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Microscopical observations of inter-fibre failure under tension

Correa Montoto, Elena; Valverde, María Inmaculada; Velasco López, María Luisa; París Carballo, Federico

Abstract

The numerical study of the inter-fibre failure at micromechanical level predicts the appearance of different stages in the development of this damage mechanism; these studies have also allowed the main features of each stage (such as the interfacial debond length and the kinking angle) to be identified. The development of experimental studies aiming to check the relevance of the aforementioned numerical results is crucial. Based on this, this research focused on the tensile test under different loading levels of specimens manufactured from carbon-epoxy cross-ply symmetrical laminates. The microscopic observation of the 90° layers leads to the analysis of the appearance of the transverse cracks as a function of the load, the identification of the previously numerically predicted stages of the mechanism of damage, the measurement of key parameters and the evaluation of the influence of nearby fibres. A clear connection between the numerical and experimental results has been found.

Full text

Depósi o de In es igación de la Uni e sidad de Se illa h ps://idus.us.es/ This is an Accep ed Manusc ip o an a icle published by Else ie in Composi es Science and Technology, Vol. 158, on Feb ua y 2018, a ailable a : h ps://doi.o g/10.1016/j.compsci ech.2017.12.009 © 2017 Else ie . En idUS Licencia C ea i e Commons CC BY-NC-ND Mic oscopical obse a ions o in e - ib e ailu e unde ension Elena Co ea, Ma ía Inmaculada Val e de, Ma ía Luisa Velasco, Fede ico Pa ís Depa amen o de Mecánica de Medios Con inuos y Teo ía de Es uc u as, G upo de Elas icidad y Resis encia de Ma e iales, Escuela Técnica Supe io de Ingenie ía, Uni e sidad de Se illa, Camino de los Descub imien os s/n, 41092, Se illa, España Abs ac The nume ical s udy o he in e - ib e ailu e a mic omechanical le el p edic s he appea ance o di e en s ages in he de elopmen o his damage mechanism; hese s udies ha e also allowed he main ea u es o each s age (such as he in e acial debond leng h and he kinking angle) o be iden i ied. The de elopmen o expe imen al s udies aiming o check he ele ance o he a o emen ioned nume ical esul s is c ucial. Based on his, his esea ch ocused on he ensile es unde di e en loading le els o specimens manu ac u ed om ca bon-epoxy c oss-ply symme ical lamina es. The mic oscopic obse a ion o he 90º laye s leads o he analysis o he appea ance o he ans e se c acks as a unc ion o he load, he iden i ica ion o he p e iously nume ically p edic ed s ages o he mechanism o damage, he measu emen o key pa ame e s and he e alua ion o he in luence o nea by ib es. A clea connec ion be ween he nume ical and expe imen al esul s has been ound. Keywo ds: debonding; ans e se c acking; op ical mic oscopy; c oss-ply. A.1. In oduc ion Ma ix/In e - ib e ailu e a ises in plies subjec ed o ans e se loads, being cha ac e is ic, among o he s, o 90° plies belonging o c oss-ply lamina es subjec ed o loads pa allel o hei 0° plies. P e ious nume ical s udies allowed he iden i ica ion o h ee main s ages in he mechanism o damage a mic omechanical le el, Figu e A.1. In pa icula , in he case o ensile loads (Pa ís e al [1]), damage ini ia es wi h he appea ance o small debonds a he ib e-ma ix in e aces aligned wi h he applied load (S age I); hese debonds g ow uns ably in Mixed Mode along he in e aces un il eaching an ex ension (semi-debonding angle,  