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A procedure to track vibration modes under changing external factors : application to a pedestrian bridge

Soria, José M.; Díaz, Iván M.; García-Palacios, Jaime H.; Ibán, Norberto; Lorenzana, Antolín

Abstract

A low-cost vibration monitoring system has been developed and installed on an urban steel- plated stress-ribbon footbridge. The system continuously measures: the acceleration (using 18 triaxial MEMS accelerometers distributed along the structure), the ambient temperature and the wind velocity and direction. Automated output-only modal parameter estimation based on the Stochastic Subspace Identification (SSI) is carried out in order to extract the modal parameters, i.e., the natural frequencies, damping ratios and modal shapes. Thus, this paper analyzes the time evolution of the modal parameters over a whole-year data monitoring. Firstly, for similar environmental/operational factors, the uncertainties associated to the time window size used are studied and quantified. Secondly, a methodology to track the vibration modes has been established since several of them with closely-spaced natural frequencies are identified. Thirdly, the modal parameters have been correlated against external factors. It has been shown that this stress-ribbon structure is highly sensitive to temperature variation (frequency changes of more than 20%) with strongly seasonal and daily trends.

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A p ocedu e o ack ib a ion modes unde changing ex e nal ac o s: applica ion o a pedes ian b idge So ia, José M.1; Díaz, I án M.2; Ga cía-Palacios, Jaime H.3; Ibán, No be o4; Lo enzana, An olín5 ABSTRACT A low-cos ib a ion moni o ing sys em has been de eloped and ins alled on an u ban s eel- pla ed s ess- ibbon oo b idge. The sys em con inuously measu es: he accele a ion (using 18 iaxial MEMS accele ome e s dis ibu ed along he s uc u e), he ambien empe a u e and he wind eloci y and di ec ion. Au oma ed ou pu -only modal pa ame e es ima ion based on he S ochas ic Subspace Iden i ica ion (SSI) is ca ied ou in o de o ex ac he modal pa ame e s, i.e., he na u al equencies, damping a ios and modal shapes. Thus, his pape analyzes he ime e olu ion o he modal pa ame e s o e a whole-yea da a moni o ing. Fi s ly, o simila en i onmen al/ope a ional ac o s, he unce ain ies associa ed o he ime window size used a e s udied and quan i ied. Secondly, a me hodology o ack he ib a ion modes has been es ablished since se e al o hem wi h closely-spaced na u al equencies a e iden i ied. Thi dly, he modal pa ame e s ha e been co ela ed agains ex e nal ac o s. I has been shown ha his s ess- ibbon s uc u e is highly sensi i e o empe a u e a ia ion ( equency changes o mo e han 20%) wi h s ongly seasonal and daily ends. Keywo ds: Modal analysis; Foo b idge; Con inuous dynamic moni o ing; En i onmen al e ec s. 1. INTRODUCTION The long- e m ib a ion moni o ing o ci il enginee ing s uc u es is inc easingly used o moni o bo h, he s uc u e in eg i y and he ib a ion se iceabili y. A numbe o examples o b idges and oo b idges equipped wi h a moni o ing sys em can be ound [7, 9, 10, 16]. In hese moni o ing sys ems, he ib a ions due o a ic o wind a e measu ed and eco ded. These da a can be used o con inuously ex ac he modal pa ame e s (na u al equencies, damping a ios and modal shapes) which may be employed o assess he s uc u al in eg i y since s uc u al damages lead o changes in he modal pa ame e s. Thus, ib a ion-based S uc u al Heal h Moni o ing (SHM) sys ems using au oma ed ou pu -only modal iden i ica ion (also known as Ope a ional Modal