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E. Torroja's bridge: Tailored experimental setup for SHM of a historical bridge with a reduced number of sensors

Pachón García, Pablo; Castro Triguero, Rafael; García Macías, Enrique; Compán Cardiel, Víctor Jesús; Puertas García, María Esther

Abstract

This paper presents the design of an experimental setup with a reduced number of sensors for the structural health monitoring of the historical bridge of Posadas (Córdoba, Spain), designed by the eminent engineer Eduardo Torroja in 1957. The motivation of this study stems from the need for safeguarding this piece of cultural heritage. In particular, the singularity of this historical construction, a steel–concrete composite typology consisting of a concrete deck slab and inverted bowstring steel trusses, makes continuous in-service condition assessment essential for its maintenance. Nevertheless, the application of existing continuous monitoring systems to such large-scale structures entails considerable investments as well as complex signal processing algorithms. Whereby the optimization of the number of sensors and their location is of the utmost interest. In this line, this work presents the application of an Optimal Sensor Placement (OSP) methodology to tailor an experimental setup for a cost-efficient continuous monitoring of the E. Torroja’s bridge. Due to the fact that most OSP approaches are model-based, it is essential to count on a sufficiently accurate numerical model. To this aim, an extensive vibration-based operational modal analysis is first conducted with a large number of accelerometers. Afterward, a three-dimensional finite element model of the E. Torroja’s bridge is updated on the basis of the experimentally identified dynamic properties with a genetic optimization algorithm. Finally, an optimal sensor placement methodology is utilized to design an experimental setup with a limited number of sensors for long-term monitoring purposes. The results demonstrate that few sensors are needed to accurately assess the main resonant frequencies and mode shapes.

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UNCORRECTED PROOF Enginee ing S uc u es xxx (2018) xxx-xxx Con en s lis s a ailable a ScienceDi ec Enginee ing S uc u es jou nal homepage: www.else ie .com E. To oja’s b idge: Tailo ed expe imen al se up o SHM o a his o ical b idge wi h a educed numbe o senso s Pablo Pachón⁠a⁠, ⁠⁎, Ra ael Cas o⁠b, En ique Ga cía-Macías⁠c, Víc o Compan⁠a, Es he Pue as⁠d aDep . o Con inuum Mechanics, Uni e sidad de Se illa, A enida Reina Me cedes, 41012 Se illa, Spain bDep . o Mechanics, Uni e sidad de Có doba, Campus de Rabanales, 14071 Co doba, Spain cDepa men o Con inuum Mechanics and S uc u al Analysis, Uni e sidad de Se illa, Camino de los Descub imien os s/n, 41092 Se ille, Spain dDep . o Mechanical S uc u es and Hyd aulic Enginee ing, Uni e sidad de G anada, A enida Fuen enue a, 18001 G anada, Spain ARTICLE INFO Keywo ds: Ambien ib a ion Cul u al he i age Gene ic algo i hm His o ical cons uc ions Ope a ional modal analysis Op imal senso placemen S uc u al Heal h Moni o ing ABSTRACT This pape p esen s he design o an expe imen al se up wi h a educed numbe o senso s o he s uc u al heal h moni o ing o he his o ical b idge o Posadas (Có doba, Spain), designed by he eminen enginee Ed- ua do To oja in 1957. The mo i a ion o his s udy s ems om he need o sa egua ding his piece o cul u al he i age. In pa icula , he singula i y o his his o ical cons uc ion, a s eel–conc e e composi e ypology