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applied sciences Article Effect of Harsh Environmental Conditions on the Impact Response of Carbon Composites with Filled Matrix by Cork Powder Marco P. Silva 1,* , Paulo Santos 1, João Parente 1, Sara Valvez 1and Paulo N. B. Reis 2 Citation: Silva, M.P.; Santos, P.; Parente, J.; Valvez, S.; Reis, P.N.B. Effect of Harsh Environmental Conditions on the Impact Response of Carbon Composites with Filled Matrix by Cork Powder. Appl. Sci. 2021,11, 7436. https://doi.org/ 10.3390/app11167436 Academic Editor: Valentino Paolo Berardi Received: 15 July 2021 Accepted: 9 August 2021 Published: 12 August 2021 Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. Copyright: © 2021 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https:// creativecommons.org/licenses/by/ 4.0/). 1C-MAST, Department of Electromechanical Engineering, University of Beira Interior, Calçada Fonte do Lameiro, 6201-100 Covilhã, Portugal; paulo.ser[email protected] (P.S.); [email protected] (J.P.); [email protected] (S.V.) 2CEMMPRE, Department of Mechanical Engineering, University of Coimbra, 3030-788 Coimbra, Portugal; [email protected] *Correspondence: mar[email protected] Abstract: Composites are used in a wide range of engineering applications, as a result, exposure to hostile environments is rather common and its mechanical properties degradation is unavoidable. It is necessary to have a complete understanding of the impact of hostile environments on mechanical performance, namely critical solicitations as low velocity impacts. Therefore, this work intends to analyse the low velocity impact response of a carbon fibre/epoxy composite, and a similar architecture with an epoxy matrix filled with cork, after immersion into different solutions: diesel, H 2 SO 4 , HCl, NaOH, distilled water, seawater, and seawater at 60 ◦ C. These solutions significantly affected the impact properties. In this context, the maximum load, maximum displacement, and restored energy behaviour were studied to understand the influence of exposure time. It was possible to conclude that such impact parameters were significantly affected by the solutions, where the exposure time proved to be determinant. The benefits of cork on the perforation threshold were investigated, and this parameter increased when the epoxy matrix was filled with cork. Finally, cork filled epoxy laminates also show less variation in maximum load and recovered energy than carbon/epoxy laminates. Keywords: composite laminates; hostile solutions; experimental tests; low velocity impact 1. Introduction Fibre-reinforced composites have been used in a variety of engineering fields such as aircraft, space, automotive, sport, marine industries, and military applications due to their excellent performance in terms of high specific strength and stiffness, good static and dynamic properties, good corrosion resistance, adjustable properties, competitive cost, and fast manufacture [ 1 – 4 ]. Carbon fibres, for example, have great strength and hardness, as well as excellent temperature resistance, chemical resistance, and low thermal expansion. They are ideal candidates for use in the aerospace/aeronautical, automotive, construction, military, and sports industries due to their advantages [1,3,5–9]. Numerous studies have been conducted to increase interfacial adhesion with the matrix [ 10 – 14 ], as a consequence of the low surface energy and chemically inert surface of some fibres. On the other hand, literature reports that the addition of low concentrations of nanoparticles to the matrix is an excellent solution to improve the mechanical performance of composite laminates without compromising their density, toughness or manufacturing process [ 4 , 15 , 16 ]. Nowadays, for reasons of environmental sustainability, composites incorporating natural reinforcements have gained popularity due to their low density, abundance, abrasiveness during processing, low cost, renewable, and biodegradable properties [ 17 ]. In this context, cork has unique characteristics, and its powder, which is a by-product of agriculture, is a viable option for use in polymeric composites. For example, Appl. Sci. 2021,11, 7436. https://doi.org/10.3390/app11167436 https://www.mdpi.com/journal/applsci
