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Thermomechanical Properties of Carbon Fabric Reinforced Epoxy Laminates with h-BN and MoS2 Fillers

Abstract

This work endeavors to investigate thermomechanical performance of carbon fabric reinforced epoxy composite (CEC) with fillers – hexagonal boron nitride (h-BN) and molybdenum disulfide (MoS2). The filler of 2, 4, 6, and 8 Wt.% was dispersed precisely in the epoxy resin through magnetic stirring and ultrasonication, prepared the filler loaded CEC using vacuum bag technique and studied the composite behavior at an elevated temperature by dynamic mechanical analysis. The 6 Wt.% MoS2-CEC showed 70% enhancement of storage modulus since the filler in the epoxy networks increased the composite stiffness. The increase in G-band intensity of Raman spectra in the filler loaded composites confirmed the improved matrix-fiber stress transfer. The 4 Wt.% BN-CEC revealed the highest glass-transition temperature 92°C. The thermogravimetric analysis of the composite exhibited a two-step thermal decomposition: epoxy matrix (nearby 260°C) and carbon fibers (beyond 420°C). The 4 Wt.% MoS2-CEC showed the maximum degree of crosslinking, twice the neat CEC, the MoS2 restrained the mobility of the epoxy chains and decreased the thermal decomposition. Both the filler loaded composites have comparable thermal stability and are significantly improved than the neat CEC. Thus, the composite containing solid lubricant filler up to 6 Wt.% shall be used for high-temperature applications.

Keywords:
Boron nitride; Molybdenum disulfide; Glass-transition temperature; Storage modulus; Raman spectroscopy

1. Introduction

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The phase transition from glassy to rubbery occurs in the polymer matrix at a temperature of glass transition (Tg)1414 Buragohain MK. Composite structures: design, mechanics, analysis, manufacturing and testing. Boca Raton: CRC Press; 2017.. It is also an indicator of the status of curing of the polymer matrix1515 Startsev OV, Vapirov YM, Lebedev MP, Kychkin AK. Comparison of glass-transition temperatures for epoxy polymers obtained by methods of thermal analysis. Mech Compos Mater. 2020;56(2):227-40. http://dx.doi.org/10.1007/s11029-020-09875-5.
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. The polymer composites subjected to a temperature beyond Tg remarkably reduced their strength, stiffness, fracture toughness. Further, the polymer composite started burning when the temperature was increased, it became char, and disintegration took place. Hence, the polymer composite should be operated at a temperature far below the Tg.

The FRP composite in many circumstances is subjected to dynamic loading, wear, and excessive heat. In such cases the thermal stability and thermomechanical properties are essential1616 Adams D. Glass transition temperature testing of composites. Composites World; 2018.. In this regard, several researchers paid attention to improve the thermal stability, storage modulus (E′), Tg, and toughness of the epoxy matrix by incorporating the fillers. The commonly used fillers are alumina (Al2O3)1717 Nayak RK, Mahato KK, Routara BC, Ray BC. Evaluation of mechanical properties of Al2O3 and TiO2 nano filled enhanced glass fiber reinforced polymer composites. J Appl Polym Sci. 2016;133(47):44274. http://dx.doi.org/10.1002/app.44274.
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, boron carbide (B4C)1818 Muralidhara B, Babu SPK, Suresha B. Studies on dynamic mechanical and thermal properties of boron arbide filled carbon fiber/epoxy composites. Mater Today Proc. 2021;46(Pt 19):9145-9. http://dx.doi.org/10.1016/j.matpr.2019.12.204.
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, silicon dioxide (SiO2)1919 Divya GS, Suresha B, Somashekar HM, Jamadar IM. Dynamic mechanical analysis and optimization of hybrid carbon-epoxy composites wear using taguchi method. Tribol Ind. 2020;43(2):298-309., nanoclay2020 Chowdhury FH, Hosur MV, Jeelani S. Investigations on the thermal and flexural properties of plain weave carbon/epoxy-nanoclay composites by hand-layup technique. J Mater Sci. 2007;42(8):2690-700. http://dx.doi.org/10.1007/s10853-006-1370-3.
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,2121 Zhou Y, Hosur M, Jeelani S, Mallick PK. Fabrication and characterization of carbon fiber reinforced clay/epoxy composite. J Mater Sci. 2012;47(12):5002-12. http://dx.doi.org/10.1007/s10853-012-6376-4.
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, graphene2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
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23 Hossain MK, Chowdhury MMR, Bolden NW. Evaluation of thermo-mechanical properties of carbon/epoxy amino-functionalized graphene nanoplatelet composite. Glob J Eng Sci. 2020;4(4):1-10.
-2424 Cai L, Al Ostaz A, Li X, Drzal LT, Rook BP, Cheng AHD, et al. Processing and mechanical properties investigation of epoxy-impregnated graphene paper. J Nanomech Micromech. 2016;6(3):04016005. http://dx.doi.org/10.1061/(ASCE)NM.2153-5477.0000108.
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, boron nitride (BN)2525 Patki AM, Goyal RK. Investigation of non-isothermal crystallization, dynamic mechanical and dielectric properties of poly(ether-ketone) matrix composites. Polym Technol Mater. 2021;60(1):70-83. http://dx.doi.org/10.1080/25740881.2020.1786583.
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,2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
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, molybdenum disulfide (MoS2)2727 Madeshwaran SR, Jayaganthan R, Velmurugan R, Gupta NK, Manzhirov AV. Mechanical and thermal properties of MoS2 reinforced epoxy nanocomposites. J Phys Conf Ser. 2018;991:12054. http://dx.doi.org/10.1088/1742-6596/991/1/012054.
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,2828 Zhao M, Liu L, Zhang B, Sun M, Zhang X, Zhang X, et al. Epoxy composites with functionalized molybdenum disulfide nanoplatelet additives. RSC Advances. 2018;8(61):35170-8. http://dx.doi.org/10.1039/C8RA07448H.
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. The thermomechanical properties improvement depends on the type, size, shape, and quality of the filler dispersion. The high filler concentration in polymer matrix creates agglomerations, voids, and poor adhesion. These aspects reduce the structural integrity and in some cases the functional properties of the resulting composites2929 Podsiadlo P, Kaushik AK, Arruda EM, Waas AM, Shim BS, Xu J, et al. Ultrastrong and stiff layered polymer nanocomposites. Science. 2007;318(5847):80-3. http://dx.doi.org/10.1126/science.1143176.
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.

