Multiphase carbon fiber MWNT / epoxy resin composites
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https://www.eduzhai.net International Journal of Composite M aterials 2013, 3(6A): 1-9 DOI: 10.5923/s.cmaterials.201309.01 Multi-Phase Carbon Fiber-MWNT/Epoxy Composites Antonio F. Ávila1,*, Glaúcio Carley2, Viviany Geraldo3, Sergio de Oliveira3 1Department of M echanical Engineering, Universidade Federal de M inas Gerais, Belo Horizonte, 31270-901, Brazil 2Graduate Studies Program in M echanical Engineering, Universidade Federal de M inas Gerais, Belo Horizonte, 31270-901, Brazil 3Department of Physics, Universidade Federal de M inas Gerais, Belo Horizonte, 31270-901, Brazil Abstract The concept of mult i-phase carbon fiber/nanotube was successfully introduced to high performance composites. This new laminated co mposite was characterized by Raman spectroscopy, X-ray d iffraction, scanning electron microscopy and tensile tests. An increase on peak stress close to 85% was witnessed when the multi-phase interlayer with 206.30 mg of carbon nanotubes (CNTs) was p laced into carbon fiber/epo xy laminates. The failure mechanis ms are associated to CNTs distribution between and around carbon fibers. These CNTs are also responsible for crack bridging formation and the increase on peak stress. Initial stiffness is strongly affected by the CNT interlayer, however, changes on stiffness is associated to changes on nano/micro-structure due to damage. Three d ifferent behaviors can be described, i.e. for mult i-phase interlayer with appro ximately 60 mg of CNT; the failure mode is based on cracks between and around carbon fibers, wh ile fo r ones with CNT contents between 136 mg and 185 mg cracks were spotted on fibers and inside the CNT/ matrix interface. The third, and final, failure mechanism is based on carbon fiber breakage, as a strong interface between CNT/ mat rix and carbon fibers was observed. Keywords Carbon nanotubes, Carbon fiber/Epo xy co mposites, Multi-phase composites, Raman spectroscopy 1. Introduction In recent years, a new t rend on co mposite materials is emerging, i.e. mu lti-phase composites. This is due to the increase on demand in aerospace and automotive industries due to their good characteristics of light weight, imp roved strength, corrosion resistance, reduced manufacturing and maintenance costs. Multi-scaled composites (MSC) are mu lti-phase reinforced composites, i.e. in addition to traditional reinfo rcement carbon fibers; the matrix is replaced by nanocomposites. As commented by Joshi and Dikshirt, nanocomposites can be obtained by dispersing nanoparticles/nanostructures into the polymeric matrix. According to Gouda et al, carbon based nano-structures, i.e. carbon nanotubes (CNT) and graphene nano sheets (GN), present remarkable mechanical, electrical and thermal properties. CNT capabilities have been observed experimentally and verified by numerical simulat ions. Although carbon nanotubes have great potential for applications in a large variety of usages, e.g. aerospace industry, medical and electronic devices, there is no consensus about their exact mechanical properties. As described by Saito et al, carbon nanotube is a honeycomb lattice rolled into a cylinder. Carbon nanotubes (CNTs) have been the center of many researches due to * Corresponding author: firstname.lastname@example.org (Antonio F. Ávila) Published online at https://www.eduzhai.net Copyright © 2013 Scientific & Academic Publishing. All Rights Reserved their dimensions and remarkable electro-mechanical properties. In general, a CNT diameter has a nanometer size and its length can be more than 1μm. Its large aspect ratio (length/diameter) is appointed as one of the reasons for the CNTs notable properties. According to Kalamkarov et al, single-walled nanotubes (SWNTs) have predicted specific strength around 600 t imes larger than steel. CNT capabilit ies have been observed experimentally and verified by numerical simu lations. Frankland et al, Jin and Yuan  and Agrawal et al are among those researchers who emp loyed molecu lar dynamics for analyzing CNTs. The atomistic simulation approach was employed by Belytschko et al, Lu rie et al, Gates et al, while the nano-mech anics modeling was described by Liu et al, Ruoff and Pugno, Li and Chou, Ávila et al. Although CNTs