Appl. Sci. 2021,11, 7436 2 of 17 literature reports that, compared to laminates with neat matrices, polymer composites containing cork powder have higher absorbed impact energy and glass transition temperature, promote less damage areas and have the best elastic recovery performance. At the same time, it became clear that cork powder increases the penetration threshold [17–19] . Therefore, high tolerance to damage from impact loads, wear and fire resistance, low thermal conductivity, and excellent damping are important characteristics for the use of cork in composites used in harsh environments [20–23]. The open literature reports several studies on the effect of hostile environments on the mechanical properties of composite materials. For example, the effects of alkaline (NaOH) and acid (HCl) solutions in fibre-reinforced polymer composites were studied by Amaro et al. [ 24 ] and, according to the authors, alkaline solutions proved to be more harmful than acid solutions, resulting in lower flexural strength and modulus. Another study showed that flexural strength is insensitive up to 30 days after immersion in HCl, after which there is a 10% decrease [ 25 ]. Kawada and Srivastava [ 26 ] studied the exposure of a composite laminate to a corrosive environment and observed that sharp cracks begin to develop and spread when the acid weakens the fibres, resulting in very low strength and highly flat fracture with low failure stress. The resins used as matrix in laminated composites, according to Banna et al. [ 27 ], have a considerable influence on the final mechanical performance. When subjected to higher temperatures or for longer periods of time, authors conclude that polyester resin has a lower modulus than bisphenol A epoxy vinyl ester. Due to the importance of the matrix to the composite structural integrity, the epoxy resin’s ability to deal with progressively adverse conditions will determine the composite’s suitability for specific applications [27]. According to the literature, composite laminates are strong in the in-plane loading direction, but very weak in the out-of-plane loading direction [ 28 ]. Impact damage is believed to be the main source of composite delamination in service, which is quite dangerous because it significantly affects the performance of these materials [ 8 , 9 , 29 ] and, simultaneously, is difficult to identify visually [ 30 ]. However, there is a lack of research that incorporates impact loads and harsh environmental conditions, in particular involving composites reinforced with cork. Therefore, the main goal of this work is to investigate the benefit of cork powder on low velocity impact strength in carbon/epoxy composites after immersion into hydrochloric acid (HCl), sodium hydroxide (NaOH), sulphuric acid (H2SO4), diesel, distilled water, and seawater. 2. Material and Experimental Procedure Nine ply laminates of carbon fibre bidirectional plain weave fabric (taffeta weave with 160 g/cm 2 ), all in the same direction, and an Ampreg 22 epoxy resin with an Ampreg 22 hardener standard, both supplied by Gurit, were used to produce composite laminates. Plates with overall dimensions of 330 × 330 × 2.4 ± 0.1 (mm 3 ) were produced by the hand lay-up process. This system was placed inside a vacuum bag and a load of 2.5 kN was applied for 48 h to maintain a constant fibre volume fraction and a uniform laminate thickness. During the first 10 h the bag remained attached to a vacuum pump to eliminate any air bubbles existing in the composite. The post-cure was carried out in an oven at 45 ◦C for 48 h. Using the same manufacturing process, composite laminates with epoxy matrix filled with cork powder were also produced. The bulk density of the cork powder used is about 0.11 g · cm −3 and the particles’ size, in terms of percentile, is d(0.1) = 18.6 µ m, d(0.5) = 78.9 µm and d(0.9) = 208.3 µ m. More details can be found in [ 17 ]. The cork powder was dried in an oven (Heraus, model UT 6060) at about 120 ◦ C during 2 h and dried in a desiccator until use. Epoxy resin and cork powder were mixed at 900 rpm for 2 h and, at same time, subjected to ultrasonic bath sonicator. Finally, the mixture was degassed in a vacuum oven, followed by addition of the hardener with special care to avoid the presence of air bubbles. The filler content was 3 wt.% of the epoxy resin-hardener mixture as reported in [19].
