• Nie Znaleziono Wyników

The Egg model

N/A
N/A
Protected

Academic year: 2021

Share "The Egg model"

Copied!
8
0
0

Pełen tekst

(1)

Research note

The Egg Model

Jan Dirk Jansen†, Rahul Mark Fonseca†, Siavash Kahrobaei†, Mohsin Siraj§, Gijs van Essen†, Paul Van den Hof§

Department of Geoscience and Engineering, TU Delft §

Department of Control Systems, TU Eindhoven Version 1d, November 2013

(2)

The Egg Model, v.1d, November 2013 2/8

Title: The Egg Model

Version 1d

Authors: Jan Dirk Jansen†, Rahul Mark Fonseca†, Siavash Kahrobaei†, Mohsin Siraj§, Gijs van Essen† and Paul Van den Hof§

Date: November 2013

Type of report: Research note

Organizations: † Delft University of Technology

Department of Geoscience and Engineering P.O. Box 5048

2600 GA Delft The Netherlands

§

Eindhoven University of Technology Department of Control Systems P.O. Box 513

5600 MB Eindhoven The Netherlands

Contact: j.d.jansen@tudelft.nl

Keywords: reservoir simulation, reservoir model, water flooding

channelized reservoir, geological ensemble, bench mark, test case

Copyright  2013 The authors

All rights reserved. No part of this publication may be reproduced without permission of the authors listed above.

(3)

Abstra

The "Eg small t flooding numero flooding settings publicat test cas the perm four re (Stanfor describe various access t

Model

The Eg van Ess single, used in has bee history [5] to [9 permeab referenc the form which 1 an-egg-layers realizat The pe assume permeab Figure of 101 m Figure permea

act

gg Model" three-dimen g condition ous publica g optimizat s are not a tions. We p e in future meability fi eservoir sim rd Universi es the inpu simulators to external u

l descript

g Model wa sen. The fir

determinist several pub en used fre matching o 9]. Moreov bility field ces [2] to [4 m of discre 18.553 cells -shaped mo has been ions display ermeability d to be con bility fields 1. The com models whi 1: Six ra ability mean is a synthe nsional rea ns with eig ations to de tion and h always iden present a "st publication ield used fo mulators: D ity) and MR ut parameter s, it has be users.

tion

as develope rst publicati tic reservoi blications; s equently to or, in comb er, a recent has been pr 4] consists o ete permea s are active. odel of activ hand-drawn ys a clear ch values hav nstant. The s are almost mbination of ich together andomly ch dering chan tic reservoi lizations o ght water i emonstrate istory matc ntical and tandard ver ns, and a da or the standa Dynamo/M RST (Sinte rs of the sta en be uplo ed as part of ion that refe

r model wa see e.g. refe

test algori bination, clo version, w resented in r of an ensem ability field The non-ac ve cells. Ea n using a hannel orien ve not been seven laye t two-dimen the determi r form the “s hosen realiz nnels in a lo ir model co of a chann injectors an a variety ching. Unfo not always rsion" of the ata set of 10 ard model. ores (Shel ef), which p andard mod oaded in the f the PhD th fers to it app as used. Th erences [2] t ithms for c osed-loop re with the sam

reference [1 mble of 100 ds modeled ctive cells a ach of the simple co ntation with n condition ers have a nsional. A inistic mod standard mo zations, dis ow-permeab onsisting of nelized rese nd four pro of aspects ortunately t s fully doc e Egg Mode 00 permeabi We implem l), Eclipse produced ne del. Togeth e 3TU.Data hesis work pears to be hereafter, a to [4], while computer–a eservoir ma me reservoir 10]. The ori realization with 60 × are all at the