have tremendous potential in a large variety of applications, e.g. aerospace and medical industries, there is no consensus about their exact mechanical properties. The experiments performed up to now have presented large variability due to the inherent complexity of man ipulating these materials. However, their potential is unquestionable, in special for co mposites. As mentioned by Ávila et al, carbon based nano-structures, i.e. carbon nanotubes and graphene nano sheets (GN), can be combined to traditional co mposites for a mu lti-scale reinforcement. Moreover, the recent developments on CNT synthesis led to dramat ically decreased into its cost. As a consequence, the number of researchers using carbon based nanostructures increased, and the results on nano-reinforcement of co mposites 2 Antonio F. Ávila et al.: M ulti-Phase Carbon Fiber-M WNT/Epoxy Composites laminates are encouraging. Among those researchers are Kim et al who m described no significant increase on tensile properties of the addition of CNTs to carbon fibers/epoxy laminates. Nonetheless, they noticed an enhancement on flexural modu lus (≈12%) and strength (≈18%) with the addition of 0.3 wt. % of CNT to the epo xy system. This increase can be attributed to changes into flexu ral failure mechanis ms. Fo llo wing the same idea, Chou et al discussed the influence of CNTs into the failure of laminated composites. They even proposed the concept of a mu lti-phase inter-laminar architecture that can bridge inter-laminar cracks. Wicks et al actually produced the mu lti-phase nano reinforced laminated composites proposed by Chou et al In their laminate, CNTs were grown in situ in all fibers leading to a “fuzzy” fibers configuration. As mentioned by Wicks, aligned CNTs bridges the plies interfaces, wh ich can lead to an increase on toughness, for the steady state condition, 76% higher than the conventional laminated systems. Notice that fo r the interlayer nano reinforcement some issues must be considered, i.e. the interfacial bonds between carbon nanotubes, fiber/matrix system and the length effect into this “grip condition”. To understand the failure mechanis m, Shokrieh and Rafiee modeled the CNT length effect on reinforcement effectiveness. Moreover, they concluded that for carbon nanotubes with length less than 100 n m, the imp rovement on stiffness for CNT/poly meric systems is neglig ible. Experimental data provided by Ma et al demonstrated the limitat ions of using CNTs with aspect ratio smaller than 100 into polymeric systems. The “fuzzy” fibers configuration developed by Wicks et al is also limited as all plies have to be loaded with carbon nanotubes. This increase on “fiber density” due to the “CNTs loads” can lead to manufacturing limitations, e.g. a severe decrease on res in flow channels into vacuum assis ted impregnation. It is clear that alternative techniques must be developed. Different techniques have being tested for incorporating CNTs into composite materials. The CNT in fusion into laminated composites and its alignment by applying an electric field after the infusion was studied by Domingues et al. The major crit icis m on Do mingues’ work is the amount of CNT d ispersed which is around 0.1 wt. %. Another approach tried to lin k CNTs to laminated composites was imp lemented by Wu et al. Wu’s work was based on electrochemical grafting of CNTs on carbon fibers surface. Although the technique described by Wu et al seems to be effect ive, it is limited to the CNT concentration into the solution. Moreover, as noticed by Wu, there were “preferential regions” for CNTs direct attachment to carbon fibers. These preferred sites were fibers’ grooves and edges. This phenomenon led to a non-uniform d istribution of CNT on carbon fibers surface. Another technique used for attaching CNTs to carbon fibers was studied by De Riccard is et al and Vilatela et al. In their case, the chemical vapor deposition (CVD) technique was emp loyed for directly gro wn CNTs into carbon fibers. De Riccard is’ work was based on deposition of nickel clusters and later on the CNTs were grown by hot filament chemical vapor deposition (HFCVD) technique. By using ferrocene as precursor, and CVD as the growing process, Vilatela was also able to obtain good quality CNTs. Moreover, the CVD technique employed by Vilatela