1 StaticandseismicdesignofDryStoneRetainingWalls(DSRWs)followingEurocode1 standards2 NathanaëlSAVALLE1,2a*,ChristineMONCHAL3b,EricVINCENS4c,StenFORCIOLI3dandPauloB.LOURENÇO1e 3 1UniversityofMinho,ISISE,DepartmentofCivilEngineering,Guimarães,Portugal4 2UniversitéClermontAuvergne,ClermontAuvergneINP,CNRS,InstitutPascal,F‐63000Clermont–Ferrand,5 France6 3Géolithe–Grenoble:181ruedesBécasses38920Crolleshttp://www.geolithe.fr/ingenieurs‐conseils/7 4EcoleCentraleLyon–LTDSUMR5513:36AvenueGuydeCollongue69134EcullyCedex8 a[email protected],*correspondingauthor9 b[email protected]10 ceric.vincens@ec‐lyon.fr11 d
[email protected]12 e[email protected]13 Abstract14 DryStoneRetainingWallsarestructuresmadeofrubblestonesassembledwithoutmortarandhavebeen15 presentworldwideforcenturies.Today,theystillconstituteanattractivealternativetobuildingtechniques16 involvinghigherembodiedenergy,suchasreinforcedconcretewalls.Thisstudyusesapseudo‐staticapproach17 togivedesignrecommendationstomaintainthisbuiltheritageandallowitsmodernconstruction.Bothnon‐18 seismic(Eurocode7)andseismic(Eurocode8)casesareaddressed.Thepresentworkconfirmsthataseismic19 designisnotcriticalandisthereforenotrequiredforzoneswithadesignaccelerationbelow0.05g.Inaddition,20 thisworkhighlightsthesignificantpositiveeffectofthestonebedinclinationandtheinternalwallfacebatter.21 Finally,dependingonthewallsiteconditionsandtheseismiczoneassociatedwiththeproject,generaldesign22 recommendationsaregiventooptimisethevolumeofstonesused,whichareillustratedinthecaseofFrance.23 Theserecommendationsbasedonpseudo‐staticanalysesarealreadyusableinpracticeforlowtomoderate24 seismicareasastherequiredretainingwalldimensionscanbeeasilyimplementedon‐site.Inaddition,itisalso25 shownthattheactualFrenchrecommendationsforthesewallsfullycomplywithEurocode7.26 Keywords27 Masonry,Drystone,Retainingwalls,Pseudo‐static,Earthquakes,Coulomb'swedge,Standards28
2 Introduction29 Drystonestructureshavebeenbuiltinmostregionsoftheworld,sometimesshapingtypicalandvaluable30 landscapes.Thesevernacularstructuresaremadeofrubblestonescarefullyassembledbyhandandwithout31 mortar.DryStoneRetainingWalls(DSRWs)arelikelytoconstitutethemostrepresentativepartofthisbuilt32 heritage,allowingagriculturalactivitiesonterracesandtrafficonruralroadsinmountainousorslopedareas.33 Therefore,DSRWsplayanessentialeconomicroleintheseregionsthatbenefitlessfromglobalisationand34 major investments. Inaddition, they alsohold a highcultural value, sometimes labelledby UNESCO(e.g.,35 Douro's Valley in Portugal or the Lavaux's Terraces in Switzerland). In fact, the art of dry stone walling,36 knowledgeandtechniquesweredesignatedasIntangibleCulturalHeritageofHumanitybyUNESCOin2018.37 However,thesestructureshaveoftenfacedalackofmaintenanceinrecentdecadesandrequireurgentrepair.38 GiventheneedtopreserveandrepairoldDSRWs,severalresearchstudieshavebeenconductedmainlyin39 Europe.Experimentalworks[1]–[3],analytical[4]–[7]andnumericalstudies[8]–[15]focusedonthestatic40 mechanicalbehaviourof2DslopedDSRWs,whileotherstudiesinvestigatedthe3Dmechanicalbehaviourof41 thesewallsincaseofaconcentratedtrafficload[16]–[19].InFrance,theseresearchesledtotwopractical42 handbooksthatincludedesignrulesforDSRWsretainingslopes.Thesearevalidforanycountrywithsimilar43 buildingtechniques,whichcanbefoundworldwide[20],[21].However,eventhoughtherecommendations44 areusedinpracticeandrecognisedbythedrystonemasonryandcivilengineeringcommunities,theydonot45 considerseismicaction.OnlyafewstudycaseshavebeeninvestigatedaccordingtothepastFrenchseismic46 recommendations[22],[23].Moreover,thevalidationoftherecommendationsaccordingtoEurocode7[24]–47 [26]hasnotbeeninvestigatedexhaustively,evenifpartlyconsideredinthelatestDSRWsFrenchhandbook48 [21].49 ToaddresstheseismicdesignofDSRWsinslopes,theauthorsdevelopedapseudo‐staticanalyticaltoolbased50 onCoulomb'swedgetheory,whichwasvalidatedbypseudo‐staticscaled‐downlaboratoryexperiments[27].51 Thefirstsectionofthispaperrevisedtheanalyticalmethod,whilethesecondsectionprovidesacomparison52
