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The SMP Concept-based 3D Constitutive Models for Geomaterials HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE i — #1 BALKEMA-ProceedingsandMonographs inEngineering,Water,andEarthSciences HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE ii — #2 The SMP Concept-based 3D Constitutive Models for Geomaterials Hajime Matsuoka Department of Civil Engineering, Nagoya Institute ofTechnology,Japan De’an Sun Department of Civil Engineering, Shanghai University,China LONDON / LEIDEN / NEW YORK / PHILADELPHIA / SINGAPORE HAJIME: “FM” — 2006/2/4 — 16:00 — PAGE iii — #3 ©2006Taylor&FrancisGroup,London,UK TypesetinTimesNewRomanby NewgenImagingSystems(P)Ltd,Chennai,India PrintedandboundinGreatBritainby TJInternationalLtd,Padstow,Cornwall Allrightsreserved.Nopartofthispublicationortheinformationcontained hereinmaybereproduced,storedinaretrievalsystem,ortransmittedinany formorbyanymeans,electronicormechanical,byphotocopying,recordingor otherwise,withoutwrittenpriorpermissionfromthepublishers. Althoughallcareistakentoensureintegrityandthequalityofthis publicationandtheinformationherein,noresponsibilityisassumedbythe publishersnortheauthorforanydamagetopropertyorpersonsasa resultofoperationoruseofthispublicationand/ortheinformationcontainedherein. Publishedby:Taylor&Francis/Balkema P.O.Box447,2300AKLeiden,TheNetherlands e-mail:[email protected] www.balkema.nl,www.tandf.co.uk,www.crcpress.com BritishLibraryCataloguinginPublicationData AcataloguerecordforthisbookisavailablefromtheBritishLibrary LibraryofCongressCataloginginPublicationData Matsuoka,Hajime,1943– TheSMPconcept-based3Dconstitutivemodels forgeomaterials/HajimeMatsuoka,De’anSun. p.cm. Includesbibliographicalreferencesandindex. ISBN0–415–39504–6(hardcover:alk.paper)1.Soilmechanics– Mathematicalmodels.I.Sun,De’an,1962–II.Title. TA710.A1.M372006 (cid:1) 624.15136015118–dc22 2005035141 ISBN100–415–39504–6 ISBN13978–0–415–39504–5 HAJIME: “FM” — 2006/2/4 — 16:00 — PAGE iv — #4 Contents Listoffigures vii Listoftables xiii Preface xv 1 Spatiallymobilizedplane(SMP)andSMPcriterion 1 1.1 OriginofSMP 1 1.2 Stress–strainrelationbasedoncompositelymobilizedplane(CMP) 1 1.3 Stress–strainrelationbasedonSMP 9 1.4 Failurecriteriaformetalsandgranularmaterials 14 1.5 Failurecriterionforcohesive-frictionalmaterials 20 References 24 2 IntroductiontoCam-claymodel 27 2.1 Introduction 27 2.2 OriginalCam-claymodel 29 2.2.1 Principaldirectionofplasticstrainincrementandadopted stressandstrainvariables 29 2.2.2 Determinationofplasticpotentialandyieldfunctions 31 2.2.3 Determinationofstrain-hardeningrule 34 2.2.4 Determinationofdεe 37 ij 2.2.5 Detailedderivationofdεp 38 ij 2.3 ModifiedCam-claymodel 48 2.3.1 Principaldirectionofplasticstrainincrementandadopted stressandstrainvariables 48 2.3.2 Determinationofplasticpotentialandyieldfunctions 48 2.3.3 Determinationofstrain-hardeningrule 51 2.3.4 Determinationofdεe 52 ij 2.3.5 Detailedderivationofdεp 52 ij References 60 3 TheCam-claymodelrevisedbytheSMPcriterion 61 3.1 Introduction 61 3.2 TheSMPcriterionandatransformedstresstensor 62 3.3 TheCam-claymodelrevisedbytheSMPcriterion 66 HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE v — #5 vi Contents 3.4 Comparisonofmodelpredictionswithexperimentaldata 72 3.5 Concludingremarks 76 Appendix1 Derivationof(cid:2) 77 0 Appendix2 DerivationofelastoplasticconstitutivetensorD 78 ijkl References 80 4 Elastoplasticconstitutivemodelsforgeomaterialsusing transformedstress 83 4.1 Anelastoplasticmodelforsandsandclays 83 4.1.1 Introduction 83 4.1.2 Aunifiedhardeningparameterforbothclaysandsands 84 4.1.3 Aunifiedelastoplasticmodelforbothclaysandsands 91 4.1.4 Predictionversusexperiment 92 4.1.5 Modelingconfiningpressuredependenceofstrengthand deformation 93 4.1.6 Conclusions 95 4.2 AnelastoplasticmodelforK -consolidatedsoils 95 0 4.2.1 Introduction 95 4.2.2 TheSekiguchi-Ohtamodelanditsstress–dilatancyrelation 