Delft University of Technology
The impact of reduction of doublet well spacing on the Net Present Value and the life time
of fluvial Hot Sedimentary Aquifer doublets
Willems, Cees; Nick, H.M.; Goense, Twan; Bruhn, David
DOI
10.1016/j.geothermics.2017.02.008
Publication date
2017
Document Version
Final published version
Published in
Geothermics
Citation (APA)
Willems, C., Nick, H. M., Goense, T., & Bruhn, D. (2017). The impact of reduction of doublet well spacing on
the Net Present Value and the life time of fluvial Hot Sedimentary Aquifer doublets. Geothermics, 68, 54-66.
https://doi.org/10.1016/j.geothermics.2017.02.008
Important note
To cite this publication, please use the final published version (if applicable).
Please check the document version above.
Copyright
Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons. Takedown policy
Please contact us and provide details if you believe this document breaches copyrights. We will remove access to the work immediately and investigate your claim.
This work is downloaded from Delft University of Technology.
ContentslistsavailableatScienceDirect
Geothermics
j ou rn a l h o m e pa g e :w w w . e l s e v i e r . c o m / l o c a t e / g e o t h e r m i c s
The
impact
of
reduction
of
doublet
well
spacing
on
the
Net
Present
Value
and
the
life
time
of
fluvial
Hot
Sedimentary
Aquifer
doublets
C.J.L.
Willems
a,∗,
H.M.
Nick
a,b,
T.
Goense
a,
D.F.
Bruhn
a,caDepartmentofGeoscienceandEngineering,DelftUniversityofTechnology,Delft,Netherlands
bTheDanishHydrocarbonResearchandTechnologyCentre,TechnicalUniversityofDenmark,Copenhagen,Denmark cHelmholtzCentrePotsdam–GFZGermanResearchCentreforGeosciences,Germany
a
r
t
i
c
l
e
i
n
f
o
Articlehistory:
Received8November2016
Receivedinrevisedform24January2017 Accepted28February2017 Keywords: Directuse Districtheating Lowenthalpy Fluvialsandstone Geothermaldoublet NieuwerkerkFormation
a
b
s
t
r
a
c
t
Thispaperevaluatestheimpactofreductionofdoubletwellspacing,belowthecurrentWestNetherlands Basinstandardof1000–1500m,ontheNetPresentValue(NPV)andthelifetimeoffluvialHot Sedimen-taryAquifer(HSA)doublets.First,asensitivityanalysisisusedtoshowthepossibleadvantageofsuch reductionontheNPV.TheparametervaluerangesarederivedfromWestNetherlandsBasinHSAdoublet examples.Theresultsindicatethatareductionofwellspacingfrom1400to1000mcouldalreadyimprove NPVbyupto15%.ThiseffectwouldbelargerinmoremarginallyeconomicHSAdoubletscomparedtothe WestNetherlandsBasinbasecasescenario.Thepossibilitytoreducewellspacingissupportedbyfinite elementproductionsimulations,utilizingdetailedfaciesarchitecturemodels.Furthermore,ourresults underlinethenecessityofdetailedfaciesarchitecturemodelstoassessthepotentialandrisksofHSA doublets.Thisfactorsignificantlyaffectsdoubletlifetimeandnetenergyproductionofthedoublet.
©2017TheAuthors.PublishedbyElsevierLtd.ThisisanopenaccessarticleundertheCCBYlicense (http://creativecommons.org/licenses/by/4.0/).
1. Introduction
Large potentialresources of heat are stored in sedimentary rocks.IntheNetherlandsalone,theDutchgeologicalsurvey esti-matedthetotalrecoverableheatfromthistypeofresourcetobe approximately55timeslargerthantheannualheatconsumption
(Kramersetal.,2012; CBS).HotSedimentaryAquifers(HSA)are
especiallysuitablefor‘directuse’orheatproduction,becausethey areoftenfoundin areaswithaveragethermal gradient(Boxem
etal.,2011;Pluymaekersetal.,2012).Intheseareastemperatures
forcommercialelectricityproduction(e.g.,Shengjunetal.,2011) arefound atdepths where pore space is generallydiminished. However,heatingaccountsforhalfofthetotalenergy consump-tionin,forexample,theEuropeanUnion(EuropeanCommission, 2016).Therefore,HSAshouldbeconsideredasimportantenergy resources.Unfortunately,alargegapcurrentlyexistsbetweenHSA potentialandexploitation.Thisgapisaresultofacombinationof highinitialinvestmentcostsandlargeuncertaintiesinboth dou-bletlifetime and capacity.The heightoftheinitialinvestment ismainlyinfluencedbyacombinationofhighdrillingcostsand
∗ Correspondingauthor.
E-mailaddresses:c.j.l.willems@tudelft.nl(C.J.L.Willems),h.m.nick@tudelft.nl
(H.M.Nick),t.goense@student.tudelft.nl(T.Goense),d.f.bruhn@tudelft.nl
(D.F.Bruhn).
thereplacement of existing fossilfuel basedheating networks. ThesetwofactorsdecreasethecompetitivenessofHSA exploita-tionwithotherenergysourcesand therebylimit itsgrowth.In theNetherlands,forexample,twonewgeothermalprojectsare realisedinHSAeachyear,whilemorethan100explorationlicences havebeengrantedsince2007.Areductionoftheinitialinvestment costswouldreducetherisksfordevelopersandhencestimulatethe growthofHSAexploitation.Inthispaper,weevaluatetheeffectof wellspacingreductionontheNetPresentValue(NPV)ofaHSA doublet.Also,wediscusstheeffectsuchareductionwouldhave onthelifetimeofadoublet.Thecurrentwellspacing standard intheWestNetherlandsBasin(WNB)andParisBasin(Mijnlieff
andVan Wees,2009; Lopezet al.,2010;Mottaghy etal.,2011;
Daniilidisetal.,2016),is1000–1500m.Partially,thelargedistance
isusedtopreventearlycoldwaterbreakthrough.Overdesign, how-ever,couldleadtounnecessarilylongthermalbreakthroughtime. Forexample,nothermalbreakthroughhasyetbeenreportedin thepast40yearsofexploitationintheParisBasin.Awellspacing reductioncouldstillresultin sufficientlifetime,while improv-ingthefinancialsituationofadoubletintwoways.First,itmay reducethedrillingcostsbymakingtheoverallwelllengthshorter, atleastforthecurrentstandarddoubletlayoutwithtwodeviated wellsfromthesamesurfacelocation.Second,itcouldreducethe requiredpumpenergyduetoshorterflowpathsbetweenthewells. Anotheradvantageis thedecreaseof chanceongeologicalflow bafflesbetweenthewells,suchassealedsub-seismicfaults(e.g., http://dx.doi.org/10.1016/j.geothermics.2017.02.008
Baileyetal.,2002)orpoorsandstonebodyconnectivity(Larueand
Hovadik,2006;PranterandSommer,2011).Finally,moredoublets
couldberealisedinthesameaquiferwhichincreasestheamount ofproducedgeothermalheat(MijnlieffandVanWees,2009).The numberofstudiesonoptimisationofgeothermalsystemsis lim-itedandoftenfocusonmaximizingenergyproduction(e.g.,Sauty
etal.,1980;EkneligodaandMin,2014;Adams,2015).Boththe
pos-siblefinancialadvantageofwellspacingreductionanditsimpact ondoubletlifetimeisevaluatedinthispaper.Inthefirstpart,the effectofavariationinwellspacingontheNetPresentValue(NPV) foratypicalWNBdoubletisdetermined.Thisisderivedfroma sen-sitivityanalysisinwhichbothproductionandfinancialparameters arevaried.ParameterrangesarederivedfromaWestNetherlands Basincasestudy.Theanalysisisbasedonfinite-element produc-tionsimulationsinhopermeableandimpermeablefaciesbodies intheaquifercouldsignificantlyaffectdoubletlifetimeand capac-ity(e.g.,Pranteretal.,2007;HammandLopez,2012;Poulsenetal.,
2015;Crooijmansetal.,2016).Homogeneousaquifermodelsdonot
capturethisuncertainty.Inourstudy,detailedfluvialfacies archi-tecturerealisationsaregeneratedutilizingaprocess-basedfacies modellingapproach(Cojanetal.,2004;Grappeetal.,2012;Hamm
andLopez,2012)basedonaWNBgeologicaldataset.Minimum
wellspacingisanalysedintermsoflifetimeandNPV.Theresults ofthisstudycouldbeusedasanincentiveforre-evaluationofHSA wellspacingstandards.Utilizingdetailedfaciesarchitecture mod-els,moreprofoundestimatesofdoubletlifetimeandcapacitycan bemade.Thisshouldpreventoverdesignandtherebyimprovethe competitivenessofHSAexploitation.