3 withthecurrentstandardsongeotechnicalengineeringandseismicengineering,respectively,Eurocode7&853 [24]–[26],[28],[29].Finally,followingtheEurocodes,recommendationsaregivenfordesigningDSRWsinareas54 rangingfromverylowtohighseismicity.55 Analyticalmethod 56 Theanalyticalmethodreliesonthelimit‐equilibriumtheoryunderplanestrainconditions(Figure1).TheDRSW57 ischaracterisedbyaheightH,abasewidthB,anexternalslopetotheverticalof v andaninternalslopetothe58 verticalof m .Thebedinclinationofthewallisreferredtoas andthebackfillslopeas .Contrarytothestatic59 limit‐equilibrium approach of Villemus [30], the analytical method includes seismic forces modelled as60 equivalenthorizontalpseudo‐staticactions.Briefly,thepseudo‐staticequilibriumofaCoulomb'swedgeofsoil61 isfirstcomputedtoobtainthepseudo‐staticactiveearthpressure[31]–[33].Thewall'sequilibriumisthen62 computed,statingthepossibletypesoffailure:aninternalslidingortopplingmode[34].63 64 Figure1:DSRWwithitsgeometricparameterisationa):actualbackfill‐wallsystem;b):modelledbackfill‐wallsystem.Thepresentsignconvention65 makestheinternalbatter(λ m )negative.66 Figure2describesthebackfill‐wallsystem,withallgeometricalandmechanicalparametersclarified.Thewall67 ischaracterisedbyahomogeneousmedium(Figure1)withitshomogeneousunitweight γ rw (accountingfor68 voidsbetweenstones) and jointfrictionalangle φ rw .Similarly,the backfillismodelledas a homogeneous69 medium described by its unit weight γ f , cohesion C f andfrictionangle φ f . Compared to other retaining70
4 structures,theparticularityofDSRWsliesinafailurelinedevelopingthroughthedryjoints,whichismodelled71 asanequivalentstraightfailurelinewithaninclination ω (Figure1).Inpractice,theinclinationofthisfailure72 linefromthebedjointsislimitedbyamaximumvalueof20°,see[27].Thisinclinationisalsodifferentfrom73 thehomogenisedinclination θ ofthefailurelinecrossingthebackfill,whichmainlydependsonmaterial(soil74 frictionandcohesion),geometrical(slopeofthebackfill)andseismic(pseudo‐staticaccelerations)parameters,75 asexplainedbelow.76 Themechanicalsystemhasthreeunknowns( θ , ω andhg)thatshouldbedeterminedtocomputetheearth77 pressure F δ .AccordingtotheCoulombsoil'swedgetheory,foreachcombinationoftheseparameters,thelimit78 equilibriumofthesoil'swedge D1D2D3canbecalculated(Figure2b‐c)toevaluatetheactiveearthpressureF δ . 79 Inparticular,theweightPfofthesoilisproportionaltothewedgearea(triangleD1D2D3)andisappliedatthe80 gravity centre of the triangle D1D2D3.Similarly,thepseudo‐staticaction(inertialforceduetothe seismic81 motion)Ffisalsoproportionaltothewedgeareaandappliedatitsgravitycentre.Thebackfillfrictionalreaction82 Rφapplicationpointandintensityareunknown,butitsorientationisgivenbythebackfillfrictionangle φ fsince83 thelimit‐equilibriumisassumed.Similarly,theorientation,yetnottheapplicationpoint,ofthebackfillcohesive84 reactionRCisknown.Regardingthebackfill‐wallinterface,theinterfacecohesivereactionRCinthasanunknown85 point of application and a known orientation. The intensities of the cohesive forces (RC and RCint) are86 proportionaltothecohesivestrengthandthelengthoftheinterface(D1D3andD1D2).Hereafter,theinterface87 cohesive strength (RCint) always equals zero, as the drain directly behind a DSRW is usually made of dry88 cohesivelessgravel.89 Finally,theearthpressureFδhasaknownorientation δ (internalfaceofthewall)andapplicationpointbut90 unknownintensity.Theintensityisdeducedfromthemechanicalequilibriumofthesoil’swedge(Figure2c).In91 theabsenceofpseudo‐staticactionFfandcohesiveresistance,theapplicationpointoftheearthpressureis92 located at one‐third of the height of the retaining structure. Then, adding cohesive effects decrease the93