Appl. Sci. 2021,11, 7436 3 of 17 The samples used in this study were cut from these plates to square specimens with 100 mm side, which were completely submerged into different solutions and different immersion times, both summarized in Table 1. All solutions have a concentration of 10% by weight (wt.%), which corresponds to a pH of 13.0 for NaOH and 1.5 for acids. Except for seawater at 60 ◦ C, all the other solutions in which the specimens were immersed are at room temperature. Finally, the samples were washed with clean water and dried at room temperature. Table 1. Different solutions and immersion times used in this study. Solutions Immersion Time (Days) Diesel 15, 30 and 45 Sulphuric acid (H2SO4), pH = 1.5 10, 20 and 30 Hydrochloric acid (HCl), pH = 1.5 10, 20 and 30 Sodium hydroxide (NaOH), pH = 13.0 10, 20 and 30 Distilled water 15, 30, 60 and 90 Seawater at room temperature 15, 30, 60 and 90 Seawater at 60 ◦C 15, 30 and 45 Low-velocity impact tests were performed using a drop weight testing machine IMATEK-IM10. More details of the impact machine can be found in [ 31 ]. An impactor diameter of 20 mm with a mass of 3.005 kg was used. The tests were performed on square section samples of dimensions 75 × 75 mm and the impactor stroke at the centre of the samples obtained by centrally supporting the 100 × 100 mm specimens. Impact energies of 2, 4, 8, 10, 12, 16, 20 and 24 J were used to analyse the impact strength and the effect of cork powder on the impact strength. The effect of hostile solutions on the impact strength was evaluated for the energy of 12 J. For each condition/environment, five specimens were tested, and the results presented in terms of average values. 3. Results The benefits obtained with cork powder were evaluated by impact tests carried out for different impact energies. Figure 1shows typical load and energy versus time curves of control samples and laminates with resin filled with 3% of cork powder tested for an impact energy of 2 J. Figure 1. For an impact energy of 2 J, typical: (a) load versus time curves; (b) energy versus time curves.
Appl. Sci. 2021,11, 7436 4 of 17 Both curves shown in Figure 1represent the typical profile of all tests and are in good agreement with the literature [ 8 , 32 – 34 ]. The oscillations in the load-displacement curves (Figure 1a) are caused by the elastic wave and the vibrations of the samples [ 35 ]. In detail, the load-displacement curves show that the load rises until it reaches a maximum value, and then drops abruptly after reaching its maximum value. A non-perforating impact was identified because the impact energy was insufficient to completely penetrate the sample. In fact, the impactor stuck into the sample and always rebounded. Therefore, the beginning of the plateau in the energy-time curves (Figure 1b) corresponds to the loss of contact between the striker and the specimen [ 19 , 36 ], so this energy is the one absorbed by the specimen. Finally, in both figures it is possible to observe the influence of the resin filled with cork powder on the impact behaviour of the composite. For example, Figure 1a shows an increase in displacement with the presence of cork powder, while Figure 1b shows less absorbed energy and longer contact time. In detail, the effect of the cork powder is shown in Figure 2in terms of maximum load, maximum displacement, and restored energy for all impact energies. Symbols represent average values. This figure shows how these parameters evolve with impact energy, while Table 2summarizes all average values and their respective statistical variations in terms of standard deviation. Figure 2. For different impact energies: (a) maximum load, (b) maximum displacement, (c) restored energy. Table 2. Summary of all parameters obtained from the impact tests and respective standard deviation. Impact Energy (J) Maximum Load (kN) Maximum Load (mm) Contact Time (ms) Restored Energy (%) Average Std Dev Average Std Dev Average Std Dev Average Std Dev Carbon Laminates 2 1.56 0.21 3.0 0.3 7.24 0.29 60.8 2.1 4 2.29 0.18 3.3 0.5 7.07 0.46 48.5 2.3 8 2.67 0.20 5.4 0.3 7.73 0.35 28.6 1.4 10 2.82 0.22 5.7 0.6 7.93 0.36 24.3 1.9 12 3.16 0.23 6.6 0.3 8.04 0.31 21.4 1.2 16 3.12 0.19 9.0 0.3 8.55 0.35 17.8 1.6 20 2.93 0.17 10.6 0.7 9.77 0.64 15.1 1.3 24 3.21 0.24 11.9 0.4 10.49 0.67 13.9 1.1 Carbon Laminates with Cork 2 1.56 0.21 3.0 0.2 7.55 0.32 64.2 3.2 4 1.89 0.23 4.5 0.2 8.51 0.29 31.0 3.9 8 2.22 0.19 6.6 0.3 9.31 0.37 20.7 3.5 10 2.27 0.22 7.8 0.3 10.38 0.24 19.1 2.7 12 2.44 0.19 8.8 0.5 10.17 0.43 16.6 2.8 16 2.27 0.17 10.8 0.6 10.95 0.39 14.4 3.6 20 2.44 0.19 12.8 0.2 11.89 0.31 12.2 3.1 24 2.41 0.24 17.2 0.3 15.68 0.37 10.3 3.0