permeabilit omputer-ass h a typical c ned on the strong vert sample of s el and the e odel” as des splaying th bility backg an ensembl ervoir prod oducers. It related to the details cumented in el which is m ility realiza mented and (Schlumb ear-identica her with the acentrum re of Maarten reference [ an ensemble e also the de ssisted floo anagement; shape but a iginal stoch s of a chann 60 × 7 = 25 e outside of ty fields in isted draw channel dist wells, wh tical correla six realizati ensemble re scribed in th he typical ground. le of 101 re duced unde has been o computer-of the par n several o meant to se ations in add tested the m berger), AD al output. T e input files epository w n Zandvliet a [1] in which e version h eterministic oding optim see e.g. re an entirely d hastic model nnelized rese 5.200 grid f the model, n each of th wing progra tance and si hile the por ation, such ions is disp esult in an e his note. structure o elatively er water used in -assisted rameters of these erve as a dition to model in D-GPRS This note s for the with free and Gijs h only a has been c version mization, ferences different l used in ervoir in cells of , leaving he seven am. The inuosity. rosity is that the played in nsemble of

(4)

high-The Egg In all p Because and the product Figure Unfortu always constrai fully do numeric version publicat permeab materia flow an Model, v.1d, publications e the mode production tion wells, s 2: Reservoi unately the identical. ints, and pr ocumented cal results " of the E tions. The p bility field al to this not nd Buckley-November 20 s the Egg M el has no aq n mechanism see Figure 2 ir model dis details of t Difference roduction pe which som of those p Egg Model parameters s are avail te. Figure 3 Leverett so 013 Model has quifer and n m is water fl 2. splaying the the paramet s concern eriods. In a metimes mak publications which is of the stan lable in Ec displays th lution. been used no gas cap, flooding wit e position of ters settings fluid para addition, the kes it diffic s. Therefor meant to s ndard model clipse form he relative p to simulat primary pr th the aid of f the injecto s in the pub ameters, gri e parameter ult, or even re, in this serve as a l have been mat (ASCII ermeabilitie e two-phas roduction is f eight injec ors (blue) an blications li id cell size r setting hav n impossibl note we p standard t n listed in in text files) es and the a se (oil-wate s almost ne ction wells a nd producer isted above zes, well o ve not alwa le, to reprod present a "s test case in n Table 1. T as supple associated fr 4/8 er) flow. gligible, and four rs (red). e are not operating ays been duce the standard n future The 101 ementary ractional

(5)

Implementation

We implemented the standard Egg Model in four different reservoir simulators: 1) Dynamo/MoReS, the proprietary Shell simulator that was used to generate the original Egg Model, 2) Eclipse 100, the commercial black oil simulator developed by Schlumberger [11], 3) AD-GPRS, the academic General Purpose Research Simulator developed by Stanford University [12], and 4) the Matlab Reservoir Simulation Toolbox (MRST), an open-source simulator developed by Sintef [13], [14]. The four simulators require slightly different parameter settings for e.g. time stepping and solver performance. Moreover, MRST requires user-written code to compute e.g. phase rates from the total rates as computed in the standard implementation. In all simulators the input was chosen as prescribed rates in the injectors and prescribed bottom-hole pressures in the producers. Additional pressure constraints in the injectors and rate constraints in the producers (if required by the simulator) where chosen so high that they were never encountered during the simulations. The exact input files for the four simulators, including the user-written code, are available as supplementary material to this note and have been uploaded in the 3TU.Datacentrum [15]. The results obtained with the four simulators are almost identical, as illustrated by the phase rates in the four producers displayed in Figure 4.

Figure 3: Relative permeabilities (top-left), fractional flow (top-right), derivative of fractional flow (bottom-left) and Buckley-Leverett solution (bottom-right).

