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Optimization-Based Inverse Identification of the Parameters of a Concrete Cap Material Model

Abstract

Issues concerning the advanced numerical analysis of concrete building structures in sophisticated computing systems currently require the involvement of nonlinear mechanics tools. The efforts to design safer, more durable and mainly more economically efficient concrete structures are supported via the use of advanced nonlinear concrete material models and the geometrically nonlinear approach. The application of nonlinear mechanics tools undoubtedly presents another step towards the approximation of the real behaviour of concrete building structures within the framework of computer numerical simulations. However, the success rate of this application depends on having a perfect understanding of the behaviour of the concrete material models used and having a perfect understanding of the used material model parameters meaning. The effective application of nonlinear concrete material models within computer simulations often becomes very problematic because these material models very often contain parameters (material constants) whose values are difficult to obtain. However, getting of the correct values of material parameters is very important to ensure proper function of a concrete material model used. Today, one possibility, which permits successful solution of the mentioned problem, is the use of optimization algorithms for the purpose of the optimization-based inverse material parameter identification. Parameter identification goes hand in hand with experimental investigation while it trying to find parameter values of the used material model so that the resulting data obtained from the computer simulation will best approximate the experimental data. This paper is focused on the optimization-based inverse identification of the parameters of a concrete cap material model which is known under the name the Continuous Surface Cap Model. Within this paper, material parameters of the model are identified on the basis of interaction between nonlinear computer simulations, gradient based and nature inspired optimization algorithms and experimental data, the latter of which take the form of a load-extension curve obtained from the evaluation of uniaxial tensile test results. The aim of this research was to obtain material model parameters corresponding to the quasi-static tensile loading which may be further used for the research involving dynamic and high-speed tensile loading. Based on the obtained results it can be concluded that the set goal has been reached.

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Optimization-Based Inverse Identification of the Parameters of a Concrete Cap Material Model