Nayak et al.1717 Nayak RK, Mahato KK, Routara BC, Ray BC. Evaluation of mechanical properties of Al2O3 and TiO2 nano filled enhanced glass fiber reinforced polymer composites. J Appl Polym Sci. 2016;133(47):44274. http://dx.doi.org/10.1002/app.44274.
http://dx.doi.org/10.1002/app.44274...
noticed a decrease in dynamic modulus due to the addition of hybrid metal oxide nanofillers such as Al2O3 and titanium dioxide (TiO2) in the glass fiber reinforced epoxy composite. This was due to the Al2O3 hindrance for the movement of the epoxy molecules and the agglomeration of fillers in addition to the decreased crosslink between polymer and particles. Also, the authors mentioned that the filler concentration of 0.1, 0.3, and 0.7 Wt.% caused a minor change in Tg and thermal stability. It is reported in the literature that the addition of B4C in the carbon fabric reinforced epoxy composite (CEC) improved its E′, loss modulus (E′′), and damping factor1818 Muralidhara B, Babu SPK, Suresha B. Studies on dynamic mechanical and thermal properties of boron arbide filled carbon fiber/epoxy composites. Mater Today Proc. 2021;46(Pt 19):9145-9. http://dx.doi.org/10.1016/j.matpr.2019.12.204.
http://dx.doi.org/10.1016/j.matpr.2019.1...
. The silicon carbide (SiC) also improved E′ and E′′ of the CEC in addition to the improvement of Tg. However, the SiC reduced the damping factor of the CEC3030 Kumaresan K, Chandramohan G, Senthilkumar M, Suresha B. Dynamic mechanical analysis and three-body wear of carbon–epoxy composite filled with SiC particles. J Reinf Plast Compos. 2012;31(21):1435-48. http://dx.doi.org/10.1177/0731684412459250.
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. Similar kind of effect was observed when the nano SiO2 was added to the CEC1919 Divya GS, Suresha B, Somashekar HM, Jamadar IM. Dynamic mechanical analysis and optimization of hybrid carbon-epoxy composites wear using taguchi method. Tribol Ind. 2020;43(2):298-309..