d) o 60°-70° (S age II); a his posi ion, a change o s able g ow h in pu e Mode II akes place (caused by he appea ance o a physically ele an con ac zone a he c ack ip), a ou ing he kinking o he c ack owa ds he ma ix (S age III). The c ack inally p opaga es along he ma ix (uns ably and in Mode I) ollowing he di ec ion pe pendicula o he load applied. The coalescence o his ype o c acks coming om di e en ib es gi es ise o ans e se mac o-c acks in he ply, e en ually leading o i s ca as ophic ailu e. Figu e A.1. S ages o he mechanism o damage. Pa ís e al [1]. The e ec ha he p esence o a seconda y load (Pa ís e al [2], Co ea e al [3]) has on he e olu ion o hese s ages, he conside a ion o he mal esidual cu ing s esses (Co ea e al [4]), and he case o cyclic loading (Co ea e al [5]), ha e also been s udied nume ically. The impo an ole ha mic omechanical s udies can play in helping i s in he unde s anding o he mechanism o ailu e and second in e i ying and p oposing ailu e c i e ia was poin ou in hese wo ks. In pa icula , his ou s anding ques ion was deeply analysed in Pa ís [6]. A common pa e n o hese s udies is he usage o a single ib e (assumed isola ed) Bounda y Elemen model. Mo e ecen wo ks, ocusing on S age II o he mechanism o damage, also include a la ge numbe o ib es, see o ins ance Sandino e al [7] ( wo- ib es models), Tá a a e al [8] ( en- ib es models) and Tá a a e al [9] (one hund ed- ib es models). FEA has also been used o s udy his p oblem; see o ins ance Hojo e al [10], Kushch e al [11] y Sai o e al [12]. A his poin , i u ns ou c ucial o check, by means o expe imen al s udies, he alidi y o he esul s de i ed om he nume ical models, speci ically, by means o mic oscopic obse a ion o es ed samples. P e ious wo ks om di e en au ho s ocusing on he expe imen al mic omechanical obse a ion o he ma ix ailu e can be ound in he li e a u e; among hem i can be s ood ou he al eady classical wo ks by Zhang e al [13] (single ib e es s unde ension) and Gams ed and Sjög en [14] (based on Zhang bu s udying he e ec o cyclic load), and also hose om Sai o e al [15] (analysing he e ec o he 90º ply hickness in c oss ply lamina es), Ba al e al [16] (s udying he e ec o he ib e ype), Hobbieb unken e al [17] (compa ing he beha iou be ween high and low cu ing empe a u e esins in h ee poin s bending es s) o STAGE I a ≈10º  d=60-70º STAGE II STAGE III Genz e al [18] (e alua ing he p esence o he mal esidual s esses). In he p esen wo k, an op ical mic oscope is used o obse e he 90 plies o c oss-ply specimens es ed unde longi udinal ensile load (which will be hus ans e se o he 90 plies), in o de o check i he nume ically p edic ed mic omechanical s ages o he ma ix/in e - ib e ailu e a e in ac p esen and can be dis inguished. The iden i ica ion o he di e ences ha hese s ages show in eal lamina es wi h a high ib e olume con en e sus he nume ical single (and isola ed) ib e models, is also pu sued. In addi ion, he measu emen o he inal ex ension o he c ack a he in e ace ha gi es ise o he kinking owa ds he ma ix (  d= 60-70, om he nume ical models), as well as he s udy o he di e en damage ypologies, he analysis o he in luence o he applied loading le el and he e ec o he p esence o neighbou ing ib es, a e also objec i es o he s udy. A.2. Coupons manu ac u ing and es ing [03,903]s ensile coupons we e manu ac u ed om ca bon-epoxy (AS4-8552) p e-p eg, ein o cing hei ends wi h glass-epoxy abs. Thei dimensions a e de ailed in Figu e B.2. Figu e A.2. Coupons dimensions. A i s se o 5 coupons was selec ed o es ing unde ension. The esul s p o ided by he