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COSTAc(onTU1208CivilEngineeringApplica(onsofGroundPenetra(ngRadar
Structuralevalua(onofexis(ngpavementsbasedondeflec(onandGPRmeasurementsAuthor:CarlVANGEEMBRRC,Belgium
Thispresenta(onispartoftheTU1208Educa(onPack
ThankyoutoLoredanaMateraandSantoPronteraforcontribu=ngtotheedi=ngandlayou=ngofthislecture.
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Summaryofthelecture(1/2)
§ Old-fashionedway:theequivalentsinglelayermodel§ Modernway:theback-calcula=onapproach§ Mul=-layermodelofaroad§ Applica=onofloadsandmeasurementofdeflec=ons
Introduc(ontoapproachesfortheevalua(onofthestructuralproper(esofpavement
Evolu(onofmathema(calmodelsofpavement
§ Pavementmodelsbasedonthetheoryofelas=city§ Pavementmodelsbasedonthestrengthofmaterials§ ModelproposedbyBurmister(1943)
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Summaryofthelecture(2/2)
§ Theequivalentsemi-infinitebody§ Deflec=onsandinterpreta=onofthesurfacemodulus§ Example:Back-calcula=onforathree-layermodelofaroad§ Sensi=vityoftheprocedure
Evalua(onofthebearingcapacityofamul(layeredroadstructure
Applica(on:Back-calcula(onandredesignofaroad
§ Measureddeflec=onsandpresentroadstructure§ Back-calcula=onandredesignwithQualidim§ Studyoftheinfluenceoflayerthicknessesontheroadlife=me
BiographyandcontactdetailsoftheAuthor
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Introduc(ontoapproachesfortheevalua(onofthe
structuralproper(esofpavement
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Theold-fashionedway:equivalentsinglelayermodel
§ Replaceeachlayerofthemul=-layermodeloftheroadbyonelayerwith"equivalent"thicknesshe(thickerthanthesumofthicknesseshi)
Ø Mul=-layermodel:thicknessesh1,h2,…Ø Theso-called‘equivalentfactors’
a1,a2,…canbecalculatedbyusingthefollowingformula:
Ø Thicknessoftheequivalentlayer:
Here, Ei is the layer elas=citymodulus, measured or takenfromatable(thisisaparameterdependingonthelayermaterial)
ai = Ei /5003
he = ai +hi∑
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Equivalentsinglelayermodel:thicknessofoverlay…
§ Determinetraffic(kNc):Past,presentandfuturetraffic § Graphsestablishedin1991(BRRCreportR56/85)
Thicknessesofcrushedstonebasecourseandasphaltlayer
Thicknessofgranularsubbase(fordifferentsoils)
Traffic(kNc) Traffic(kNc)
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Equivalentsinglelayermodel:thicknessofoverlay…
§ TrafficmapsareusedtodeterminethethicknessesH1,H2,H3oftheidealmul=-layerroad.
§ Theidealequivalentthicknessis:He=Σai·Hi(fortheequivalent1-
layermodel).§ Then,dooverlay:W=(He–he)/2.7(withai=2.7forabituminous
layer)istheneededthicknessofthebituminousoverlay,inordertoachieveequivalencewiththeidealmul=-layerroadstructure.
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Themodernway:back-calcula(onapproach
§ Objec=ve:DetermineE-modulesofalllayers
Ø Computedeflec=onbowlfromamul=-layermodelØ Comparethecomputeddeflec=onbowlwiththemeasureddeflec=onbowlØ Ifdeflec=onbowlsarenot"iden=cal"thenmodifyE-modulesanditerate…
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Themodernway:back-calcula(onapproach
§ Thenredesignthe"currentstructure+overlay"(asifyouaredesigninganewroad)withasuitablesojwareandes=matetheexpectedlife=me.
§ Ifresultsarepoor,thendochangesindeeperpartoftheroadstructure.