Analysis, OMA) ha e been ex ensi ely p oposed, o ins ance [8, 13]. One o he main p oblems o hese sys ems is ha hey ha e 1 Dp o. CMM and Theo y o S uc u es. ETSICCP, UPM (Spain). [email p o ec ed] (Co esponding au ho ) 2 Dp o. CMM and Theo y o S uc u es. ETSICCP, UPM (Spain). i an.m[email p o ec ed] 3 Dp o. Ci il Enginee ing: Hid aulic and Ene gy. ETSICCP, UPM (Spain). jaime.ga cí[email protected] 4 Mechanical Enginee ing Di ision. Ca i Resea ch Cen e (Spain). no iba@ca i .es 5 EII/ITAP, Uni e sidad de Valladolid (Spain). [email p o ec ed] 41 o cope wi h changing en i onmen al/ope a ional condi ions ha o en signi ican ly a ec he modal es ima ion. The main obs acle o a mo e widesp ead adop ion o hese moni o ing sys ems is he cos associa ed o hei ins alla ion. Recen ly, a success ul a emp o educe he cos o a moni o ing sys em has been ca ied ou h ough he use o low-cos senso s o measu e s uc u al ib a ions on a oo b idge. Thus, a low-cos con inuous ib a ion moni o ing sys em using small MEMS (Mic o Elec o-mechanical Sys ems) accele ome e s has been de eloped and ins alled on Ped o Gómez Bosque (PGB) oo b idge (Valladolid, Spain) in o de o ack i s long- e m dynamic pe o mance. The sys em con inuously measu es: he accele a ion (using 18 iaxial MEMS accele ome e s dis ibu ed along he s uc u e), he ambien empe a u e and he wind eloci y and di ec ion [18]. PGB oo b idge is a singula s eel-pla ed s ess- ibbon oo b idge wi h a single span o 85 m. The dynamic beha io shows se e al low- equency ib a ion modes wi h closely-spaced na u al equencies and low damping a ios. A p ocedu e o ack ib a ion modes has been p og ammed o ca y ou an au oma ic modal pa ame e es ima ion. This p ocedu e has o cope wi h ib a ion modes wi h closely-spaced na u al equencies. In his case, so ing ib a ion modes using equency c i e ia and emo ing ou lie s ha lay ou o in e als o equency a ia ion migh no be adequa e [14, 16]. This pape desc ibes he de ailed p ocedu e ca ied ou o ack ib a ion modes o PGB oo b idge o e ime. The p ocedu e uses h ee ole ances based on he Modal Assu ance C i e ion (MAC). This app oach allows eliable moni o ing o ib a ion modes ha a e main ained o e ime. Rega ding he use o modal pa ame e a ia ions as possible damage de ec o in s uc u es, i is necessa y o obse e he modal a ia ions o e ime due o he in luence o some ex e nal agen s ac ing on he undamaged s uc u e [12, 14]. I is impo an o e alua e he magni ude o his modal a ia ion, as well as he main ac o s ha in luence he ela ionship be ween hem. The empe a u e is usually he mos signi ican en i onmen al ac o [20]. Howe e , o he ac o s, such as ope a ional o bounda y condi ions, may signi ican ly a ec he modal es ima es [1, 12]. Fini e Elemen (FE) models a e usually upda ed using he modal pa ame e s [4, 15]. Howe e , when he modal pa ame e s show signi ican a iabili y wi h changing en i onmen al ac o s, he upda ed model migh no be as accu a e as equi ed [2]. Hence, i is impo an o es ima e unce ain ies in he modal pa ame e iden i ica ion in o de o es ablish he deg ee o con idence o he upda ed model. This upda ed model can be use ul o gua an ee a success ul s uc u al in e en ion du ing s uc u al ehabili a ion [6, 11]. Tha is, non- des uc i e es s, such as an OMA, oge he wi h calib a ed models g ea ly bene i eliable s uc u al e alua ions. The pape con inues wi h he desc ip ion o he s uc u e and i s moni o ing sys em. Sec ion 3 analyzes he unce ain ies associa ed o a single ime his o y eco d. The ou pu -only modal pa ame e es ima ion using di e en da a blocks is ca ied ou . Thus, unce ain ies due o he selec ion o he da a block a e quan i ied. The esul s o con