Author: Král, Petr; Hokeš, Filip; Hušek, Martin; Kala, Jiří; Hradil, Petr
Publisher: IOP Publishing
Year: 2017
DOI: 10.1088/1757-899X/245/3/032078
Source: https://dspace.vut.cz/bitstreams/8348cd4f-1907-4ff5-9549-359031fb0314/download
IOP Con e ence Se ies: Ma e ials Science and Enginee ing
PAPER • OPEN ACCESS
Op imiza ion-Based In e se Iden i ica ion o he
Pa ame e s o a Conc e e Cap Ma e ial Model
To ci e his a icle: Pe K ál e al 2017 IOP Con . Se .: Ma e . Sci. Eng. 245 032078
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IOP Con . Se ies: Ma e ials Science and Enginee ing 245 (2017) 032078 doi:10.1088/1757-899X/245/3/032078
Op imiza ion-Based In e se Iden i ica ion o he Pa ame e s
o a Conc e e Cap Ma e ial Model
Pe K ál 1, Filip Hokeš 1, Ma in Hušek 1, Jiří Kala 1, Pe H adil 1
1 Facul y o Ci il Enginee ing, Ins i u e o S uc u al Mechanics, B no Uni e si y o
Technology, Ve eří 331/95, 602 00 B no, Czech Republic
[email p o ec ed]
Abs ac . Issues conce ning he ad anced nume ical analysis o conc e e building s uc u es in
sophis ica ed compu ing sys ems cu en ly equi e he in ol emen o nonlinea mechanics
ools. The e o s o design sa e , mo e du able and mainly mo e economically e icien
conc e e s uc u es a e suppo ed ia he use o ad anced nonlinea conc e e ma e ial models
and he geome ically nonlinea app oach. The applica ion o nonlinea mechanics ools
undoub edly p esen s ano he s ep owa ds he app oxima ion o he eal beha iou o conc e e
building s uc u es wi hin he amewo k o compu e nume ical simula ions. Howe e , he
success a e o his applica ion depends on ha ing a pe ec unde s anding o he beha iou o
he conc e e ma e ial models used and ha ing a pe ec unde s anding o he used ma e ial
model pa ame e s meaning. The e ec i e applica ion o nonlinea conc e e ma e ial models
wi hin compu e simula ions o en becomes e y p oblema ic because hese ma e ial models
e y o en con ain pa ame e s (ma e ial cons an s) whose alues a e di icul o ob ain.
Howe e , ge ing o he co ec alues o ma e ial pa ame e s is e y impo an o ensu e
p ope unc ion o a conc e e ma e ial model used. Today, one possibili y, which pe mi s
success ul solu ion o he men ioned p oblem, is he use o op imiza ion algo i hms o he
pu pose o he op imiza ion-based in e se ma e ial pa ame e iden i ica ion. Pa ame e
iden i ica ion goes hand in hand wi h expe imen al in es iga ion while i ying o ind
pa ame e alues o he used ma e ial model so ha he esul ing da a ob ained om he
compu e simula ion will bes app oxima e he expe imen al da a. This pape is ocused on he
op imiza ion-based in e se iden i ica ion o he pa ame e s o a conc e e cap ma e ial model
which is known unde he name he Con inuous Su ace Cap Model. Wi hin his pape ,
ma e ial pa ame e s o he model a e iden i ied on he basis o in e ac ion be ween nonlinea
compu e simula ions, g adien based and na u e inspi ed op imiza ion algo i hms and
expe imen al da a, he la e o which ake he o m o a load-ex ension cu e ob ained om he
e alua ion o uniaxial ensile es esul s. The aim o his esea ch was o ob ain ma e ial model
pa ame e s co esponding o he quasi-s a ic ensile loading which may be u he used o he
esea ch in ol ing dynamic and high-speed ensile loading. Based on he ob ained esul s i can
be concluded ha he se goal has been eached.
1. In oduc ion
Con inuous and ex ensi e use o conc e e o he pu pose o building he new s uc u es cu en ly
leads o he e o s o e ine he design o conc e e s uc u es h ough he compu e nume ical
simula ions based on he ini e elemen me hod [1-3]. These e o s ela ed o he design o sa e , mo e
du able and mo e economically e icien conc e e s uc u es, howe e , equi e he in ol emen o
2