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Back-calcula(onsoWwaretools
§ Freesojware:Ø “Qualidim”:IntendedforBelgium,tobeusedbynon-specialists
§ Commercialsojware:
Ø Alizé-LCPC(itech-soj)Ø PAVERS(VIAAperta)Ø Rosy(SWECO–carlBro)Ø ELMOD(Dynatest)
Ø …
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Defini(onandseZngsofthedeflec(ondeviceused
Deflec(onsandsurfacemodulus
Comparisonbetweenmeasuredand
computeddeflec(ons
Computedelas(citymoduli
Proper(esofmaterialsDivers
Back-calcula(on:Qualidim
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Modeloftheroad:amul(-layer
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Applica(onofloadsandtheireffects
chargeof50kN,p=0,7MPa(r=150mm)
Subbase E3,µ3
Basecourse E2,µ2
Soil E4,µ4
Tensilestress
Ver(caldeforma(on
Asphaltlayer E1,µ1Tensilestress
§ Aloadisappliedtothemul=-layersystem…
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h 1 E 1 Pavement
h 2 E 2 Base course
h 3 E 3
E 4
Subbase
Soil
Distribu(onoftheloadandmeasurementofdeflec(ons
Ø Thefartherthedeflec=onismeasuredfromthecentreofimpact,thelessthedeflec=oniscausedbytheupperpartoftheroadstructure…
§ Onlythepartofthepavementthatissubjectedtostresses,willdeform…(i.e.onlytheareainsidetheredcone,inthesketch)
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Evolu(onofmathema(calmodelsinpavementdesign
Seealsothebook:
FransVanCauwelaert,«Pavementdesignandevalua(on:Therequiredmathema(csandapplica(ons,»ISBN978-2-960043-00-6
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Pavementmodelsbasedonthetheoryofelas(city
Ø Thesubgradeisanisotropicbody(Boussinesq,1883)
σ z =−3P2πz2
Ø Defini=onofastressconcentra=onfactor(Fröhlich,1934)
σ z =−νP2πz2
Concentra(on:ν>3Dispersion:ν<3
Ø Thesubgradeisanorthotropicbody(Lekhnitskii,1963)
σ z =−1+ s+ s2s2
P2πz2
s2 = n−µ2
n2 −µ2 n=EvertEhor
§ Semi-infinitebodysubjectedtoaver=calloadP
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Vertical stress vs anisotropy
0
0.2
0.4
0.6
0.8
1
0 50 100 150 200 250Depth z
Stre
ss n=2n=1n=0.5
(Lekhnitskii,1963)
Pavementmodelsbasedonthetheoryofelas(city
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Pavementmodelsbasedonthestrengthofmaterials
Ø Equilibriumequa=on
∂2
∂r2+1r∂
∂r
⎛
⎝⎜⎜
⎞
⎠⎟⎟∂2w∂r2
+1r∂w∂r
⎛
⎝⎜⎜
⎞
⎠⎟⎟=
p−qD
Ø Westergaard(1924):Thesubgradeisaseriesofver=calsprings(k)
q= kw
Ø Pasternak (1954): The subgrade is a series of ver=cal (k) andhorizontalsprings(G)
q=−G ∂2w∂r2
+1r∂w∂r
⎛
⎝⎜⎜
⎞
⎠⎟⎟+kw
§ Slabsubjectedtoaver=calpressurep
p
q
E,I
k,G
D
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Surface deflection
0
0.05
0.1
0.15
0.2
0.25
0 500 1000 1500 2000 2500
Distance from the axis
Def
lect
ion
WestergaardPasternak
Pavementmodelsbasedonthestrengthofmaterials
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Ø Hypothesesofthetheoryofelas=city:equilibrium,con=nuityandelas=cityforeachlayer
ModelproposedbyBurmister(1943)§ Mul=layeredstructure
p
E1
E2
E3
h1
h2
∞
2a
∂2
∂r2+1r∂
∂r+∂2
∂z2⎛
⎝⎜⎜
⎞
⎠⎟⎟∂2ϕi
∂r2+1r∂ϕi
∂r+∂2ϕi
∂z2⎛
⎝⎜⎜
⎞
⎠⎟⎟=0
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§ Mathema=calsolu=on(here,weskipthemathema=calsteps,butyouareencouragedtocalculatethem!)