5 applicationpointheightwhileaddingapseudo‐staticactionincreasesitsheight.Thereadercanrefertothe94 literaturefordeeperinsightsintothelocationoftheapplicationpointofearthpressureinthiscase[34]–[36].95 Theanalyticalmethodalsoaccountsforthetensilecracksthatclassicallyoccuratthetopofcohesivebackfill96 andreducethecohesiveforces(R C andR Cint ).Inaddition,inthepresentwork,thepresenceofdeadloadson97 topofthebackfillandsaturatedretainedbackfill[34]canbeaccountedfor,yetnotdescribedhereforbrevity.98 99 Figure2:Parametrisationofthemechanicalsystemandgeometricalequilibriumofthesoil’swedgeinordertocomputetheearthpressureF δ. 34 100 Inasecondstageofthecalculation,theequilibriumofthewallitselfiscomputed(Figure3)includingitsown101 weightandthepseudo‐statichorizontalaction,appliedatthecentreofgravityofthestudiedportionofwall102 A 2 A 3 D 1 E,correspondingtothepartabovethefailurelineD 1 E.TheinterfaceactionsF δ andR Cint (aswellastheir103 line of actions) are derived from the previous stage of calculation. Subsequently, the wall equilibrium is104 computedintheXandYdirectionstoevaluatethebasereactionR b .Theequilibriumintermsofmomentum105 givestheapplicationpointofR b .Finally,thestabilityofwallportionA 2 A 3 D 1 Eiscomputedconsideringatoppling106 modeoffailure(e.g.applicationpointinsidethewall,i.e.l b >0,oranyothercriteriadefinedinthefollowing107 sections)oraslidingmodeoffailure.Forthislastpoint,thebasereactionR b isprojectedontheplanedefined108 bytheorientationofthebedjoints(axesX s andY s inFigure3),andthenMohr‐Coulombcriterionischecked.109
6 Notethatthebedjoints'orientationisupdatedbecauseofthepossibleinternalrotationofstonesinsideDSRWs110 (see[34]formoredetails).Finally,theunknownsofthesystem( θ , ω andh g )areoptimisedforeachfailure111 modetofindthemostcriticalsituationforthecriterionchecked.SeveraliterationsinvolvingthebasewidthB112 ofthewallallowstoidentifytheminimumBvaluethatbarelysatisfiesthestabilitycriteria.113 114 Figure3:Equilibriumofthedrystoneretainingwall[34]115 Themethodhasbeenvalidatedonscaledpseudo‐staticexperimentsonatiltingtable,usingdryjointbrick116 retainingwallsretainingasandybackfill[27].Figure4givestheresults,showingthatthedevelopedpseudo‐117 staticapproachisaspreciseasmoresophisticatedDiscreteElementModelling(DEM)simulations[37].118 119 Figure4:ComparisonofDEMsimulation,analyticalsimulationandexperimentaltiltingtests[37]120
7 Asadditionalvalidation,theanalyticalmethodwasusedtomodeltwosetsofexperimentalcampaignscarried121 outonfull‐scaleDSRWswith1)ahydrostaticload[1];2)adrybackfillload,asdisplayedinFigure5[2],[3].122 Table1describesthegeometricandmechanicalparametersoftheexperiments,alongwiththeanalytical123 results,whichareinexcellentagreementforbothcampaigns.Moreover,thedevelopedanalyticalapproach124 providesasimilarlevelofaccuracytotheresultsofVillemusetal.[1]andColasetal.[6],[38].125 126 Figure5:ExperimentaltopplingfailureobtainedbyColas[39]127 Table1:Parametersofthefull‐scaleDSRWsexperimentalcampaignsfrom[1]–[3].Experimentalandanalyticalresultsarealsogiven.128 Name* V1l V2l V3l V4l V5s C1g† C2s C3s C4l Geometricalparameters HeightH(m) 2 1.95 4 2 4.25 2.5 2.5 2.5 2.5 BasewidthB(m) 0.9 0.91 1.8 0.9 1.8 0.6 0.6 0.7 0.65 Externalbatterλ v (%) 15 0 15 12 15 6 6 6 6 Bedsinclinationα(°) 0 0 0 4 8.5 3.4 3.4 9.1 9.1 Backfillslopeβ(°) NA NA NA NA NA 26.4 31.7 32.6 34.9 Mechanicalparameters Wallweight(kN/m 3 ) 15.4 14.9 15.7 15.7 18.0 21.0 20.0 20.0 21.8 Stonefriction(°) 36 36 36 36 28.5 27 25 25 35 Internalrotation(°)‡ 5 5 5 5 5 5 5 5 5 Soil weight γ r (kN/m 3 ) NA NA NA NA NA 14.9 14.9 14.9 14.9 Soilfrictionϕ r (°) NA NA NA NA NA 37.7 37.7 37.7 37.7 Experimentalresults Criticalheight(m) 1.74 1.9 3.37 1.94 3.62 >2.1 7 2.41 2.96 2.95 Failuremode(S/T) S S/T S S/T S NA S/T T T Analyticalresults Criticalheight(m) 1.73 1.84 3.48 1.86 3.68 2.86 2.69 3.02 2.82 Failuremode(S/T)§ S S/T S S/T S T S/T T T