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IOP Con . Se ies: Ma e ials Science and Enginee ing 245 (2017) 032078 doi:10.1088/1757-899X/245/3/032078
ools o he ad anced nume ical analysis. The in ol emen o ools o he ad anced nume ical analysis
especially means ha i is necessa y o conside he nonlinea beha iou o conc e e wi hin he con ex
o compu e simula ions in ended o he analysis and design o conc e e s uc u es. Cu en
compu a ional sys ems based on he ini e elemen me hod, which include o example he p og ams
ANSYS [4], LS-Dyna [5] o A ena [6], o e a ela i ely la ge amoun o ma e ial models which a e
sui able o desc ibing he nonlinea beha iou o conc e e. These nonlinea ma e ial models o
conc e e may ind he use in he s a ic nume ical simula ions bu also in he dynamic nume ical
simula ions and a numbe o publica ions is de o ed o hei desc ip ion and p ac ical applica ion [7-
10]. Howe e , he bigges p oblem ela ed o he use o he nonlinea ma e ial models o conc e e is
o en he inabili y o p ope ly de ine he alues o he ma e ial pa ame e s (cons an s) because hey can
o en be ob ained only on he basis o he special es s o conc e e. Some pa ame e s ha e e en only
pu ely ma hema ical meaning and de ining o hei alues is no , he e o e, so easy. Howe e , he
co ec de ini ion o pa ame e alues o he used ma e ial model is ex emely impo an o he co ec
desc ip ion o he beha iou o conc e e wi hin he compu e simula ion. Solu ion o he men ioned
p oblem is cu en ly possible wi h he use o so-called he in e se analysis [11, 12].
In e se analysis, o he wise known as in e se iden i ica ion, allows o ind such pa ame e alues o
he used nonlinea conc e e ma e ial model whe ein he esul ing esponse o he s uc u e ob ained
om he compu e simula ion is e y simila o he expe imen ally measu ed esponse o he conc e e
s uc u e. The p inciple o he in e se analysis is based on a combina ion o nume ical and
expe imen al analysis wi h op imiza ion algo i hms, me hods o p ocedu es. Cu en ly, he mos used
me hods o he in e se pa ame e iden i ica ion o nonlinea ma e ial models o conc e e a e me hods
based on he exe cise o a i icial neu al ne wo ks [13]. A e y powe ul ool in he ield o he in e se
analysis is also he op iSLang p og am [14] which includes a a ie y o op imiza ion algo i hms
sui able o he op imiza ion-based in e se iden i ica ion o he ma e ial pa ame e s [15, 16].
This pape is ocused on he op imiza ion-based in e se iden i ica ion o he pa ame e s o a
conc e e cap ma e ial model which is known unde he name he Con inuous Su ace Cap Model and
which is implemen ed in an explici ini e elemen sol e LS-Dyna [17]. Wi hin his pape , pa ame e s
o he ma e ial model a e iden i ied on he basis o in e ac ion be ween nonlinea compu e
simula ions, g adien based and na u e inspi ed op imiza ion algo i hms implemen ed in he op iSLang
p og am and expe imen al da a, he la e o which ake he o m o a load-ex ension cu e ob ained
om he e alua ion o uncon ined uniaxial ensile es esul s.
2. Uncon ined uniaxial ensile es s
The p ocess o he op imiza ion-based in e se pa ame e iden i ica ion pe o med in his pape
equi ed he expe imen al da a. Fo his pu pose, he expe imen al da a ob ained om he e alua ion o
uncon ined uniaxial ensile es esul s ha we e made wi hin [18] we e used. Used expe imen al da a
ook he o m o a load-ex ension cu e which desc ibed he nonlinea beha iou o conc e e es
specimens du ing he uncon ined uniaxial ensile loading. The load-ex ension cu e is shown in igu e
1.
Conc e e es specimens used wi hin he o iginal uncon ined uniaxial ensile es s pe o med in he
con ex o [18] had dimensions 305 x 60 x 19 mm3 (leng h x wid h x dep h o he c i ical c oss-
sec ional a ea). The es specimens we e manu ac u ed and hen hey we e subjec ed o he conc e e