con- sis ing o a conc e e deck slab and in e ed bows ing s eel usses, makes con inuous in-se ice condi ion as- sessmen essen ial o i s main enance. Ne e heless, he applica ion o exis ing con inuous moni o ing sys ems o such la ge-scale s uc u es en ails conside able in es men s as well as complex signal p ocessing algo i hms. Whe eby he op imiza ion o he numbe o senso s and hei loca ion is o he u mos in e es . In his line, his wo k p esen s he applica ion o an Op imal Senso Placemen (OSP) me hodology o ailo an expe imen al se up o a cos -e icien con inuous moni o ing o he E. To oja’s b idge. Due o he ac ha mos OSP app oaches a e model-based, i is essen ial o coun on a su icien ly accu a e nume ical model. To his aim, an ex ensi e ib a ion-based ope a ional modal analysis is i s conduc ed wi h a la ge numbe o accele ome e s. A e wa d, a h ee-dimensional ini e elemen model o he E. To oja’s b idge is upda ed on he basis o he expe imen- ally iden i ied dynamic p ope ies wi h a gene ic op imiza ion algo i hm. Finally, an op imal senso placemen me hodology is u ilized o design an expe imen al se up wi h a limi ed numbe o senso s o long- e m mon- i o ing pu poses. The esul s demons a e ha ew senso s a e needed o accu a ely assess he main esonan equencies and mode shapes. 1. In oduc ion His o ical b idges cons i u e a key piece o cul u al he i age, inas- much as hey bea wi ness o he cou se o his o y and hold an im- po an social, cul u al, and a is ic alue. The e exis s a g ea conce n abou hei conse a ion and, he e o e, he assessmen o hei heal h condi ion is absolu ely c ucial. S uc u al Heal h Moni o ing (SHM) en- compasses he applica ion o Non-Des uc i e Tes ing (NDT) and dam- age de ec ion in o de o ex end he li e-cycle o s uc u es. In pa ic- ula , Ope a ional Modal Analysis (OMA) is conside ed one o he mos sui able me hods o assess he condi ion o s uc u es h ough hei i- b a ional p ope ies [1,2]. OMA is pe o med unde condi ions o se - ice wi hou he need o a i icial exci a ions, ea u e ha is essen ial o moni o his o ical s uc u es whe e he use o s onge modal ex- ci e s, such as ins umen ed hamme s o shake s, is o en inadmissible. Ne e heless, OMA usually equi es a la ge numbe o senso s o p op- e ly cha ac e ize he dynamic p ope ies, ac ha limi s he scalabili y o long- e m OMA-based SHM o la ge-scale s uc u es. Gi en he high cos o such sys ems, i is essen ial o coun on echniques ha allow o ailo ing expe imen al se ups in such a way ha only a educed num- be o senso s can accu a ely iden i y he ib a ional p ope ies o s uc- u es. Plen y o s udies on Fini e Elemen Modeling (FEM) and expe i- men al in es iga ion o his o ical b idges can be ound in he li e a- u e. A no ewo hy con ibu ion was done by Chia a Pepi e al. [3] who s udied he s uc u al pe o mance o an ancien b idge loca ed in Todi (Umb ia, I aly), h ough he in eg a ion o geome ic su ey p oce ⁎Co esponding au ho . Email add ess: [email p o ec ed] (P. Pachón) h ps://doi.o g/10.1016/j.engs uc .2018.02.035 Recei ed 26 Sep embe 2017; Recei ed in e ised o m 5 Janua y 2018; Accep ed 9 Feb ua y 2018 A ailable online xxx 0141-0296/ © 2017. UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx du es, dynamic es ing and nume ical modeling. Conde e al. [4] con- duc ed ambien ib a ion es s on he Vilano a b idge, a mason y s uc- u e loca ed in Galicia (Spain), and whose o igin da es back o he 13–14 h cen u ies. Those au ho s p esen ed a mul idisciplina y ap- p oach o he s uc u al assessmen o mason y a ch b idges by using NDT echniques and h ee-dimensional