0 0.5 1 0 0.5 1 Water saturation Sw , -R e la ti v e p e rm e a b ili ty k r , -0 0.5 1 0 0.5 1 Water saturation Sw , -W a te r fr a c ti o n a l fl o w f w , -0 0.5 1 0 2 4 Water saturation Sw , -D e ri v a ti v e o f fr a c ti o n a l fl o w df w /d S w , -0 0.5 1 0 0.5 1 W a te r s a tu ra ti o n S w ,

(6)

-The Egg Model, v.1d, November 2013 6/8

Table 1: Reservoir and fluid properties

Symbol Variable Value SI units

h Grid-block height 4 m x, y Grid-block length/width 8 m  Porosity 0.2 - co Oil compressibility 1.0  10 -10 Pa-1 cr Rock compressibility 0 Pa -1 cw Water compressibility 1.0  10 -10 Pa-1

o Oil dynamic viscosity 5.0  10

-3 Pa s

w Water dynamic viscosity 1.0  10

-3 Pa s

0

ro

k End-point relative permeability, oil 0.8 

0

rw

k End-point relative permeability, water  

no Corey exponent, oil 4.0 

nw Corey exponent, water 3.0 

Sor Residual-oil saturation 0.1 

Swc Connate-water saturation 0.2 

pc Capillary pressure 0.0 Pa

R

p Initial reservoir pressure (top layer) 40  106 Pa

Sw,0 Initial water saturation 0.1 

qwi Water injection rates, per well 79.5 m

3

/d

pbh Production well bottom hole pressures 39.5  10

6 Pa

rwell Well-bore radius 0.1 M

(7)

Figure 4: Well flow rates (oil and water) in the four producers for the four simulators. The curves for the various simulators are nearly identical.

Acknowledgments

This research was carried out within the context of the Integrated Systems Approach to Petroleum Production (ISAPP) and Recovery Factory (RF) projects. ISAPP is a joint project between Delft University of Technology (TU Delft), the Netherlands Organization for Applied Scientific Research (TNO), Eni, Statoil and Petrobras. RF is a joint project between Shell and TU Delft in cooperation with the Eindhoven University of Technology (TU Eindhoven). We acknowledge Schlumberger for the use of the Eclipse simulator under an academic license. We acknowledge Shell for the use of the Dynamo/MoReS simulator as part of the RF project. We acknowledge Stanford University, in particular Hamdi Tchelepi for the use of AD-GPRS and Drosos Kourounis (now with USI Lugano) for implementing an earlier version of the egg model in that simulator, and Sintef, in particular Stein Krogstad, for assistance in running MRST. 0 500 1000 1500 2000 2500 3000 3500 4000 0 20 40 60 80 100 120 140 160 Producer 1 Time [days] O il/ W a te r P roduc ti on R a te s [m 3/day ] MoReS Eclipse MRST AD-GPRS 0 500 1000 1500 2000 2500 3000 3500 4000 0 50 100 150 200 250 300 350 Producer 2 Time [days] O il /W a te r P rodu c ti on R a te s [m 3/d a y ] MoReS Eclipse MRST AD-GPRS 0 500 1000 1500 2000 2500 3000 3500 4000 0 20 40 60 80 100 120 140 Producer 3 Time [days] O il /W a te r P ro duc ti o n R a te s [m 3/day ] MoReS Eclipse MRST AD-GPRS 0 500 1000 1500 2000 2500 3000 3500 4000 0 50 100 150 Producer 4 Time [days] O il/ W a te r P ro d u c ti o n R a te s [m 3/d a y ] MoReS Eclipse MRST AD-GPRS

(8)

The Egg Model, v.1d, November 2013 8/8

References

[1] Zandvliet, M.J., Bosgra, O.H., Van den Hof, P.M.J., Jansen, J.D. and Kraaijevanger, J.F.B.M., 2007: Bang-bang control and singular arcs in reservoir flooding. Journal of

Petroleum Science and Engineering 58, 186-200. DOI: 10.1016/j.petrol.2006.12.008.

[2] Van Essen, G.M., Zandvliet, M.J., Van den Hof, P.M.J., Bosgra, O.H. and Jansen, J.D., 2006: Robust waterflooding optimization of multiple geological scenarios. Paper SPE 102913 presented at the SPE Annual Technical Conference and Exhibition, San Antonio, USA, 24-27 September.

[3] Van Essen, G.M., Zandvliet, M.J., Van den Hof, P.M.J., Bosgra, O.H. and Jansen, J.D., 2009: Robust water flooding optimization of multiple geological scenarios. SPE Journal

14 (1) 202-210. DOI: 10.2118/102913-PA.

