Integration of Reservoir Uncertainties
   into Flow Assurance Strategies


                 Dr Martin J Watson

            SPE Applied Technology Workshop
   Bridging the Gap Between Reservoir Engineering and
                     Facilities Design
          14th&15th February 2012, San Antonio
Facilities Thermal Design & the Reservoir

 Many uncertainties in the thermal hydraulic design of Facilities lie in
 the reservoir
    How much is going to flow
    At what temperature


 The traditional approach to Facilities design is to design to a FWHT
 and a “design rate”
    But such decisions are arbitrary
        Over conservative for some, under conservative for others
        E.g. What FWHT is conservative for both wax and corrosion management?


 Thermal Hydraulic IPM can help manage these risks more rigorously
    Rigorous thermal hydraulic model from reservoir to processing facilities
    Can investigate how the reservoir uncertainties effect Facilities Design
    Without the need for arbitrary intermediate boundary conditions


 What follows is an example in hydrate management
    But equally applicable to wax, corrosion, chemical injection, etc           2
Hydrate Management for a Deepwater Oil System




    Phi, Beta, Kappa fields
    7 production wells planned
    25mile daisy chained tieback in deep water   3
Deepwater Oil Hydrate Management & Cooldown Time


                    350
                                               Hydrate
                              Require a good cooldown
                                               Dissociation
                              time as a hold time before
                    300                        Curve
                              the expensive hydrate
                                    Hydrates                                                 No Hydrates
                              management operation
                    250       needs to be carried out
                              Typically >10hours is
  Pressure (bara)




                                                                                              Normal
                              required, making most                        Hot                Operation
                    200
                              shutdowns recoverable                        Restart
                              with a Hot Restart
                                                                                                   Shut in
                    150
                                                                            Cooldown

                    100
                                                              Blowdown
                                                              & Dead Oil Displacement
                    50


                     0
                          0         5       10      15        20     25       30        35        40         45   50
                                                               Temperature (°C)                                        4
Life of Field Cooldown Time

      The Cooldown Time of a production system changes through life
         As the watercut, GOR and relative rates from each well changes


      On the FEESA website is described a method for turning a life of field
      thermo hydraulic simulation and a transient simulation into an
      estimate for cooldown time throughout life
         http://www.feesa.net/consultancy/casestudies.html
         Based on Newton’s Law of Cooling

                                         Min Pipeline Temp at Steady State
                         Tmin SS − Tamb
                 t = Bln                              Ambient Temperature
                          Thyd − Tamb
Cooldown time                           Hydrate Avoidance Temperature

                              Fitting parameter

                                                                               5
Life of Field Cooldown Time
Oil Rate




                                              Phi
                              Beta
                Kappa

                                                                                    Year
                                                                                     Upside

                                                                           Most Likely Temps
Cooldown Time




                                                                                   Downside


                                                               Target Cooldown Time [18hrs]


                 What’s the chance that all wells are on their downside?              Year
                                                                                               6
                 What’s the probability that the cooldown time will be less than 18hours?
What is the probability the cooldown time is <18hours?

     Make some assumptions about the probabilities of the uncertainties
        I.e. Probability of upside, expected and downside, PI and Reservoir temp
        Probability density function
     Generate multiple combinations scenarios who’s probability we can
     calculate
        E.g. Kappa and Beta on expected, Phi on downside, etc
     We could simulate each combination to calculate cooldown time
     Generate a distribution of probability vs cooldown time

     However, there are too many possible scenarios
        Even if there we assumed there was only upside, expected and downside;
        for six uncertainties (PI & Tres for three reservoirs)
        36=729 combinations
        729 life of field simulations is impractical, even with the fastest thermal
        hydraulic simulator
        In reality there are many more
        We needed to choose the least number of runs to yield the most
        information about how these uncertainties affect cooldown time
                                                                                      7
Design of Experiment (DOE)
Design of Experiment (a.k.a. Experimental Design) is the process of
reducing the number of experiments whilst still ensuring statistically
meaningful results

Various Experimental Design methods in the literature
   Most famously the “Monte Carlo” method
   This requires too many simulations to be run (tens of thousands)
   We used the Taguchi method
       Developed to improve product design and manufacturing methods
       Procedural


In this case we used Taguchi to reduce the number of simulations to just
enough to develop a correlation for cooldown time versus our
uncertainties
   Which we can then use in a Monte Carlo Simulation