inuous dynamic analysis a e desc ibed in Sec ion 4. A acking me hod o ollow he e olu ion o he pe sis en ib a ion modes o e ime is p oposed. The in luence o he en i onmen al/ope a ional ac o s on he modal es ima es is s udied. Finally, some conclusions a e d awn and sugges ions o u u e wo k a e gi en. 42 2. THE FOOTBRIDGE AND ITS VIBRATION MONITORING 2.1. S uc u e desc ip ion PGB oo b idge, si ed in Valladolid (Spain), is a slende and ligh weigh s uc u e ha c ea es a pedes ian link o e he Pisue ga Ri e be ween a spo complex and he ci y cen e (see Figu e 1). This b idge, buil in 2011, is a singula s ess- ibbon oo b idge bo n by a p e ensioned ca ena y-shape s eel band wi h a single span o 85 m ha p o ides minimal impac on he su oundings. The s uc u e mainly consis s o a Co en s eel band o 94 m long, 3.6 m wide and only 30 mm hick which is p e- ensioned and ancho ed o he wo abu men s. The comple e s eel band is ab ica ed by welding 8-me e long shee s and a numbe o 110 p ecas conc e e slabs lay on he s eel band [17]. These slabs do no ha e bea ing capaci y in such a way ha he only s uc u al elemen is he band. The s uc u e is comple ed by ubbe loo ing and a s ainless s eel glass hand ail. Figu e 1. Ped o Gómez Bosque oo b idge. Landscape iew. 2.2. Moni o ing sys em A s uc u al ib a ion moni o ing sys em was de ised in o de o con inuously es ima e he modal pa ame e s o he s uc u e and o assess hei changes unde a ying en i onmen al condi ions. The e o e, apa om he accele ome e s needed o pe o m a modal analysis, senso s o he wind and en i onmen al empe a u e condi ions we e ins alled. The moni o ing sys em comp ises 18 iaxial accele ome e s, 9 a each side o he deck, a empe a u e senso and an anemome e wi h a ane. Wi es and accele a ion senso s we e ins alled inside he hand ail so he s uc u e aes he ic was no modi ied in any way. This ac in oduced addi ional complica ions: (i) he ins alla ion p ocess was a labo ious ask, and (ii) addi ional angula ans o ma ions a e equi ed o ob ain he accele a ion ec o in he s uc u e axes o each accele ome e . The ib a ion senso used o he moni o ing sys em was he low-cos MEMS accele ome e ADXL327 (ANALOG DEVICES) able o measu e he s a ic accele a ion o g a i y. The ADXL327 is a e y small, low powe , 3-axis accele ome e wi h signal condi ion ol age ou pu . The key p ope ies o his senso a e: measu emen ange up o ±2.5g, sensi i i y up o 500 mV/g and bandwid h up o 550 Hz. Howe e , his senso is no designed o ansmi he signal o e long dis ances. To o e come his p oblem, an ad-hoc condi ioning ci cui was designed o enhance i s long-dis ance pe o mance. Fi s , h ee 43 capaci o s, one o each channel, we e placed o ix he equency bandwid h o 100 Hz. Second, since he accele ome e has o be supplied by 3.6 V o ge i s maximum nominal sensi i i y o 500 mV/g, he powe supply uni o 12 V and a ol age egula o o 3.6 V we e in eg a ed in o each ci cui boa d in o de o a oid powe losses by he long dis ance wi es. Thi dly, an ope a ional ampli ie was used o educe signi ican ly he ou pu impedance, achie ing hus a good signal- o-noise a io o accele a ion pa ame e (cons an sensi i i y and low noise). The achie ed signal- o-noise a io was 25 μg/√Hz, which was conside ed o be enough o moni o ing he s uc u al ib a ions. Finally, each ci cui boa d wi h all i s componen s was co e ed wi h a plas ic coa ing o p o ec i om en i onmen al condi ions. Then, he accele ome e s we e eady o be ins alled inside he ube o he hand ail. The sensing sys em was comple ed by a empe a u e senso (model T0110 ansmi e o Come ) and a wind sen y (model 03002L o R.M. Young Company) o measu e he speed and di ec ion o