ensile s eng h (X) show a mean alue o 942.47 MPa, a s anda d de ia ion o 41.25 MPa and a a ia ion coe icien o 4.38%, he e o e implying an excellen esul in e ms o dispe sion. Subsequen es ing campaigns we e pe o med unde maximum loads lowe han he p e iously measu ed X, in o de o gene a e damage in he 90 plies wi hou eaching he ca as ophic ailu e o he whole lamina e. In pa icula , he loads applied can be g ouped in 5 le els: 80%X, 60%X, 40%X, 30%X and 20%X. The numbe and denomina ion o he coupons es ed as well as he exac loading le el applied a e included in Table A.1. Table A.1. Denomina ion o he coupons and co esponding es ing load. Coupons denomina ion Tes ing load (%X) 80-1 84.2 80-2 82 60-1 62.4 60-2 59.5 60-3 60.5 40-1 42.6 40-2 40.3 40-3 39.2 30-1 31.5 30-2 29 30-3 27.6 20-1 21 A.3. P epa a ion o samples The cen al pa o he specimens was cu in wo hal es o app oxima ely 28 mm leng h; each pai was encapsula ed in esin (using he Ve soCi -2 ki ). A e ha , he samples we e polished using Saphi 20 polishe (au oma ic head and p og ammable) om NEURTEK Ins umen s, LaboDose liquide dispense and LaboPol-5 as pe iphe al polishe om S ue s. The esul o he polishing p ocess mus allow he ib es co esponding o he 90 plies o be clea ly obse ed in an op ical mic oscope a 1000x magni ica ion. A sui able polishing p ocess should also a oid he appea ance o ma ks ha could in e e e in he la e mic oscopical inspec ion. To his pa icula end, a speci ic polishing p ocess was designed and es ed, consis ing o ou s eps. 40N p essu e and 50 pm speed a e selec ed o all s eps, he disc ype, e ige a o liquid and ime used a e de ailed nex : S ep 1: Disc: SiC #320. Liquide: Wa e . Time: 5’. S ep 2: Disc: MD-La go. Liquide: DiaP o Alleg o/La go 9 μm (2). Time: 6’. S ep 3: Disc: MD-Dac. Liquide: DiaP o Dac 3 μm (1). Time: 5’. S ep 4: Disc: MD-Dac. Liquide: DiaP o Nap B1 1 μm (3). Time: 4’. A.4. Mic oscopic obse a ion Once he samples ha e been polished he mic oscopic inspec ion is unde aken. The e is a double objec i e he e: i s , using low magni ica ion (25x), he analysis o he appea ance o ans e se c acks in he 90 plies as a unc ion o he load applied. Second, he s ages o he mechanism o damage p e iously iden i ied by he nume ical models wan o be de ec ed, along wi h he expe imen al alues o hei main pa ame e s; o his end, obse a ion a high magni ica ion (500x and 1000x) is equi ed. A.4.1. Inspec ion a low magni ica ion A i s inspec ion is made a 25x in o de o coun he numbe o ans e se mac o-c acks ha appea s in each specimen, and hus i s loading le el dependence. In Table A.2 he numbe o c acks obse ed pe cm in each coupon is de ailed. The mos ele an conclusion is ha o loads lowe han 30%X no ans e se mac o-c acks a e obse ed in he samples. A la e inspec ion a g ea e magni ica ion will also show, Sec ion A.4.2, ha no damage o any ype is de ec ed below his loading le el. I is also obse ed ha he numbe o c acks encoun e ed inc eases as he loading le el does. No ice in any case he educed numbe o samples chosen o he lowes loading le els. Table A.2. Numbe o mac o-c acks as a unc ion o he loading le el. %X Numbe o mac o-c acks/cm 84.2 9 82 9.2 62.4 6.4 59.5 4 60.5 3.6 42.6 3.5 40.3 1.2 39.2 0.8 31.5 2.3 29 0 27.6 0 21 0 Al hough no being di ec ly he objec i e o his pape , making use o he Classical Lamina e Theo y (CLT) and selec ing a sui able ailu e c i e ion i is possible o p edic he s ess associa ed wi h i s -ply ailu e (XFPF). Then, i is in e es ing a his poin o check i he lowes s ess alue o which damage has been de ec ed in he ma e ial (31.5%X in