and collaborators seems to be much simp ler and easier to control. Although the results presented by De Riccard is et al and Vilatela et al seem to be encouraging, much work has to be done for applicat ions to laminated composites, in special h igh performance carbon fiber/epo xy s ys tems . This paper focuses on synthesis and analysis of carbon fiber/epo xy laminated composites with the addition of an extra interlayer where CNTs were d irectly grown by thermal CVD. 2. Experimental Procedure 2.1. Materials The plain weave fiber g lass used in this research has an areal density of 180 g/ m2. To be able to understand the carbon nanotubes effect as interlayer into carbon/epoxy laminated composites, five different CNTs forests were grown in situ into the plain weave fiber glass. These fiber glass fabrics loaded with CNTs were p laced between two layers of carbon fibers. The carbon fibers have a plain weave configuration and areal density of 200 g/ m2. The epo xy system employed here is based on diglycidil ether bisphenol A (DGBA ) resin and an amine hardener, i.e. AR300 and a mix of AH30/AH150 supplied by Barracuda Co mposites Inc. The resin/hardener ratio employed was 100:27. The fiber/epo xy system ratio is equal to 50:50. To be able to create a mu lti-phase/hybrid composite, a nano-phase was added to the fiber. Note that this procedure is different fro m the ones proposed by Ma et al which dis persed CNTs into the res in and also distinct from the ones proposed by Wicks et al. Instead of using a “fuzzy” configuration as described by Wicks, in this research the CNTs were grown in radia l direction in a “carpet” format ion. The carbon nanotubes (CNT’s) were grown directly to the fibers using a therma l che mical vapor deposition (CVD). 2.2. Synthesis and Characterizati on As discussed by Mathur et al, thermal CVD has high growth rate, i.e. 10µm/ min , and the CNTs diameters ranges fro m ≈ 40-60 n m. Moreover, Raman spectroscopy indicates a good crystallinity of mult iwall carbon nanotubes. In this research, a thermal CVD device fro m FirstNano was used for growing CNTs directly into glass fibers. CNTs can be grown over a te mperature range of 600-900 C using thermal CVD. After a series of tests, the optimu m temperature, considering the CNTs alignment, was selected as 750 C at an inert atmosphere (argon). The precursor used in this research was developed at UFMG’s Nano materials Laboratory (LN) fro m Physics Department. The catalyst emp loyed was based on Iron (Fe) and Cobalt (Co) supported by Magnesium o xide International Journal of Composite M aterials 2013, 3(6A): 1-9 3 (MgO). The catalyst powder was evenly distributed into the fibers’ cloth, and later on the fibers’ cloth was placed in the furnace main heating zone at 400 C for o xidation for 1 hour. The carbon source for the CVD process was ethylene (C2H2) at 300 sccm and the inert at mosphere was based on argon at 500 sccm. The CVD synthesis temperature was 750 C and each synthesis batch took around 30 minutes. The CNTs produced were main ly mu ltiwall carbon nanotubes with average diameter of 35 n m and length ranging from 5-50 μ. Once the CNTs were d irectly grown into the fibers, the next step is the composite manufacture. One of the most common techniques for composites’ production is the resin impregnation based on hand lay-up while the composite final consolidation is performed by cure under vacuum. The total time for cure was 24 hours, 6 under vacuum and the remaining under air. As we are dealing with mu lti-phase composites, it is impo rtant to characterize the nanostructures formation and location. According to Rodriguez et al, during the nanoparticles dispersion into polymeric mat rices nano-structures are formed. The two most co mmon detection techniques to nano-structures identification are X-ray diffract ion and electron microscopy. In this research, X-ray diffraction (XRD) experiments were carried out on a Rigaku GEIGERFLEX 2037 X-ray diffract meter with Cu (λ=0.154 nm) irrad iation at 40 kV and 30 mA using a Ni filter. Data were recorded in the range fro m 2 to 80 deg in a continuous scanning at 2 degrees per minute and sampling pitch of 0.02 deg. The high resolution scanning electron microscope (HRSEM ) used was a Quanta 200 - FEG - FEI, wh ile the transmission electron microscope (TEM) employed was a Tecnai – G2-20-FEI. As commented by Dresselhaus et al, Raman spectroscopy is also a powerful tool for studying carbon based nanostructures, i.e. CNTs and graphene nanosheets. In this study, the Raman spectroscopy analysis was performed using a micro-Raman NuSpec using green light (wavelength of 510 n m). The mu lti-phase laminated composite mechanical characterizat ion is based on tensile tests following ASTM D 3039 standard. An EMIC DL-10000 universal testing mach ine with 10 KN and a 500N load cells was used to perform the tensile tests at constant displacement of 0.5 mm/ min . Load and displacement were continually measured by the load cell and e xtensometer, respectively. Furthermore, as this research focuses on understanding the CNT inter-lamina effect into laminated composites, the concept of representative volume element (RVE) described by Heinrich et al was employed. Figure 1 is a schemat ic representation of a RVE as described by Gao et al. Note that carbon nanotubes are dispersed into the resin around the carbon fibers. In our case, the mult i-phase composite laminate was composed of two layers of carbon fiber/epo xy with an extra inter-layer of fiber glass fabric where CNTs were grown in situ by thermal CVD. The total average thickness was around 0.145 mm. The other dimensions followed the ASTM D 3039 standard. By applying the RVE concept, it was possible to obtain a d irect relation between the CNTs effects into the composite’s macroscopic behavior. Figure 1. RVE representation from Gao et al 3. Data Analysis As this research deals with multi-scale composite reinforcement, i.e. fro m nano to macro, two different approaches are emp loyed. The first one is related to nano and micro structure analysis based on HSEM, Raman spectroscopy and x-ray diffraction analysis. The second one is based to tensile tests and failure mode analysis. By analyzing the two sets of data, it is possible to correlate the nano/micro structure formed and the multi-phase composite overall behavior. Figures 2A-B shows the Raman spectroscopy, while the x-ray diffraction signatures are shown in Figure 2C. As it can be observed in Figure 2A, for CNTs (the lower curve), three bands can be easily identified. The D band is around 1340 cm-1, wh ile the G band is located around 1580 cm-1 and the G’ band is nearby 2685 cm-1. As described by Mallard et al, these peak values are typical fro m carbon based materials. Furthermore, the narrow and intense D band could be associated to the small nanotube diameter (≈ 20 n m) and the high intensity can be related to CNTs length. Moreover, the narrow G band is related to the CNT’s crystallin ity, wh ich is confirmed by the XRD signature shown in Figure 2C. By analyzing the second curve (fibers + CNTs), it is possible to observe the carbon fibers’ amorphous behavior represented by the smooth curve. However, the carbon nanotubes G band is also observed superposed to the smooth curve. The G band is indicated by the arrow and a region’s zoom is shown on Figure 2B. Finally, the last curve (upper curve on Figure 2A) indicates the fiber-glass amorphous behavior. Five different CNTs interlayers were tested. The amount of CNTs grown in each fiber glass interlayer can be described as 52.50 mg , 64.75 mg, 136.50 mg, 185.25 mg, and 206.30 mg, respectively. These CNTs contents can be translated as 1.18 wt.%, 1.32 wt.%, 2.39 wt.%, 3.28 wt.% and 3.64 wt.% with respect to the composite overall mass. 4 Antonio F. Ávila et al.: M ulti-Phase Carbon Fiber-M WNT/Epoxy Composites (a) Figure 3. Stress-strain curve (b) (c) Figure 2. Fibers and CNT s characterization. (a) Raman spectroscopy; (b) Zoom at Raman peak; (c) CNTs’ XRD signature Figure 3 shows the stress-strain curves for the multi-phase composites. As it can be noticed, as we are dealing with a thin laminate the stresses are “naturally” high. As it can be observed in Fig. 3, as the carbon nanotube concentration increases, two phenomena can be described. The first one is an increase on stiffness at CNT low concentration. This increase on stiffness is represented by the sharp stress-strain slope. The change into stiffness represented by the slope modificat ion can be due to damage initiat ion. As expected for materials with high stiffness, the displacements at failu re were small. As it