ABAQUSAnalysisUr'sManual17.7.1Timedomainviscoelasticity
Products:ABAQUS/StandardABAQUS/ExplicitABAQUS/CAE
References
“Materiallibrary:overview,”Section16.1.1
“Elasticbehavior:overview,”Section17.1.1
“Frequencydomainviscoelasticity,”Section17.7.2
*VISCOELASTIC
*SHEARTESTDATA
*VOLUMETRICTESTDATA
*COMBINEDTESTDATA
*TRS
Overview
Thetimedomainviscoelasticmaterialmodel:
describesisotropicrate-dependentmaterialbehaviorformaterials
inwhichdissipativelossprimarilycaudby“viscous”
(internaldamping)effectsmustbemodeledinthetimedomain;
assumesthattheshear(deviatoric)andvolumetricbehaviorsare
independentinmultiaxialstressstates(exceptwhenudforanelastomericfoam);
canbeudonlyinconjunctionwith“Linearelasticbehavior,”
Section17.2.1;“Hyperelasticbehaviorofrubberlikematerials,”
Section17.5.1;or“Hyperelasticbehaviorinelastomericfoams,”
Section17.5.2,todefinetheelasticmaterialproperties;
isactiveonlyduringatransientstaticanalysis(“Quasi-static
analysis,”Section6.2.5),atransientimplicitdynamicanalysis
(“Implicitdynamicanalysisusingdirectintegration,”Section
6.3.2),anexplicitdynamicanalysis(“Explicitdynamicanalysis,”
Section6.3.3),asteady-statetransportanalysis(“Steady-state
transportanalysis,”Section6.4.1),afullycoupled
temperature-displacementanalysis(“Fullycoupledthermal-stress
analysis,”Section6.5.4),oratransient(consolidation)coupled
porefluiddiffusionandstressanalysis(“Coupledporefluid
diffusionandstressanalysis,”Section6.7.1);
canbeudinlarge-strainproblems;and
canbecalibratedusingtime-dependentcreeptestdata,
time-dependentrelaxationtestdata,orfrequency-dependentcyclictestdata.
Definingtheshearbehavior
TimedomainviscoelasticityisavailableinABAQUSforsmall-strain
applicationswheretherate-independentelasticresponcanbedefined
withalinearelasticmaterialmodelandforlarge-strainapplications
wheretherate-independentelasticresponmustbedefinedwitha
hyperelasticorhyperfoammaterialmodel.
注释:小应变简化为弹性,大应变超弹性或超弹泡沫
Smallstrain(小应变)
Considerasheartestatsmallstrain,inwhichatimevaryingshearstrain,
,ponistheshearstressTheviscoelasticmaterialmodeldefines
as
.
where事迹材料 isthetime-dependent“shearrelaxationmodulus”(剪切松弛模量)
thatcharacterizesthematerial'nstitutivebehaviorcanbeillustrated
byconsideringarelaxationtestinwhichastrainissuddenlyappliedtoaspecimen
inningoftheexperiment,whenthe
strainissuddenlyapplied,istakenaszerotime,sothat(t=0,初始应变突然施加)
coelasticmaterialmodelis“long-termelastic”
(长期弹性)inthenthat,afterhavingbeensubjectedtoaconstantstrainfora
verylongtime,,
.
as
Theshearrelaxationmoduluscanbewrittenindimensionlessform:
where
istheinstantaneousshearmodulus(瞬时剪切模量),sothat
theexpressionforthestresstakestheform
Thedimensionlessrelaxationfunctionhasthelimitingvalues
.
Largestrain(大应变)
Theequationforthestresscanbetransformedbyusingintegrationby
parts:
and
Itisconvenienttowritethiquationintheform
where
rmallowsa
straightforwardgeneralization(简单概括)tononlinearelasticdeformationsbyreplacingthelinearelasticrelation
withthenonlinearelasticityrelation
.Thisgeneralizationyieldsalinearviscoelasticitymodel,inthenthat
thedimensionlessstressrelaxationfunctionisindependentofthemagnitudeofthe
deformation.