Appl. Sci. 2021,11, 7436 5 of 17 Regarding the maximum load (Figure 2a and Table 2), and regardless of the impact energy, it is possible to observe higher values for composites with neat resin than for composites with resin filled with cork powder. On the other hand, for both laminates, higher impact energies promoted higher maximum loads up to 12 J, after which the maximum impact load seems to remain constant. While the maximum load increased around 56.4% between 2 J and 12 J for composites with cork powder, this value was about 102.6% (around twice higher) for composite laminates with neat resin. In fact, literature reports that the maximum load increases with increasing impact energy [ 16 , 19 , 31 , 37 ], and this trend can be observed in this study up to 12 J for both laminates. According to Gustin et al. [ 38 ] the differences observed in the maximum loads are a consequence of the different failure modes introduced in the laminate and, in this context, it is possible to note that for impact energies higher than 12 J the severity of the damage is so significant that the effect is not visible in terms of maximum load. Similar behaviour was observed by Reis et al. [ 37 ], as well as the non-linearity also observed in Figure 2a and that according to Hosur et al. [ 39 ], the maximum load should increase almost linearly with the increase of the impact energy. This parameter is controlled by the impact energy and reflects the maximum load that the composite laminate can tolerate before severe damage occurs [37]. The benefits obtained with the cork powder and respective influence of impact energy on the displacement is shown in Figure 2b and Table 2. Independently of the impact energy, the average results show that laminates with cork powder have the highest displacements. For the studied energy range, for example, displacements increased around 298% and 476% for laminates with neat resin and laminates with epoxy filled by cork powder, respectively. Consequently, as shown in Table 2, the contact time is higher for laminates with cork powder. Under compressive loading during the impact, when cork deforms, the cell walls bend and buckle and can undergo large strain deformation. Therefore, this explains the higher displacements and the lowest maximum loads observed in composites that incorporate cork powder. On the other hand, when cell walls bend and buckle, they can absorb large amounts of energy with high viscoelastic return. This means that, after an impact, the capacity of the cork to continue to absorb energy is almost unchanged due to its elastic deformation [ 40 , 41 ]. The benefits reported are expressed in Figure 2c, where the lower restored energy to laminates with cork powder is a consequence of the higher energy absorption capacity. For carbon/epoxy laminates, it is possible to observe a decrease in the elastic recovery around 53%, between 2 and 8 J, but this value drops drastically to 77% between 2 and 24 J. When the cork powder is added to the resin, the behaviour is similar, but in this case with values around 68% and 84%, respectively. From Figure 2c it is possible to observe that the elastic energy is never equal to zero, which means that the absorbed energy is never equal to the impact energy. Therefore, the penetration threshold was not reached because the excess energy is used to rebound the impactor [ 42 , 43 ]. In this context, if the elastic energy versus impact energy is plotted and the data fitted by polynomial equations, the penetration thresholds can be determined [19,43] . Figure 3shows the methodology used to obtain the penetration threshold for all laminates, and values of 34.5 J and 37.6 J were found for control laminates and cork-filled laminates, respectively.
Appl. Sci. 2021,11, 7436 6 of 17 Figure 3. Penetration threshold for laminates with neat resin and matrix filled with cork powder. The effect of hostile solutions on the impact strength was evaluated for the energy of 12 J. For each condition, five specimens were used, and the results presented in terms of average values. The influence of the exposure time on the maximum load, maximum displacement and restored energy were analysed and the results shown in Figures 4–6 , respectively. In these representations, each result was dimensionless/divided by the respective value obtained with the control specimens (without immersion in any solution). The average results and respective standard deviations will be summarized in form of tables. Therefore. the benefit achieved with the introduction of cork powder in the resin is notorious, which promotes an increase in the penetration threshold about 9% higher than that of the control samples. This is a consequence of the significant amount of energy absorbed by cork associated with the high viscoelastic return [ 40 , 41 ]. A similar benefit was obtained by Reis et al. [ 19 ] for Kevlar laminates, when the epoxy matrix was filled with cork powder. In this case, the penetration threshold was around 30.9 J for the control samples, while for laminates with cork powder this value was about 34.8 J, promoting, in this case, a benefit around 12.6%. However, the greatest benefit observed by the authors in relation to that obtained in the present study is due to Kevlar fibres being more tolerant to damage than carbon fibres. Figure 4. Cont.