A reference
   Manivannan, S. et al, 2010, Taguchi Based Linear Regression Modelling of Flat
   Plate Heat Sink, J Eng & App Sci, Vol 5, Issue 1, 36-44                       8
Applying the Taguchi Method to this Problem
    Requires the user to do sensitivity studies
        Rate the uncertainties in order of most important to least
        Phi PI, Phi Tres, Kappa Tres, Beta Tres, Kappa PI, Beta PI
    The rest is procedural
    In this case, there are 6 variables, a L8 orthogonal array was used
        Selects 27 runs from the 729 possible
                          Phi          Kappa          Beta
              Phi PI   Temperature   Temperature   Temperature   Kappa PI   Beta PI
     Run 1      0          0             0             0            0         0
     Run 2      0          0             -1            -1           0         1
     Run 3      0          0             1             1            0         -1
     Run 4      0          -1            0             -1           1         -1      Keys
     Run 5      0          -1            -1            1            1         0         -1   Downside
     Run 6      0          -1            1             0            1         1         0    Most Likely
     Run 7      0          1             0             1            -1        1         1    Upside
     Run 8      0          1             -1            0            -1        -1
     Run 9      0          1             1             -1           -1        0
     Run 10    -1          0             0             -1           -1        -1
     Run 11    -1          0             -1            1            -1        0
     Run 12    -1          0             1             0            -1        1
     Run 13    -1          -1            0             1            0         1
     Run 14    -1          -1            -1            0            0         -1
     Run 15    -1          -1            1             -1           0         0
     Run 16    -1          1             0             0            1         0
     Run 17    -1          1             -1            -1           1         1
     Run 18    -1          1             1             1            1         -1
     Run 19     1          0             0             1            1         1
     Run 20     1          0             -1            0            1         -1
     Run 21     1          0             1             -1           1         0
     Run 22     1          -1            0             0            -1        0
     Run 23     1          -1            -1            -1           -1        1
     Run 24     1          -1            1             1            -1        -1
     Run 25     1          1             0             -1           0         -1
                                                                                                           9
     Run 26     1          1             -1            1            0         0
     Run 27     1          1             1             0            0         1
Method

 Each of the 27 Maximus runs gives us a CDTmin. We then use this data
 set to fit a correlation
                                             2      2
     CDTmin     C0    aXn    bXn 1 ...     eXn    fXn 1 ... R
    C0 = Constant                          The values of these are
                                           fitted by regression, e.g.,
    Italics a, b, c etc. = Coefficients    in Excel
    Xn = The outcome of variable n, taking the value of +1 or 0 or -1. Variable
    n refers to the set {Phi temperature, PI…etc.}
    Xn2 = Square of Xn hence can only be 1 or 0
    R = Residual term, assumed negligible



 The effect of these parameters on CDT can now be predicted without
 running a full simulation by entering +1, 0, -1 into the equation




                                                                              10
Comparison of Correlation vs Simulation
              40




              35




              30




              25
  CDT (hrs)




              20




              15




              10




              5
                                                                   CDT calculated from Maximus results
                                                                   CDT calculated using polynomial
              0
                   1   3   5   7   9   11   13      15   17   19     21         23          25           27

                                            Run number

The average difference was 2%
         This was deemed acceptable, given the assumptions about the uncertainties
         This correlation was then entered into Crystal Ball for the Mote Carlo Simulations                   11
Results




Conclusion; given the reservoir uncertainties, the P90 CDT is 18hrs
   90% chance that the CDT will be equal to or greater than 18 hrs throughout field life
   On Normal Operation
                                                                                           12
Other Uses - MEG Injection System Sizing

                                 Montini et al (2011)
                                 “A Probabilistic Approach to
                                 Prevent the Formation of
                                 Hydrates in Gas Production
                                 Systems”
                                 ICGH 2011 (Edinburgh)
                                 West Nile Delta Project
                                 Large offshore gas condensate
                                 network
                                   34 wells, ~380km of pipelines
                                 Traditional design approaches
                                 would lead to it being the
                                 world’s largest MEG injection
                                 system!
                                   All the worst case scenarios
                                   occurring at once
                                 The Operator sought an
                                 alternative approach!




                                                                   13
A Probabilistic Approach to MEG

    An alternative approach to the traditional worst of the worst of the
    worst……
    A life of field thermo-hydraulic compositional evaluation
       Proved that many of these worst cases can’t happen in the same year

    A statistical investigation
       Reduced the MEG design rates by a factor of four
       Still 99% confident that hydrates are avoided
       Why not 100%?
           It takes hours to form a hydrate blockage in such systems
           Remediation is possible

    Scope for future work
       A better quantification of the risk of forming blockages
       A better cost estimate of remediation
       A better justification for “99% certainty”

     But BP were happy
     Help make the project feasible
                                                                             14
     Moved into FEED
Conclusion

 Facilities Engineers have a lot to learn from Subsurface Engineers!
    Life of Field Approach
        Viewing issues on a life of field basis rather than “mass sensitivity studies”
        Easier to understand the problem, easier to explain to others
    Integrated Production Modelling
        Removing arbitrary and erroneous boundary conditions (e.g. FWHT)
        Investigating the impact of Reservoir Uncertainties
    A statistical approach to uncertainties
        Rather than assuming all worst cases happen at once
        Build a picture of what is statistically likely to happen
        “We believe this is good for 90% of all scenarios we expect, and have a plan for
        the other 10%, do you want to go ahead or not?”