his case, see Table A.2) is accu a ely p edic ed by he Lamina e Theo y in combina ion wi h ailu e c i e ia. To his end, a selec ion o ailu e c i e ia (Maximum S ess, Tsai-Hill (Azzi and Tsai [19]), Tsai- Wu [20], Maximum S ain, Hashin [21], Hashin and Ro em [22] and Puck [23]) has been pe o med, and hei XFPF p edic ions calcula ed, see Table A.3. Table 3. Fi s -ply and ul ima e ailu e p edic ions o a selec ion o ailu e c i e ia. Failu e C i e ion XFPF (MPa) XUF (MPa) XFPF/XUF (%) Maximum S ess 374.4 1112.9 33.6 Tsai-Hill 374.1 1109.5 33.7 Tsai-Wu 368.1 1149.1 32.0 Maximum S ain 367.2 1124.6 32.7 Hashin 374.4 1112.9 33.6 Hashin-Ro em 374.4 1112.9 33.6 Puck 374.4 1113.8 33.6 Fi s o all, i can be obse ed ha all ailu e c i e ia show simila p edic ions wi h a mean alue o 372 MPa. This alue can be compa ed wi h he lowes expe imen al load o which ans e se c acks a e obse ed, 31.5%X in his case, which co esponds o a s ess alue o 297 MPa. Taking in o accoun ha he numbe o coupons included in he 30%-40%X g oup is small (see Table A.2) and also ha all o hem show a e y educed numbe o ans e se c acks, a good ag eemen be ween he analy ical p edic ion and he expe imen al esul is ound. The appea ance o he i s c ack a a alue lowe han ha p edic ed by he c i e ia o he ailu e o he ply is, on he o he hand, a e y cohe en ac , as he appea ance o one ans e se c ack does no mean he o al ailu e o he ply. The appea ance o ans e se c acks in a 90 ply is a con inuous (no sudden) phenomenon, and i can be checked ha (as men ioned abo e), o he i s ply ailu e p edic ed by he c i e ia, only a e y educed numbe o c acks appea in he specimen, his ac no implying a signi ican educ ion in he con ibu ion o he 90 ply o he p ope ies and pe o mance o he lamina e. Ano he in e es ing ea u e a ises when using he CLT o also p edic he s ess associa ed wi h he ul ima e ailu e (XUF) and hen o calcula e he a io be ween XFPF and XUF (Table A.3), i.e. using only he analy ical ool o e alua e a which pe cen age o he analy ical ul ima e s ess he heo y p edic s he ini ia ion o damage. This calcula ion o XUF has been pe o med by means o a p og essi e damage model, using a deg ada ion coe icien D equal o 0.1 ha ac s on all ma e ial p ope ies bu jus sligh ly in his pa icula case due o i s small alue. The esul s show again simila p edic ions o all c i e ia and an app oxima e alue o 33%XUF is ob ained o XFPF. An excellen ag eemen is ound now be ween his p edic ion and he expe imen al esul , as he i s ans e se c acks we e de ec ed a 31.5%X. The obse a ion o he 25x mic og aphs shows some ele an di e ences be ween he di e en loading le els, in pa icula : 1) Specimens es ed a 20%X (see Figu e A.3a as an example): No damage is de ec ed. 2) Specimens es ed a 30%X (see Figu eA.3b as an example): Jus a ew and e y hin ans e se c acks a e ound in one specimen. A educed numbe o delamina ions be ween 90º and 0º plies a e p esen . 3) Specimens es ed a 40%X (see Figu e A.3c as an example): Some ans e se c acks a e ound al hough hey appea like hin lines in he mic oscope. Delamina ions be ween 90º and 0º plies a e p esen . 