Intheaboveequationtheinstantaneousstress,,appliedattime
influencesthestress,,ore,tocreateaproper
finite-strainformulation,itisnecessarytomapthestressthatexisted
ABAQUSthisisdonebymeansofamixed“push-forward”transformationwiththerelativedeformationgradient
:
Toensurethatthestressremainssymmetric,ABAQUSustheintegralform:
wmac强制退出 hereisthedeviatoricpartoftheKirchhoffst贪婪拼音 ress.基尔莫夫应力偏量
Thefinite-straintheoryisdescribedinmoredetailin“Finite-strain
viscoelasticity,”Section4.8.2oftheABAQUSTheoryManual.
Definingthevolumetricbehavior定义体
Thevolumetricbehaviorcanbewritteninaformthatissimilartotheshearbehavior:
wherepisthehydrostaticpressure,(静水压力)
bulkmodulus,
volumestrain.
Theaboveexpansionappliestosmallaswellasfinitestrainsincethe
volumestrainsaregenerallysmallandthereisnoneedtomapthepressure
fromtimetotimet.
istheinstantaneoulastic
isthe
isthedimensionlessbulkrelaxationmodulus,and
Temperatureeffects温度效应
Theeffectoftemperature,,onth演讲自我介绍 ematerialbehaviorisintroduced
throughthedependenceoftheinstantaneousstress,,ontemperature
ressionforthelinear-elasticshearstressisrewrittenas
wheretheinstantaneousshearmodulus
,and
istemperaturedependent,
isthereducedtime,definedby
ducedtimeconceptfor
temperaturedependenceisusuallyreferredtoasthermo-rheologicallysimple(TRS)
heshiftfunctionisapproximatedbythe
Williams-Landell-Ferry(WLF)form:
where,
isthereferencetemperatureatwhichtherelaxationdataaregivenand
,
deformationchangeswillbeelastic,badontheinstantaneousmoduli.
Thereducedtimeconceptisalsoudforthevolumetricbehaviorandthe
itionalinformationontheWLFequation,
e“Viscoelasticity,”Section4.8.1oftheABAQUSTheoryManual.
Numericalimplementation数值执行结果
ABAQUSassumesthattheviscoelasticmaterialisdefinedbyaPronyriexpansionofthedimensionlessrelaxationmodulus:
whereN,
,and
,
,tutionin
thesmall-strainexpressionfortheshearstressyields
where
The
areinterpretedasstatevariablesthatcontrolthestressrelaxation,and
isthe“creep”strain:thedifferencebetweenthetotalmechanicalstrainandthe
instantaneoulasticstrain(thestressdividedbytheinstantaneoulasticmodulus).InABAQUS/Standard
isavailableasthecreepstrainoutputvariableCE
(“ABAQUS/Standardoutputvariableidentifiers,”Section4.2.1).
AsimilarPronyriexpansionisudforthevolumetricrespon,whichisvalidforbothsmall-andfinite-strainapplications:
where
ABAQUSassumesthat.
ThePronyriexpansion,incombinationwiththefinite-strain
expressionfortheshearstress,producesthefollowinglarge-strainshearmodel:
where
The
areinterpretedasstatevariablesthatcontrolthestressrelaxation.
Iftheinstantaneousmaterialbehaviorisdefinedbylinearelasticityorhyperelasticity,thebulkandshearbehaviorcanbedefined
r,iftheinstantaneousbehaviorisdefinedbythe
hyperfoammodel,thedeviatoricandvolumetricconstitutivebehaviorare
coupledanditisnecessarytouthesamerelaxationdataforbothbehaviors.
Inalloftheaboveexpressionstemperaturedependenceisreadilyintroducedbyreplacing
by
and
by
.