 On real Flow Assurance projects, such methods have;
    Reduced the number of excessive design margins
    Have proved conventional (proven) insulation systems could work, where
    traditional design methods pointed to less proven low U value solutions
    Made MEG injection practical for a large gas network

                                                                                         15

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Integration of Reservoir Uncertainties into Flow Assurance Strategies

  • 1. Integration of Reservoir Uncertainties into Flow Assurance Strategies Dr Martin J Watson SPE Applied Technology Workshop Bridging the Gap Between Reservoir Engineering and Facilities Design 14th&15th February 2012, San Antonio
  • 2. Facilities Thermal Design & the Reservoir Many uncertainties in the thermal hydraulic design of Facilities lie in the reservoir How much is going to flow At what temperature The traditional approach to Facilities design is to design to a FWHT and a “design rate” But such decisions are arbitrary Over conservative for some, under conservative for others E.g. What FWHT is conservative for both wax and corrosion management? Thermal Hydraulic IPM can help manage these risks more rigorously Rigorous thermal hydraulic model from reservoir to processing facilities Can investigate how the reservoir uncertainties effect Facilities Design Without the need for arbitrary intermediate boundary conditions What follows is an example in hydrate management But equally applicable to wax, corrosion, chemical injection, etc 2
  • 3. Hydrate Management for a Deepwater Oil System Phi, Beta, Kappa fields 7 production wells planned 25mile daisy chained tieback in deep water 3
  • 4. Deepwater Oil Hydrate Management & Cooldown Time 350 Hydrate Require a good cooldown Dissociation time as a hold time before 300 Curve the expensive hydrate Hydrates No Hydrates management operation 250 needs to be carried out Typically >10hours is Pressure (bara) Normal required, making most Hot Operation 200 shutdowns recoverable Restart with a Hot Restart Shut in 150 Cooldown 100 Blowdown & Dead Oil Displacement 50 0 0 5 10 15 20 25 30 35 40 45 50 Temperature (°C) 4
  • 5. Life of Field Cooldown Time The Cooldown Time of a production system changes through life As the watercut, GOR and relative rates from each well changes On the FEESA website is described a method for turning a life of field thermo hydraulic simulation and a transient simulation into an estimate for cooldown time throughout life http://www.feesa.net/consultancy/casestudies.html Based on Newton’s Law of Cooling Min Pipeline Temp at Steady State Tmin SS − Tamb t = Bln Ambient Temperature Thyd − Tamb Cooldown time Hydrate Avoidance Temperature Fitting parameter 5
  • 6. Life of Field Cooldown Time Oil Rate Phi Beta Kappa Year Upside Most Likely Temps Cooldown Time Downside Target Cooldown Time [18hrs] What’s the chance that all wells are on their downside? Year 6 What’s the probability that the cooldown time will be less than 18hours?
  • 7. What is the probability the cooldown time is <18hours? Make some assumptions about the probabilities of the uncertainties I.e. Probability of upside, expected and downside, PI and Reservoir temp Probability density function Generate multiple combinations scenarios who’s probability we can calculate E.g. Kappa and Beta on expected, Phi on downside, etc We could simulate each combination to calculate cooldown time Generate a distribution of probability vs cooldown time However, there are too many possible scenarios Even if there we assumed there was only upside, expected and downside; for six uncertainties (PI & Tres for three reservoirs) 36=729 combinations 729 life of field simulations is impractical, even with the fastest thermal hydraulic simulator In reality there are many more We needed to choose the least number of runs to yield the most information about how these uncertainties affect cooldown time 7
  • 8. Design of Experiment (DOE) Design of Experiment (a.k.a. Experimental Design) is the process of reducing the number of experiments whilst still ensuring statistically meaningful results Various Experimental Design methods in the literature Most famously the “Monte Carlo” method This requires too many simulations to be run (tens of thousands) We used the Taguchi method Developed to improve product design and manufacturing methods Procedural In this case we used Taguchi to reduce the number of simulations to just enough to develop a correlation for cooldown time versus our uncertainties Which we can then use in a Monte Carlo Simulation A reference Manivannan, S. et al, 2010, Taguchi Based Linear Regression Modelling of Flat Plate Heat Sink, J Eng & App Sci, Vol 5, Issue 1, 36-44 8