can be seem in Figs. 4A-C, for co mposites with lo w CNT concentration the failure is mainly around and near the fibers. One possible explanation for such behavior could be the local stress distribution at nanostructures formed near and around the fibers. As discussed by Coleman et al, debonding will occur when either nanotube-matrix interface fails or the matrix fails under the large shear stresses near the interface. By analy zing Figs. 4A-C, it is possible to observe a failu re mode that it is a mix of the two cases. Failures around the fiber/ matrix interface were spotted in addition to matrix failure near the fibers. As the nanotube-matrix interface has a much higher stiffness (based on rule of mixture), a large portion of the load was transferred fro m the fibers to the interface nanotube-matrix. Th is phenomenon was captured by the increase on stiffness (stress-strain slope). After the interface nanotube-matrix failure, the stress-stain curve slope decreased and after some additional loading failure occurred. This “second stage” failure can be described by matrix failure due to crack init iation/propagation. The second phenomenon observed could be described as an increase on peak stresses and displacement at failu re. As explained by Chou et al, these conditions are related to a decrease on stiffness. They even proposed a mention that a possible competing mechanism between the increase on stiffness and crack nucleat ion/propagation due to differences between fiber/ matrix/ CNT stiffness could be the reason for the overall decrease on stiffness. This seems to be the case for the composites with higher CNT concentrations. As it can be International Journal of Composite M aterials 2013, 3(6A): 1-9 5 noticed in Figs. 4D-E cracks spread all over the co mposite area. These cracks, however, have its path blocked by CNTs bridges. These bridges (Fig. 4F-H) are CNTs connecting the two sides of a crack opening. As they (CNTs) are very stiff materials, the energy required for this crack propagation increases. This seems the case when the CNTs content increased from 2.39 wt. % to 3.28 wt. %. In this case, an increase on peak stress from 1350 M Pa to 2300 MPa was observed. Moreover, the CNTs bridging effect was spotted in Figs. 4F-H. The same failure mechanis m on crack propagation was observed on samples with CNT content of 3.64 wt. %. In this case, however, the CNTs bridging mechanis mseems to occur far fro mthe fiber/ matrix interface. This could stimu late a better stress distribution that can lead to an increase on peak stress and displacement at failure. As expected, the increase on CNTs content to 3.64 wt. % led to the highest peak stress (≈ 2800 M Pa). This performance can be attributed to the strong bond between fibers and CNTs as (c) it can be observed in Figs. 4F-H. (d) (a) (b) (e) 6 Antonio F. Ávila et al.: M ulti-Phase Carbon Fiber-M WNT/Epoxy Composites As the textile fibers used in this research had a pla in weave configuration, it was possible to assume a quasi-isotropic condition into the X-Y plane. Furthermore, the overall composite behaviour can be assumed transversely isotropic, as the mechanical properties through the thickness (Z –axis) were uniform and different fro m the ones from the X-Y plane. (f) (a) (g) (b) (h) Figure 4. SEM observations of multi-phase composite ; (a) 1.18 wt.%; (b-c) 1.32 wt.%; (d-e) 2.39 wt.%; (f) 3.28 wt.%; (g-h) 3.64 wt.% (c) International Journal of Composite M aterials 2013, 3(6A): 1-9 7 To understand the failure mechanism a finite element analysis based on RVE described by Gao et al was performed. An interphase between the CNTs and the carbon fiber was also modeled. The interphase properties were based on composite cylinder assemblage model described by Pagano and Tandon. In this model, the interphase thickness was based on measurements from Figure 4G. The carbon fiber diameter was 0.007 mm, while it’s Young’s modulus was assumed to be 360 GPa and the Poisson ratio of 0.10 as described by Sun. Notice that although carbon fibers were transversely isotropic materials as described by Sun and Vaidya, as in this paper is dealing with representative volume element (RVE) through the thickness, carbon fibers can be described as isotropic. This assumption, based on Generalized Cells Model, can only be emp loyed due to the