Appl. Sci. 2021,11, 7436 7 of 17 Figure 4. Influence of solution type and exposure time on the maximum impact load after immersion into: ( a ) diesel; (b) H2SO4, (c) HCl, (d) NaOH, (e) distilled water and seawater; (f) seawater at room temperature and at 60 ◦C. Figure 5. Cont.
Appl. Sci. 2021,11, 7436 8 of 17 Figure 5. Influence of solution on the displacement after immersion into: ( a ) diesel; ( b ) H 2 SO 4 , ( c ) HCl, ( d ) NaOH, (e) distilled water and seawater; (f) seawater at room temperature and at 60 ◦C. Figure 6. Cont.
Appl. Sci. 2021,11, 7436 9 of 17 Figure 6. Influence of solution type and exposure time on the restored energy after immersion into: ( a ) diesel; ( b ) H 2 SO 4 , (c) HCl, (d) NaOH, (e) distilled water and seawater; (f) seawater at room temperature and at 60 ◦C. From Figure 4, it is possible to observe that, for all harsh environments, laminates with neat resin are much more sensitive to exposure to such solutions than carbon laminates with matrix filled with cork. It is also noticed that the maximum load decreases when the samples are exposed to different environments and this tendency is highly dependent on the exposure time. This evidence agrees with the studies reported in the open literature [24,44,45] . Although the values are always lower than those observed in specimens not exposed to hostile environments, Table 3also shows that the behaviour of laminates with matrix filled with cork powder always revealed a maximum impact load lower than that observed in control laminates. For example, comparing the maximum impact load obtained for 30 days of immersion into different solutions and the value obtained for the respective laminates without any degradation (no immersion in such solutions), it is possible to assess the severity of harsh environments in this parameter (maximum impact load). This effect is summarized in Table 4, in which the decrease observed for the different solutions is presented in percentage terms.
Appl. Sci. 2021,11, 7436 16 of 17 16. Iqbal, K.; Khan, S.U.; Munir, A.; Kim, J.K. Impact damage resistance of CFRP with nanoclay-filled epoxy matrix. Compos. Sci. Technol. 2009,69, 1949–1957. [CrossRef] 17. Reis, P.N.B.; Ferreira, J.A.M.; Silva, P.A.A. Mechanical behaviour of composites filled by agro-waste materials. Fibers Polym. 2011 , 12, 240–246. [CrossRef] 18. Reis, P.N.B.; Ferreira, J.A.M.; Costa, J.D.M.; Santos, M.J. Fatigue performance of Kevlar/epoxy composites with filled matrix by cork powder. Fibers Polym. 2012,13, 1292–1299. [CrossRef] 19. Reis, P.N.B.; Ferreira, J.A.M.; Santos, P.; Richardson, M.O.W.; Santos, J.B. Impact response of Kevlar composites with filled epoxy matrix. Compos. Struct. 2012,94, 3520–3528. [CrossRef] 20. Rosa, M.; Fortes, M. Deformation and fracture of cork in tension. J. Mater. Sci. 1991,26, 341–348. [CrossRef] 21. Rosa, M.E.; Fortes, M. Water absorption by cork. Wood Fiber Sci. 1993,25, 339–348. 22. Mano, J.F. The viscoelastic properties of cork. J. Mater. Sci. 2002,37, 257–263. [CrossRef] 23. Silva, S.P.; Sabino, M.A.; Fernandes, E.M.; Correlo, V.M.; Boesel, L.F.; Reis, R.L. Cork: Properties, capabilities and applications. Int. Mater. Rev. 2005,50, 345–365. [CrossRef] 24. Amaro, A.M.; Reis, P.N.B.; Neto, M.A.; Louro, C. Effects of alkaline and acid solutions on glass/epoxy composites. Polym. Degrad. Stab. 2013,98, 853–862. [CrossRef] 25. Mahmoud, M.K.; Tantawi, S.H. Effect of strong acids on mechanical properties of glass/polyester GRP pipe at normal and high temperatures. Polym. Plast. Technol. Eng. 2003,42, 677–688. [CrossRef] 26. Kawada, H.; Srivastava, V.K. The effect of an acidic stress environment on the stress-intensity factor for GRP laminates. Compos. Sci. Technol. 