nume ical modeling. Gen ile and Saisi [5] conduc ed he dynamic cha ac e iza ion o wo his o ic s uc- u es, namely he Collegia a o San Vi o e bell owe (A cisa e, I aly), and he San Michele b idge (Milan, I aly), an a ch b idge buil in 1889. In he la e case, hose au ho s in es iga ed he a ia ion o he dy- namic cha ac e is ics o he b idge unde di e en a ic condi ions. Fi- nally, i is also wo h no ing he wo k done by Al unisik e al. [6] on a mid-nine een h cen u y b idge in Tu key, he Mik on a ch. Those au- ho s epo ed abou he de ini ion o a h ee-dimensional FEM o he b idge, an OMA campaign, and he upda ing o he FEM on he basis o he expe imen ally iden i ied modal p ope ies. O e all, despi e g ea e o s ha e been pu in o he implemen a ion o hese echniques o he conse a ion o his o ical cons uc ions, he ele a ed cos s o hese sys- ems s ill emain an impo an obs acle. This pape is aimed a p esen ing a me hodology o ailo a cos -e - icien expe imen al se -up wi h a educed numbe o senso s o he long- e m SHM o he E. To oja’s b idge. This b idge was cons uc ed in 1951 o e he Guadalqui i i e by he enowned ci il enginee Ed- ua do To oja (Fig. 1). The cul u al and his o ical impo ance o his b idge jus i ies he implemen a ion o a long- e m SHM sys em, so ha p e en i e ac ions can be aken in o de o p e en o mi iga e s uc- u al aging and acciden al damages. Following he p e ious discussions, he p esen me hodology p oposes he use o a limi ed numbe o sen- so s which a e placed a op imal loca ions de e mined by means o an OSP algo i hm. OSP algo i hms, which a e ypically based on a nume - ical model o he s uc u e, maximize he modal in o ma ion wi h a e- duced numbe o deg ees o eedom and, he e o e, a limi ed numbe o senso s. Hence, he sui abili y o he ailo ed expe imen al se -up is c i - ically de e mined by he accu acy o he nume ical model. A ho ough ambien - ib a ion es wi h a la ge numbe o senso s is i s conduc ed o assess he ib a ional p ope ies o he s uc u e and o se e as a ba- sis o he upda ing o he p elimina y nume ical model. A e wa d, he disc epancies be ween he heo e ical and expe imen al esul s a e min- imized by upda ing di e en a iables o he nume ical model h ough a gene ic op imiza ion algo i hm. Once he nume ical model is p op- e ly uned, he op imal loca ions o a educed se o senso s a e de e - mined by an OSP algo i hm. The esul s demons a e ha ew senso s a e needed o accu a ely assess he main esonan equencies and mode shapes. The emainde o his pape is o ganized as ollows. Sec ion 2 con- cisely desc ibes he his o ical e olu ion o he b idge and i s geome - ic con igu a ion. Sec ion 3 in oduces he p elimina y FE model o he b idge. Sec ion 4 p esen s he dynamic cha ac e iza ion o he b idge by means o an expe imen al OMA campaign. Sec ion 5 de ails he up da ing p ocess o he p elimina y FE model. Sec ion 6 o e iews he he- o e ical o mula ion o he u ilized OSP echnique and epo s he p o- posed op imal se -up o a long- e m SHM o he E. To oja’s b idge. Fi- nally, Sec ion 7 d aws he main conclusions o his s udy. 2. E. To oja’s b idge: Cons uc ion and e olu ion Edua do To oja Mi e (1899–1961) is conside ed one o he majo igu es o Spanish ci il enginee ing, wi h a undamen al con ibu ion o he design o hin-shell conc e e s uc u es. In his book “Razón y Se de ipos es uc u ales”[7], his oeu e is concei ed as a ques o s uc u al u h, a concep h ough which E. To oja ad oca es ha beau y lies in a ionali y and no in a i icial o namen a ion. Wi h his in mind, E. To oja de eloped new ways o designing s uc u es whe eby aes he