8 Differencetoexp. ‐1% ‐3% +3%‐4%+2%NA+11 %+2%‐4% *VreferstoVillemus[1]withhydrostaticloadingandCtoColas[2],[3]withbackfill loading,whilelreferstolimestoneblocks,stoschistblocksandgtograniteblocks. †Thisexperimentfailed.However,thewallresistedatleastaloadingcorrespondingtoa backfillheightof2.17m. ‡Thisinformaonisbasedonexperimentalresults,usingadefaultvalue.Detailscanbe foundin[1]–[3]fortheexperimentsandin[34],[40]fortheanalyticalmethod. §Acombinedsliding‐overturningfailurehasbeendefinedifthecriticaltheoreticalheights ofthetwofailuremodeswerewithinarangeof±5%. DesignofDSRWsfollowingEurocodes129 ThepresentsectionaimsatdesigningDSRWsusingtheanalyticalmethodandthepartialsafetyfactors(actions,130 materialpropertiesandresistance)fromEurocode7and8[24]–[26],[28].First,itisemphasisedthatina131 seismiccontext,apseudo‐staticmethod(liketheonepresentedabove)willneveraccuratelypredictthetrue132 timeevolutionofthedynamicresponseorresistanceofarealDSRWduringanearthquake.Therefore,itisonly133 usedasasimplifieddesignmethodproposedbyEurocode8togivefastseismicassessmentofretainingwalls.134 Nopartialsafetyfactorrelatedtothemethodisconsideredsincenoconstantbiashasbeenfoundinthe135 validationprocessesbetweentheoreticalandexperimentalresults.Moreover,onlythewall'sinternalsliding136 andtopplingfailuresareconsidered:thebearingcapacityofthefoundationsoilatultimateorserviceability137 limitstatesareassumednottobereached.Similarly,thepassivesoilisconsideredinfinitelyrigid,whichis138 reasonable according to Alejano et al. [5]. Finally, liquefaction and the failure of the entire soil slopeare139 disregarded.Table2presentsthesafetyfactorsusedforthecomputationsaswellasthosefromtheFrench140 professionalrules,whicharesimilar[21].141 Regarding non‐seismic verifications, the Ultimate Limit State Equilibrium (ULS EQU), the142 Structural/Geotechnical Ultimate Limit State with the second approach (ULS STR/GEO), see [41], and the143 ServiceabilityLimitState(SLS)areexamined.TheUltimateLimitState(ULSSEISM)isappliedfortheseismic144 verification.145
9 Table2:Partialsafetyfactorsfornon‐seismicandseismicsafetyverifications;AnnexAoftheEurocode7[24]andENTPE(Eds.)etal.[21].146 Eurocode7[24] French professional rules[21] ULS SLS EQU STR/GEO SEISM Safetyfactorsforactions Favourableweightactionsfactor(γG,fav) 0.9 1 1 1 1 Unfavourableweightactionsfactor(γG, unfav) 1.1 1.35 1 1 1.35 Safetyfactorsformaterialproperties Drainedsoilfrictionanglefactor(γφ') 1.25 1 1.25 1 1 Drainedsoilcohesionfactor(γC') 1.25 1 1.25 1 1.25 Safetyfactorsforresistances Slidingfactor(γR,h) 1 1.1 1 NA 1 Topplingfactor(γR,v) 1NA1NA1 Eccentricityfactor(1–2e/B) NA 1/15 NA 1/2 1 Modelresistantfactor(γR,d) 1 1 1 1 1.2 147 ForthetopplingverificationoftheSLSandtheULSSTR/GEO,thedesigncriteriontosatisfycorrespondstothe148 maximumeccentricity(notede)ofthetransmittedloadthroughthewall,asstatedinEurocode7[25],[26].In149 thecontextoftheULSEQUandSEISMverifications,thepartialsafetyfactorsγm(γφ'andγC')forthematerials150 areonlyappliedtothebackfillsoilpropertiesandnottothefrictionbetweenblocks(asmentionedin[41]–151 [43].Thefrictionbetweenblocksislinkedtothewallresistance,thustotheresistancesafetyfactorγR.Asa152 consequence,applyingasafetyfactorfortheblockmaterial(block‐blockfriction)wouldpenalisetwicethe153 sameparameters,whichisnotinagreementwiththeframeworkofEurocodes. Moreover,intheseismic154 verification(ULSSEISM),thesafetyfactorsformaterialsarelinkedtothedegradationoftheshearstrengthof155 soilsathighstrainand/orinthepresenceofporepressures.Theseareunlikelytooccurfordryblock‐block156 joints[42]–[44].157 Non‐seismiccase158 Computations discarding the seismic action are carried out on five walls, whose main characteristics are159 presentedinTable3.ThewallsarebuiltofstoneswithgeologicalnaturesrepresentativeofEuropeanand,in160 particularFrench,geology(molasseormarlsandstone,schist,limestoneandgranite).Theyincludetypical161
16 accelerations larger than 0.25g, due to the inherent approximations of the pseudo‐static approach, the249 maximumextra‐widthsexceed100%ofthenon‐seismicdesignwhichseemsnonreasonableinpractice.For250 thesecases,thepseudo‐staticmodellingapproachmayalsobeinadequate,giventheweakconsiderationof251 dynamicsandthefactthatwalldisintegrationisignored.252 Table4:Maximumextra‐widthsforDSRWsrequiredbyapseudo‐staticseismicdesigncomparedtoanon‐seismicdesigndependingonthereference253 acceleration(a gR ).TheanalysisonlycoversDSRWsbelongingtothenormalclassofimportance(γ I ≤1.0).Accordingtotheseismichazardmapof254 