4) Specimens es ed a 60%X (see Figu e A.3d as an example): Many and well de ined ans e se c acks a e ound. Some c acks show a pa h de ia ed om he ans e se di ec ion. Delamina ions be ween 90 and 0 plies a e de ec ed. 5) Specimens es ed a 80%X (see Figu e A.3e as an example): Many and well de ined ans e se c acks a e ound (mo e han in he p e ious case). Mos o hem appea like hick lines a he mic oscope, which is associa ed wi h a clea ly de eloped damage and p obably wi h a signi ican opening o he c ack lips. Mo e de ia ed c acks a e obse ed. Delamina ions be ween 90 and 0 plies a e also de ec ed. I should be ema ked ha he h ough hickness c ack loca ion does no show a p e e en ial pa e n, which seems o be in acco dance wi h CLT p edic ions (assuming he 90 ply as homogeneous) and also wi h he ou comes o a ecen nume ical s udy by he au ho s (modeling he 90º ply as he e ogeneous and dis inguishing be ween ib es and ma ix), Pa ís e al [24]. (a) (b) (c) (d) (e) Figu e A.3. 25x mic og aphy om (a) 20-1 specimen, (b) 30-1 specimen, (c) 40-1 specimen, (d) 60-1 specimen, (e) 80-2 specimen. A.4.2. Inspec ion a high magni ica ion The inspec ion o he samples using a g ea e magni ica ion is nex pe o med in o de o y o expe imen ally iden i y he di e en phases o he mechanism o damage nume ically p edic ed in [1] (Figu e A.1); in pa icula , he occu ence o S ages I, II and III, hei connec ion wi h he loading le el as well as he measu emen o speci ic pa ame e s ele an o he de elopmen o he mechanism o damage, a e pu sued. Indeed, he obse a ion o samples a high magni ica ion exposes he appea ance o all s ages o he ailu e mechanism (I, II and III, Figu e A.1) o loading le els highe han 30%X. Speci ically, damage appea s in clea ly less quan i y in he 30%X g oup, maximizing i s appea ance in he 60%X g oup (p obably associa ed wi h he ac ha in he 80%X g oup isola ed s ages disappea o ming a g ea e numbe o mac o-c acks). Figu e A.4 shows 1000x images o S ages I and II (a), and S age III (b). No ice ha he nominal ib e adius is 3.56 m, use ul as scale e e ence o Figu e A.4 and he o hcoming Figu es A.5, A.7, A.8 and A.9. (a) (b) (c) Figu e A.4. 1000x mic og aphies o : (a) S ages I and II (30%X), (b) S age III (40%X), (c) Aligned debonds (40%X). I is necessa y o ema k ha i is no possible o dis inguish be ween S ages I and II wi h he a ailable ools because, among o he hings, i is no nume ically clea i a eal sepa a ion be ween bo h s ages exis s. The uns able cha ac e o he mechanism o ailu e and he dependence o he ini ia ion o ailu e on he p ope ies o he in e ace (in pa icula on he ac u e oughness) a e some o he ea u es ha poin i as an open ques ion. The mo e ecen publica ions on Fini e F ac u e Mechanics (Man ič [25], Man ič and Ga cía [26]) s udy in dep h his p oblem. Wi h e e ence o S age II, i is common o ind he debonds a his s age e y close o a eas whe e mac o-c acks al eady exis , al hough a low loading le els hey a e also de ec ed as isola ed, a om hese a eas. The S age II debonds o en appea aligned in high ib e densi y zones, so ha he pa h ollowed by he u u e mac o-c ack can be en isaged, Figu e A.4c. No e y equen ly, ib es wi h bi-la e al debonds a e obse ed (Figu e A.5a) al hough cu en ly bo h debonds do no p esen he same ex ension and hus, no simul aneous g ow h is deduced. The exis ence o hese bi-la e al debonds can be also obse ed in mac o-c acks, Figu e A.5b; in hese cases he bi-la e al debond seems o appea when he ib e is placed in he middle o he pa h o he mac o-c ack. (a) (b) Figu e A.5. 1000x mic og aphies o bi-la e al debonds (a) a S age II (60%X), (b) in mac o-c acks (60%X). Re e ing o S age III, se e al kinking pa hs addi ional o he nume ical heo e ical one ha e been iden i ied using he mic oscope. Figu e A.6 shows all ypologies ound, ha ing been named as de ailed: A. Theo e ical, B.1. De ia ed +, B.2. De ia ed –, C. Bila e ally angen ial, D. G adual ansi ion and E. Spli ing. STAGE I STAGE II STAGE III [20] S.W. Tsai, E.M. 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