∂2
∂r2+1r∂
∂r+∂2
∂z2⎛
⎝⎜⎜
⎞
⎠⎟⎟∂2ϕi
∂r2+1r∂ϕi
∂r+∂2ϕi
∂z2⎛
⎝⎜⎜
⎞
⎠⎟⎟=0
Byintroducingintheequa=ontheexpressionφ(r,z)=J0(mr)f(z),weobtain:
∂2
∂r2+1r∂
∂r
⎛
⎝⎜⎜
⎞
⎠⎟⎟ J0(mr)=−m2 J0(mr)
J0(mr) m4 −2m2 ∂2
∂z2+∂4
∂z4⎛
⎝⎜⎜
⎞
⎠⎟⎟ f (z)=0
ϕi(r ,z)= J0(mr) Aiemz −Bie−mz + zCiemz − zDie−mz( )
ModelproposedbyBurmister(1943)
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§ Stressesanddisplacements(again,weignorethemathema=calstepsleadingtotheseformulas):
σ z = f (r) Am2emz +Bm2e−mz −(1−2µ+mz)Cmemz +(1−2µ−mz)Dme−mz{ }
τ rz = f (r) Am2emz −Bm2e−mz +(2µ+mz)Cmemz +(2µ−mz)Dme−mz{ }
u= f (r)E
Am2emz +Bm2e−mz +(1+mz)Cmemz −(1−mz)Dme−mz{ }
w =f (r)E
Am2emy −Bm2e−my −(2−4µ−mz)Cmemz −(2−4µ+mz)Dme−mz{ }
ModelproposedbyBurmister(1943)
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Boundarycondi(ons(Burmister)§ Surface(load) p
Ø Ver=calstress=-pØ Shearstress=0
§ Interfaces(layersincontact)Ø Ver=calstressesareallequalØ ShearstressesareallequalØ Deflec=onsareallequal
§ Interfaces:horizontalcondi=on,therearethreealterna=ves:Ø Displacementsareequal:Fric=onØ Shearforcesarenull:SlipØ Intermediatescenario:Par=alfric=on
§ Subgrade,therearetwoalterna=vesØ Semi-infinitebodyØ Fixedbouom
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Evalua(onofthebearingcapacityofamul(layeredroadstructure
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Theequivalentsemi-infinitebody
r r
E1h1
E2h2
E0
A A
E0h1,eq
E0h2,eq
E0 B
z
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Thefurtherawayfromthecentreofpressure…
)()()1()(2
20 iwir
paiE µ−=
§ Deflec=on “at the centre of impact”: is influencedby thewhole roadstructureàhence,thederivedsurfacemoduluscharacterizesthewholeroadstructure
§ Deflec=on“faraway”fromthecentreofimpact:itisinfluencedbythelowerpartoftheroadstructure,onlyà hence, the derived surface modulus characterizes the lower part of theroadstructure
h 1 E 1 Pavement
h 2 E 2 Base course
h 3 E 3
E 4
Subbase
Soil
r(0),w(0) r(600),w(600)
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Iden(caldeflec(ons
2a
r
z
z1r1
A
B
w(z)= 1+µE
P2π .z (3−2µ)
w(r)= 2(1−µ2)
EP2π .r
w(r)=w(z /2→2z /3)Simpletransforma=on:
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Interpre(ngthesurfacemodulus
§ ThesurfacemodulusE0(i)correspondstothedeflec=onw(i)measuredatadistancer(i)
E0(i)=2(1−µ2)r(i)w(i)
P2π = pa2 (1−µ
2)r(i)w(i)
Ø Pressurep,radiusa,Poissoncoefficient(Poisson’sra=o)μ
Ø Modelused:Boussinesq’stheory,computa=onoftheelas=cmodulusofahomogeneoushalf-space
§ So,fromthemeasureddeflec=onw(i)atadistancer(i),wecancomputethesurfacemodulusE0(i)
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Example:ComputeE0,thendrawconclusionsontheE-moduliofthedifferentlayersofthe3-layermodel
030060090012001500180021002400
0 500 1000 1500 2000 2500
E0
Distances
030060090012001500180021002400
0 500 1000 1500 2000 2500 3000 3500
E0
Distances
030060090012001500180021002400