  • 9. Applying the Taguchi Method to this Problem Requires the user to do sensitivity studies Rate the uncertainties in order of most important to least Phi PI, Phi Tres, Kappa Tres, Beta Tres, Kappa PI, Beta PI The rest is procedural In this case, there are 6 variables, a L8 orthogonal array was used Selects 27 runs from the 729 possible Phi Kappa Beta Phi PI Temperature Temperature Temperature Kappa PI Beta PI Run 1 0 0 0 0 0 0 Run 2 0 0 -1 -1 0 1 Run 3 0 0 1 1 0 -1 Run 4 0 -1 0 -1 1 -1 Keys Run 5 0 -1 -1 1 1 0 -1 Downside Run 6 0 -1 1 0 1 1 0 Most Likely Run 7 0 1 0 1 -1 1 1 Upside Run 8 0 1 -1 0 -1 -1 Run 9 0 1 1 -1 -1 0 Run 10 -1 0 0 -1 -1 -1 Run 11 -1 0 -1 1 -1 0 Run 12 -1 0 1 0 -1 1 Run 13 -1 -1 0 1 0 1 Run 14 -1 -1 -1 0 0 -1 Run 15 -1 -1 1 -1 0 0 Run 16 -1 1 0 0 1 0 Run 17 -1 1 -1 -1 1 1 Run 18 -1 1 1 1 1 -1 Run 19 1 0 0 1 1 1 Run 20 1 0 -1 0 1 -1 Run 21 1 0 1 -1 1 0 Run 22 1 -1 0 0 -1 0 Run 23 1 -1 -1 -1 -1 1 Run 24 1 -1 1 1 -1 -1 Run 25 1 1 0 -1 0 -1 9 Run 26 1 1 -1 1 0 0 Run 27 1 1 1 0 0 1
  • 10. Method Each of the 27 Maximus runs gives us a CDTmin. We then use this data set to fit a correlation 2 2 CDTmin C0 aXn bXn 1 ... eXn fXn 1 ... R C0 = Constant The values of these are fitted by regression, e.g., Italics a, b, c etc. = Coefficients in Excel Xn = The outcome of variable n, taking the value of +1 or 0 or -1. Variable n refers to the set {Phi temperature, PI…etc.} Xn2 = Square of Xn hence can only be 1 or 0 R = Residual term, assumed negligible The effect of these parameters on CDT can now be predicted without running a full simulation by entering +1, 0, -1 into the equation 10
  • 11. Comparison of Correlation vs Simulation 40 35 30 25 CDT (hrs) 20 15 10 5 CDT calculated from Maximus results CDT calculated using polynomial 0 1 3 5 7 9 11 13 15 17 19 21 23 25 27 Run number The average difference was 2% This was deemed acceptable, given the assumptions about the uncertainties This correlation was then entered into Crystal Ball for the Mote Carlo Simulations 11
  • 12. Results Conclusion; given the reservoir uncertainties, the P90 CDT is 18hrs 90% chance that the CDT will be equal to or greater than 18 hrs throughout field life On Normal Operation 12
  • 13. Other Uses - MEG Injection System Sizing Montini et al (2011) “A Probabilistic Approach to Prevent the Formation of Hydrates in Gas Production Systems” ICGH 2011 (Edinburgh) West Nile Delta Project Large offshore gas condensate network 34 wells, ~380km of pipelines Traditional design approaches would lead to it being the world’s largest MEG injection system! All the worst case scenarios occurring at once The Operator sought an alternative approach! 13
  • 14. A Probabilistic Approach to MEG An alternative approach to the traditional worst of the worst of the worst…… A life of field thermo-hydraulic compositional evaluation Proved that many of these worst cases can’t happen in the same year A statistical investigation Reduced the MEG design rates by a factor of four Still 99% confident that hydrates are avoided Why not 100%? It takes hours to form a hydrate blockage in such systems Remediation is possible Scope for future work A better quantification of the risk of forming blockages A better cost estimate of remediation A better justification for “99% certainty” But BP were happy Help make the project feasible 14 Moved into FEED
  • 15. Conclusion Facilities Engineers have a lot to learn from Subsurface Engineers! Life of Field Approach Viewing issues on a life of field basis rather than “mass sensitivity studies” Easier to understand the problem, easier to explain to others Integrated Production Modelling Removing arbitrary and erroneous boundary conditions (e.g. FWHT) Investigating the impact of Reservoir Uncertainties A statistical approach to uncertainties Rather than assuming all worst cases happen at once Build a picture of what is statistically likely to happen “We believe this is good for 90% of all scenarios we expect, and have a plan for the other 10%, do you want to go ahead or not?” On real Flow Assurance projects, such methods have; Reduced the number of excessive design margins Have proved conventional (proven) insulation systems could work, where traditional design methods pointed to less proven low U value solutions Made MEG injection practical for a large gas network 15