ics a ises om he a ionali y o he di e en s uc u al membe s. Fu he - mo e, E. To oja showed in e es in undamen al a o ms and a e p e- sen in mos o his s uc u es. Nowadays, nume ous b idges designed by his eminen enginee a e conside ed as his o ical cons uc ions, such as he Muga b idge (Fig. 2a) o he Ped ido b idge (Fig. 2b). A e he Spanish ci il wa , E. To oja was commissioned o subs i- u e he b idge o e he Guadalqui i i e in Posadas (Có doba, Spain) which had been se iously damaged in he con lic . The o iginal s uc- u e, which consis ed o ein o ced conc e e a ches, was eplaced by i e isos a ic s eel-conc e e composi e spans o 43m (Fig. 3). The new so- lu ion was de ined wi h a 7m wid h ein o ced conc e e deck and wo in e ed bows ing s eel usses, whose bo om cho ds we e de ined as pa abolic a ches wi h a maximum ise o 6m. Fig. 4 shows wo pho- og aphs o he o iginal b idge unde cons uc ion. In 1983, some new deck epai s we e conduc ed, including he con- s uc ion o new dila a ion join s, injec ions, as well as epai s o he piles’and abu men s’walls. In addi ion, some damaged s eel compo- nen s we e eplaced and, e en ually, he me allic s uc u e and he hand ails we e epain ed. None heless, he s uc u al ypology was kep unal e ed (see Fig. 5). In 1991, E. To oja’s g andson, An onio To oja, was en us ed o ca y ou an ex ension o he deck wid h om 6.5m (Fig. 6(a)) o 11m (Fig. 6(b)). To his end, wo new a ches we e added and connec ed o he o iginal ones by a ubula uss s uc u e. The o iginal deck had o be comple ely emo ed because new uppe ein o cemen s we e needed o bea he ans e se nega i e momen s (Fig. 7). I should be no ed ha all he modi ica ions expe ienced by he s uc u e en ail a high le el o unce ain y, a ec ing bo h he ma e ial p ope ies and he s uc u al beha io . Mo eo e , due o he singula geome y ha cha ac e izes he b idge, he me allic pa o he s uc- u e is no physically accessible (Fig. 8) and, he e o e, he expe imen al modal cha ac e iza ion o he b idge mus be ca ied ou on he oad. In his sense, he nume ical model ep esen s a undamen al ool o e al- ua e he cu en s a e o conse a ion o he b idge in gene al and he s eel s uc u e in pa icula . Fig. 1. E. To oja’s b idge in Posadas, Có doba (Spain). 2 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx Fig. 2. Views o (a) Muga b idge, 1939 (Gi ona, Spain), and (b) To de a b idge, 1939 (Ba celona, Spain). Fig. 3. F on iew o E. To oja’s b idge (dimensions in m). Fig. 4. Pho og aphs o he o iginal b idge unde cons uc ion (1940–1951). Fig. 5. Pho og aphs o he o iginal b idge in se ice (1966). 3. Fini e elemen modal analysis This sec ion de ails he p elimina y FEM o he E. To oja’s b idge. Fi s ly, o p o ide some insigh in o he s uc u al e olu ion o he b idge, he esul s epo ed in a p e iously published wo k by he au- ho s [8] on he s udy o he a ia ion o he dynamic p ope ies o he b idge along i s his o y a e b ie ly p esen ed. Then, he p elimina y h ee-dimensional FEM o he b idge, which se es as a basis o he ol- lowing upda ing p ocess, is p esen ed in de ail. 3.1. S uc u al e olu ion o he b idge As p e iously indica ed, he b idge has expe ienced impo an modi- ica ions since i s cons uc ion. Some o he o iginal elemen s we e p e- se ed, whils some o he s we e la e inco po a ed. In o de o shed 3 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx Fig. 6. C oss sec ions o he b idge (dimensions in m). Fig. 7. Views o (a) ini ial and (b) inal ope a ions o deck’s wid h inc emen (1992). Fig. 8. Views o he cu en b idge in se ice. some ligh on he e olu ion o he