0 100 200 300 400 500 600 700
E0
Distances
0
300
600900
1200
1500
18002100
2400
0 500 1000 1500 2000 2500 3000 3500
E0
Disatances Athree-layerroadmodelwithanincreasing
modulusofthesubgradeoras(ffbolom
Athree-layerroadmodelwithaweakinterlayer
Athree-layerroadmodelwithas(ffinterlayer
Athree-layerroadmodelwithdecreasingmoduli
§ Input:Measureddeflec=onsatdifferentdistancesfromloadcentre
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Back-calcula(onofathree-layer(1/2)
§ Letw1,w2,…wnbethedeflec=onsatthedistancesr1,r2,…,rn
§ LetusassumetheseedvaluesE10,E20,E30
§ Wecomputethetheore=caldeflec=onsz0(1),z0(2),…,z0(n)
§ WechooseE11=E10∙z0(1)/w0,E21=E20∙z0(2)/w1,E31=E30∙z0(n)/wn
§ WithE11,E20,E30,wecomputez1(1),z1(2),…z1(n)
§ WithE10,E21,E30,wecomputez2(1),z2(2),…z2(n)§ WithE10,E20,E31,wecomputez3(1),z3(2),…z3(n)
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Back-calcula(onofathree-layer(2/2)
§ Weapplythe“AlBushIII”algorithm:Ø Fork=0to3,wedefine:
zk(i)=a(i)logE1.+b(i)logE2.+c(i)logE3.+d(i)
§ Fromthis,wecomputethesolu=onfora(i),b(i),c(i),d(i)Ø Weintroducetheseinthenequa=ons(i=1,..,n):
z0(i)=a(i)logE1+b(i)logE2+c(i)logE3+d(i)
Ø Weminimise [ ]2)()(
10∑ −
n
iziw andobtaintheexpectedvaluesE1,E2,E3
§ Ifthissumofsquaresis“smallenough”thenwestopØ ElseweiteratewithE1,E2,E3asnewseedvalues…
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Sensi(vityoftheprocedure§ GivenE1=10000,E2=3000,E3=500
Ø Wecomputew(0)=69.6,w(1)=38.1,w(2)=26.2,w(3)=19.1,w(4)=14.3,w(5)=11.2,w(6)=9.0,w(7)=7.5,w(8)=6.5
Backcalcula(on
w(0) E1 E2 E3 Fit Loops
69.6 10036 2993 500 0.02 7
75.0 6469 3351 503 0.06 6
58.0 33840 2371 497 0.10 7
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Applica(on:Back-calcula(onandredesignofaroad
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Deflec(ons&presentroadstructure
Distancesri(mm) 0 300 600 900 1200 1500 1800
Deflec(onswi(µm) 91 76 59 46 36 30 26
§ Deflec=onsmeasuredwithaFWDinthemiddleofaconcreteslab:
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Layer/Typeofmaterial Thickness(mm)
Modulus(N/mm2) PoissonRa(o
Concreteslabs(nodowels) 180 37000 0.20
Basecourse 500 2000 0.35
Stabilizedsubbase 350 0.50
§ Presentroadstructure,hypothe=calE-moduli(seedvalues):
Deflec(ons&presentroadstructure
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Back-calcula(on
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Layer/Typeofmaterial Thickness(mm)
Modulus(N/mm2)
PoissonRa(o
Concreteslabs(nodowels) 180 35928 0.20
Basecourse 500 1081 0.35
Stabilizedsubbase 335 0.50
§ Results(withsojwareQualidim©):
Layer/Typeofmaterial Thickness(mm)
Modulus(N/mm2)
PoissonRa(o
Concreteslabs(nodowels) 180 37000 0.20
Basecourse 500 2000 0.35
Stabilizedsubbase 350 0.50
§ Presentstructure,hypothe=calE-moduli(seedvalues):
Back-calcula(on
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Qualidim§ Designingnewroads…