fiber periodicity. A similar approach for (d) modeling carbon composite materials with carbon nanotubes was employed by Liu and Chen. The pure epo xy resin was considered an isotropic material with Young’s modulus of 3.0 GPa and Poisson ratio of 0.35. As mentioned before, the overall composite behavior is considered transversely isotropic. The prescribed d isplacements applied and the stiffness for the 1.18 wt. % and 3.64 wt. % specimens were obtained from the e xperimental data. Figure 5A-F show the shear strain field for 3 conditions, i.e. (i) fiber and pure resin; (ii) fiber, interphase CNT+resin and resin outside the interphase; (iii) fiber and CNT+resin surrounding the fibers. The addition of CNTs led to high shear strains at failu re in p laces with the largest stiffness discontinuity. This large d ifference builds a high strain discontinuity. For the pure resin and carbon fiber this critical location was between the carbon fiber and the resin (Figs. 5 A and D). For the models with an interphase, the critical (e) location was between the interphase and the resin (Figs. 5 B and E). When the CNT resin interphase was used outside the carbon fiber reg ion, again the critical region was around the fiber surface. Due to the large difference on stiffness between the interphase and the pure resin, a large shear strain was obtained. These locations are the ones with the highest probability of failure. 4. Conclusions (f) Figure 5. Shear strain (ϒxy) fields for the following specimens: (a) No CNT s and prescribed displacement for 1.18 wt.% CNT; (b) 1.18 wt.% CNT interphase and pure resin outside; (c) 1.18 wt.% CNT and mix CNT resin at the interphase and outside; (d) No CNT s and prescribed displacement for 3.64 wt.% CNT ; (e) 3.64 wt.% CNT interphase and pure resin outside; (f) 3.64 wt.% CNT and mix CNT resin at the interphase and outside Carbon fibers/CNT mu lti-phased structures were successfully introduced to carbon fibers/epoxy laminated composites. An increase on peak stress close to 85% was witnessed when CNTs interlayer with 3.64 wt. % was placed in carbon fiber/epo xy laminates. The failure mechanis ms are associated to CNTs distribution between and around carbon fibers. These CNTs are also accountable for crack bridging formation and the increase on peak stress. The init ial stiffness is strongly affected by the CNT interlayer, however, changes on stiffness is related to changes on nano/microstructure due to damage. Cracks between fibers were observed in mu lti-phase composites with interlayers with CNTs contents of 1.18 wt. % and 1.32 wt. %. When the 8 Antonio F. Ávila et al.: M ulti-Phase Carbon Fiber-M WNT/Epoxy Composites nanotubes content is increased to 2.39 wt. % and 3.28 wt. %, no cracks are noted between fibers, but cracks were spotted on fibers and inside the CNT/ matrix mix. Finally, when the CNT content reached 3.64 wt. %, the main failure mode was fiber breaking, as a strong bond between fiber/CNTs was observed by SEM. ACKNOWLEDGEMENTS dispersed composites”, Comput. M at. Sci. vol. 28, p. 529-539, 2003.  T.S. Gates, G.M . Odegard, S.J.V. Frankland and C. Clancy, “Computational materials: M ulti-scale modeling and simulation of nanostructured materials”, Compos. Sci. Tech. vol. 65, p. 2416-2434, 2005.  W.K. Liu, E.G. Karpov, S. Zhang and H.S. Park, “An intro-duction to computational nanomechanics and materials”, Appl. M ech. Eng. Vol. 193, p. 1529–1578, 2004. This research was supported in part by the AFOSR under contract FA9550-10-1-0050, the Brazilian Research Council (CNPq ) under grants number 303447/2011-7 and 472583/ 2011-5, and the Minas Gerais State Research Foundation (FAPEMIG) grant TEC-PPM00192-12. The authors are also grateful to the UFMG’s Centre of Microscopy and Microanalysis for the technical support. The authors would like to recognize the technical support provided by the Nanomaterial’s Laboratory fro m the Physics department of Universidade Federal de M inas Gerais for the CNTs in situ growing into the fibers.  R.S. Ruoff and R. Pugno, M echanics of nanostructures, in: Nanomechanics of M aterials and Structures, T.S. Chuang et al. (Eds.) Springer, New York, pp. 199-203, 2006.  C. Li and T.W. Chou, “An introduction to computational nanomechanics and materials”, Int. J. 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