2001,61, 1109–1114. [CrossRef] 27. Banna, M.H.; Shirokoff, J.; Molgaard, J. Effects of two aqueous acidic solutions on polyester and bisphenol A epoxy vinyl ester resins. Mater. Sci. Eng. A 2011,528, 2137–2142. [CrossRef] 28. Richardson, M.; Wisheart, M. Review of low-velocity impact properties of composite materials. Compos. Part A Appl. Sci. Manuf. 1996,27, 1123–1131. [CrossRef] 29. Amaro, A.M.; Reis, P.N.; De Moura, M.F. Residual strength after low velocity impact in carbon-epoxy laminates. In Materials Science Forum; Trans Tech Publ.: Stafa-Zurich, Switzerland, 2006; Volume 514, pp. 624–628. 30. Amaro, A.M.; Reis, P.N.B.; De Moura, M.F.S.F.; Santos, J.B. Damage detection on laminated composite materials using several NDT techniques. Insight-Non-Destr. Test. Cond. Monit. 2012,54, 14–20. [CrossRef] 31. Amaro, A.M.; Reis, P.N.B.; Magalhães, A.G.; De Moura, M.F.S.F. The influence of the boundary conditions on low-velocity impact composite damage. Strain 2011,47, e220–e226. [CrossRef] 32. Hosur, M.; Adbullah, M.; Jeelani, S. Studies on the low-velocity impact response of woven hybrid composites. Compos. Struct. 2005,67, 253–262. [CrossRef] 33. Amaro, A.M.; Reis, P.N.B.; De Moura, M.F.S.F.; Neto, M.A. Influence of multi-impacts on GFRP composites laminates. Compos. Part B Eng. 2013,52, 93–99. [CrossRef] 34. Reis, P.N.B.; Ferreira, J.A.M.; Zhang, Z.Y.; Benameur, T.; Richardson, M.O.W. Impact response of Kevlar composites with nanoclay enhanced epoxy matrix. Compos. Part B Eng. 2013,46, 7–14. [CrossRef] 35. Schoeppner, G.A.; Abrate, S. Delamination threshold loads for low velocity impact on composite laminates. Compos. Part A Appl. Sci. Manuf. 2000,31, 903–915. [CrossRef] 36. Gómez-del Rıo, T.; Zaera, R.; Barbero, E.; Navarro, C. Damage in CFRPs due to low velocity impact at low temperature. Compos. Part B Eng. 2005,36, 41–50. [CrossRef] 37. Reis, P.N.B.; Santos, P.; Ferreira, J.A.M.; Richardson, M.O.W. Impact response of sandwich composites with nano-enhanced epoxy resin. J. Reinf. Plast. Compos. 2013,32, 898–906. [CrossRef] 38. Gustin, J.; Joneson, A.; Mahinfalah, M.; Stone, J. Low velocity impact of combination Kevlar/carbon fiber sandwich composites. Compos. Struct. 2005,69, 396–406. [CrossRef] 39. Hosur, M.V.; Chowdhury, F.; Jeelani, S. Low-Velocity Impact Response and Ultrasonic NDE of Woven Carbon/Epoxy—Nanoclay Nanocomposites. J. Compos. Mater. 2007,41, 2195–2212. [CrossRef] 40. Fernandes, F.A.O.; Pascoal, R.J.S.; Alves de Sousa, R.J. Modelling impact response of agglomerated cork. Mater. Des. 2014 ,58, 499–507. [CrossRef] 41. Oliveira, V.; Rosa, M.E.; Pereira, E. Variability of the compression properties of cork. Wood Sci. Technol. 2014 ,48, 937–948. [CrossRef] 42. Shim, V.P.W.; Tan, V.B.C.; Tay, T.E. Modelling deformation and damage characteristics of woven fabric under small projectile impact. Int. J. Impact Eng. 1995,16, 585–605. [CrossRef] 43. Akta¸s, M.; Atas, C.; ˙ Içten, B.M.; Karakuzu, R. An experimental investigation of the impact response of composite laminates. Compos. Struct. 2009,87, 307–313. [CrossRef] 44. Amaro, A.M.; Reis, P.N.B.; Neto, M.A.; Louro, C. Effect of different acid solutions on glass/epoxy composites. J. Reinf. Plast. Compos. 2013,32, 1018–1029. [CrossRef] 45. Mortas, N.; Er, O.; Reis, P.N.B.; Ferreira, J.A.M. Effect of corrosive solutions on composites laminates subjected to low velocity impact loading. Compos. Struct. 2014,108, 205–211. [CrossRef] 46. Arun, K.V.; Basavarajappa, S.; Sherigara, B.S. Damage characterisation of glass/textile fabric polymer hybrid composites in sea water environment. Mater. Des. 2010,31, 930–939. [CrossRef]