s uc u al beha io o he b idge, he au ho s ca ied ou a p elimina y esea ch ha was p esen ed a he In e na ional Modal Analysis Con e ence (IMAC 2015) [8]. In ha s udy, bo h he o iginal and he cu en designs o he b idge (see Fig. 6) we e simula ed by p elimina y FEMs. Then, a compa ison o bo h models in e ms o hei dynamic p ope ies was made in o de o aid in he unde s anding o he s uc u al e olu ion. Beam elemen s we e used o all he componen s excep o he deck o which hick shell elemen s we e u ilized. Finally, he esonan equencies o bo h s uc- u es we e compu ed by modal analysis, and i was obse ed ha only small di e ences a e ound in he i s i e na u al modes. This ac in- dica es ha , despi e he conside able modi ica ions expe ienced by he s uc u e, he dynamic beha io o he b idge has no been signi ican ly al e ed. The e o e, i was concluded ha he inc ease in he s i ness o he b idge has been coun e ac ed by a simila inc ease in i s mass, whe e he change o weigh o s eel pe a ea o he deck om 66.22 o 79.33kg/m⁠2 is indica i e o his conclusion. I was also concluded ha , since he dynamic cha ac e is ics ha e no been appa en ly al e ed, he di e en ope a ions conduc ed in he b idge may ha e in oduced un- ce ain ies de i ed om di e en ial aging p ocesses. 3.2. P elimina y FEM o he E. To oja’s b idge In o de o inco po a e all he geome ical de ails o he s uc u e, a sophis ica ed h ee-dimensional FEM o he E. To oja’s b idge is de- eloped. Due o he la ge size o he b idge, including i e simply sup- po ed spans, a FEM o he comple e s uc u e would esul in an ex- cessi e compu a ional cos . Mo eo e , since he e is no s uc u al con- nec ion be ween adjacen spans, each span o he b idge beha es inde- penden ly o he o he s. The e o e, only one single span is modeled as 4 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx common p ac ice in he s udy o his ype o b idges. Only shell ele- men s a e de ined in such a way ha he connec ions be ween he s eel a ches and he conc e e desk can be accu a ely simula ed (Fig. 9). The ho izon al b aces a e de ined as buil -up sec ions wi h UPN-120 p o- iles and ba en pla es o dimensions 400×50×8mm e e y 50cm. The a ches a e also buil -up sec ions wi h IPN-200 p o iles and ba en pla es o dimensions 210×50×8mm e e y 50cm. Wi h ega d o he nume - ical de ini ion o he s uc u al membe s, 4-node iangula shell ele- men s a e used o he conc e e slab and all he s eel membe s. O e - all, he comple e model has 374.928 elemen s, 388.679 nodes and 2.332.074 deg ees o eedom. The bounda y condi ions a e de ined as cons ained displacemen s and ee o a ions, as can be obse ed in he de ails o Fig. 9. Table 1 summa izes he ma e ial p ope ies used in he modeling. No e ha all he selec ed p ope ies a e common alues o he design o his ype o s uc u es, wi h he excep ion o he mass den- si y o s eel, whose alue is inc eased by 1.9% wi h espec o he s an- da d alue o 7850kg/m⁠3. This decision is aken o accoun o all hose ac o s ha ha e no been explici ly included in he nume ical model, such as welds, bol s, and o he ancilla y elemen s. The weigh o he ba ens and he pa emen is also included in e ms o added mass. A e wa d, he modal p ope ies o he s uc u e a e compu ed by a modal analysis in Abaqus CAE [9]. The i s eigh mode shapes a e shown in Fig. 10. I is obse ed ha he b idge exhibi s a na ow band o low esonan equencies wi h na u al modes ha a e highly coupled, wha makes he dynamic ea u es o he s uc u e qui e complex. 