ha dening p ocess which las ed 28 days. The uniaxial comp ession s eng h o he 28 days old and
ha dened conc e e was 44 MPa. The maximum agg ega e size used was 10 mm. The expe imen al da a
we e measu ed in 85 mm leng h o each es specimen. Du ing he uncon ined uniaxial ensile loading,
conc e e es specimens we e s e ched a a quasi-s a ic cons an loading eloci y.
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I is clea om igu e 1 ha du ing he uncon ined uniaxial ensile loading, he conc e e es
specimens i s exhibi ed linea ly elas ic beha iou be o e eaching he maximum ensile o ce (i.e. he
maximum ensile load capaci y o he conc e e es specimens). A e eaching he maximum ensile
o ce, he conc e e es specimens began o show signs o ensile s ain so ening. The ensile s ain
so ening o he conc e e began o asse i sel as a esul o he damage o he conc e e es specimens
as he ul ima e s eng h o he conc e e in uniaxial ension was eached.
Figu e 1. Expe imen ally-measu ed load-ex ension cu e.
3. Compu e simula ions
The p ocess o he op imiza ion-based in e se pa ame e iden i ica ion pe o med in his pape u he
demanded pe o ming o nonlinea compu e simula ions. Fo his pu pose, he simpli ied
compu a ional model o he uncon ined uniaxial ensile es was c ea ed in LS-Dyna so wa e which is
based on an explici ini e elemen me hod and in which he nonlinea compu e simula ions we e
pe o med.
3.1. The compu a ional model
Agains he eal uncon ined uniaxial ensile es , he compu a ional model o his es c ea ed wi hin
his pape was e y simpli ied. Only he c i ical pa o he es specimen was modelled. This means
ha he ini e elemen model o he es specimen ook he o m only o he measu ed pa o he es
specimen wi h he leng h o 85 mm. Explici 3-D s uc u al ini e elemen s we e used o c ea ion o
he ini e elemen model. In e ms o bounda y condi ions, suppo s we e no applied wi hin he
con ex o he ini e elemen model. Howe e , linea ly inc eased e ical displacemen s o e ime we e
p esc ibed o nodes o bo h bases o he ini e elemen model, see igu e 2. These displacemen s
simula ed he axial s e ching o he model a a cons an loading eloci y. The nonlinea ma e ial
beha iou o he model was modelled h ough he Con inuous Su ace Cap ma e ial model [19, 20].
The men ioned simpli ica ions in oduced in o he compu a ional model o he uncon ined uniaxial
ensile es we e accep able because leng h and c oss-sec ional a ea o he ini e elemen model
co esponded o leng hs and c i ical c oss-sec ional a eas o he conc e e es specimens o which he
expe imen al da a we e measu ed. The simpli ica ions we e also accep able om he an age poin o
damage. In eal es s he damage occu ed always jus on he measu ed leng h o he es specimen in
he place o he c i ical c oss-sec ional a ea. I ollows ha in e ms o he damage, i was necessa y o
cons uc a ini e elemen model a leas as he measu ed pa o he es specimen wi h he c i ical
c oss-sec ional a ea. This necessi y was me wi hin he con ex o his pape .
The compu a ional model used wi hin his pape is shown in igu e 2.
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IOP Con . Se ies: Ma e ials Science and Enginee ing 245 (2017) 032078 doi:10.1088/1757-899X/245/3/032078
Figu e 2. The compu a ional model.
3.2. Nonlinea ma e ial model o conc e e
In his pape , nonlinea ma e ial beha iou was included in o he compu a ional model h ough he
ma e ial model which is known unde he name he Con inuous Su ace Cap Model [19, 20]. This
ma e ial model is a pa o he ma e ial model lib a y which is implemen ed in LS-Dyna so wa e.
Theo e ical backg ound o he Con inuous Su ace Cap Model is based on a yield su ace which is
de ined as a unc ion o h ee s ess in a ian s acco ding o he equa ion [21, 22]:
22
123 2 3 1 1
(, , ) ( ) () (,)
c
YI J J J J F I F I