2. Dataandaquifermodelling
Theaquifermodelsinthis paperwerebased onageological datasetofthefluvialLowerCretaceousNieuwerkerkFormationin theWestNetherlandsBasin(DeVaultandJeremiah,2002;Jeremiah
et al., 2010; Donselaar et al., 2015). This dataset was chosen,
becausemostoftheapproximately40explorationlicencestarget thisHSAintervalintheWNB.Parametervalues,whichwereusedin aquifermodellingandproductionsimulations,werederivedfrom thisdataset.Furthermore,productionratesandreinjection tem-peratureswerederivedfromWNBdoubletexamples.Byusingthis dataseta realisticrange ofheterogeneities wasderived to con-straintthesetoffaciesrealisations.Twotypesofaquifermodels werecreated:(1)detailedfaciesarchitecturerealisationsand(2) homogeneousmodels.Thefirsttypeofrealisationsweregenerated withaprocess-basedapproach.Thefollowingsectionsdescribethe geologicaldataandthemodellingapproach.
2.1. Geologicaldataset
AsubsurfacedatasetofthefluvialNieuwerkerkFormationin theWNB formedthebasis for the geologicalmodelling in this study.Thesamedatasetandmodellingapproachasdescribedin
Crooijmansetal.(2016)andWillemsetal.(2017)wasused.The
datasetcomprisedofcoresandGamma-ray(GR)logsof geother-malwellsIntheWNB.Thecorestudyprovidedthicknessranges offaciesbodieswhichwereusedasinputparametersto gener-ateprocess-basedfaciesrealisations.Inapproximately75mofcore inMKP-11and25minQ13-09,fivedifferenttypesoffacies bod-ieswererecognized:floodplainfines,crevassesplays,single-storey channelbodiesandamalgamatedsandstonecomplexes.The maxi-mumfiningupwardsequencethatwasrecognizedinthecoreswas 4m(Fig.1).Thereforeitwasassumedthatthepaleobank-fullflow depthofthefluvialsystemthatformedtheNieuwerkerk Forma-tionwas4m.Basedonflowdepth,thepaleobank-fullflowwidth wasestimatedat40m(Williams,1986)(Fig.1).Furthermore,cores
providedporosity-permeabilityrelationsfortheaquiferproperty modelling.ThegammaraylogswereusedtoderiveN/G ranges oftheNieuwerkerkFormation.GRlogsintheWNBshowedthat theNieuwerkerkFormationsignificantlyvariesinthicknessand N/G.Thethicknessvariesfrom50toalmost200mandtheN/Gthe approximately15–70%indifferentsectionsoftheaquifer(Fig.1). 2.2. Process-baseddetailedfaciesarchitecturerealisations
Togeneratethedetailedfaciesarchitecturerealisations,a simi-larapproachasinCrooijmansetal.(2016)andWillemsetal.(2017)
wasused.Inputparametersfortheprocess-basedfaciesmodelling (Fig.2)were(1) channelwidthand depth, (2)maximum over-bankflooddepositthickness(Hth),(3)avulsionfrequency,(4)flood
frequency,and(5)floodplaintopographyparameter(henceforth: FT-parameter)(Fig.2).Influvialsystems,thethicknessoffloodplain depositdecreasesawayfromthechannel.Thedistanceatwhich thethicknessdecreasedexponentiallyistheFT-parameter(Fig.2). AhighFT-parametermeansthattheflooddepositiswideandthick, whichincreasesthesedimentaggradationrateanddecreasesthe N/Goftherealisation.Thepaleobank-fullflowdepthwasderived fromthecoreanalysisandanalogues,respectively.Asitwasnot straightforwardderivevaluesoftheotherparameterfromcores suchasthefloodplaindepositthickness(e.g.,Bridge,2006),values rangeswereassumedtocapturetheuncertaintyoftheparameter valuesandtoobtainrealisationsthatrangeinN/G.Floodfrequency, maximumflooddepositthickness(Hth)andtheFTfactorwerethe
primarycontrolsonN/G.Toobtainrealisationswithawiderange ofN/Gvaluesbetween15and70%,overbankfloodfrequencywas variedbetween20and120years,Hthbetween0.2and0.6mand
theFT-factorbetween300and600m.Avulsionfrequencyisvaried from600to1600years(TörnqvistandBridge,2002).Duringevery simulatedfluvialflood,sedimentsweredeposited onthe flood-plainwithamaximumthicknessHthnearthechannel(Fig.2).In
thesimulations,sedimentaryprocessesdistributeandshape differ-entfaciesbodiessuchaschannellags,point-bars,crevassesplays, mudplugsandfloodplainfines.Realisationshavedimensionsof 1km×2km×50mandthepaleoflowdirectionisparalleltothe longedgeoftherealisations.Theprocess-basedFlumysoftware methodwasexplainedinmoredetailinCojanetal.(2004),Grappe
etal.(2012)andLopezetal.(2009).
2.3. Heterogeneousaquifermodels
Faciesgrid blocks in the realisations weredivided into two classes,aquiferand non-aquifer.Thenon-aquiferclass included finegrainedfaciessuchascrevassesplays,overbankalluviumand mudplugs.Thesebodieswereallassumedtoberelatively imper-meable.Theirassumedpermeabilitywas5mDandporosity10%. Sandyfaciesbodiessuchaspoint-barsandchannellagswereall assumedtobeaquifergridblocks.Porosityvalueswereassignedto theseblocksbasedonthecoreplugporositydata.Fromthisdata, abetadistributioncorrelationfunctionwasderived.The distribu-tioncharacteristicsincluding:mean,standarddeviation,skewand kurtosiswereequalto0.28,0.075,0.35and2.3,respectively. Sec-ondly,thepermeabilityofeachgridblockwasdeterminedbya porosity-permeabilityrelationobtainedfrompetrophysicaldataof wellMKP-11(TNO,1977):k=0.0633e29.5.Inthisequation,kisthe
permeability[mD]andistheporosity[–]. 2.4. Homogeneousaquifermodels
FortheNPVsensitivityanalysis,homogeneousaquifermodels werecreatedbasedonthesamegeologicaldataset.Thesemodels hadanaverageporosityof28%andpermeabilitybetween250and 2000mD.ThispermeabilityrangewasderivedfromWNBHSAwell
Fig.1.Gamma-raylogof1offshorehydrocarbonwellwithcore(well1)andtheassociatedsedimentarylog.Well2–5aregeothermalwells.
tests(Lingen,2014)andcoreplugmeasurements(TNO,1977).The thicknessofthehomogeneousmodelsinthesensitivityanalysis variedbetween50and120m.
