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COST is supported by the EU Framework Programme Horizon2020 COST Ac(on TU1208 Civil Engineering Applica(ons of Ground Penetra(ng Radar Structural evalua(on of exis(ng pavements based on deflec(on and GPR measurements Author: Carl VAN GEEM BRRC, Belgium This presenta(on is part of the TU1208 Educa(on Pack Thank you to Loredana Matera and Santo Prontera for contribu=ng to the edi=ng and layou=ng of this lecture.

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Page 1: COST Ac(on TU1208 · COST is supported by the EU Framework Programme Horizon2020 COST Ac(on TU1208 Civil Engineering Applica(ons of Ground Penetra(ng Radar Structural evaluaon

COST is supported by the EU Framework Programme Horizon2020

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)

Page 3: COST Ac(on TU1208 · COST is supported by the EU Framework Programme Horizon2020 COST Ac(on TU1208 Civil Engineering Applica(ons of Ground Penetra(ng Radar Structural evaluaon

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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∑

Page 6: COST Ac(on TU1208 · COST is supported by the EU Framework Programme Horizon2020 COST Ac(on TU1208 Civil Engineering Applica(ons of Ground Penetra(ng Radar Structural evaluaon

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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.

Page 8: COST Ac(on TU1208 · COST is supported by the EU Framework Programme Horizon2020 COST Ac(on TU1208 Civil Engineering Applica(ons of Ground Penetra(ng Radar Structural evaluaon

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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

www.facebook.com/COSTAc(onTu1208/

[email protected]

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