[4] Jansen, J.D., Bosgra, O.H. and van den Hof, P.M.J., 2008: Model-based control of multiphase flow in subsurface oil reservoirs. Journal of Process Control 18 (9) 846-855. DOI: 10.1016/j.jprocont. 2008.06.011.

[5] Jansen, J.D., Douma, S.G., Brouwer, D.R., Van den Hof, P.M.J., Bosgra, O.H. and Heemink, A.W., 2009: Closed-loop reservoir management. Paper SPE 119098 presented at the SPE Reservoir Simulation Symposium, The Woodlands, USA, 2-4- February.

[6] Astrid, P., Papaioannou, G.V., Vink, J.C. and Jansen, J.D., 2011: Pressure preconditioning using proper orthogonal decomposition. Paper SPE 141922 presented at the SPE Reservoir Simulation Symposium, The Woodlands, USA, 21-23 February. [7] Kaleta, M.P., Hanea, R.G., Heemink, A.W. and Jansen, J.D., 2011: Model-reduced

gradient-based history matching. Computational Geosciences 15 (1) 135-153. DOI: 10.1007/s10596-010-9203-5.

[8] Van Essen, G.M., Van den Hof, P.M.J. and Jansen, J.D., 2011: Hierarchical long-term and short-term production optimization. SPE Journal 16 (1) 191-199. DOI: 10.2118/124332-PA.

[9] Kourounis, D., Durlofsky, L.J., Jansen, J.D. and Aziz, K., 2013: Adjoint formulation and constraint handling for gradient-based optimization of compositional reservoir flow. Accepted for publication in Computational Geosciences.

[10] Van Essen G.M., Van den Hof, P.M.J. and Jansen, J.D., 2013: A two-level strategy to realize life-cycle production optimization in an operational setting. SPE Journal. Published online. DOI: http://dx.doi.org/10.2118/149736-PA.

[11] ECLIPSE http://www.software.slb.com/products/foundation/pages/eclipse.aspx

[12] General Purpose Research Simulator (GPRS): https://pangea.stanford.edu/ researchgroups/supri-b/research/research-areas/gprs .

[13] Matlab Reservoir Simulation Toolbox (MRST) http://www.sintef.no/Projectweb/MRST/

[14] Lie, K.-A., Krogstad, S., Ligaarden, I. S., Natvig, J. R., Nilsen, H. M. and Skaflestad, B., 2012. Open source MATLAB implementation of consistent discretisations on complex grids. Computational Geosciences 16 (2) 297-322. DOI: 10.1007/s10596-011-9244-4. [15] Jansen, J.D., Fonseca, R.M, Kahrobaei, S., Siraj, M.M., Van Essen, G.M. and Van den

Hof, P.M.J., 2013. The Egg Model – data files. 3TU.Datacentrum, The Netherlands. Dataset. doi:10.4121/uuid:916c86cd-3558-4672-829a-105c62985ab2.

Cytaty

Powiązane dokumenty

that means United states has large reserves and can transfer some econom- ic resources within present amount of military spending; america’s naval superiority is also

Aleksandra Oko-

Eks- presjonistyczne tło dla Soli ziem i stanowią w pracy Jakow skiej najczęściej d ram aty (Zegadłowicza, Zarem biny oraz niemieckich ekspresjonistów), znacznie

The error probability 1/3 in an rptas can be cut down to any given δ > 0 by the following method: Run the algorithm many times (say m, where m is odd), and take the median of

Therefore: we are dealing with random variables defined over some probabilistic space; the realizations of these random variables are the collected data.. Problem: we do not know

Since the transport formulations use offshore climate properties as an input, a translation of some of the wave parameters to characteristic deep water conditions has been

Therefore also insight into the coastal sediment transport, both cross-shore and longshore, as presented in the literature has been used for the calibration of the governing

Throughout the successive stages of design evolvement, a wide range of models may be used, from generative to illustrative modelling types, using physical and digital platforms