Determinationofviscoelasticmaterialparameters定义粘弹性材料参数
Theaboveequationsareudtomodelthetime-dependentshearand
axationparameters
canbedefinedinoneoffourways:directspecificationoftheProny
riesparameters,inclusionofcreeptestdata,inclusionofrelaxation
testdata,orinclusionoffrequency-dependentdataobtainedfrom
atureeffectsareincludedin
thesamemannerregardlessofthemethodudtodefinetheviscoelasticmaterial.
ABAQUS/CAEallowsyoutoevaluatethebehaviorofviscoelasticmaterials
byautomaticallycreatingresponcurvesbadonexperimentaltestdata
elasticmaterialcanbeevaluatedonlyifitis
definedinthetimedomainandincludeshyperelasticand/orelastic
“Evaluatinghyperelasticandviscoelasticmaterial
behavior,”Section12.4.6oftheABAQUS/CAEUr'sManual.
Directspecification(直接参数)ThePronyriesparameters
,
,andcanbedefineddirectlyfor
snorestrictiononthenumberof
termsthatcanbeud.(应用数目没有限制)Ifarelaxationtimeis
associatedwithonlyoneofthetwomoduli,leavetheotheroneblankor
enterazero.(如果松弛时间仅于两个模量的一个有关联,则另外一个设为1
或0)Thedatashouldbegiveninascendingorder(升序)oftherelaxation
beroflinesofdatagivendefinesthenumberofterms甲醛中毒表现 in
thePronyries,modelisudinconjunctionwiththe
hyperfoam(超弹泡沫材料模型)materialmodel,thetwomodulusratioshavetobethesame(
).
InputFileUsage:
*VISCOELASTIC,TIME=PRONY
Thedatalineisrepeatedasoftenasneededtodefinethe
first,cond,third,nthePronyries.
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:TimeandTime:
age:
Prony
Enterasmanyrowsofdatainthetableasneededtodefine
thefirst,cond,third,nthePronyries.
Creeptestdata
Ifcreeptestdataarespecified,ABAQUSwillcalculatethetermsinthe
malizedshearandbulkcompliancesaredefinedas
whereand
istheshearcompliance,
isthetotalshearstrain,
isthe
istheconstant
.
istheconstantshearstressinashearcreeptest;
isthetotalvolumetricstrain,and
,
volumetriccompliance,
Thecreepdataareconvertedtorelaxationdatathroughtheconvolutionintegrals
ABAQUSthenusthenormalizedshearmodulus
modulus
parameters.
Usingtheshearandvolumetrictestdataconcutively
andnormalizedbulk
inanonlinearleast-squaresfittodeterminethePronyries
Thesheartestdataandvolumetrictestdatacanbeudconcutively
todefinethenormalizedshearandbulkcompliancesasfunctionsoftime.
Aparateleast-squaresfitisperformedoneachdatat;andthetwo
derivedtsofPronyriesparam上海十大古镇排名 eters,intoonetofparameters,
InputFileUsage:
.
and
,aremerged
stoptionis
eofthecondandthirdoptionsis
required.
*VISCOELASTIC,TIME=CREEPTESTDATA
*SHEARTESTDATA
*VOLUMETRICTESTDATA
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:TimeandTime:
age:
Creeptestdata
Inaddition,lectoneorbothofthefollowing:TestData
TestData
Usingthecombinedtestdata
ShearTestData
VolumetricTestData
Alternatively,thecombinedtestdatacanbeudtospecifythe
normalizedshearandbulkcompliancessimultaneouslyasfunctionsoftime.
Asingleleast-squaresfitisperformedonthecombinedtoftestdatatodetermineonetofPronyriesparameters,
InputFileUsage:
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:Time,Time:
age:
Creeptestdata,andTestDataCombinedTestData
Relaxationtestdata
Aswithcreeptestdata,ABAQUSwillcalculatethePronyriesparametersautomaticallyfromrelaxationtestdata.
Usingtheshearandvolumetrictestdataconcutively
.