Chowdhury et al.2020 Chowdhury FH, Hosur MV, Jeelani S. Investigations on the thermal and flexural properties of plain weave carbon/epoxy-nanoclay composites by hand-layup technique. J Mater Sci. 2007;42(8):2690-700. http://dx.doi.org/10.1007/s10853-006-1370-3.
http://dx.doi.org/10.1007/s10853-006-137...
reported that the addition of montmorillonite nanoclay did not have much effect on the Tg but a positive effect on the E′ and E′′ of the CEC. Similar observation was noticed by Zhou et al.2121 Zhou Y, Hosur M, Jeelani S, Mallick PK. Fabrication and characterization of carbon fiber reinforced clay/epoxy composite. J Mater Sci. 2012;47(12):5002-12. http://dx.doi.org/10.1007/s10853-012-6376-4.
http://dx.doi.org/10.1007/s10853-012-637...
. Muralidhara et al.2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
http://dx.doi.org/10.1007/s40033-020-002...
reported that the addition of graphene platelet (GP) in the CEC showed improvement in the E′ and damping capacity. However, they stated that the GP did not favor in improving the Tg of the composite. Adak et al.3131 Adak NC, Chhetri S, Kim NH, Murmu NC, Samanta P, Kuila T. Static and dynamic mechanical properties of graphene oxide-incorporated woven carbon fiber/epoxy composite. J Mater Eng Perform. 2018;27(3):1138-47. http://dx.doi.org/10.1007/s11665-018-3201-5.
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reported that the wrinkled graphene oxide (GO) sheet enhanced the E′, E′′, and damping. This was attributed to the mechanical interlocking of GO sheet with the epoxy in the composites. Hossain et al.2323 Hossain MK, Chowdhury MMR, Bolden NW. Evaluation of thermo-mechanical properties of carbon/epoxy amino-functionalized graphene nanoplatelet composite. Glob J Eng Sci. 2020;4(4):1-10. showed that the addition of amine-functionalized graphene nanoplatelet (f-GNP) enhanced the E′, E′′, crosslink density, and Tg of the CEC. Wan et al.3232 Wan YJ, Gong LX, Tang LC, Wu LB, Jiang JX. Mechanical properties of epoxy composites filled with silane-functionalized graphene oxide. Compos, Part A Appl Sci Manuf. 2014;64:79-89. http://dx.doi.org/10.1016/j.compositesa.2014.04.023.
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reported that the silane functionalized graphene oxide (f-GO) improved the E′ of epoxy due to reduced mobility of the epoxy matrix in the filler vicinity. The covalent interactions between the f-GO and epoxy chains improved the dynamic property of epoxy composite. Tareq et al.3333 Tareq MS, Zainuddin S, Woodside E, Syed F. Investigation of the flexural and thermomechanical properties of nanoclay/graphene reinforced carbon fiber epoxy composites. J Mater Res. 2019;34(21):3678-87. http://dx.doi.org/10.1557/jmr.2019.302.
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reported that the nanoclay increased the E′ of the CEC. The amino group functionalized graphene improved the E′′ and toughness of the CEC. However, the hybrid nanoclay-graphene improved the Tg of the CEC slightly. Loos et al.3434 Loos MR, Coelho LAF, Pezzin SH, Amico SC. Effect of carbon nanotubes addition on the mechanical and thermal properties of epoxy matrices. Mater Res. 2008;11(3):347-52. http://dx.doi.org/10.1590/S1516-14392008000300019.
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demonstrated that randomly oriented single-wall carbon nanotubes (SWCNTs) of 0.25 Wt.% reinforced epoxy resin improved the E′ by 16% due to the rigid and enormous surface area of SWCNTs causing better interactions with the epoxy but it slightly reduced the Tg.

Cai et al.2424 Cai L, Al Ostaz A, Li X, Drzal LT, Rook BP, Cheng AHD, et al. Processing and mechanical properties investigation of epoxy-impregnated graphene paper. J Nanomech Micromech. 2016;6(3):04016005. http://dx.doi.org/10.1061/(ASCE)NM.2153-5477.0000108.
http://dx.doi.org/10.1061/(ASCE)NM.2153-...
developed the composites of graphene porous paper reinforced epoxy resin of a single layer and a 15-layer. They found the E′ of the 15-layer graphene composite was 170% higher due to a higher stiffening effect compared to the neat epoxy and single layer graphene composite. Bera et al.3535 Bera T, Acharya SK, Mishra P. Synthesis, mechanical and thermal properties of carbon black/epoxy composites. Int J Eng Sci Technol. 2018;10(4):12. http://dx.doi.org/10.4314/ijest.v10i4.2.
http://dx.doi.org/10.4314/ijest.v10i4.2...
reported that the carbon black (CB) filler in the epoxy increased its Tg from 68 to 90°C. This was attributed to the consumption of unreacted monomers on the surface of the CB.