 (1)
whe e I1 is he i s in a ian o he s ess enso , J2 and J3 a e in a ian s o he de ia o y s ess enso
(second and hi d), (J3) is he Rubin s eng h educ ion ac o and

is he cap ha dening pa ame e .
The yield su ace is composed o wo pa s. These being he shea ailu e su ace F (I1) and he
ha dening compac ion su ace Fc (I1,

). The exp ession o he shea ailu e su ace is gi en by
equa ion:
1
11
() expI
FI I




  (2)
whe e

,

, λ, and

a e he ma e ial cons an s which a e usually de e mined on he basis o he iaxial
comp ession es s. The ha dening compac ion su ace is de ined by equa ions:
2
1
12
(())
(,) 1 (() ())
c
IL
FI XL



  o 1()IL

 (3)
1
(,) 1
c
FI


o 1()IL


(4)

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in a con ex wi h equa ions:
()L



o 0


 (5)
0
()L



o 0



(6)
1
() () ()
XLRFI



 (7)
whe e R is he cap aspec a io. Wi hin he yield su ace, he shea ailu e su ace and ha dening
compac ion su ace a e combined using a mul iplica i e o mula ion which allows hei combina ion
o be con inuous and smoo h a hei in e sec ion.
The Con inuous Su ace Cap Model allows wi hin i s o mula ion o ake in o accoun he e ec o
s ain a e on he esul ing s ess s a e. Howe e , his model capabili y can be neglec ed du ing he
calcula ions. The esponse o he model is hen always quasi-s a ic and independen o compu a ional
ime. Due o he men ioned ac s, i is clea ha he ma e ial model can be used in dynamic, bu also in
quasi-s a ic o s a ic, compu e simula ions. The ac , ha he ma e ial model allows o calcula e he
quasi-s a ic esponse, was used wi hin his pape .
Table 1. The iden i ied ma e ial pa ame e s o he Con inuous Su ace Cap Model.
Ma e ial
pa ame e Pa ame e desc ip ion Uni
RO Mass densi y, ρ. Mg/mm3
E Young’s modulus, E. MPa
PR Poisson’s a io, ν. -
ALPHA T iaxial comp ession su ace cons an e m, α. MPa
THETA T iaxial comp ession su ace linea e m, θ. -
LAMDA T iaxial comp ession su ace nonlinea e m, λ. MPa
BETA T iaxial comp ession su ace exponen , β. MPa-1
ALPHA1 To sion su ace cons an e m, α1. -
THETA1 To sion su ace linea e m, θ1. MPa-1
LAMDA1 To sion su ace nonlinea e m, λ1. -
BETA1 To sion su ace exponen , β1. MPa-1
ALPHA2 T iaxial ex ension su ace cons an e m, α2. -
THETA2 T iaxial ex ension su ace linea e m, θ2. MPa-1
LAMDA2 T iaxial ex ension su ace nonlinea e m, λ2. -
BETA2 T iaxial ex ension su ace exponen , β2. MPa-1
R Cap aspec a io, R. -
X0 Cap ini ial loca ion, X0. MPa
W Maximum plas ic olume compac ion, W. -
D1 Linea shape pa ame e , D1. MPa
D2 Quad a ic shape pa ame e , D2. MPa2
B Duc ile shape so ening pa ame e , B. -
GFC F ac u e ene gy in uniaxial s ess, G c. N/mm
D B i le shape so ening pa ame e , D. -
GFT F ac u e ene gy in uniaxial ension, G . N/mm
GFS F ac u e ene gy in pu e shea s ess, G s. N/mm
The Con inuous Su ace Cap ma e ial model is implemen ed in LS-Dyna so wa e in wo
modi ica ions, speci ically as he gene al e sion *MAT_CSCM and he modi ied e sion
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*MAT_CSCM_CONCRETE [17]. The gene al e sion *MAT_CSCM o he ma e ial model was used
in calcula ions pe o med wi hin his pape . In o de o ob ain he mos ealis ic esponse o he model,
a o al o 25 pa ame e s (cons an s) o he ma e ial model e sion *MAT_CSCM we e iden i ied.
Howe e , he ma e ial pa ame e s G (shea modulus) and K (bulk modulus), which o iginally
belonged be ween iden i ied pa ame e s, we e eplaced by pa ame e s E (Young’s modulus) and PR
(Poisson’s a io, ν) due o hei dependency on hese pa ame e s acco ding o he equa ions:
2(1 )
E
G



(8)
3(1 2 )
E
K

 (9)
Desc ip ions and used uni s o men ioned 25 iden i ied ma e ial pa ame e s a e gi en in able 1
[17].
4. Op imiza ion-based in e se pa ame e iden i ica ion
In his pape , he op imiza ion-based in e se pa ame e iden i ica ion was pe o med using he
op iSLang p og am and consis ed o h ee s eps:
1. Sensi i i y analysis
2. Global op imiza ion
3. Local op imiza ion
4.1. Sensi i i y analysis
The sensi i i y analysis [23, 24] o med he i s s ep o he whole ma e ial pa ame e iden i ica ion
p ocess. Wi hin he con ex o his i s s ep he sensi i i y o he inpu a iable da a o he de ined
e e ence esponse was analyzed. The inpu a iable da a we e ep esen ed by indi idual ma e ial
pa ame e s ha we e o be iden i ied and ha o med so-called design ec o . Re e ence esponse was
ep esen ed by indi idual poin s lying on he used expe imen ally-measu ed load-ex ension cu e. The
majo goal o he sensi i i y analysis was o educe he numbe o iden i ied ma e ial pa ame e s in he
design ec o o he necessa y minimum. Ano he goal was o modi y he ange o a iabili y o he
indi idual ma e ial pa ame e s con ained in he design ec o .
Sensi i i y analysis was ca ied ou ia he s a is ical me hod known as he La in Hype cube
Sampling (LHS) me hod [14]. Based on his me hod, a o al o 300 andom ealiza ions o he design
ec o we e gene a ed. The gene a ed amoun o andom ealiza ions su icien ly co e ed he design
space.
The esul s p oduced by he sensi i i y analysis indica ed ha only 11 iden i ied ma e ial
pa ame e s ou o he o al o 25 exe ed majo in luence on he esul an o m o he nume ically-
simula ed load-ex ension cu e. The e o e, o he subsequen global and local op imiza ion he
o iginal design ec o , which con ained all 25 iden i ied ma e ial pa ame e s gi en in able 1, was
educed o he design ec o which con ained only men ioned 11 pa ame e s exe ed majo in luence
on he esul an o m o he load-ex ension cu e. A e he educ ion he design ec o acqui ed he
ollowing o m:

