartesian coordinates x, y, z.

  • 4. Material Balance Equations

    At every grid cell (control volume)

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    𝑎𝑐 =𝑉𝑏ϕ𝑜𝐶𝑓

    α𝑐 Δ𝑡

    −𝜕

    𝜕𝑥𝜌𝑢𝑥𝐴𝑥 𝛥𝑥 −

    𝜕

    𝜕𝑦𝜌𝑢𝑦𝐴𝑦 𝛥𝑦 −

    𝜕

    𝜕𝑧𝜌𝑢𝑧𝐴𝑧 𝛥𝑧 +

    𝑞𝑚𝑎𝑐

    =𝑉𝑏𝑎𝑐

    𝜕

    𝜕𝑡𝜙𝜌

    𝑢𝑥 = −𝛽𝑐𝑘𝑥𝜇

    𝜕𝑃

    𝜕𝑥

    𝜕

    𝜕𝑥𝛽𝑐𝐾𝑥𝐴𝑥

    𝐾𝑟𝑜𝜇𝑜𝐵𝑜

    𝜕𝑃𝑜𝜕𝑥

    ∆𝑥 +𝜕

    𝜕𝑦𝛽𝑐𝐾𝑦𝐴𝑦

    𝐾𝑟𝑜𝜇𝑜𝐵𝑜

    𝜕𝑃𝑜𝜕𝑦

    ∆𝑦=𝑉𝑏𝑎𝑐

    𝜕

    𝜕𝑡

    𝜙 𝑆𝑜𝐵𝑜

    − 𝑞𝑜𝑠𝑐

    From material balance equation:

    From Darcy equation:

    Reservoir Engineering form of mass balance equation:

    PermeabilityRelative PermeabilityPorosity

    PressureControl volume dimensionsTime Steps Dt

    Sink/Source FlowForm Vol FactorFluid Viscosity

    Variables:

  • 5. Fluid mechanics at perforation tunnel

    Equations developed for mass transfer in porous media

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    ∆𝑷 =𝟏𝟓𝟎𝝁𝑳

    𝑫𝒑𝟐

    𝟏 − 𝝓 𝟐

    𝝓𝟑𝒗𝒔 +

    𝟏. 𝟕𝟓𝑳𝝆

    𝑫𝒑

    𝟏 − 𝝓

    𝝓𝟑𝒗𝒔 𝒗𝒔

    Based on Ergun equation (Ergun 1952)

    Application of pipe packed with spherical beads (Jamiolahmady, et al. 2006).

    The first term is the Carman-Kozeny equation: Laminar fluids.

    The second term: Correction for intermediate to turbulent flow regime

  • 6. Results

    Scenarios created for demonstration of Simulator Capabilities

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Scenario 1Homogeneous grid

    Scenario 2Horizontal Lamination

    Scenario 3Damaged vs Improved

    Injection Scheme

    Driving Force: Constant Injection Flow Rate: 7 BPMElapsed time: 100 s

  • 6. Results

    Constant Injection Rate in Homogeneous Formation

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    t = 10 st = 20 st = 40 st = 60 st = 80 st = 100 s

    Perforation and Crushed Zone 2D Pressure Distribution

    Elapsed time

  • 6. Results

    Constant Injection Rate in Homogeneous Formation

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Pressure Profile at tunnel

    Pressure Profile at Crushed ZonePressure Profile at vertical section

    Gridblock simulation

  • 6. Results

    Constant Injection Rate in Low Permeability Laminated Formation

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    t = 10 st = 20 st = 40 st = 60 st = 80 st = 100 s

    Perforation and Crushed Zone 2D Pressure Distribution

    Elapsed time

  • 6. Results

    High Damage vs Low Damage Crushed Zone

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    High-Damage Crushed ZonePermeability K = 0.3 KoPorosity f = 0.3 fo

    Low Damage Crushed ZonePermeability K = 0.8 KoPorosity f = 0.8 fo

  • 6. Results

    Dynamic Underbalance Perforation

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Technique to create a temporary pressure drawdown in the gun casing and create a surge in the perforation tunnelIntended to clean out the debris inside the tunnel and reduce the damage in the crushed zone

    Simulated Pressure Profile Driving Force: Dynamic UnderbalanceElapsed time: 1 sec

  • 6. Results

    Dynamic Underbalance Perforation

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    t = 0 st = 0.1 st = 0.2 st = 0.4 st = 0.6 st = 0.8 st = 1.0 s

    Elapsed time DUB Pressure Profile 2D Pressure Distribution

    Velocity Vector Field

  • 6. Results

    Two Perforations through a Conductive Fracture

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    t = 0 st = 50 st = 100 st = 200 st = 300 st = 400 st = 500 s

  • 6. Results

    Two Perforations through a Conductive Fracture

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Pressure Mapping @ = 500 s

  • 7. Convergence Analysis

    Matrix size and computing time

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    Calculated Pressure at Tip of Tunnel

    50 x 50 grid

    Calculated Pressure at Tip of Tunnel

    35 x 35 grid

    Matrix size: 35x35

    Matrix size: 50x50

  • 7. Conclusions

    2019-NAPS-XX Numerical simulation for near borehole fluid dynamics at perforation tunnel

    The proposed fluid mechanics perforation simulator in the near borehole region is a powerful tool to visualize and evaluate the pressure transient at the perforation tunnel, crushed zone and nearby region.

    The simulator is flexible enough to process a wide range of variables. Pressure transient or pumping schedule Perforation parameters Rock texture and Reservoir fluid characteristics

    Initial development of the mathematical solution is a single plane, and it is not a realistic representative of the entire model.

    Simulation results must be compared to experimental data for validation.

  • 2019-NAPS-XXCarlos Vega, University of UtahJohn McLennan, University of UtahIan Walton, Energy and Geoscience Institute

    DALLAS - FORT WORTH. AUGUST 5-6, 2019. QUESTIONS? THANK YOU


Recommended