3. Numericalproductionsimulations
Intheproductionsimulations,theaquiferwasconfinedbetween two50mthickimpermeableover-andunderburdenlayersthat providethermalrecharge.Theenergybalancewassolvedforarigid mediumfullysaturatedwithwater,inwhichthermalequilibrium wasassumedbetweenthefluidandsolidphases:
C
∂
∂
tT+wCw∇
·(qT)−∇
·(I∇
T)=0 (1)Inthisbalance,t(s)istime,T(K)isthetemperature,isthemass density(kg/m3),C
w(J/kgK)isthespecificheatcapacity,(W/mK)
isthethermalconductivity,Itheidentitymatrix,andq(m/s)isthe Darcyvelocityvector.Thesuffixwreferstotheporefluidandsto thesolidmatrix.Theheatcapacity,densityandconductivity val-uesforaquifergridblocksare730J/kgK,2650kg/m3and2.7W/mK
respectively.Forthenon-aquiferblocksthesevaluesare950J/kgK, 2600kg/m3and2.0W/mK.Thethermalconductivityandthe
vol-umetricheat capacityare described interms of a localvolume average.Heatconductivity,densityandheatcapacityareassumed tobeindependentoftemperatureforsimplicityanddescribedby =(1−)s+wandC=(1−)sCs+wCwinwhichisthe
porosity.ThisDarcyflowvelocityvectorcanbedeterminedby: q=(kP)/,whereisk(m2)theintrinsicpermeability,the
tem-peratureandsalinitydependentviscosityexplainedinCrooijmans
etal.(2016),andP(Pa)thepressure.Thepressurefieldisobtained
throughsolvingthecontinuityequation:(
∂
w)/∂
t+(wq)=wS,whereS(s–1)isexternalsinksandsources.Thedetailedmodelling
procedurefollowstheapproach explainedin Saeidet al.(2014,
2015).Theproductionsimulationsyieldaproductiontemperature
developmentovertimeandtherequiredinjectionandproduction pressureforthedefinedproductionrate.Thedifferencebetween thesepressuresforeach timestepi(Pi)wasusedtoestimate
pumpenergylosses(Epump,i)asindicatedinEq.(2)(e.g.,Willems
etal.,2016),whereQ istheconstantproductionrateandεthe pumpefficiency.Theproducedenergy(Eprod,i)wasestimatedby
Eq.(3)oneachtimestepi(e.g.,Willemsetal.,2016)inwhichw
isthewaterdensityof1050kg/m3andT
ithedifferencebetween
injectionandproductiontemperature.Thenetenergyproduction, orthedoubletcapacitywasdeterminedbythesumoftheproduced energyandthepumpenergylosses.
Epump,i=
QPi
ε (2)
Fig.2. (1)Process-basedfaciesmodellinginputparametersinacross-sectionofapointbar.Lateralaccretionsurfacesandcoarsechannellagdepositsareindicatedinthe pointbar.(2)Mapviewoffaciesinthedepositionalenvironment.
Table1
EconomicparametersfortheNPVrealisationbasedonVanWeesetal.(2010).
Basecaseeconomicparameters
Heatprice D6.00 D/GJ
Electricitypriceforoperations D22.22 D/GJ
Discountrate 7 % CAPEX Wellcosts D1.5 MD/km Pump D0.50 MD Heatexchanger D0.10 MD Separator D0.10 MD Contingencycosts(10%) D0.89 MD SEI(insurance) D0.69 MD OPEX 5 %ofCAPEX/year
Tax 25.5 %oftaxableincome
Depreciationperiod 10 years Feed-intariff(SDE+)
Baseenergyprice(2015) D0.052 D/kWh Correctionprice(2015) D0.019 D/kWh ContributionSDE+ D9.17 D/GJ
4. NetPresentValuemodel
ANPVmodeldevelopedbyVanWeesetal.(2010)wasutilized torelateproductionsimulations toNPV. InputfortheNPV cal-culationswerenetenergyproductioninWattandtheeconomic parameters listedin Table1. In ourstudy,additional separator costswereincluded,becauseinmanyWNBdoubletsnaturalgas co-productionoccurs.TheNPVisthedepreciated,discounted, net-cumulativeincomeafter15years.Thisperiodwaschosen,because it is themaximumduration of theDutchfeed-in tariff scheme (SDE+)forgeothermalenergy(VanHeekerenandBakema,2013, 2015).0.25MD pumpwork-overcostsweretakenintoaccount everyfiveyears,whichisequaltohalfoftheestimatedpumpcosts. 40%down-timewasassumedformaintenancethroughouttheyear. Becausedoubletwellsaredrilledfromonesurfacelocation, dou-bletwellspacinginfluencesthewelllength(Fig.3).Inthisstudy,
thelengthofa singlewell(WL)wasapproximatedbythesum ofavertical(Dvert)andadeviatedsection(Ddev),WL=Dvert+Ddev.
Theverticalsectionwasassumedtobe1500m.Thelengthofthe deviatedsection,wasapproximatedby:
Ddev=
(TVD−Dvert)2+ 1 2L 2 (4) InEq.(4),TrueVerticalDepth(TVD)isthetotalwelldepthwhich is2.2kmandListhedoubletwellspacing.Reductionofthewell spacingfrom1000mto800mcouldthereforeresultinareduction ofthetotalwelllengthby2%.Becauseoftheassumedwellcostper kilometerinTable1,drillingcostsreduceaccordingly.For exam-ple,typicallydrillingcostsofa2.2kmdeepgeothermaldoubletis∼7.2MD(VanWeesetal.,2010;NielsonandGarg,2016).Utilizing
equation4,thereductioninspacingfrom1000to800mcouldlead toareductionofinvestmentofupto0.16MD.Areductionfromthe 1500mstandardto800mwoulddecreasethetotalwelllengthby approximately9%andtheassociatedwellcostsbyapproximately 0.66MD.
5. Analyses
5.1. NPVsensitivityanalysis
Inthesensitivityanalysis,theeffectofa100mand400mwell spacingvariation froma1000mbasecase scenarioontheNPV wasevaluated.Thiswascomparedtotherelativeimpactofother parameters.In thisanalysis,homogeneousaquifermodelswere utilized.Twocategoriesofparameterswerecompared,financial andproductionrelatedparameters.Thefinancialparameterswere variedby±10%ofthebasecasevalue.Productionrelated param-eterrangeswerederivedfromthegeologicaldataandcurrently activeWNBdoublets.TheparameterrangesarelistedinFig.6.In theanalysis,eachparameterwasvariedindividually,whilekeeping theothersatthebasecasevalue.
Fig.3.Welllay-outexampleofaconceptualdoubletintheWNB.Theblackdottedlinesindicatehowawellspacingreductioninfluencesthetotaldoubletwelllength.The wellstargetafluvialsandstonefaultaquiferboundedbyfaultsdrilleddeviatedfromonesurfacelocation.Yellowcoloursindicatesandstoneandgreenishandgreycolours indicateimpermeablefloodplainfines.(Forinterpretationofthereferencestocolourinthisfigurelegend,thereaderisreferredtothewebversionofthearticle.)
Fig.4. (A)Exampleofafaciesrealisationusedinaproductionsimulationwithfourwellspacingdistances,paralleltothepaleoflowdirection.Homogeneousmodelswith adjustedheighttocompensatefortheuncertaintyinnetaquifervolumefor(B)15%and(C)70%N/G.