Ubothofthefollowingoptions:
*VISCOELASTIC,TIME=CREEPTESTDATA
*COMBINEDTESTDATA
Again,thesheartestdataandvolumetrictestdatacanbeud
concutivelytodefinetherelaxationmoduliasfunctionsoftime.A
paratenonlinearleast-squaresfitisperformedoneachdatat;and
thetwoderivedtsofPronyriesparameters,aremergedintoonetofparameters,
InputFileUsage:
.
and
,
stoptionis
eofthecondandthirdoptionsis
required.
*VISCOELASTIC,TIME=RELAXATIONTESTDATA
*SHEARTESTDATA
*VOLUMETRICTESTDATA
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:TimeandTime:
age:
Relaxationtestdata
Inaddition,lectoneorbothofthefollowing:TestData
TestData
Usingthecombinedtestdata
ShearTestData
VolumetricTestData
Alternatively,thecombinedtestdatacanbeudtospecifythe
e
least-squaresfitisperformedonthecombinedtoftestdatatodetermineonetofPronyriesparameters,
InputFileUsage:
*VISCOELASTIC,TIME=RELAXATIONTESTDATA
*COMBINEDTESTDATA
Ubothofthefollowingoptions:
.
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:Time,Time:
age:
Relaxationtestdata,andTestDataCombinedTest
Data
Frequency-dependenttestdata
ThePronyriestermscanalsobecalibratedusingfrequency-dependent
caABAQUSusanalyticalexpressionsthatrelate
expressionsfortheshearmoduli,obtainedbyconvertingthePronyries
termsfromthetimedomaintothefrequencydomainbymakinguofFouriertransforms,canbewrittenasfollows:
where
isthestoragemodulus,
isthelossmodulus,
isthe
angularfrequency,
expressionsareudinanonlinearleast-squaresfittodeterminethePronyries
parametersfromthestorageandlossmodulicyclictestdataobtainedatMfrequenciesbyminimizingtheerrorfunction
:
where
and
arethetestdataand
and
,respectively,arethe
ressionsforthebulkmoduli,
and
,arewrittenanalogously.
Thefrequencydomaindataaredefinedintabularformbygivingthereal
andimaginarypartsofand—whereisthecircularfrequency—as
functionsoffrequencyincyclespertime.
istheFouriertransform
ofthenondimensionalshearrelaxationfunction
thefrequency-dependentstorageandlossmoduliand
,therealandimaginarypartsof
and
,
.Given,
,
arethengivenas
whereandarethelong-termshearandbulkmodulideterminedfrom
theelasticorhyperelasticproperties.
InputFileUsage:
*VISCOELASTIC,TIME=FREQUENCYDATA
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:TimeandTime:
age:
Frequencydata
CalibratingthePronyriesparameters
Youcanspecifytwooptionalparametersrelatedtothecalibrationof
Pronyriesparametersforviscoelasticmaterials:theerrortolerance
ortoleranceistheallowableaverageroot-mean-square
errorofdatapointsintheleast-squaresfit,anditsdefaultvalueis
aximumnumberoftermsNinthePronyries,andits
default(andmaximum)willperformtheleast-squares
fitfromtountilconvergenceisachievedforthelowest
Nwithrespecttotheerrortolerance.
Thefollowingaresomeguidelinesfordeterminingthenumberoftermsin
ntheguidelines,youcanchoo
.
Thereshouldbeenoughdatapairsfordeterminingalltheparameters
,assumingthatNisthenumberof
Pronyriesterms,thereshouldbeatotalofatleastdata
pointsinsheartestdata,datapointsinvolumetrictestdata,
datapointsincombinedtestdata,如何添加脚注 anddatapointsinthe
frequencydomain.
ThenumberoftermsinthePronyriesshouldbetypicallynotmore
thanthenumberoflogarithmic“decades”spannedbythetestdata.
Thenumberoflogarithmic“decades”isdefinedas
,where
and
arethemaximumandminimum
timeinthetestdata,respectively.