Patki and Goyal2525 Patki AM, Goyal RK. Investigation of non-isothermal crystallization, dynamic mechanical and dielectric properties of poly(ether-ketone) matrix composites. Polym Technol Mater. 2021;60(1):70-83. http://dx.doi.org/10.1080/25740881.2020.1786583.
http://dx.doi.org/10.1080/25740881.2020....
noticed that the addition of 30 Wt.% hexagonal boron nitride (h-BN) in polyether-ketone (PEK) remarkably improved the E′, E′′ of the h-BN/PEK composite. However, there was not much change in the Tg. Joy et al.2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
http://dx.doi.org/10.1039/C9NJ05834F...
reported the addition of the filler h-BN improved stiffness and stress transferability of the composite. They found that the epoxy reinforced with 1 Wt.% h-BN improved the E′ up to 11.8% compared to the neat epoxy. They also mentioned that the 0.25 Wt.% h-BN improved the Tg by 10°C. However, the h-BN reinforced epoxy lowered the tan δ peak height, which confirmed a lesser amount of mobile polymer chains. Madeshwaran et al.2727 Madeshwaran SR, Jayaganthan R, Velmurugan R, Gupta NK, Manzhirov AV. Mechanical and thermal properties of MoS2 reinforced epoxy nanocomposites. J Phys Conf Ser. 2018;991:12054. http://dx.doi.org/10.1088/1742-6596/991/1/012054.
http://dx.doi.org/10.1088/1742-6596/991/...
reported a maximum Tg of 73°C for 0.1 Wt.% exfoliated MoS2 reinforced epoxy composite. This was attributed to the restriction for epoxy chain mobility due to the presence of MoS2. Zhao et al.2828 Zhao M, Liu L, Zhang B, Sun M, Zhang X, Zhang X, et al. Epoxy composites with functionalized molybdenum disulfide nanoplatelet additives. RSC Advances. 2018;8(61):35170-8. http://dx.doi.org/10.1039/C8RA07448H.
http://dx.doi.org/10.1039/C8RA07448H...
reported an increment in the Tg by 11°C and decrement in the E′ by 105 MPa for 0.7% silane functionalized MoS2reinforced epoxy resin composite.

The h-BN has good thermal shock resistance, chemical stability, wear, and oxidation resistance3636 Xue Y, Jin X, Fan Y, Tian R, Xu X, Li J, et al. Large-scale synthesis of hexagonal boron nitride nanosheets and their improvement in thermal properties of epoxy composites. Polym Compos. 2014;35(9):1707-15. http://dx.doi.org/10.1002/pc.22824.
http://dx.doi.org/10.1002/pc.22824...

37 Ayyanar S, Gnanavelbabu A, Rajkumar K, Loganathan P. Studies on high temperature wear and friction behaviour of AA6061/B4C/hBN hybrid composites. Met Mater Int. 2021;27:3040-57. http://dx.doi.org/10.1007/s12540-020-00710-z.
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38 Weng Q, Wang X, Wang X, Bando Y, Golberg D. Functionalized hexagonal boron nitride nanomaterials: emerging properties and applications. Chem Soc Rev. 2016;45(14):3989-4012. http://dx.doi.org/10.1039/C5CS00869G.
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-3939 Jia D, Zhou L, Yang Z, Duan X, Zhou Y. Effect of preforming process and starting fused SiO2 particle size on microstructure and mechanical properties of pressurelessly sintered BNp/SiO2 ceramic composites. J Am Ceram Soc. 2011;94(10):3552-60. http://dx.doi.org/10.1111/j.1551-2916.2011.04540.x.
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. The thermal conducting and electrically insulating h-BN finds its importance in heat-dissipating nanoelectronics components4040 Rathinasabapathy S, Santhosh MS, Asokan M. Significance of boron nitride in composites and its applications. In: Aydin M, editor. Recent advances in boron-containing materials. Rijeka: IntechOpen; 2020. http://dx.doi.org/10.5772/intechopen.81557
http://dx.doi.org/10.5772/intechopen.815...
. The important properties of the MoS2 are lubricious, thermal stability, chemical inertness4141 Li X, Zhu H. Two-dimensional MoS2: properties, preparation, and applications. J Mater. 2015;1(1):33-44.. They retain lubricative properties even in oxygen-deficient environments and at elevated temperatures4242 Apsarraj AD, Suresha B. Dynamic mechanical analysis and abrasive wear behavior of carbon-epoxy with molybdenum disulfide. In: International Conference on Innovations and Emerging Trends in Mechanical Engineering (IIETME-2014); 2014; Bangalore. Proceedings. Bangalore, India: Department of mechanical engineering, Nagarjuna college of engineering & technology; 2014.. It is found from the literature that these two solid and soft lubricant fillers have the ability to improve the thermomechanical properties of various resins. Hence, we attempted to investigate the thermomechanical properties and thermal stability of the carbon fabric/h-BN/epoxy and the carbon fabric/MoS2/epoxy composites. The material combination and the brief thermomechanical properties of various filler loaded CECs reported in the latest literature have been summarized and presented in Table 1.