T
,,, ,,2,2,2,,,
E
ALPHA THETA LAMDA BETA THETA BETA D D GFT GFS
educed
X (10)
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IOP Con . Se ies: Ma e ials Science and Enginee ing 245 (2017) 032078 doi:10.1088/1757-899X/245/3/032078
In he educed design ec o X educed you can see he men ioned 11 ma e ial pa ame e s.
The alues o he p e-op imized ma e ial pa ame e s and objec i e unc ion (EUCLID_NORM)
ob ained om he bes andom ealiza ion gene a ed by LHS me hod a e gi en in able 2.
Table 2. The esul ing iden i ied ma e ial pa ame e alues o he Con inuous Su ace Cap Model.
Ma e ial pa ame e Uni
Sensi i i y
analysis
(LHS me hod)
Global and local
op imiza ion
(NLPQL and PSO
me hods)
Global
op imiza ion
(NLPQL
me hod)
Local
op imiza ion
(PSO
me hod)
P e-op imized
alues De e minis ic alues Op imized
alues
Op imized
alues
RO Mg/mm3 2.32910-9 2.40010-9 - -
E MPa 31600 - 31600 30862
PR - 0.1855 0.1500 - -
ALPHA MPa 15.509 - 15.509 15.432
THETA - 0.3432 - 0.3216 0.3186
LAMDA MPa 10.388 - 10.388 10.257
BETA MPa-1 2.18510-2 - 2.18910-2 2.19710-2
ALPHA1 - 0.7441 0.6500 - -
THETA1 MPa-1 1.14810-3 0.70010-3 - -
LAMDA1 - 0.1908 0.1600 - -
BETA1 MPa-1 6.22410-2 4.50010-2 - -
ALPHA2 - 0.6184 0.5800 - -
THETA2 MPa-1 7.99510-4 - 7.99510-4 8.51410-4
LAMDA2 - 0.1645 0.1200 - -
BETA2 MPa-1 7.11210-2 - 7.11210-2 7.26410-2
R - 5.2871 4.7000 - -
X0 MPa 104.584 95.000 - -
W - 6.61410-2 4.00010-2 - -
D1 MPa 2.84910-4 2.00010-4 - -
D2 MPa2 3.44510-7 - 3.44510-7 3.42410-7
B - 81.988 100.000 - -
GFC N/mm 4.6363 2.6000 - -
D - 0.2678 - 0.1638 0.1000
GFT N/mm 4.97410-2 - 4.79810-2 4.82710-2
GFS N/mm 4.11610-2 - 6.34310-2 6.28410-2
EUCLID_NORM kN 0.344427 - 0.280801 0.252410
4.2. Global op imiza ion
The global op imiza ion o med he second s ep o he whole ma e ial pa ame e iden i ica ion p ocess.
Wi hin his second s ep he op imized ma e ial pa ame e alues we e sough so ha he esul o
compu e simula ion app oxima ed he expe imen al da a so well as possible. De ined objec i e
unc ion was used o he e alua ion o global op imiza ion esul s. The e o e, wi hin he global
op imiza ion he op imized ma e ial pa ame e alues we e sough so ha he alue o de ined
objec i e unc ion was minimized. Based on p e ious in o ma ion, i is clea ha he global
op imiza ion was based on minimizing he objec i e unc ion [25]. The objec i e unc ion de ined o
he pu poses o his pape ook he o m o Euclidean no m which was, o cou se, minimized:
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IOP Con . Se ies: Ma e ials Science and Enginee ing 245 (2017) 032078 doi:10.1088/1757-899X/245/3/032078
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n2
ii
i=1
_minEUCLID NORM y y 
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 (11)
whe e, o yi, we subs i u ed he o ce alues ob ained om he app op ia e nume ically-simula ed
load-ex ension cu e a he ce ain de o ma ions, and yi* was subs i u ed wi h he o ce alues ob ained