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Completelynewroadstructure
Es(ma(onoftrafficandexpectedlife(me
Qualidim
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§ Overlayonexis=ngroad…
Qualidim
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Es(mateoftrafficandexpectedlife-(me
Exis(ngstructure,Back-calculatedE-moduli
Qualidim
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Evalua(onwithatheore(calmodel
Layer/Typeofmaterial Thickness(mm)
Modulus(N/mm2) PoissonRa(o
Concreteslabs(nodowels)
Between180and200 37661 0.20
Unboundbasecourse,granularmaterialTypeI 400 650 0.45
subbase(stabilizedwithchalk) 200 2000 0.50
Clayground 20 0.50
Axleload: 50kN 90kN 120kN
100trucksperday,300daysperyear
20% 60% 20%
§ Concept:Theore=calstructure:
§ Traffic:100trucks/day,300days/year,growth+2%peryear:
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Studyoftheinfluenceofthicknessontheroadlife(me…
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Stucturesimilartotheexis(ngone
Study:usealterna(velyback-calculatedandtheore(calE-moduli…
Es(ma(onoftrafficandexpected
life(me
Studyoftheinfluenceofthicknessontheroadlife(me…
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2cmextrathicknessisimportant!§ Loweringthethicknessoftheconcreteslabinthetheore=cal
modelmakesthees=matedlife=medropdras=cally
Thicknessofconcreteslab(mm) 200 190 180
NumberofstandardaxlesNcthatcangoovertheroad
2.45*106 6.60*105 1.52*105
Es(matedlife-(me(inyears) >40 18 5
Ø Note:thisdoesnotmeanthatthethicknessesofthelayersunderneathareofnosignificance…
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AuthorDr.CarlVanGeem([email protected]) isa researcher inroadmanagement andmonitoring techniques, since 2004he is working in the Mobility, security and roadmanagement(MSM)divisionoftheBelgianRoadResearchCentre(BRRC),inBrussels,Belgium.HeisaWorkingGroupMemberoftheCOSTAc=onTU1208.In 1996, Carl Van Geem earned the doctoral degree intechnicalsciencesfromtheResearch Ins=tuteonSymbolicComputa=on (RISC-Linz), Johannes Kepler University, Linz,Austria.TheBRRChasseveraldevicesfortheevalua=onofroadsurfaceproper=es(roughness,skidresistence), for pavement management (visual inspec=on device “SAND”), and formeasuringthebearingcapacityofroads(FWD,curviameter,GPR).ThemaintopicofCarl’sresearchistheinterpreta=onofdataobtainedwiththesemonitoringdevicesforanop=malmanagementof roadmaintenance.Carl par=cipated in several na=onal and interna=onalresearchprojects,includinga“na=onalpre-norma=veresearchprojectontheindicatorsofroughness”,theCOSTAc=on354“PerformanceIndicatorsforRoadPavements”,thePIARCtechnicalcommiueeD1“ManagementofRoadInfrastructureAssets”,andtheFP7project“Tomorrow'sRoadInfrastructureMonitoringandManagement(TRIMM)”.
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Thank you COSTAc(onTU1208CivilEngineeringApplica(onsofGroundPenetra(ngRadar
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