he wind. The empe a u e senso and wind sen y we e ins alled on he public ligh owe si ed closed o he s uc u e (see Figu e 2). Figu e 2. Moni o ing sys em. Dis ibu ion o senso s. The moni o ing sys em hen comp ises 57 ol age channels ha a e p ocessed con inuously. The da a logge Compac RIO 9076 (Na ional Ins umen s) wi h wo NI 9205 wi h 32 analog inpu channels is used o eal- ime da a acquisi ion. The equency sampling o each channel was chosen o be 200 Hz, enough o iden i y he modal pa ame e s o he s uc u e and o a oid aliasing p oblems du ing he pos -p ocessing. The ac ual o ien a ion o he accele ome e s ins alled inside he hand ail is unknown. Howe e , he Eule angles be ween he accele ome e coo dina e sys em and he s uc u e coo dina e sys em can be de i ed aking in o accoun he ollowing: (i) he longi udinal axis o each accele ome e ma ches wi h he longi udinal axis o he oo b idge, and (ii) he accele ome e s a e able o measu e accele a ion due o g a i y. The e o e, he ans o ma ion ma ix be ween bo h coo dina e sys ems is ob ained, and hen, he accele a ion in he global axes can be inally calcula ed [18]. Be o e i s inal ins alla ion, a labo a o y alida ion was ca ied ou and a e he ins alla ion, an in-si u alida ion was pe o med by compa ing agains con en ional piezoelec ic accele ome e s. 3. PEERED ANALYSIS OF ONE TEST The unce ain ies associa ed o he modal iden i ica ion o one es , co esponding o he eco d measu ed on 01/05/2013 a 19:16 (60-minu e es ), a e analyzed he ein. The dynamic beha io o he s uc u e is mainly go e ned by he e ical esponse (p e ious ime-his o y analyses ha e shown ha 44 la e al and longi udinal accele a ions a e small and negligible, espec i ely, as compa ed o e ical ones). Tha is he eason why his analysis concen a es on he e ical ib a ion. The p ocess ollowed is, i s ly, he signal p ocessing unde aken be o e he modal iden i ica ion is p esen ed. A e wa ds, using SSI-co echnique is applied o di e en 20-minu e ime windows o he 60-minu e es . 3.1. Da a p ocessing The e ical esponse o he s uc u e o 1-hou es is analyzed (wi h an ini ial sampling equency o 200 Hz). The signal is il e ed by a low-pass Bu e wo h il e o o de 4 wi h a cu o equency o 5 Hz. A decima ion ac o o 16 is applied ob aining a Nyquis equency o 6.25 Hz. As an example, Figu e 3a and b show he il e ed and decima ed esponse in ime and equency domain, espec i ely, co esponding o he ou cen al channels o ups eam side. Up o en peaks below 4 Hz can be obse ed in Figu e 3b. (a) Time domain. (b) F equency domain. Figu e 3. P ocessed aw da a o 4 cen al channels o ups eam side. 3.2. Ope a ional Modal Analysis using he same SSI echnique The modal pa ame e s ha e been acked o e ime o cap u e he dynamic beha io o he s uc u e as bes as possible. As a ule o humb, he minimum du a ion o he measu emen should be a leas 45 1000 cycles o he lowes na u al equency is expec ed o be iden i ied [19]. This du a ion is usually ecommended as he minimum one o noise-con amina ed signals and close ib a ion modes. The e o e, his du a ion, which co esponds app oxima ely o 20 minu es, has been adop ed he e o ca y ou he modal acking. Th ee consecu i e windows o 20-minu e da a a e conside ed o iden i y he modal pa ame e s using only SSI-co . These esul s a e compa ed wi h hose ob ained using he 60-minu e eco d. Table 1 shows he es ima es ob ained om he ou da a blocks. A MAC co ela ion be ween he modal shapes es ima ed by h ee echniques has been ca ied ou . Modes ha exhibi a MAC alue g ea e han 0.95 o all o he c oss alues a e highligh ed in bold. Modes wi h na u al equencies o e 4 Hz (0.8 imes he cu o equency o he il e ) a e no included. Modes