96 4.2.3 Ananisotropichardeningelastoplasticmodelfor K -consolidatedclaysandsands 98 0 4.2.4 Comparisonofmodelpredictionswithexperimentalresults 102 4.2.4.1 Modelingtriaxialbehavior 102 4.2.4.2 Modelingplanestrainbehavior 104 4.2.5 Elastoplasticconstitutivetensor 107 4.2.6 Conclusions 108 4.3 Anelastoplasticmodelforunsaturatedsoils 109 4.3.1 Introduction 109 4.3.2 Effectivestressforunsaturatedsoils 110 4.3.3 TransformedstresstensorbasedonExtendedSMPcriterion 112 4.3.4 Formulationofmodelforunsaturatedsoils 114 4.3.4.1 Strengthofunsaturatedsoil 114 4.3.4.2 Formulationofmodelinisotropicstressstate 115 4.3.4.3 Formulationofmodelingeneralstress 117 4.3.5 Triaxialtestsonunsaturatedsoils 120 4.3.5.1 Triaxialtestapparatusforunsaturatedsoils 120 4.3.5.2 Unsaturatedsoilspecimen 121 4.3.5.3 Stresspaths 122 4.3.6 Comparisonofmodelpredictionswithexperimentalresults 122 4.3.6.1 Modelparametersandtheirdetermination 122 4.3.6.2 Modelpredictionsversusexperimentalresults 124 4.3.7 Generalstress–strainrelationforunsaturatedsoils 128 4.3.8 Concludingremarks 129 References 129 5 Concludingremarks 133 Index 135 HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE vi — #6 Figures 1.1 Directsheartestonanassemblyofaluminumrods 2 1.2 Directsheartestonanassemblyofphotoelasticrods 2 1.3 Biaxialcompressiontestonanassemblyofaluminumrods 3 1.4 Biaxialcompressiontestonanassemblyofphotoelasticrods 3 1.5 NormalandshearstressesonmobilizedplanesandSMP 4 1.6 GeometricalrepresentationsofmobilizedplanesandSMPin three-dimensionalspace 5 1.7 “Two”two-dimensionalmobilizedplanesundertriaxialcompressionand triaxialextensionconditions 5 1.8 Deformationoftriaxialcompressionandtriaxialextensionspecimens aftertests 6 1.9 “Two-dimensional”principalstrainincrementsunderrespectivepairsof principalstresses 6 1.10 Aplanewhereshear–normalstressratioismaximum 8 1.11 Relationbetweenτ/σ and−dε /dγ ononemobilizedplaneobtained N N bytriaxialcompressionandextensiontestsonToyourasand 8 1.12 Relationbetweenτ/σ ,γ andε ononemobilizedplaneobtainedby N N triaxialcompressionandextensiontestsonToyourasand 9 1.13 Predictedandmeasuredrelationsbetweenσ /σ ,ε andε obtainedby 1 3 1 3 triaxialcompressionandextensiontestsonToyourasand 9 1.14 Amountsofstrainincrementsdε∗ anddγ∗ inprincipalstrain SMP SMP incrementspace 11 1.15 Relationbetweenτ /σ and−dε∗ /dγ∗ obtainedbytriaxial SMP SMP SMP SMP compressionandextensiontestsonToyourasand 11 1.16 Relationbetweenτ /σ and−dε∗ /dγ∗ obtainedbytrue SMP SMP SMP SMP triaxialtestsonToyourasand 12 1.17 Relationbetweenτ /σ and−dε /dγ obtainedbythesametests oct oct oct oct asFigure1.15 12 1.18 Relationbetweenτ /σ ,γ∗ ,andε∗ obtainedbytriaxial SMP SMP SMP SMP compressionandextensiontestsonToyourasand 13 1.19 Relationbetweenτ /σ ,γ∗ ,andε∗ obtainedbytruetriaxial SMP SMP SMP SMP testsonToyourasand 13 1.20 Relationbetweenτ /σ ,γ ,andε obtainedbythesametestsas oct oct oct oct Figure1.18 14 HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE vii — #7 viii Figures 1.21 Predictedandmeasuredrelationsbetweenprincipalstressratioand principalstrainsobtainedbytruetriaxialtestsonToyourasand 15 1.22 Normalandshearstresseson45◦planesandoctahedralplane 16 1.23 NormalandshearstressesonmobilizedplanesandSMP 16 1.24 Geometricalrepresentationsof45◦planesandoctahedralplanein three-dimensionalspace 17 1.25 GeometricalrepresentationsofmobilizedplanesandSMPin three-dimensionalspace 18 1.26 MutualrelationshipsbetweentheTresca,Mises,Mohr-Coulomb,and Matsuoka-Nakai(SMP)failurecriteriadescribedintheπ-plane 19 1.27 ShapesoftheTresca,Mises,Mohr-Coulomb,andMatsuoka-Nakai (SMP)failurecriteriainprincipalstressspace 20 1.28 ComparisonoftheMatsuoka-Nakai(SMP)andMohr-Coulombcriteria withstressstatesatfailureintheπ-planeobtainedbytriaxial compression,triaxialextensionandtruetriaxialtestsonToyourasand 20 1.29 NormalandshearstressesonmobilizedplanesandExtendedSMPfor cohesive-frictionalmaterials 21 1.30 