5.2. Impactoffluvialfaciesarchitectureonlifetime
Inthesecondpartofthispaper,theeffectofaquifer architec-tureontheadvantageofreductioninwellspacingwasevaluated.In thispart,productionsimulationswerecarriedoututilizingdetailed fluvialfacies architecturerealisations.In thesetof realisations, N/Gvariedbetween15and70%N/G.Doubletwellswereplaced at400,600,800and1000m(Fig.4A)undertheconditionthatboth wellsintersectthesameamountofsandstonegridblocks,likein
Crooijmansetal.(2016).Doubletwellpairswereplacedparallelto
thepaleoflowdirectionasthisreducestherequiredpumpenergy losses(Willemsetal.,2017).Forcomparison,twohomogeneous modelsweregeneratedinwhichthethicknesswasadjustedby15 and70%respectively(Fig.4BandC).Inthisway,bothmodeltypes hadthesamenet-aquifervolumerange.Twolifetimescenarios wereconsidered.InthefirstscenarioA,thelifetimewasreached aftertheproduction temperaturedecreased by10%ofitsinitial
Fig.5. (A)Basecasescenariocumulativediscountedcashflowandnetannualincome.(B)Productiontemperaturedevelopmentfor1000mwellsspacing,100m3/hproduction
rateinthebasecasescenarioandina50mthickaquifer.
Fig.6. TornadoplotsillustratingtheimpactofseveralparametersonNPVinpercentages.Theparameterrangesandtheirbasecase(BC)valuesarepresentedontheright sideofthetornadoplots.
value.InthesecondscenarioB,thelifetimewasreachedwhenthe temperaturedecreasedby1◦C.
6. Results
6.1. Basecasescenario
Thethermalcapacityofourbasecasedoubletis4.1MW(Eqs. (2)and(3)).Theassociateddiscountedcumulativecashflowand thenetannualincomearepresentedinFig.5A.Forthebasecase scenario the NPV is approximately 3.7MD and representsthe
cumulative discounted cash flowafter 15 years. Theassociated InternalRateofReturnonInvestments(IRR)would be approxi-mately8years.Thethermalbreakthroughmomenthappensafter morethan60years,evenifaquiferthicknessisreducedto50m (Fig.5B).Afterthisthermalbreakthroughtheproduction temper-atureonlydecreasesbyapproximately1–2◦Cperdecade.
6.2. NPVsensitivityanalysis
TheresultofthesensitivityanalysisispresentedinFig.6.A tor-nadoplotshowsthechangeinNPVinpercentages(NPV)which
Fig.7.DiscountedcumulativecashflowforscenarioA(basecaseparameters),B (L=600,Q=100/h)andC(L=1000,Q=110m3/h)inthesensitivityanalysis.
isdefinedas:(NPVBC−NPVx)/NPVBC×100%,asaresultofthe
vari-ationofasingleparameter.NPVBCisthebasecaseNPV,andNPVx
istheNPVasaresultofadjustmentofaparameterinthe sensi-tivityanalysis.Theparameterrangesarepresentedontheright sideofthetornadoplot.Thisanalysisindicatesthatvariationofthe temperaturedifferencebetweeninjectionandproduction water (T)hasthemostsignificantimpactonaHSAdoubletNPV.Afive degreeCelsiusvariationcouldchangetheNPVbyapproximately 50%.A10m3/hvariationoftheproductionratecouldvarytheNPV
byupto40%.Reducingthewellspacingfrom1400to1000mcould improvetheNPVupto15%.Becausewelllengthisestimatedby equation4,thewelllengthdecreasesby5.5%ifthewellisreduced from1400to1000m.Anadditionalreductionfrom1000to600 changeswelllengthby4.2%.Thereforethetornadoplotshowsa slightasymmetricalresult.Anadditionalwellspacing reduction from1000to600mincreasestheNPVbyapproximately13%.The 100mwellspacingvariation hassmallerimpactontheNPV of approximately4%.Permeability,aquiferthicknessandpump effi-ciencyhave alimitedeffectontheNPV.Becauseoftheinverse relationbetweeninjectionpressureandpermeability,thenegative effectofa750mDpermeabilityreductiononNPV islargerthan thepositiveeffectofa1000mDpermeabilityincrease.Variation ofthepumpenergyefficiencyby±10%didnothaveasignificant impactonNPV(lessthan1%).Otherparametersthathavea sig-nificantimpactonNPV areCAPEXandtheheightofthefeed-in tariffsubsidy.10%variationofdiscountrate,heatpriceandOPEX affecttheNPVbyapproximately10%.Inouranalysis,wellspacing istheonlyindependentparameter,whichisdeterminedpriorto drilling.ProductionrateandTdependongeological uncertain-ties,surfacefacilityefficiencyandonrequiredheatconsumption. Also,allfinancialparametersdependoneconomyorgovernment policy.Therefore,theseresultsalsoindicatetheuncertaintyinNPV asaresultofuncertaintyingeologicalandfinancialcircumstances. Notethattheseresultsarebasedonhomogeneousaquifermodels, theeffectoffaciesandpropertyheterogeneitiesarenotincluded.
TheparametersinthesensitivityanalysisaffecttheNPVofa doubletbecausetheyinfluencethediscounted cumulativecash flow.Thisisbecausetheinitialinvestmentcostsarechangedorthe netincomeis affected.Examplesofdiscountedcumulativecash flowinthreescenarios(A,BandC)fromthesensitivityanalysis arepresentedinFig.7.ScenarioAisthebasecasescenario.In sce-narioBthewellspacingisreducedby400mfrom1000to600m whileallotherparametersarekeptattheirbasecasevalue(Fig.6). Asaresult,theinitialinvestmentscostsarereducedwhilethenet
incomeisconstant.Therefore,thediscountedcumulativecashflow curveisshiftedupward,increasingtheNPVafter15years(Fig.7). InscenarioCtheproductionrateisincreasedfrom100to110m3/h
whileallotherparametersarekeptattheirbasecasevalues.The higherproductionrateincreasedtheslopeofthediscounted cumu-lativecashflow,whichalsoincreasesNPV(Fig.7).
ThetheoreticaladvantageofawellspacingreductiononNPV inFig.6,appliestoatypicalWNBHSAdoublet.Toevaluatethe effectofwellspacingvariationonNPVindoubletsinotherbasins orcountries,thesensitivityanalysisisrepeatedfordoubletswith differentdrillingcosts,productionorreinjectiontemperaturesand productionrates.Thesethreeparametersarechosenbecausethey havethemostsignificantimpactonNPVaccordingtoour analy-sisresultsinFig.6.Inscenario1and2,drillingcostsarevariedby
0.3MD/kmfromtheWNBbasecase(Table1).Inscenario3theT
is5degreeshigherthaninourbasecasescenario.Thiscouldbea resultofahigherproductiontemperatureorhigherheatextraction efficiencyandaffectsthenetenergyproduction(Eq.(3)).Incontrast inscenario4theTis5degreelower.Finallytheproductionrateis changedby20m3/hinscenario5and6.Inthesesixscenariosonly
thebasecasevalueoftheindicatedparameterinscenario1–6is variedwhileallothervaluesarekeptatthesamevalueasinFig.6. Foreach scenario,a newNPV valueiscalculated.Subsequently, theeffectofa100mwellspacingvariationfrom1000monthis NPViscalculated.TheresultsarepresentedinFig.8.Theresults indicatethatwellspacingvariationhasgreaterimpactonNPVin areaswithhigherdrillingcosts.Ifthedrillingcostsare0.3MD/km higherthanintheWNB,the10%wellspacingreductionchanges NPVbyapproximately10%whichisapproximately5%more com-paredtotheresultinFig.6.Ifthedoubletcapacityislowerbecause ofthe5degreereductionofT,a10%wellspacingreductioncould increasetheNPVbyupto15%.Wellspacingreductionhasaneven higherimpactonNPVindoubletwithlowerproductionrates.Ina doubletwithan80m3/hproductionrate,a10%wellspacing
reduc-tionincreasedtheNPVbyapproximately25%.In doubletswith lowerdrillingcosts,higherT,orhigherproductionrates com-paredtheWNBbasecase,theimpactofwellspacingreductionon NPVremainsafewpercentages.Theseresultsimplythatreducing thewellspacingtoimproveNPVismorerelevantformarginally economicdoublets.