Europeancountries,thesecondcolumngivesthecorrespondingregionsofeachreferenceacceleration.ThereaderisreferredtoFigure7andFigure255 8.256 In257 conclusion,thesystematicuseofastonebedinclinationαisrecommended.Wheneverpossible,anexternal258 batterequaltothestonebedinclinationtofacilitatetheconstructionprocessisalsosuggested.Forlowto259 mediumseismicregions(agR<0.11g),astonebedinclinationαof10%issuitable,whereas,forlargerseismic260 hazards(agR≅0.16‐0.2g),avalueof20%canhelptoreducetherequiredextra‐widthssignificantly.261 Frenchcasestudy262 ThissectionprovidesamoredetailedcasestudyforFrance,chosenasanillustratingexampleoflowtomedium263 seismicityEuropeancountries.Thesectionhelpstounderstandthetrendsandpracticalseismicdesignfor264 DSRWs,dependingonthreedifferentbuttypicalcasesforthebackfill‐wallcondition.Thefirstcase(MAX)265 correspondsto thepreviousEuropean study, i.e., large amplificationforthesoil(S=1.8)andastandard266 construction(importancefactorγI=1.0).Thesecond(ROCK)representsthemostcriticalcasewhentheDSRW267 isdirectlyfoundedonthebedrock(S=1.0),consideredareferencecaseforfoundationconditions.Thelastone268 (RURAL)correspondstowallsoflessimportance(γI=0.8),builtfarfromanyroadorbuilding.Inpractice,269
17 accordingtotheFrenchregulations,thesespecificcases(RURAL)arenotsubjectedtoseismicregulations.270 However,thisworkgivesreferencevalues,whicharehelpfulfor DSRWs stakeholders. These three271 configurationsareanalysedaccordingtothefourseismiczonesofmetropolitanFrance(agR=0.04,0.07,0.11272 and0.16g),leadingtoatotalof12casestudies(Table5).273 Table5:Horizontalseismicdesignaccelerations𝑎fordifferentcriticalcases(asaproportionof 𝑔 9.81𝑚. 𝑠).Theverticalaccelerationavis274 systematicallytakenequalto0.5*ah.275 a gR MAX RURAL ROCK Formulasusedtocomputeah ‐ ah,max=agR*1.20 ah,rural=agR*0.96 ah,rock=agR*0.67 VeryLowSeismiczone(S1) 0.04g 0.05g 0.04g 0.03g LowSeismiczone(S2) 0.07g 0.09g 0.07g 0.05g ModerateSeismiczone(S3) 0.11g 0.13g 0.11g 0.07g MeanSeismiczone(S4) 0.16g 0.20g 0.16g 0.11g 276 Table6sumsupthemaximum(andmean)extra‐widths(amongthedifferentwallsandstonestype)obtained277 foreachseismicsituationdependingonthestonebedinclinations.InseismiczonesS1toS3,onecanagain278 notethatbedinclinationαdramaticallyimpactstheresults;however,abedinclinationof20%doesnotprovide279 asignificantincreaseinresistancecomparedwithaninclinationof10%(seealsoFigure8b‐c).Therefore,as280 usualintheSouthofFrance,aninclinationofthestonebedof10%isrecommended:seismicdesignrequires281 nomorethan40%extra‐width(comparedtoanon‐seismicdesign).InseismiczoneS4,wallsbuiltwithastone282 bed inclination of 10% require an extra‐width of 90%, which induces substantial extra costs for the wall283 construction.Inthiscase,one shouldeitheruse a steeperbedinclinationorconductaspecific analytical284 computationtooptimisethegeometryoftheDSRW.However,ifthewallisbuiltfarawayfromroadsand285 buildings(RURAL)andwithaninclinationbedof10%,themaximumexpectedextra‐widthonlyreaches50%.286 Onthecontrary,ifthewallisdirectlyfoundedonthebedrock(ROCK),theseismicrequiredextra‐widthdrops287 toamaximumof30%.Ifbothconditionsarefulfilled(RURAL&ROCK),therequiredextra‐widthsdonotexceed288 20%(casenotaddressedinTable6).Finally,thegeneralrecommendationsofTable6(maximumvalues)can289
18 be readily used for practical non‐seismic and seismic design of DSRWs without requiring more detailed290 computations.291 Table6:Influenceofthestonebedinclinationαontheextrawidthrequiredforseismicdesign.Maximumvalues,togetherwithaveragevaluesin292 parentheses,aregiven.293 294 Asalreadynoted,specificanalyticalcomputationsshouldbecarriedoutforthesituationMAX‐S4ormore295 criticalseismicimplantationsinsteadofusingthegeneralapproachwiththemaximumvaluesdisplayedinTable296 6.Morespecifically,oneshouldpayattentiontospecificparametersoftheDSRWinthedesignthatplaysa297 criticalroleintheseismiccomputation(seefulldetailsin[40]).Apartfromthepositiveinfluenceofthestone298 bedinclinationandthenegativeeffectoftheretainedslopeanglealreadyhighlighted,apositiveinternalwall299 batterisrecommended(thisisthecaseofaself‐stablewall).Tosupportthisrecommendation,Walls1to5300 (withvariousstonetypesandbedinclinations)havebeendesignedtowithstandaspecificseismicacceleration301 (0.05g,0.10g…and0.35g).Inasecondstep,eachwallsectiongeometryhasbeenmodified,addinganinternal302 batter(λ m =5%,10%and15%)butkeepingthesamesurfaceareaasbefore.Itmeansthatthetotalvolumeof303 stonesusedinthatcaseisthesamebutthatthegeometryofthewallsectionisdifferent(i.e.,withalarger304 width at the base). Finally, the maximum acceleration withstood by the walls with an internal batter is305 comparedtothemaximumaccelerationfoundforthosewithoutthebatter(Figure9).Thecurvescorrespond306 totheaveragevaluesfoundthroughoutthedifferentwallsandstones.Onlypositivevalueshavebeenfound,307 meaningasystematicimprovementoftheseismicresistancewhenaddinganinternalbatter.Thisimprovement308 isparticularlysignificantforwallswithnon‐zerostonebedinclinationandlow(S2)tomoderate(S3)seismic309 hazardregions.310
19 311 Figure9:Effectoftheinternalbatterλ m (keepingthesameareaforthewallsection)ontheseismicresistanceofaDSRWfordifferentbedinclinations312 a)α=0%;b)α=10%;c)α=20%.313 Toconclude,inzoneS2,noDSRWextra‐widthisrequiredtofulfilaseismicdesignifbothaninclinationbedof314 10%andaninternalbatterofatleast10%areused.Thismeansthatanadequatechoiceforthewallgeometry315 compensatesfortherequiredextraresistancerequiredtosatisfyaseismicdesignincaseoflowseismicity.316 Conclusions 317 Thepresentstudyaddressesnon‐seismicandseismicdesignsofDryStoneRetainingWalls(DSRWs)according318 to the European standards (Eurocodes) used for conventional retaining walls while proposing an adapted319 methodology (e.g. including internal failure of DSRW). It has been shown that the current French320 recommendationsforthenon‐seismicdesignofDSRWscomplywithEurocode7(geotechnicalengineering)321
20 standardsbeingslightlymoreconservativethanthelatter.Moreover,inverylowseismiczones(ah<0.05g),322 non‐seismiclimitstatesarethemostcriticalstatesforthedesignofDSRWs,whichconfirmsthataseismic323 designisnotrequiredintheseregions[29].Thisisgenerallynotthecaseinzonesofhigherseismicitywhere324 theseismicdesignaccordingtoEurocode8(seismicengineering)standardisalmostalwaysthemostcritical.325 ThestudyrevealeddifferentgeometricaloptimisationoptionsforDSRWs.Itishighlyrecommendedtouse326 systematically:i)abedinclinationofatleast10%;ii)aflatretainedbackfill;iii)andapositiveinternalbatterof327 at least 10%. These three geometric parameters have a significantimpactonseismicdesign.Ifthese328 recommendationsarefollowedinlowseismiczones(uptoah=0.08g),thereisalsonoincreaseindimensions329 tofulfilaseismicdesign.330 Thepseudo‐staticapproachgenerallygivespracticalglobalrecommendationsforlowtomoderateseismic331 hazardzones(uptoah=0.2g).Inaddition,aspecificgeometricallyoptimised(asstatedabove)pseudo‐static332 designcanstillproduceaffordablerecommendationsinmorecriticalcases(uptoah=0.3g).However,for333 higherdesignaccelerationorparticularlycriticalcases,thepseudo‐staticapproachfortheseismicdesignleads334 tovalueshigherthan50%fortheextra‐widths.Inthiscase,dynamic time history computations are335 recommendedtoobtainmoreaccurateresultsthataccountforwalldisintegrationfailure.Indeed,thisfailure336 modemaybecriticalforhighseismicityareas,particularlyifcombinedwithpoorexecutionconditions.337 Finally,asanexampleillustratingEuropeancountries,Franceisusedasacasestudyofseismicdesignapplied338 toDSRWsinlowtomoderateseismicityareas.InmetropolitanFrance,wheremanyDSRWscanbefound,the339 expectedextra‐widthprovidedbyseismicdesigndoesnotexceed40%forwallslocatedinlowseismiczones340 presentingastonebedinclinationof10%,incasethefoundationisnotonthebedrock.Inthesameconditions,341 wallsbuiltinmoderateseismichazardzonesneedeitherastonebedinclinationof20%oraspecificanalytical342 computationtooptimisethesection.Finally,wallsdirectlyfoundedonthebedrock,inthecaseoflowand343 moderateseismicityareas,requireamaximumof30%extrawidthtofulfilaseismicdesign.344