InputFileUsage:
*VISCOELASTIC,ERRTOL=
error_tolerance
,NMAX=
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:Time;Time:
age:
Creeptestdata,Relaxationtestdata,orFrequency
data;MaximumnumberoftermsinthePronyries:
;andAllowableaverageroot-mean-square
error:
error_tolerance
Temperatureeffects
Regardlessofthemethodudtodefinetheviscoelasticbehavior,
thermo-rheologicallysimpletemperatureeffectscanbeincludedby
ft
functioncanbedefinedbytheWilliams-Landell-Ferry(WLF)approximation.
InputFileUsage:
*TRS,DEFINITION=WLF
InABAQUS/Explicituthefollowingoption:
*TRS
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:Time,Time:any
age:
method
,andSuboptionsTrs:Shiftfunction:WLF
UrsubroutinespecificationinABAQUS/Standard
InABAQUS/Standarduthefollowingoption:
InABAQUS/Standardtheshiftfunctioncanalternativelybespecifiedin
ursubroutineUTRS.
InputFileUsage:
*TRS,DEFINITION=USER
ABAQUS/CAEUs
Propertymodule:materialeditor:Mechanical
ElasticityViscoelastic:Domain:Time,Time:any
age:
method
,andSuboptionsTrs:Shiftfunction:Ur
subroutineUTRS
Definingtherate-independentpartofthematerialrespon
Inallcalasticmodulimustbespecifiedtodefinethe
-strainlinear
elasticbehaviorisdefinedbyanelasticmaterialmodel(“Linearelastic
behavior,”Section17.2.1),andlarge-deformationbehaviorisdefinedby
ahyperelastic(“Hyperelasticbehaviorofrubberlikematerials,”Section
17.5.1)orhyperfoam(“Hyperelasticbehaviorinelastomericfoams,”
Section17.5.2)e-independentelasticityforany
ofthemodelscanbedefinedintermsofeitherinstantaneoulastic
iceofdefiningtheelasticity
intermsofinstantaneousorlong-termmoduliisamatterofconvenienceonly;itdoesnothaveaneffectonthesolution.
Theeffectiverelaxationmoduliareobtainedbymultiplyingthe
instantaneoulasticmoduliwiththedimensionlessrelaxationfunctions
elasticmaterials
Forlinearelasticmaterialbehavior
and
whereandaretheinstantaneousshearandbulkmodulideterminedfrom
and
:
thevaluesoftheur-definedinstantaneoulasticmoduli
and
.
Iflong-termelasticmoduliaredefined,theinstantaneousmoduliaredeterminedfrom
Hyperelasticmaterials
Forhyperelasticmaterialbehaviortherelaxationcoefficientsare
appliedeithertotheconstantsthatdefinetheenergyfunctionor
polynomialfunctionandits
particularcas(reducedpolynomial,Mooney-Rivlin,neo-Hookean,andYeoh)
fortheOgdenfunction
fortheArruda-BoyceandVanderWaalsfunctions
andfortheMarlowfunction
Forthecoefficientsgoverningthecompressiblebehaviorofthepolynomial
modelsandtheOgdenmodel
fortheArruda-BoyceandVanderWaalsfunctions
and国土面积排名前十的国家 fortheMarlowfunction
Iflong-termelasticmoduliaredefined,theinstantaneousmoduliaredeterminedfrom
whiletheinstantaneousbulkcompliancemoduliareobtainedfrom
fortheMarlowfunctionswehave
Elastomericfoams
Forelastomericfoammaterialbehaviortheinstantaneousshearandbulk
relaxationcoefficientsareassumedtobeequalandareappliedtothe
materialconstantsintheenergyfunction:
Ifonlytheshearrelaxationcoefficientsarespecified,thebulk
relaxationcoefshearandbulkrelaxation
coefficientsarespecifiedandtheyareunequal,ABAQUSissuesanerrormessage.