4. Ambien ib a ion es and ope a ional modal analysis The dynamic es ing o he s uc u e can p o ide an accu a e p edic- ion o i s global modal pa ame e s. In o de o ensu e an e icien iden- i ica ion o he modal p ope ies o he b idge, an ex ensi e ambien ib a ion campaign wi h a la ge numbe o senso s was i s pe o med on Ma ch 14, 2017, on he E. To oja’s b idge. In his way, he expe i- men ally iden i ied dynamic p ope ies se e as a basis o he upda ing o he p elimina y FEM o he b idge. 4.1. Ambien ib a ion es The expe imen al layou o he p elimina y ambien ib a ion es is schema ically ep esen ed in Fig. 11. Accele a ions we e egis e ed in h ee o hogonal di ec ions wi h he aim o iden i ying he ib a- ion modes in he la e al, longi udinal and e ical di ec ions o he b idge. Twel e se -ups we e de ined wi h ou mobile senso s, whils one was kep ixed as a e e ence (placed a poin 6, Fig. 11), wha amoun ed o a o al o 36 measu ing poin s. The posi ion o he e e - ence accele a ion senso was chosen acco ding he esul s p o ided by he nume ical model [10]. In each one o hese se -ups, a sampling ime o 10min and a sampling a e o 100Hz we e selec ed, aking in o ac Fig. 9. FEM o he E. To oja’s b idge. 5 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx Table 1 Ma e ial p ope ies used in he FEM. P ope y Uni Value Mass o secu i y ba ie s kg/m 14.66 Mass o asphal kg/m⁠2 110 Young’s modulus o conc e e slab MPa 30,000 Poisson’s a io o conc e e slab –0.2 Densi y o conc e e slab kg/m⁠3 2500 Young’s modulus o s eel MPa 210,000 Poisson’s a io o s eel –0.3 Densi y o s eel kg/m⁠3 8000 coun he empi ical ule p oposed by J. Rod igues in his Phd Thesis [11]. These assump ions ensu e ha equencies om 1 o 50Hz a e p ope ly eco ded. The equipmen used in he es s included i e sel -con ained eco de ins umen s manu ac u ed by he company GeoSIG Measu ing Sys ems. These ins umen s ha e h ee in e nal senso s, an i-aliasing il e s, a bandwid h anging om 0.01 o 250Hz, a dynamic ange o 146dB, a sensi i i y o 10V/g, and 4.70kg o weigh (model GMSplus) (Fig. 12). The same condi ions o empe a u e and humidi y we e aken in o accoun du ing he whole campaign in o de o a oid a ia ions in he modal pa ame e s [12]. In addi ion, he modal exci a ion o he b idge was always caused by en i onmen al loads, such as wind o a ic (Fig. 13). Fig. 10. Fi s eigh nume ical eigenmodes compu ed by he FEM o he E. To oja’s b idge. Fig. 11. Plan iew o he accele ome e loca ions ( e e ence accele ome e in ed). (Fo in e p e a ion o he e e ences o colo in his igu e legend, he eade is e e ed o he web e sion o his a icle.) 6 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx Fig. 12. Sel -con ained eco de ins umen (GMSplus). Fig. 13. Time his o y o accele a ion egis e ed by accele ome e numbe wo, 4 h se -up. 4.2. Ope a ional modal analysis The A emis So wa e [13] is used o analyze he da a ob ained du ing he expe imen al campaign. The Enhanced F equency Domain Decomposi ion (EFDD) echnique [14,15] and he S ochas ic Subspace Iden i ica ion (SSI) me hod [16,17] a e he wo di e en iden i ica ion me hods used o ob ain he modal pa ame e s o he b idge (Fig. 14). Wi h ega d o he signal p ocessing o he eco dings, a decima ion ac o o 5 is applied in o de o ake in o conside a ion ha he ex- pec ed na u al equencies a e below 10Hz, acco ding o he esul s o he nume ical modal analysis p e iously shown in Fig. 10. In addi ion, Fig. 14. Expe imen al iden i ica ion o he esonan equencies by he EFDD and SSI echniques. 