21 Funding345 ThisworkwaspartlyfinancedbyFCT/MCTESthroughnationalfunds(PIDDAC)undertheR&DUnitInstitute346 forSustainabilityandInnovationinStructuralEngineering(ISISE),underreferenceUIDB/04029/2020.This347 studyhasalsobeenpartlyfundedbytheSTAND4HERITAGEproject(NewStandardsforSeismicAssessmentof348 Built Cultural Heritage) that has received funding from the European Research Council (ERC) under the349 EuropeanUnion’sHorizon2020researchandinnovationprogramme(GrantagreementNo.833123),asan350 AdvancedGrant.Inaddition,theauthorswanttoacknowledgetheFrenchMinistryofEducationandResearch351 fortheirfinancialsupportthroughaPhDgrantattributedtothefirstauthor.Theopinionsandconclusions352 presentedinthispaperarethoseoftheauthorsanddonotnecessarilyreflecttheviewsofthesponsoring353 organisations.354 Competinginterest355 Theauthorsdeclaretherearenocompetinginterests.356 Authors'contribution357 NS: Investigation, Formal Analysis, Visualisation, Writing – original draft; CM: Methodology, Resources,358 Investigation; EV: Funding acquisition, Writing – original draft, Methodology, Supervision; SF: Resources,359 Writing–review&editing,Methodology;PBL:Supervision,Fundingacquisition,Writing–review&editing.360 Dataavailability361 Thedataarisingfromtheanalyticalsimulationspresentedinthepaperisnotavailablepublicly.362 References363 [1] B.Villemus,J.‐C.Morel,andC.Boutin,‘Experimentalassessmentofdrystoneretainingwallstabilityon364 a rigid foundation’, Engineering Structures, vol. 29, no. 9, pp. 2124–2132, 2006, doi:365 10.1016/j.engstruct.2006.11.007.366
22 [2] A.‐S.Colas,J.‐C.Morel,andD.Garnier,‘Full‐scalefieldtrialstoassessdry‐stoneretainingwallstability’,367 EngineeringStructures,vol.32,no.5,pp.1215–1222,2010,doi:10.1016/j.engstruct.2009.12.047.368 [3] A.‐S.Colas,J.‐C.Morel,andD.Garnier,‘Assessingthetwo‐dimensionalbehaviourofdrystoneretaining369 wallsbyfull‐scaleexperimentsandyielddesignsimulation’,Géotechnique,vol.63,no.2,pp.107–117,2013,370 doi:10.1680/geot.10.P.115.371 [4] C.Mundell,P.McCombie,C.Bailey,A.Heath,andP.Walker,‘Limit‐equilibriumassessmentofdrystone372 retainingstructures’,ProceedingsoftheInstitutionofCivilEngineers(GeotechnicalEngineering),vol.162,no.373 4,pp.203–212,2009,doi:10.1680/geng.2009.162.4.203.374 [5] L.R.Alejano,M.Veiga,J.Taboada,andM.Díez‐Farto,‘Stabilityofgranitedrystonemasonryretaining375 walls:I.Analyticaldesign’,Géotechnique,vol.62,no.11,pp.1013–1025,2012,doi:10.1680/geot.10.P.112.376 [6] A.‐S. Colas, J.‐C. Morel, and D. Garnier, ‘Yield design modelling of dry joint retaining structures’,377 ConstructionandBuildingMaterials,vol.41,pp.912–917,2013,doi:10.1016/j.conbuildmat.2012.07.019.378 [7] B.Terrade,A.‐S.Colas,andD.Garnier,‘UpperboundlimitanalysisofmasonryretainingwallsusingPIV379 velocityfields’,Meccanica,vol.53,no.7,pp.1661–1672,2018,doi:10.1007/s11012‐017‐0673‐6.380 [8] R.M.Harkness,W.Powrie,X.Zhang,K.C.Brady,andM.P.O’Reilly,‘Numericalmodellingoffull‐scale381 tests on drystone masonry retaining walls’, Géotechnique, vol. 50, no. 2, pp. 165–179, 2000, doi:382 10.1680/geot.2000.50.2.165.383 [9] W.Powrie,R.M.Harkness,X.Zhang,andD.I.Bush,‘Deformation and failure modes of drystone384 retainingwalls’,Géotechnique,vol.52,no.6,pp.435–446,2002,doi:10.1680/geot.2002.52.6.435.385
23 [10] M.Claxton,R.A.Hart,P.F.McCombie,andP.J.Walker,‘Rigidblockdistinct‐elementmodellingofdry‐386 stoneretainingwallsinplanestrain’,ASCEJournalofGeotechnicalandGeoenvironmentalEngineering,vol.131,387 no.3,pp.381–389,2005,doi:10.1061/(ASCE)1090‐0241(2005)131:3(381).388 [11] P.Walker,P.McCombie,andM.Claxton,‘Planestrainnumericalmodelfordrystoneretainingwalls’,389 ProceedingsoftheInstitutionofCivilEngineers‐GeotechnicalEngineering,vol.160,no.2,pp.97–103,2007,390 doi:10.1680/geng.2007.160.2.97.391 [12] L.R.Alejano,M.Veiga,I.Gómez‐Márquez,andJ.Taboada, ‘Stability of granite drystone masonry392 retainingwalls:II.Relevantparametersandanalyticalandnumericalstudiesofrealwalls’,Géotechnique,vol.393 62,no.11,pp.1027–1040,2012,doi:10.1680/geot.10.P.113.394 [13] J.J.Oetomo,E.Vincens,F.Dedecker,andJ.