Iflong-termelasticmoduliaredefined,theinstantaneousmoduliaredeterminedfrom
Materialresponindifferentanalysisprocedures
Thetime-domainviscoelasticmaterialmodelisactiveduringthefollowingprocedures:
transientstaticanalysis(“Quasi-staticanalysis,”Section
6.2.5),
transientimplicitdynamicanalysis(“Implicitdynamicanalysis
usingdirectintegration,”Section6.3.2),
explicitdynamicanalysis(“Explicitdynamicanalysis,”Section
6.3.3),
steady-statetransportanalysis(“Steady-statetransport
analysis,”Section6.4.1),
fullycoupledtemperature-displacementanalysis(“Fullycoupled
thermal-stressanalysis,”Sect学科英文 ion6.5.4),and
transient(consolidation)coupledporefluiddiffusionandstress
analysis(“Coupledporefluiddiffusionandstressanalysis,”
Section6.7.1).
Viscoelasticmaterialresponisalwaysignoredinastaticanalysis.
Itcanalsobeignoredinacoupledtemperature-displacementanalysisor
inasoilsconsolidationanalysisbyspecifyingthatnocreepor
viscoelasticresponisoccurringduringthestepevenifcreepor
viscoelasticmaterialpropertiesaredefined(e“Fullycoupled
thermal-stressanalysis,”Section6.5.4,or“Coupledporefluiddiffusion
andstressanalysis,”Section6.7.1).Inthecasitisassumedthat
theloadingisappliedinstantaneously,sothattheresultingrespon
correspondstoanelasticsolutionbadoninstantaneoulasticmoduli.
ABAQUS/Standardalsoprovidestheoptiontoobtainthefullyrelaxed
long-termelasticsolutiondirectlyinastaticorsteady-statetransport
g-term
cousdampingstress(theinternal
stressassociatedwitheachoftheProny-riesterms)areincread
graduallyfromtheirvaluesatthebeginningofthesteptotheirlong-termvaluesattheendofthestepifthelong-termvalueisspecified.
Materialoptions
Theviscoelasticmaterialmodelmustbecombinedwithanelasticmaterial
edwiththeisotropiclinearelasticitymodel(“Linear
elasticbehavior,”Section17.2.1)todefineclassical,linear麻杏石甘散 ,small-strain,viscoelasticbehaviororwiththehyperelastic
(“Hyperelasticbehaviorofrubberlikematerials,”Section17.5.1)or
hyperfoam(“Hyperelasticbehaviorinelastomericfoams,”Section17.5.2)
modelstodefinelarge-deformation,nonlinear,viscoelasticbehavior.
Theelasticpropertiesdefinedforthemodelscanbetemperaturedependent.
Viscoelasticitycannotbecombinedwithanyoftheplasticitymodelsor
“Combiningmaterial
behaviors,”Section16.1.3,formoredetails.
Elements
Thetimedomainviscoelasticmaterialmodelcanbeudwithany
stress/displacementorcoupledtemperature-displacementelementinABAQUS.
Output
InadditiontothestandardoutputidentifiersavailableinABAQUS
(“ABAQUS/Standardoutputvariableidentifiers,”Section4.2.1,and
“ABAQUS/Explicitoutputvariableidentifiers,”Section4.2.2),the
followingvariableshavespecialmeaninginABAQUS/Standardifviscoelasticityisdefined:
EE
CE
Thestrainmeasuresareudtoapproximatethestrainenergy,SENER,andthe
viscousdissipation,pproximationsmayleadtounderestimationof
thestrainenergyandoverestimationoftheviscousdissipationsincetheeffectsof
nbeparticularly
noticeableinthecaofnon-monotonicloading.
Forthecaoflarge-strainviscoelasticity,ABAQUS/Explicitdoesnot
performthecomputationoftheviscousdissipationforperformance
d,thecontributionofviscousdissipationisincludedin
thestrainenergyoutput,SENER;uently,
specialcaremustbeexercidwheninterpretingstrainenergyresults
oflarge-strainviscoelasticmaterialsinABAQUS/Explicitsincetheyincludeviscousdissipationeffects.
Elasticstraincorrespondingtothestressstateattime
tandtheinstantaneoulasticmaterialproperties.
Equivalentcreepstraindefinedasthedifferencebetweenthetotalstrainandtheelasticstrain.
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