6.3. Impactoffluvialfaciesarchitectureondoubletlifetime The resultsof theproduction simulationswith detailed flu-vialfacies architecturerealisationsarecompared tosimulations inhomogeneousaquifermodelsinFig.9.Twolifetimescenarios andtwoproductionratesarecompared.Threeobservationscan bemade.First,800mspacingissufficienttoobtaina15yearslife timeinbothlifetimescenariosandaproductionrateof100m3/h.If
theproductionrateis150m3/h,800misonlysufficientwhenT
is7.5◦C.With600mspacingthelifetimeexceeds15yearsonly witha100m3/hproductionrateandwithTof7.5◦C.Secondly,
theseresultsalsoindicateanunderestimationoftheuncertainty inlifetimebythehomogeneousaquifermodels.Therangeoflife timeresultsperwellspacingdistanceislarger,whendetailedfacies architecturerealisationsareused.Thisuncertaintyincreasesfor largerwellspacing distances.In contrast,it is lowerfor higher production rates.The uncertainty in lifetime increases slightly forhigherallowedproductiontemperaturedrop(T).Thirdly,the resultsimplythatlifetimeestimationsarelowerinthe homoge-neousmodels.Thepeaksofthedistributionsof lifetimeofthe detailedfaciesrealisationsareclosertothelifetimeofthe70% homogeneousaquifermodel,especiallyforlargerwellspacings.
Fig.8.Effectof10%wellspacingreductiononNPVfrom1000to900m,fordifferentbasecasescenarios.Inscenario1–6allotherparametersareequaltothebasecase valuesofFig.6.Tisthedifferencebetweeninjectionandproductiontemperatures.Forcomparison,theeffectof100mwellspacingvariationinthebasecasescenariois presentedontop.
Fig.9.Lifetimefordifferentwellspacinginhomogeneousmodels(blueandblackline)andfaciesrealisations(reddots)utilizinglifetimescenarioofa7.5◦Cproduction temperaturedrop(leftcolumn)ofa1◦Cdrop(rightcolumn).N/Gvariesbetween15and70%inthefaciesrealisations.Thefirstrowrelatesto100m3/hproductionrate,the
secondrowto150m3/hproductionrate.Thehorizontalblackdottedlineindicatestheminimalrequired15yearlifetimeforthefeed-intariffscheme.Theredlineindicates
thelifetimedistributionoflifetimeperwellspacingforthefaciesrealisations.(Forinterpretationofthereferencestocolourinthisfigurelegend,thereaderisreferredto thewebversionofthearticle.)
6.4. ImpactoffluvialfaciesarchitectureonNPV
TheNPVishigherwhenhomogeneousaquifermodelsareused (Fig.10A).ThiscouldbeexplainedbyFig.10B.Thisfigurepresents theratioofproducedheat(Eprod)andpumpenergylosses(Epump)
ineachdoubletscenario.Itshowsthatinthedetailedfacies realisa-tions,pumpenergylossesaresignificantlyhigherwhichdecreases thenetincome.Fig.10Bshowsthatthefluvialfaciesarchitecture
couldsignificantlyinfluencethenetenergyproductionandthereby alsotheNPV.Thisisaresultof therisk offlowpathformation betweenthewells.Thereforenocleartrendisobservedbetween theenergyratioandwellspacinginthefaciesmodels.Incontrast, aslightreductionoftheenergyratioisrecognizedwithincreasing wellspacingforthe70%N/Ghomogeneousmodel.Theenergyratio isapproximately5%lowerfor400mspacingcomparedto1000m spacing.Forthe15%homogeneousmodelthisreductionisnot
rec-Fig.10. (A)NPVrelatedtowellspacing.NPVofdoubletsinfaciesrealisationsareaveragedperwellspacingdistance(reddottedline).(B)Ratiosofproducedenergyover pumpenergylossesafterthefirstyear,associatedto(A).Reddotsindicatetheenergyratioofadoubletinasinglefaciesrealisations.(C)Pumpenergyandheatproduction developmentovertimefor25%N/Ganda(D)45%N/Grealisationwith1000mwellspacingand100m3/hproductionrate.NotethatthesamescaleontheverticalaxesinC
andDwhiletheabsolutepumpenergyvaluesvary.(Forinterpretationofthereferencestocolourinthisfigurelegend,thereaderisreferredtothewebversionofthearticle.)
ognizableinthisfigure.Asimilartrendwouldhavebeenobserved forthedetailedfaciesmodelsifsufficientrealisationswereused. Nevertheless,theeffectofwellspacingonpumpenergylosseswill nothaveasignificantimpactonNPVinthiswellspacerange.Note thattheratiosinFig.10Bapplytoa singlemomentintime as pumpenergyvaluesaretimedependent(Fig.10CandD).Thisis becauseofthetransientpressurestabilisationintheaquiferand becauseofthetemperaturedependentviscosityofthebrineinour simulations.Pumpenergyvariesmoresignificantlyovertimein lowerN/Grealisations(Fig.10C)comparedtohighN/Grealisations (Fig.10D).Heatproductionremainedconstantuntilthermal break-through(Fig.10C).Thevariationinpumpenergylossesandheat productionwere,however,smallandvariedbylessthan0.02MW in20years.
Aconsequenceofreducingthewellspacingisareductionof themaximalpossibleamountofrecoverableheat.Fig.11shows NPVandthemaximumrecoverableenergyinhomogeneousaquifer modelswithaN/Gof15,45and70%assuminglifetimescenario A(Tis7.5◦C),fortwoproductionrates.Thiscomparisonshows thatanincreasingproductionrateincreasesNPVbutdecreasesthe recoverableenergy.Incontrastlargerwellspacingincreasesthe recoverableenergyasitincreaseslifetime.Largerwellspacingis thereforefavourableinlowerN/Gaquifersorindoubletwithhigh productionrates.Theseresultssuggestthatacompromisebetween financialefficiencyandrecoveryefficiencyofadoubletcouldbe obtaineddependingontheexpectedsandstonevolume,required productionrateandrequiredlifetime.Finally,Fig.11confirmsthat reducingwellspacingreductiontoimproveNPVismorerelevant formarginallyeconomicdoubletswithlowproductionrates.Inthe
45%and70%N/Gmodelswith100m3/hproductionrate,an
opti-muminNPVismostclearlyrecognized.NopeakintheNPVcurves isobservedwhenthelifetimeistoolowbecauseofhighproduction rateorlowsandstonevolume.
7. Discussion
7.1. WellspacingreductionandtheadvantageonNPV
OurresultsshowapossibleimprovementoftheNPVof approx-imately15%,whenwellspacingwasreducedfrom1400to1000m. Evenasmallreductionof 100mcouldalready improveNPVby upto4%.Thesensitivityanalysisindicatesthatvariation ofT (Tprod−Tinj)andproductionratehaveamoresignificantimpacton
NPV.However,theseparametersaretoalargeextentdependent on(1)geologicaluncertaintiesand(2)technologicalconstraints. Geologicaluncertainties include aquifer temperatureof several degrees(Bontéetal.,2012)andaquiferproductivity.Alsoall finan-cialparametersareinfluencedbyexternalfactorssuchaseconomy, governmentpolicyandregionalratesofequipmentandtechnology. Wellspacingisoneoftheparametersinouranalysisthatcouldbe designedpriortodrilling.Sofar,wellspacingisprimarilydesigned tocreatesufficientlifetime(e.g.,Motthagyetal.,2011;Daniilidis etal.,2016).Thereforeourstudytakesamorecomprehensivelook attheeffectofwellspacing.Thisbecomesincreasinglyimportant withmorewidespreaddeploymentofgeothermaldoublets.The currentspacingstandardsignificantlylimitsthepossiblenumber ofdoubletsintheWNB(e.g.,MijnlieffandVanWees,2009).Well spacingreductionwouldthereforenotonlyimprovethefinancial
Fig.11.ComparisonofNPV(blueline)andmaximalrecoverableenergy(redline)in(A)the70%N/Gand(B)15%N/Ghomogeneousmodels.OptimisingNPVbydecreasing wellspacingalsolimitspossiblerecoverableheat.NotthechangeinscaleoftheNPVaxisinthetwocolumns.(Forinterpretationofthereferencestocolourinthisfigure legend,thereaderisreferredtothewebversionofthearticle.)
competitivenessofindividualdoubletsbutalsoenhance exploita-tiononaregionalscale.