ha exhibi a MAC alue g ea e han 0.95 o all o he c oss alues a e highligh ed in bold. The a e age empe a u e o each ime window was 16.42, 13.84 and 11.56 oC, espec i ely, and 13.94 oC o he 60-minu e eco d. Table 1. Na u al equencies and damping a ios iden i ied by SSI-co and di e en ime blocks. Mode 60 min. 1s 20 min. 2nd 20 min. 3 d 20 min. (Hz) 𝜻𝜻 (%) (Hz) 𝜻𝜻 (%) (Hz) 𝜻𝜻 (%) (Hz) 𝜻𝜻 (%) - 0.8671 0.3352 0.8663 0.2526 - - 0.8660 1.0824 - - - 1.0251 0.3793 1.0243 0.1433 1.0281 1.8147 1 1.0548 0.9622 1.0536 0.3755 1.0518 0.3513 1.0535 0.4883 2 1.4077 0.3792 1.4073 0.3523 1.4059 0.5874 1.4093 0.2594 3 1.5408 0.6762 1.5408 0.5343 1.5395 0.7945 1.5431 0.7658 4 1.7869 0.4483 1.7884 0.5036 1.7882 0.6227 1.7833 0.4014 5 1.8571 0.6381 1.8567 0.6340 1.8574 0.6775 1.8569 0.4995 - - - 1.9260 0.3870 - - - - 6 2.3020 0.4799 2.3022 0.4444 2.3020 0.5353 2.3014 0.4788 - 2.6819 0.3206 - - 2.6802 0.2709 2.6836 0.2546 - - - - - - - 2.7306 0.4594 - - - - - 2.7848 0.3825 - - - 2.8051 0.5159 2.8097 0.7520 - - 2.8041 0.4918 - - - - - 2.8147 0.1976 - - - 2.8682 0.3238 - - - - 2.8631 0.3248 - - - 2.9171 0.2887 - - - - 7 3.3674 0.4485 3.3680 0.4194 3.3659 0.4449 3.3709 0.4587 8 3.5375 0.8723 3.5356 0.6417 3.5361 0.9920 3.5343 0.8376 9 3.9487 0.5106 3.9443 0.4427 3.9458 0.5759 3.9552 0.3504 Table 2 p esen s a summa y o he selec ed modes. The able shows he mean alues o he 20-minu e es s and he maximum e o s compa ed wi h he esul s ob ained wi h he 60-minu e es . In his case, he maximum e o s ob ained a e 0.2855% and 61.09% o equencies and damping a ios espec i ely. The e o s in na u al equency es ima es using 20 minu es as compa ed wi h 60 a e negligible. 46 Table 2. Summa y o iden i ied mode equencies and s a is ical compa ison o he 20-minu e agains 1-hou ime blocks: mean equency, mean damping and co esponding e o s. Mode F equency Damping 𝒇𝒇� (Hz) E o (%) 𝜻𝜻 �(%) E o (%) 1 1.0530 0.2849 0.4050 61.09 2 1.4075 0.2416 0.3997 32.80 3 1.5411 0.2336 0.6982 26.02 4 1.7866 0.2855 0.5092 22.13 5 1.8570 0.0377 0.6037 17.80 6 2.3019 0.0348 0.4862 9.090 7 3.3683 0.1484 0.4410 3.930 8 3.5353 0.0905 0.8238 35.05 9 3.9484 0.2761 0.4563 22.55 Figu e 4 shows an example o iden i ied modal shapes co esponding o he lowes six modes ob ained wi h SSI-co o he 60-minu e es . (a) = 0.87 Hz (b) = 1.05 Hz (c) = 1.41 Hz (d) = 1.55 Hz (e) = 1.79 Hz ( ) = 1.86 Hz Figu e 4. Fi s six modes shapes ob ained wi h SSI-co . 47 4. CONTINUOUS DYNAMIC ANALYSIS The p ocedu e ca ied ou o ack he ib a ion modes is depic ed in Figu e 5. The esul s ob ained om 1-yea o con inuous dynamic moni o ing a e desc ibed om now on. A me hod o ack he e olu ion o he main ib a ion modes o e ime is desc ibed. Then, he in luence o he en i onmen al/ope a ional ac o s on he modal es ima es is s udied. 4.1. T acking o modal p ope ies Fo a single es , no special ea men on SSI i sel o sepa a e closely-spaced equencies is conside ed. Howe e , in a dynamic con inuous moni o ing amewo k, he ib a ions modes mus be ca e ully acked since hei na u al equencies can be simila and e en can change hei o de . The e o e, a p ocedu e o link modal pa ame e s iden i ied om each da a se ha a e associa ed wi h he same ib a ion mode is needed. A c i e ion based on selec ing a mode wi hin a ixed equency ange could lead o w ong esul s due o he a ia ion o equency anges be ween di e en es s. As a consequence, i p oposes a acking me hod in o de o ollow he e olu ion o he main ib a ion modes o e ime. F om he acqui ed da a, an au oma ed OMA has been implemen ed using SSI-co . The p ocedu e ca ied ou is depic ed in Figu e 5. The p ocess can be di ided in o he ollowing s eps: Figu e 5. T acking p