Appl. Sci. 2021,11, 7436 17 of 17 47. Stamenovi´c, M.; Puti´c, S.; Rakin, M.; Medjo, B.; ˇ Cikara, D. Effect of alkaline and acidic solutions on the tensile properties of glass–polyester pipes. Mater. Des. 2011,32, 2456–2461. [CrossRef] 48. Ray, B.C. Temperature effect during humid ageing on interfaces of glass and carbon fibers reinforced epoxy composites. J. Colloid Interface Sci. 2006,298, 111–117. [CrossRef] 49. Abdel-Magid, B.; Ziaee, S.; Gass, K.; Schneider, M. The combined effects of load, moisture and temperature on the properties of E-glass/epoxy composites. Compos. Struct. 2005,71, 320–326. [CrossRef] 50. Pavan, A.; Dayananda, P.; Vijaya, K.M.; Hegde, S.; Hosagade, P.N. Influence of seawater absorption on vibrational and tensile characteristics of quasi-isotropic glass/epoxy composites. J. Mater. Res. Technol. 2019,8, 1427–1433. [CrossRef] 51. Gargano, A.; Pingkarawat, K.; Pickerd, V.; Delaney, T.; Das, R.; Mouritz, A.P. Effect of seawater immersion on the explosive blast response of a carbon fibre-polymer laminate. Compos. Part A Appl. Sci. Manuf. 2018,109, 382–391. [CrossRef] 52. Tual, N.; Carrere, N.; Davies, P.; Bonnemains, T.; Lolive, E. Characterization of sea water ageing effects on mechanical properties of carbon/epoxy composites for tidal turbine blades. Compos. Part A Appl. Sci. Manuf. 2015,78, 380–389. [CrossRef] 53. Boisseau, A.; Peyrac, C. Long term durability of composites in marine environment: Comparative study of fatigue behavior. Procedia Eng. 2015,133, 535–544. [CrossRef] 54. Kafodya, I.; Xian, G.; Li, H. Durability study of pultruded CFRP plates immersed in water and seawater under sustained bending: Water uptake and effects on the mechanical properties. Compos. Part B Eng. 2015,70, 138–148. [CrossRef] 55. Jesthi, D.K.; Nayak, R.K. Improvement of mechanical properties of hybrid composites through interply rearrangement of glass and carbon woven fabrics for marine application. Compos. Part B Eng. 2019,168, 467–475. [CrossRef] 56. Hu, Y.; Li, X.; Lang, A.W.; Zhang, Y.; Nutt, S.R. Water immersion aging of polydicyclopentadiene resin and glass fiber composites. Polym. Degrad. Stab. 2016,124, 35–42. [CrossRef] 57. Gil, L. Cork Composites: A Review. Materials 2009,2, 776–789. [CrossRef] 58. Carvalho, R.; Fernandes, M.; Fangueiro, R. The influence of cork on the thermal insulation properties of home textiles. Procedia Eng. 2017,200, 252–259. [CrossRef] 59. Amaro, A.M.; Reis, P.N.B.; De Moura, M.F.S.F. Delamination Effect on Bending Behaviour in Carbon–Epoxy Composites. Strain 2011,47, 203–208. [CrossRef] 60. Amaro, A.M.; Reis, P.N.B.; De Moura, M.; Santos, J.B. Influence of the specimen thickness on low velocity impact behavior of composites. J. Polym. Eng. 2012,32, 53–58. [CrossRef] 61. David-West, O.S.; Nash, D.H.; Banks, W.M. An experimental study of damage accumulation in balanced CFRP laminates due to repeated impact. Compos. Struct. 2008,83, 247–258. [CrossRef]