Furthermore,ourresultsindicatethatwellspacingreduction hasa strongerimpactin doubletswitha lowerproductivityor netenergyproductionrate.ThisisbecausetheNPVresultsfrom a combination of initial investment and the height of the net income.Theseparametersdeterminethestartingpointandslope ofthediscountedcumulativecashflow(Fig.5).Optimisationof NPVbyreducingwellspacingisthereforeofparticularinterestfor marginallyeconomicHSAdoublets.
Our results are based on the assumption that the minimal requiredlifetimeis15years.ThisappliestoHSAdoubletsinthe Netherlands,becausethisisthemaximumdurationoftheDutch feed-intariffscheme.Asaresultthewellspacingforanoptimal NPVisthesmallestwelldistancewithaminimalproduction tem-peraturereductioninthisperiodoftime.Thisisofcourserelatedto aspecificproductionrate.Mostgeothermalsystemshowever,are designedtoproduceforamuchlongertimesuchas30–50years, whichrequiresalargerwellspacing.
TheNPVmodelbyVanWeesetal.(2010)assumesanidealHSA exploitationscenario.ItdoesnotaccuratelyreflectcurrentWNB investmentcostsandNPV.Firstly,thisisaresultofneglectingthe costswhichareassociatedtoyearsofpreparationpriortodrilling andconsultants.Inaddition,oftenunexpectedmaintenanceand workovercostsaddtotheinitialinvestmentsinthefirstyears.HSA exploitationstartedapproximately10yearsagointheWNBand currentlypassesthroughalearningcurve.Therefore,ourestimated investmentcostsapplymoretofutureDutchdoubletsthatareable totakeadvantageoftheexploitationexperienceofthefirstdecade ofHSAexploitation.Furthermore,theNPVisincreasedinthebase casescenarioofthesensitivityanalysis(Fig.5A)becauseofthe rel-ativelyhighporosityandpermeabilityvaluesof28%and1000mD, respectively.In WNBdoubletstheNPV mightbelowerbecause oftheimpactofgeologicalheterogeneityonnetenergy produc-tion(e.g.,Fig.10A).Nevertheless,wellspacingreductionwouldbe especiallyrelevantformoremarginallyeconomicdoubletsaswas showninFig.8.
Inoursimulations,verticalwellsareused.Deviatedwellscould improvetheinjectivityandproductivityincreasingthenetenergy
productionandimproveNPV.Hence,foroptimisationofdoublet design,thepreferredangleofthedeviatedwellshouldbe deter-minedforaspecificaquiferasitdependsonthegeologicalmodel, netsandstonevolumeandaquiferthickness.
7.2. Lifetime
Themainreason forthelargecurrentwellspacingstandard of1000–1500mistoavoidearlycoldwaterbreakthrough. How-ever,ourproductionsimulationsindicatethatthisspacingmight beovercautious.Thelifetimeinourproductionsimulationsvaries between60and100yearsinlifetimescenarioA,and15–35years inlifetimescenarioBbothwith150m3/hproductionrateanda
1000mwellspacing(Fig.9).Thisshowsthatdespiteour conserva-tiveaquiferthicknessof50m,stillaconsiderablelifetimecould beexpected.Mostcurrent WNBdoubletsactuallyhave alarger wellspacing.However,wellspacingoptimisationrequiresabetter understandingoftheuncertaintiesinlifetime.Doubletlifetime issignificantlyaffectedbyfaciesarchitecture(HammandLopez,
2012;Crooijmansetal.,2016).Ourproductionsimulationswith
detailedfaciesarchitecturerealisationsindicatethathomogeneous modelsunderestimatedoubletlifetime.Thisisbecause imperme-ableclaystonebodiesprovidethermalrechargetothecoldwater plumeandflowbafflesincreaseflowpathlengthbetweenthewells. Secondly,homogeneousmodelsoverestimatethenetenergy pro-ductionofthedoublet(Fig.10B)becauseflowbafflesorbarriers coulddecreaseinjectivityorproductivity.Especiallyinlow N/G aquifers,wellsmightintersectdifferentsandstonebodiesthatdo notformflowpathsbetweenthewellswhichincreasestherequired pumpenergylosses.Doubletwellpairswereorientedparallelto thepaleoflow directionandtheorientationofthefluvial sand-stone bodies. Perpendiculardoublet orientation would increase therequiredpumpenergylosses(e.g.,Willemsetal.,2016)and thereforereduceNPV.Inaddition,perpendiculardoublet orienta-tionwouldhaveincreasedlifetimeuncertainty.Thisisaresultof ahigherprobabilitythatimpermeableclaystonebodiesformflow bafflesorbarriers.Flow-barrierscanreducelifetimewhenthey cut-offpermeablepartsoftheaquiferreducingthenetreservoir volumewhiletheflowbafflesincreaselifetimewhentheyincrease flowpathlength(e.g.,Crooijmansetal.,2016).
Ourresultsshowthatastatisticalapproachwithmultiple reali-sationsisrequiredtocaptureuncertaintiesinlifetimeanddoublet capacity.Thelargespreadinlifetime(Fig.9)indicatesthatmore realisationswould berequiredtoaccuratelycapturethis uncer-taintyinlifetimeandcapacityaswereusedinourstudy.Thegoal ofourstudywas,however,toexaminehowfaciesheterogeneities influencethetheoreticaladvantageofwellspacingreductionon NPV.Ourresultssupportthepossibilitytoreducethewell spac-ing,especiallybecausethenetsandstonevolumeinourmodelsis veryconservative.Forexample,noWNBdoubletonlyencounters a15–20%N/Gaquiferof50mthickness.Ingeneral,WNBaquifers havealargerthicknessandhigherN/Gpercentage.Our conserva-tivesandstonevolumesresultsinlowdoubletcapacities(Fig.10B) andthereforelowerNPVcomparedtothebasecasescenario.In reality,doubletswithverylowinjectivityornetsandstone vol-umewouldnotbetakeninproductionwithoutanymeasures(e.g.,
Blöcheretal.,2015).Examplesofsuchameasuresaretocontinue
drillingintoahigherN/Gintervalortoincreaseheatexchange sur-facebyhydraulicstimulation.Ifwewouldcompensateforthis,life timeandNPV inourresultswouldincrease.Thedetailed facies architecturerealisations in this current studyare simplified by neglectingsmallscalepermeabilityheterogeneitiesandassuming isotropicaquiferpropertiesingridblocks.Examplesofsuchsmall scaleheterogeneitiesareshaledrapes,accretionsurfacesand bed-dingplanes(e.g.,Pranteretal.,2007).Thesefeaturesdecreaseon averagethepermeabilityperpendiculartothepaleoflowdirection.
Fig.12.Productiontemperaturedevelopmentovertimefora600mwellspacing andaproductionrateof100m3/h,forallfaciesrealisations(thincolouredlines)and
thetwohomogeneousmodelsasindicatedinthelegend.(Forinterpretationofthe referencestocolourinthisfigurelegend,thereaderisreferredtothewebversion ofthearticle.)