ocedu e o modal pa ame e s. 48 •Take he las N es s, N being he numbe o es s. N should be ep esen a i e o he a iabili y o he modal es ima es. •Fo each es , he OMA is ca ied ou . Thus, a numbe o modes o each es is iden i ied and deno ed as 𝑟𝑟𝑖𝑖 (wi h i = 1 . . .N). •The objec i e is o ind modal es ima es ha co espond o he same pe sis en mode o e ime. Each modal shape es ima e is compa ed wi h all he emainde es ima es wi hin he N es s and a coun e inc eases each ime ha wo mode shapes ma ch. The coun e indica es he epea abili y o a ib a ion mode. This is done o all he modal shape es ima es. To ca y ou his s ep, he MAC alue is used. Tha is, a numbe o �∑𝑟𝑟𝑖𝑖 𝑁𝑁 𝑖𝑖=1 � es ima es a e compa ed using he MAC alue. Th ee ole ances ha e been de ined o his pu pose: o ol1: he i s one is a MAC alue ha allows o g oup es ima es co esponding o he same ib a ion mode. The epea abili y is he numbe o es ima es o a g oup. o ol2: he second one is included in o de o ejec g oups ha a e no epea ed su icien ly o be conside ed as signi ican modes. This ole ance is he lowe limi o success a io, ha is, g oups wi h low epea ibili y a e au oma ically ejec ed. o ol3: he hi d one is a MAC alue inally included o de ec g oups o es ima es ha a e ac ually es ima ions o he same mode. Then, i mo e han one g oup co espond o he es ima ion o he same mode, he one wi h highe epea abili y is selec ed. •F om abo e p ocedu e, he mos signi ican modes o he dynamic esponse o he s uc u e a e de ec ed o he N es s. •Va ia ions o hese selec ed modes a e s a is ically s udied and co ec ed modal pa ame e s a e de i ed. The abo e acking me hod is applied o consecu i e ime-his o y eco ds e e y 20 minu es using SSI- co . A numbe o N = 21643 es s ha e been aken o he whole yea 2013. I compu a ional bu dens appea , he p ocedu e explained abo e mus be modi ied sligh ly. In ha case, he es s should be di ided in o sub-blocks (N = 500) o sol e he p oblem. Tha done, you jus ha e o join each sub-block wi h he nex sub-block using he ol1. The ole ances chosen o ca y ou he acking we e: ol1 ≥ 0.95, ol2 ≥ 40% and ol3 ≤ 0.80. Up o nine ib a ion modes below 4 Hz ha e been acked. Table 3 shows he ollowing s a is ics o he es ima ion: mean, s anda d de ia ion, absolu e pe cen age a ia ion and hei epea abili y ( he success a io is included be ween b acke s). No e ha he ou h mode, wi h a equency a ound 1.79 Hz (and wi h a damping a io o only 0.42%) is p one o be exci ed by pedes ian walking. Table 3. Summa y o iden i ied na u al equencies and damping a ios o one yea moni o ing and hei s a is ics: mean equency, mean damping, s anda d de ia ion and co esponding a ia ion. Mode F equency Damping Repea abili y 𝒇𝒇� (Hz) S d 𝝊𝝊 (%) 𝜻𝜻 �(%) S d 𝝊𝝊 (%) 1 1.0482 0.0152 14.23 0.3665 0.1710 147.89 9667 (44.7%) 2 1.4145 0.0107 35.26 0.3381 0.1513 110.74 10619 (49.1%) 3 1.5440 0.0181 27.63 0.6498 0.2357 133.62 9886 (45.7%) 4 1.7937 0.0291 20.27 0.4192 0.1502 221.88 13817 (63.8%) 5 1.8594 0.0168 6.87 0.5718 0.1605 234.74 9936 (45.9%) 6 2.3117 0.0425 15.01 0.3753 0.1474 128.54 8746 (40.4%) 7 3.3821 0.0549 42.95 0.3868 0.1191 103.96 12210 (56.4%) 8 3.5512 0.0524 51.87 0.7226 0.1884 157.48 9237 (42.7%) 9 3.9619 0.0624 8.95 0.3853 0.1185 230.82 10183 (57.8%) 49 he p ojec a e: ISOLUX CORSÁN, FCC CO, GEOCISA, CSIC and UPM. The au ho s also acknowledge he inancial suppo p o ided by Resea ch P ojec DPI2013-47441-P. REFERENCES [1] A ci, O. (2014). Modal Pa ame e Va ia ions due o Jois Bo om Cho d Ex ension Ins alla ions on Labo a o y Foo b idges. Jou nal o Pe o mance o Cons uc ed Facili ies 04014140. DOI: 10.1061/(ASCE)CF.1943-5509.0000635. 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