ExtendedSMPinthree-dimensionalspaceundertranslatedprincipal stresses 22 1.31 SchematicdiagramsofExtendedSMPfailurecriterionandgeneral Mohr-Coulombfailurecriterioninprincipalstressspace 22 1.32 MutualrelationshipsbetweentheTresca,Mises,Mohr-Coulomb, generalizedMohr-Coulomb,Matsuoka-Nakai(SMP),andExtendedSMP failurecriteria 23 1.33 ComparisonoftheExtendedSMPcriterionwithstressstatesatfailurein theπ-planeobtainedbytriaxialcompression,triaxialextension,andtrue triaxialtestsonacementedsand 24 2.1 Watercontentcontoursfromdrainedtriaxialtestsandstresspathsin undrainedtriaxialtestsonanormallyconsolidatedclay 28 2.2 Principalstressspaceandprincipalplasticstrainincrementspace 30 2.3 Plasticpotentialandstrainincrementvector 31 2.4 StressratioversusstrainincrementratiorelationadoptedinCam-clay model 32 2.5 PlasticpotentialandplasticstrainincrementvectorsinCam-claymodel 33 2.6 YieldlocususedinCam-claymodel 34 2.7 Themechanicalmeaningofyieldlocus 34 2.8 Resultsofisotropiccompressionandswellingtests 35 2.9 ThemeaningofyieldlocusinCam-claymodel 36 2.10 Predictionofstressversusstrainrelationindrainedtriaxialcompression testbyoriginalCam-claymodel 45 2.11 Predictionofstresspathsindrainedtriaxialcompressiontestbyoriginal Cam-claymodel 45 2.12 Predictionofstressversusstrainrelationinundrainedtriaxialextension testbyoriginalCam-claymodel 47 2.13 Predictionofstresspathsinundrainedtriaxialextensiontestbyoriginal Cam-claymodel 48 HAJIME: “FM” — 2006/1/28 — 14:48 — PAGE viii — #8 Figures ix 2.14 Stressratioversusplasticstrainincrementratioadoptedinmodified Cam-claymodel 49 2.15 Plasticpotentialandplasticstrainincrementvectorsinmodified Cam-claymodel 50 2.16 YieldlocusofmodifiedCam-claymodel 51 2.17 ThemeaningofyieldlocusinmodifiedCam-claymodel 52 2.18 Predictionofstressversusstrainrelationindrainedtriaxialtestby modifiedCam-claymodel 57 2.19 Predictionofstressversusstrainrelationinundrainedtriaxialextension testbymodifiedCam-claymodel 59 2.20 Predictionofstresspathsinundrainedtriaxialextensiontestsby modifiedCam-claymodel 59 3.1 ShapesofExtendedTrescaandExtendedMisesfailurecriteriaand Mohr-CoulombandSMPcriteriainprincipalstressspace 62 3.2 MutualrelationshipsbetweenExtendedTrescaandExtendedMises failurecriteriaandMohr-CoulombandSMPcriteriainπ-plane 63 3.3 ComparisonofExtendedMises,Mohr-Coulomb,andSMPcriteriawith stressstatesatfailureinπ-planeobtainedbytriaxialcompression, triaxialextension,andtruetriaxialtestsonFujinomoriclay 64 3.4 TheSMPcriterioninπ-planeandtransformedπ-plane 65 3.5 ShapesofSMPfailurecriterionexpressedintransformedprincipalstress space 66 3.6 Stress–dilatancyrelationshipsoftherevisedoriginalCam-claymodel undertriaxialcompressionandtriaxialextension 68 3.7 Stress–dilatancyrelationshipsforFujinomoriclayundertriaxial compressionandtriaxialextension 69 3.8 YieldlocioforiginalCam-claymodelgeneralizedbytheSMPcriterion intriaxialcompressionandtriaxialextension 69 3.9 Yieldsurfaceexpressedintransformedprincipalstressspaceand ordinaryprincipalstressspace 69 3.10 Stress–dilatancyrelationshipsoftherevisedmodifiedCam-claymodel undertriaxialcompressionandtriaxialextension 72 3.11 YieldlociofmodifiedCam-claymodelgeneralizedbytheSMPcriterion intriaxialcompressionandtriaxialextension 72 3.12 Predictedandmeasuredresultsoftriaxialcompressionandtriaxial extensiontestsonFujinomoriclay 73 3.13 Comparisonbetweenpredictedandmeasuredstress–strainbehavior 74 3.14 Comparisonbetweenpredictedandmeasuredstress–strainbehavior underthreedifferentprincipalstresses 75 3.15 Comparisonbetweenpredictedandmeasuredstress–strainbehavior underundrainedtriaxialcompressionandtriaxialextension 76 3.16 Comparisonbetweenpredictedandmeasuredundrainedstresspaths undertriaxialcompressionandtriaxialextension 76 4.1.1 Directionofplasticstrainincrement 85 4.1.2 Triaxialcompressiontestresultsforclayandsand 87 4.1.3 Stresspathsoftriaxialtestsforexaminingthenewhardeningparameter 89 HAJIME: “FM” 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