Thiscouldbeaccountedforadjustingthepermeabilityindifferent directionsineachgridblocklikeinBierkensandWeerts(1994). Furthermoreporositywasrandomlydistributedamongstthe sand-stonegridblocks.Inrealitytheporosityofchannellags,point-bars andsandplugsvariesmoresystematicallyacrosssandstonebodies asaresultofsedimentaryprocess(WillisandTang,2010),which couldinfluenceflowpathformationthroughthesandstonebodies
(LarueandHovadik,2008).Theseheterogeneitiescouldfurther
dif-fusethecoldwaterplume.Notethatinoursimulationsflowonly occursthroughtherockmatrixandnofracturesarepresent(e.g.
Hardeboletal.,2015;Bisdometal.,2016).Fractures,especially
par-alleltotheflowbetweenthedoubletscoulddecreasethethermal breakthroughtimeofthecoldwaterplume.
Finally,itcouldbearguedthatnotonlythesandstonevolumes inoursimulationswereconservative,alsotheassumptionsonthe minimalproductiontemperaturecouldbeconsideredassuch.The minimumrequiredproductiontemperatureforeconomic Dutch HSAexploitationforgreenhouseheatingisassumedtobe45◦C and65◦Cfordistrictheatingpurposes(Pluymaekersetal.,2012). Theseminimaltemperaturesarelowerthanthe67.5◦Cinourlife timescenarioAandmuchlowerthanthe74◦CofscenarioB. Fur-thermore,duetolikelytechnologicalimprovementsoninsulation andtechnologicalefficiencyin thenextdecades,lower produc-tiontemperatureswillmostlikelybesufficientinthefuture.Our simulationsshowthatproductiontemperaturereducesby0.5–1◦C peryear,dependingonthenetsandstonevolumeandproduction rate.Thespeedofproductiontemperaturereductioninour simula-tionsisrelativelylowcomparedtopreviousstudies(e.g.,Mijnlieff
and Van Wees, 2009) becausethermal rechargefrom over and
underburdenistakenintoaccount(Poulsenetal.,2015).InFig.12
theproductiontemperaturedevelopmentover timein homoge-neousaquifermodelsanddetailedaquiferarchitecturemodelsare compared asanexample. Doubletsin thesesimulationshave a 600mwellspacingand100m3/hproductionrate.In thelowest
N/Gaquiferrealisation,theproductiontemperaturedropsbelow 60◦Cafter60years.InthehighestN/Grealisationthisproduction temperatureisreachedafterapproximately140years.Therefore,
Fig.12underlinesconservativenatureofourminimaltemperature assumptions.
8. Conclusion
Thispaperpresentsamodellingbasedstudyontheadvantages andimpactsofawellspacingreductioninHSAdoublets.Firstly,our resultsindicatethatareductionof400mwellspacingcouldlead toaNPVimprovementofupto15%.Theimpactofwellspacing reductiononNPVismoresignificantinmarginallyeconomic dou-blets.Secondly,productionsimulationswithdetailedfaciesaquifer architecturederivedfromWNBgeologicaldataareusedto eval-uatetheimpactofsmallerwellspacingonlifetime.Ourresults suggestthatsufficientlifetimecouldbeobtained,ifthewell spac-ingis reduced belowthecurrent 1000–1500mstandard. These current standards aim toavoid early cold water breakthrough. However,ourresultsshowpotentialoverdesignofthesestandards. Thisresultsinthenegativeeffectofdecreasingthefinancial com-petitivenessofgeothermalexploitationandreducingthepossible numberofdoubletsinaregion.Finally,thecomparisonof produc-tionsimulationswithdetailedfaciesarchitecturerealisationsand homogeneousmodelsshowsthathomogeneousmodels underesti-matetheuncertaintyinlifetimeanddoubletcapacity.Theaquifer heterogeneitieshaveasignificanteffectontheflowpathformation betweenthewells.Therefore,astatisticalapproachwithmultiple realisationisrequiredtoaccuratelyassessHSApotentialandto optimiseexploitationefficiency.
Acknowledgements
WethankIsabelleCojanandherteam(MinesParisTech,Paris, France)forthepermissiontousetheFlumyprocess-basedfacies modelling software. Harmen Mijnlieff (TNO Geological Survey oftheNetherlands)is thankedfor thediscussionsand support. GeothermaloperatorsintheNetherlandsarethankedforsharing theirgeologicalandproductiondata.Wekindlythankthe consor-tiumofshare-andstakeholdersoftheDelftGeothermalProject (DAP)fortheirsupport.WethanktheEditorandtheanonymous reviewerfortheirconstructivereviewsandfeedbackthat signifi-cantlyimprovedtheinitialmanuscript.
References
Adams,B.M.,PhDthesis2015.OnthePowerPerformanceandIntegrationof Carbon-dioxidePlumeGeothermal(CPG)ElectricalEnergyProduction. UniversityofMinnesota.
Bailey,W.R.,Manzocchi,T.,Walsh,J.J.,Keogh,K.,Hodgetts,D.,Rippon,J.,Nell, P.A.R.,Flint,S.,Strand,J.A.,2002.Theeffectoffaultsonthe3Dconnectivityof aquiferbodies:acasestudyfromtheEastPennineCoalfield,UK.Petrol.Geosci. 8,263–277.
Bierkens,M.F.P.,Weerts,H.J.T.,1994.Blockhydraulicconductivityofcross-bedded fluvialsediments.WaterResour.Res.30(10),2665–2678.
Bisdom,K.,Bertotti,G.,Nick,H.M.,2016.Theimpactofin-situstressand outcrop-basedfracturegeometryonhydraulicapertureandupscaled permeabilityinfracturedreservoirs.Tectonophysics690,63–75.
Blöcher,G.,Reinsch,T.,Henninges,J.,Milsch,H.,Regenspurg,S.,Kummerow,J., Francke,H.,Kranz,S.,Saadat,A.,Zimmerman,G.,Huenges,E.,2015.Hydrolic historyandcurrentstateofthedeepgeothermalaquiferGroßSchönebeck. Geothermics63,27–43.
Bonté,D.,VanWees,J.D.,Verweij,J.M.,2012.Subsurfacetemperatureofthe onshoreNetherlands:newtemperaturedatasetandmodelling.Neth.J.Geosci. 91(4),491–515.
Boxem,T.A.P.,VanWees,J.D.,Pluymaekers,M.P.D.,Beekman,F.,Batini,F.,Bruhn, D.,Calcagno,P.,Manzella,A.,Schellschmidt,R.,2011.ThermoGISWorld AquiferViewer–aninteractivegeothermalaquiferresourceassessment web-tool.In:1stEAGESustainableEarthSciences(SES)Conferenceand Exhibition2011,Valencia,Spain.
Bridge,J.,2006.Fluvialfaciesmodels:recentdevelopments.In:Posamentier,H., Walker,R.(Eds.),FaciesModelsRevised,vol.84.SEPMSpecialPublication,pp. 85–170.
Cojan,I.,Fouche,O.,Lopez,S.,2004.Process-basedaquifermodellinginthe examplemeanderingchannel.In:Leuangthong,O.,Deutsch,C.(Eds.), GeostatisticsBanff2004.Springer,Dordrecht,pp.611–619.
Crooijmans,R.A.,Willems,C.J.L.,Nick,H.M.,Bruhn,D.F.,2016.Theinfluenceof faciesheterogeneityonthedoubletperformanceinlow-enthalpygeothermal sedimentaryreservoirs.Geothermics64,209–219.
Daniilidis,A.,Doddema,L.,Herber,R.,2016.RiskassessmentoftheGroningen geothermalpotential:fromseismictoreservoiruncertaintyusingadiscrete parameteranalysis.Geothermics64,271–288.