7 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx he esolu ion o he spec al densi y es ima ion is de ined as 1024, wha esul s in a equency line spacing o 0.005Hz. Ha monic de ec ion al- go i hms a e also applied in o de o check all he equencies in he spec um. In o de o alida e he iden i ied modal pa ame e s, he Modal As- su ance C i e ion (MAC) [18] is applied. Gi en wo mode shapes, φjand φk, hei MAC alue w i es: (1) whe e supe index T designa es ansposi ion. When he MAC alue is highe han 0.80, a good co ela ion be ween he wo modes is consid- e ed [18]. Finally, Table 2 p esen s he ob ained esul s, including he s anda d de ia ion o modal equencies and he damping a ios. As can be obse ed in Table 2, he i s eigh ib a ion modes in a equency ange up o 10Hz ha e been iden i ied. The di e ences be- ween he equencies iden i ied by he SSI and EFDD me hods a e al ways lowe han 1.5%, aking he esul s o he SSI me hod as e e - ence alue. The esul s o he damping a ios show an highe a iabil- i y, wi h a e age modal damping a ios o 0.61% and 1.64% o SSI and EFDD echniques, espec i ely. Such la ge di e ences a e ypically ound in p ac ice, ac ha indica es he need o highe le els o exci a- ion o accu a ely cap u e he damping a ios [19]. The damping alues ob ained by he EFDD me hod a e e en less eliable han hose ob ained by he SSI me hod, as can be ex ac ed om hei highe s anda d de- ia ion alues. Fu he , he MAC indica es a good co ela ion be ween he modes iden i ied by bo h me hods wi h alues highe han 0.80. The i s and he ou h modes a e o sional modes, while he o he modes co espond o bending modes o he b idge (see Fig. 15). 5. FEM upda ing On he basis o he expe imen ally iden i ied dynamic p ope ies, he p elimina y FEM has been upda ed o ep oduce he ac ual beha - io o he b idge and assis he OSP me hodology. S anda d FEMs o his kind o buildings usually include unce ain ies de i ed om un Table 2 OMA esul s: na u al equencies ( ), damping a ios (ξ) and s anda d de ia ion (s d). Mode N⁠o SSI EFDD MAC (Hz) s d( )ξ(%) s d(ξ) (Hz) s d( )ξ(%) s d(ξ) 1 3.28 0.02 0.85 0.40 3.31 0.01 1.46 0.66 0.92 2 3.68 0.07 0.79 0.46 3.72 0.03 2.14 1.17 0.94 3 3.80 0.04 0.78 0.31 3.84 0.07 1.60 1.01 0.82 4 5.14 0.01 0.60 0.17 5.16 0.01 0.63 0.22 0.98 5 5.61 0.10 0.38 0.27 5.68 0.09 2.78 1.16 0.81 6 5.64 0.05 0.41 0.26 5.69 0.07 2.01 1.22 0.80 7 7.79 0.05 0.58 0.31 7.68 0.14 1.70 1.06 0.86 8 8.02 0.02 0.49 0.27 8.07 0.05 0.84 0.39 0.84 Fig. 15. Expe imen ally iden i ied na u al ib a ion modes. 8 UNCORRECTED PROOF P. Pachón e al. Enginee ing S uc u es xxx (2018) xxx-xxx known ma e ial p ope ies, exis ing damage, complex in e nal compo- si ion o s uc u al elemen s, and modeling app oxima ions. The e o e, he calib a ion o he model wi h he aid o expe imen al in o ma ion becomes essen ial o app op ia ely model he ac ual beha io o he s uc u e. Following he same p ocedu e as in p e ious wo ks by he au ho s [20], he FEM upda ing is pe o med by means o i e a i e me hods [21], in which he use in oduces changes di ec ly on some o he physical pa ame e s ha de ine he s uc u e. To his aim, a sensi i i y s udy is i s conduc ed o de ec hose s uc u al pa ame e s ha ha e a g ea e in luence on i s dynamic beha io . In his wo k, he Young’s modulus (Ec) and he densi y o he conc e e desk (ρc) a e selec ed as design a iables. Once he upda ing pa ame e s o he nume ical model a e selec ed, and conside ing he good quali y o he expe imen al measu emen s, he i s h ee iden i ied modes a e selec ed as a ge modes in he upda - ing p ocess. Taking in o accoun he alues o he na u al equencies and he modal coo dina es, a o al o 111 esidual componen s a e ad- jus ed and minimized h oughou he model upda ing. In o de o con- side he