om he expe imen al load-ex ension cu e a he same de o ma ions.
As poin ed ou abo e, he global op imiza ion in ol ed only hose ma e ial pa ame e s ha we e
pa o he educed design ec o . The emaining pa ame e s we e de ined by he cons an alues om
hei o iginal ange o a iabili y which was ob ained o each pa ame e on he basis o es
calcula ions. The global op imiza ion o he ma e ial pa ame e alues was pe o med using he
g adien based op imiza ion me hod known as he Non-Linea P og amming by Quad a ic Lag angian
(NLPQL) [14]. NLPQL is a sequen ial quad a ic p og amming me hod which sol es p oblems wi h
smoo h con inuously di e en iable objec i e unc ion and cons ain s. The algo i hm o his me hod
uses a quad a ic app oxima ion o he Lag angian unc ion and a linea iza ion o he cons ain s. Fo
he calcula ions pe o med ia he NLPQL me hod, he bes andom ealiza ion acqui ed om he LHS
me hod was used as he s a ing poin .
The op imized alues o he ma e ial pa ame e s p o ided by he bes gene a ion o he NLPQL
me hod a e, oge he wi h he ele an minimum alue o he objec i e unc ion, gi en in able 2.
4.3. Local op imiza ion
The local op imiza ion o med he hi d s ep o he whole ma e ial pa ame e iden i ica ion p ocess.
Wi hin he con ex o his hi d s ep, aim, pu pose and objec i e unc ion a e he same as in he case o
he global op imiza ion. The objec i e unc ion was, o cou se, minimized again. The local
op imiza ion was pe o med in an e o o sea ch he icini y o he global minimum wi h a goal o y
o e ine he men ioned global minimum.
As in he global op imiza ion case, he local op imiza ion in ol ed only ma e ial pa ame e s ha
we e pa o he educed design ec o . The emaining pa ame e s we e de ined by he same cons an
alues as in he case o he global op imiza ion. The local op imiza ion o he ma e ial pa ame e s was
ca ied ou using he na u e inspi ed op imiza ion me hod known as he Pa icle Swa m Op imiza ion
(PSO) me hod [14]. I is he me hod ha is inspi ed by he beha iou o bi d locks du ing he
sea ching o ood. Fo he calcula ions pe o med ia he PSO me hod, he bes gene a ion o he
NLPQL me hod was used as he s a poin .
The op imized alues o he ma e ial pa ame e s p o ided by he bes gene a ion o he PSO
me hod a e, oge he wi h he ele an minimum alue o he objec i e unc ion, gi en in able 2.
I is clea om able 2 ha he PSO me hod p o ided he mos op imized ma e ial pa ame e s
because he alue o he objec i e unc ion was he smalles o his me hod. Figu e 3 below compa es
he load-ex ension cu e ob ained ia he compu e simula ion, in which we applied he mos
op imized pa ame e alues o he Con inuous Su ace Cap Model om he PSO me hod, wi h he
expe imen ally-measu ed load-ex ension cu e. I is hen ob ious om he ep esen a ion ha he
pa ame e s o he Con inuous Su ace Cap Model we e iden i ied e y accu a ely ia he PSO me hod
because he esul o he compu e simula ion ensu es a e y good app oxima ion o he expe imen al
da a.