‐C.Morel,‘Modelingthe2Dbehaviorofdry‐stoneretaining395 walls by a fully discrete element method’, International Journal for Numerical and Analytical Methods in396 Geomechanics,vol.40,no.7,pp.1099–1120,2016,doi:10.1002/nag.2480.397 [14] Z. Li, Y. Zhou, and Y. Guo, ‘Upper‐Bound Analysis for Stone Retaining Wall Slope Based on Mixed398 Numerical Discretization’, International Journal of Geomechanics,vol.18,no.10,pp.1–14,2018,doi:399 10.1061/(ASCE)GM.1943‐5622.0001247.400 [15] B.Pulatsu,S.Kim,E.Erdogmus,andP.B.Lourenço,‘Advancedanalysisofmasonryretainingwallsusing401 mixed discrete–continuum approach’, Proceedings of the Institution of Civil Engineers‐Geotechnical402 Engineering,pp.1–13,2020,doi:10.1680/jgeen.19.00225.403 [16] C. Mundell, P. McCombie, A. Heath, and J. Harkness, ‘Behaviour of drystone retaining structures’,404 ProceedingsoftheInstitutionofCivilEngineers(StructuresandBuilding),vol.163,no.1,pp.3–12,2010,doi:405 10.1680/stbu.2009.163.1.3.406
24 [17] H.H.Le,D.Garnier,A.‐S.Colas,B.Terrade,andJ.‐C.Morel,‘3Dhomogenisedstrengthcriterionfor407 masonry:Applicationtodrystoneretainingwalls’,JournaloftheMechanicsandPhysicsofSolids,vol.95,pp.408 239–253,2016,doi:10.1016/j.jmps.2016.05.021.409 [18] H.H.Le,J.‐C.Morel,A.‐S.Colas,B.Terrade,andD.Garnier,‘AssessingtheThree‐DimensionalBehaviour410 ofDryStoneRetainingWallsbyFull‐ScaleExperiments’,InternationalJournalofArchitecturalHeritage,vol.14,411 no.9,pp.1373–1383,2020,doi:10.1080/15583058.2019.1607627.412 [19] J.‐C.Quezada,E.Vincens,R.Mouterde,andJ.‐C.Morel,‘3Dfailureofascale‐downdrystoneretaining413 wall : a DEM modelling’, Engineering Structures, vol. 117, pp. 506–517, 2016, doi:414 10.1016/j.engstruct.2016.03.020.415 [20] CAPEB, ABPS, Muraillers de Provence, CBPS, CMA84, and ENTPE, Pierres sèches : guide de bonnes416 pratiquesdeconstructiondemursdesoutènement.ENTPE,2008.417 [21] ENTPE,ArtisansBâtisseursenPierreSèche(ABPS),EcoledesPontsParisTech,IFSTTAR,andFédération418 FrançaiseduBâtiment(FFB),Technique de construction des murs en pierre sèche : Règles professionnelles.419 ENTPE,ArtisansBâtisseursenPierreSèche(ABPS),2017.420 [22] AFPS,RecommandationsAFPS90.PressesdesPontsetChausseésParis,1990.421 [23] H.H.Le,‘Stabilitédesmursdesoutènementroutiersenpierresèche :Modélisation3Dparlecalculà422 laruptureetexpérimentationéchelle1’,PhDThesis,EcoleNationaledesTravauxPublicsdel’Etat(ENTPE),423 2013.424 [24] AFNOR,NFEN1997‐1:2005(Eurocode7) :Geotechnicaldesign‐Part1:Generalrules,vol.7,8vols.425 2005.426
25 [25] AFNOR,NF P94‐281 :Justificationdesouvrages géotechniques‐ Normes d’applicationnationalede427 l’Eurocode7‐Ouvragesdesoutènement‐Murs.2014.428 [26] AFNOR,NF P94‐261 :Justificationdesouvrages géotechniques‐ Normes d’applicationnationalede429 l’Eurocode7‐Fondationssuperficielles.2014.430 [27] N.Savalle,E.Vincens,andS.Hans,‘Pseudo‐staticscaled‐downexperimentsondrystoneretainingwalls:431 Preliminaryimplicationsfortheseismicdesign’,EngineeringStructures,vol.171,pp.336–347,Sep.2018,doi:432 10.1016/j.engstruct.2018.05.080.433 [28] AFNOR,NF EN 1998‐5:2005 (Eurocode 8) : Design of structures for earthquake resistance ‐ Part 5:434 Foundations,retainingstructuresandgeotechnicalaspects,vol.8,8vols.2005.435 [29] AFNOR,NF EN 1998‐1:2005 (Eurocode 8) : Design of structures for earthquake resistance ‐ Part 1:436 Generalrules,seismicactionsandrulesforbuildings,vol.8,8vols.2005.437 [30] B.Villemus,‘Etude desMursdeSoutènementen Maçonnerie dePierreSèches’,PhDThesis,Ecole438 NationaledesTravauxPublicsdel’Etat(ENTPE),2004.439 [31] C.A.Coulomb,Essaisuruneapplicationdesreglesdesmaximisetminimisaquelquesproblemesde440 statiquerelatifsal’architecture,vol.7.1773.441 [32] S.Okabe,‘Generaltheoryonearthpressureandseismicstabilityofretainingwallanddam’,Proc.Civil442 Engrg.Soc.,Japan,vol.10,no.6,pp.1277–1323,1924.443 [33] N.Mononobeand H.Matsuo,‘OnDetermination of Earth PressuresduringEarthquakes’, in World444 EngineeringConference,1929,vol.9,pp.177–185.445 [34] N.Savalle,E.Vincens,andP.B.Lourenço,‘Pseudo‐staticanalyticalmodelforthestaticandseismic446 stabilityofdrystoneretainingwalls’,Lisbon,Portugal,2022.doi:10.11159/icgre22.138.447