g ea e c edibili y o he iden i ied equencies wi h espec o he modal displacemen s, a weigh ac o w = 1.00 is de ined o he esonan equencies, whils a smalle ac o ws= 0.05 is assigned o he modal coo dina es. Finally, he FEM upda ing is pe o med using a gene ic algo i hm in Ma lab en i onmen [22], acco ding o an objec- i e unc ion de ined as he ela i e di e ences be ween he expe imen- al and he nume ical modal pa ame e s. This unc ion is usually o mu- la ed as a leas -squa es p oblem as ollows: (2) whe e a e he alues ela ed o he physical pa ame e s o he nume ical model, θ(Ecand ρc), while he a iables zEXP,ja e he same magni udes ob ained om he expe imen al campaign. The di e ences be ween hese a iables a e se as esidues, . I mus be no ed ha he numbe o esidues, m=m +ms(wi h m being he numbe o con- side ed na u al equencies, and ms he numbe o he coo dina es o he conside ed ib a ion modes), is g ea e han he numbe o adjus ed a iables, θ. The weigh ac o s, wj, a e he alues es ablished o each esidue. In he case o na u al equencies, he esidues ead: (3) whe e and EXP,ja e he alues o he ob ained equencies om he nume ical and expe imen al model. In a simila way, he esidues in e ms o mode shapes co espondingly w i e: (4) whe e and a e he selec ed and e e ence compo- nen o he nume ical mode j, while and a e he same mag- ni udes ob ained om expe imen al mode j. Then, in o de o minimize his objec i e unc ion, a gene ic algo i hm is applied. Fig. 16 shows he con e gence o he i ness unc ion using a ge- ne ic algo i hm. A ange o a ia ion o e e y upda ing pa ame e (Table 3) is selec ed o p e en he algo i hm om de ining physically un ealis ic es ima es. In each i e a ion, a popula ion o 1000 ec o s is conside ed by using he p inciples o gene ic algo i hms (as imple- men ed in Ma lab so wa e), and he objec i e unc ion in Eq. (2) is minimized. Such calib a ion p ocess inishes when he di e ences be- ween he mean alues (blue do s in Fig. 16) and he bes alues (g een Fig. 16. Con e gence o he i ness unc ion using a gene ic algo i hm. Fi ness alue e sus he numbe o gene a ions. Blue poin s: Mean alues o he objec i e unc ion o all he popula ion o he co esponding gene a ion. G een poin : Bes alues esul o an indi idual o he popula ion.(Fo in e p e a ion o he e e ences o colou in his igu e legend, he eade is e e ed o he web e sion o his a icle.) Table 3 Summa y o upda ed pa ame e s o he FEM by a gene ic algo i hm. Pa ame e Ini ial alue Range o a ia ion Upda ed alue Lowe Uppe Ec(MPa) 25,000 20,000 30,000 27790.51 ρc(kg/ m⁠3) 2500 2000 4000 3774.71 do s in Fig. 16) o he i ness unc ion o wo i e a ions a e less han 1×10⁠−3. Table 3 p esen s he summa y o he upda ed pa ame e s, whe e la ge di e ences can be obse ed be ween he upda ed and ini ial pa a- me e s. Table 4 shows he compa ison be ween he expe imen al esul s and hose p o ided by bo h he p elimina y and he upda ed FEMs. Table 4 Compa ison o he expe imen ally iden i ied na u al equencies, SSI, he nume ical esul s by he p elimina y FEM, , and hose p o ided by he upda ed FEM, , as well he MAC alues o he mode shapes de e mined by he expe imen s and he upda ed FEM, . Mode n⁠o SSI (Hz) (Hz) (Hz) 1 3.28 3.52 (7.31%) 3.26 (0.60%) 0.96 2 3.68 3.82 (3.81%) 3.67 (0.27%) 0.93 3 3.80 4.55 (19.73%) 3.90 (2.63%) 0.83 4 5.14 5.91 (14.98%) 5.26 (2.33%) 0.94 5 5.61 5.92 (5.52%) 5.77 (2.85%) 0.88 6 5.64 6.15 (9.04%) 5.82 (3.19%) 0.82 7 7.79 9.14 (16.81%) 7.83 (0.51%) 0.92 8 8.02 9.40 (17.20%) 8.08 (0.74%) 0.84 The pe cen ages in pa en hesis co espond o he ela i e di e ences be ween equencies. 9