DeVault,B.,Jeremiah,J.,2002.TectonostratigraphyoftheNieuwerkerkFormation (DelflandSubgroup),WestNetherlandsBasin.AAPGBull.8(10),1679–1707.
Donselaar,M.E.,Groenenberg,R.M.,Gilding,D.T.,2015.Reservoirgeologyand geothermalpotentialoftheDelftSandstoneMemberintheWestNetherlands Basin.In:ProceedingsWorldGeothermalCongress2015,Melbourne,Australia.
Ekneligoda,T.C.,Min,K.B.,2014.Determinationofoptimumparametersofdoublet systeminahorizontallyfracturedgeothermalaquifer.Renew.Energy65, 152–160.
EuropeanCommission,2016.Communicationfromthecommissiontothe EuropeanParliament,thecouncil,theEuropeaneconomicandsocial committeeandthecommitteeoftheregions.AnEUStrategyonHeatingand Cooling.
Grappe,B.,Cojan,I.,Flipo,N.,Rivoirard,J.,Vilmin,L.,2012.Developmentsin dynamicmodellingofMeanderingFluvialSystems.AAPG2012Congress.
Hamm,V.,Lopez,S.,2012.Impactoffluvialsedimentaryheterogeneitiesonheat transferataGeothermalDoubletScale.In:37thStanfordGeothermal Workshop,Stanford,UnitedStates.
Hardebol,N.J.,Maier,C.,Nick,H.M.,Geiger,S.,Bertotti,G.,Boro,H.,2015.The impactofin-situstressandoutcrop-basedfracturegeometryonhydraulic apertureandupscaledpermeabilityinfracturedreservoirs.J.Geophys.Res.: SolidEarth120,8197–8222.
Jeremiah,J.M.,Duxbury,S.,Rawson,P.,2010.LowerCretaceousofthesouthern NorthSeaBasins:reservoirdistributionwithinasequencestratigraphic framework.Neth.J.Geosci.89(2010),203–237.
Kramers,L.,VanWees,J.D.,Pluymaekers,M.P.D.,Kronimus,A.,Boxem,T.,2012.
Directheatresourceassessmentandsubsurfaceinformationsystemsfor geothermalaquifers;theDutchperspective.Neth.J.Geosci.91(4),637–649.
Larue,D.K.,Hovadik,J.M.,2006.Connectivityofchannelizedaquifers:amodelling approach.Petrol.Geol.12,291–308.
Larue,D.K.,Hovadik,J.M.,2008.Whyisaquiferarchitectureaninsignificant uncertaintyinmanyappraisalanddevelopmentstudiesofclasticchannelized aquifers?J.Petrol.Geol.31(4),337–366.
Lingen,P.,2014.LIR-GT-01–LIR-GT-02InterferenceAnalysis,Unpublished manuscriptbyPanterraGeoconsultantsBV.
Lopez,S.,Cojan,I.,Rivoirard,J.,Galli,A.,2009.Process-basedstochasticmodelling: meanderingchannelizedaquifers.AnalogueNumerModelSedimentSyst: FromUnderstandPredict(SpecialPubl.40oftheIAS),40.
Lopez,S.,Hamm,H.,LeBrun,M.,Schaper,L.,Boissier,Cotiche,C.,Gioglaris,E., 2010.40yearsofDoggeraquifermanagementinIle-de-France,ParisBasin, France.Geothermics39(4),339–356.
Nielson,D.L.,Garg,S.K.,2016.Slimholeaquifercharacterizationforriskreduction. In:Proceedings,41stWorkshoponGeothermalAquiferEngineering,Stanford, California.
Mijnlieff,H.,VanWees,J.D.,2009.RapportageRuimtelijkeOrdeningGeothermie. In:TNOReport.
Mottaghy,D.,Pechig,R.,Vogt,C.,2011.ThegeothermalprojectDenHaag:3D numericalmodelsfortemperaturepredictionandaquifersimulation. Geothermics40,199–210.
Pluymaekers,M.P.D.,Kramers,L.,vanWees,J.D.,Kronimus,A.,Nelskamp,S., Boxem,T.,Bonté,D.,2012.Aquifercharacterisationofaquifersfordirectheat production:methodologyandscreeningofthepotentialaquifersforthe Netherlands.Neth.J.Geosci.91(4),621–636.
Poulsen,S.,Balling,N.,Nielsen,S.,2015.Aparametricstudyofthethermal rechargeoflowenthalpygeothermalreservoirs.Geothermics53,464–478.
Pranter,M.J.,Ellison,A.I.,Cole,R.D.,Patterson,P.E.,2007.Analysisandmodellingof intermediate-scalereservoirheterogeneitybasedonafluvialpoint-bar outcropanalogue,WilliamsForkFormation,PiceanceBasin,Colorado.AAPG Bull.91(7),1025–1051.
Pranter,M.J.,Sommer,N.K.,2011.Staticconnectivityoffluvialsandstonesina lowercoastal-plainsetting:anexamplefromtheUpperCretaceouslower WilliamsForkFormation,PiceanceBasin,Colorado.AAPGBull.95(6),899–923.
Saeid,S.,Al-Khoury,R.,Nick,H.M.,Barends,F.,2014.Experimental–numerical studyofheatflowindeeplow-enthalpygeothermalconditions.Renew. Energy62,716–730.
Saeid,S.,Al-Khoury,R.,Nick,H.M.,Hicks,M.A.,2015.Aprototypedesignmodelfor deeplow-enthalpyhydrothermalsystems.Renew.Energy77,408–422.
Sauty,J.P.,Gringarten,A.C.,Landel,P.A.,Menjoz,A.,1980.Lifetimeoptimizationof lowenthalpygeothermaldoublets.In:AdvancesinEuropeanGeothermal Research.Springer,pp.706–719.
Shengjun,Z.,Huaixin,W.,Tao,G.,2011.Performancecomparisonandparametric optimizationofsubcriticalOrganicRankineCycle(ORC)andtranscritical powercyclesystemforlow-temperaturegeothermalpowergeneration.Appl. Energy88,2740–2754.
TNO,1977.Nlolie-engasportaal.www.nlog.nl.
Törnqvist,T.E.,Bridge,J.S.,2002.Spatialvariationofoverbankaggradationrateand itsinfluenceonavulsionfrequency.Sedimentology49,891–905.
VanHeekeren,E.V.,Bakema,G.,2013.GeothermalEnergyUse.2013Country UpdatefortheNetherlands.In:EuropeanGeothermalCongress2013,Pisa, Italy.
VanHeekeren,V.,Bakema,G.,2015.TheNetherlandsCountryupdateon geothermalenergy.In:WorldGeothermalCongress2015,Melbourne.
VanWees,J.D.A.M.,Kramers,I.,Kronimus,R.A.,Pluymaekers,M.P.D.,Mijnlieff,H.F., Vis,G.J.,2010.ThermoGisV1.0.PartII:Methodology.TNOReport.
Willems,C.J.L.,Goense,T.,Nick,H.M.,Bruhn,D.F.,2016.Therelationbetweenwell spacingandNetPresentValueinfluvialHotSedimentaryAquifergeothermal doublets;aWestNetherlandsBasincasestudy.In:41stWorkshopon GeothermalAquiferEngineeringStanfordUniversity2016,Stanford,California.
Willems,C.J.L.,Nick,H.M.,Donselaar,M.E.,Weltje,G.J.,Bruhn,D.F.,2017.Onthe connectivityanisotropyinfluvialHotSedimentaryAquifersanditsinfluence ongeothermaldoubletperformance.Geothermics65,222–233.
Williams,G.P.,1986.Rivermeandersandchannelsize.J.Hydrol.88,147–164.
Willis,B.J.,Tang,H.,2010.Three-dimensionalconnectivityofpoint-bardeposits.J. Sedimen.Res.80(5),440–454.