Table 1
Material combination and brief thermomechanical properties of various filler loaded epoxy-based composites.

2. Materials and Methods

2.1. Material

The 2 × 2 twill weaved carbon fabric (CF) derived from T300 B (TORAYCA®) grade carbon fiber has been chosen for primary reinforcement. The fabric has 5 yarns per cm in both the warp and weft, area density-200 g.m-2, thickness-0.3mm, and number of filaments and yarn fineness are 3000 and 198 tex, respectively. The diglycidyl ether of bisphenol-A (DGBA) epoxy is used with N, N-Bis (2-aminoethyl) ethane1, 2-diamine curing agent as a matrix. The MoS2 and the h-BN solid lubricants are the fillers chosen. The physical and thermal properties of the reinforcement and the matrix materials have been indicated in Table 2.

Table 2
Particulars of reinforcement and matrix materials.

2.2. Composite laminate fabrication

The calculated quantity of as-bought filler (2, 4, 6, and 8 Wt.%) was dispersed in the appropriate quantity of epoxy matrix by magnetic stirring followed by ultrasonication. The magnetic stirring was performed for 20 mins at 500 rpm and maintained 60°C. Further, the epoxy-filler solution that was blended was sonicated in a probe type ultra-sonicator for about 30 mins keeping the vibration frequency of 20 kHz and the amplitude 35%. In this process, the filler got uniformly mixed with the matrix due to cavitation effect4343 Wattanakul K, Manuspiya H, Yanumet N. Thermal conductivity and mechanical properties of BN-filled epoxy composite: effects of filler content, mixing conditions, and BN agglomerate size. J Compos Mater. 2011;45(19):1967-80.. Afterwards, the stoichiometric quantity of amine-based curing agent (one part of hardener: four parts of resin) was added to the resulting filler-resin mixture and stirred meticulously. This process accelerates the rate of reaction and causes crosslinking. The weight fraction of the epoxy resin, hardener, fillers, and carbon fabric is chosen to prepare different composites as described in Table 3.

Table 3
Material combination of the filler loaded CEC and the neat CEC.

Polyvinyl alcohol was applied to the metallic mold as release agent for easy removal of the finished component. The filler dispersed epoxy matrix was manually coated over each successive layer of the carbon fabric. The roller moved over each stacked layer distributed the resin equally and removed air pockets to a certain extent. The same procedure was followed until the desired laminate thickness of approx. 4 mm [10 layers] was achieved. The top and bottom surfaces of the composite were covered with a peel ply to protect from containments. On the top of the peel ply, porous breather fabric cloths were appended to absorb the excess resin. Besides, the breather material acted as a channel for the removal of volatiles during the curing. The entire arrangement was enclosed with a vacuum bag film, which was sealed by a butyl sealant tape. The sealed bag was connected to a vacuum pump through the vacuum valve. After sealing the system, the air leak was tested. The vacuum pressure of 150 mm of hg was maintained for 20 mins. The pressure difference between the sealed chamber and the outside ambient diffused out the air bubbles. Besides, the vacuum bag method squeezed out the excess resin. The post-curing was completed in a hot air oven at 50°C for 2 hrs. during which the residual OH group present in the epoxy resin formed ether bond and ambient curing for 24 hrs. followed it. During crosslinking, the material changed from liquid to glass-like solid via gel. The cured composites were removed from the mold and developed the eight filler loaded CEC and one neat CEC laminate as the control. The fabricated laminate had a fiber volume fraction of approximately 45% evaluated according to the resin burn-off test.

2.3. Testing and characterization methods

The microstructure of the fillers MoS2 and h-BN was studied using a field emission scanning electron microscope (FESEM) [Made TESCAN-MIRA 3 LMH]. The Raman spectra of the filler loaded CEC and neat CEC materials were obtained using a confocal Raman spectrometer [Made Witec, alpha 300 RA]. The thermomechanical properties of all the composites were investigated through dynamic mechanical analyzer [Made DMA Q800, TA instrument]. To gain an insight into the thermal stability of the composite, thermogravimetric analysis (TGA) was performed [Made Perkin-Elmer 8000] in an oxygen environment.

3. Results and Discussion

3.1. Morphology of filler

The images of FESEM of bulk MoS2 powder, as shown in Figure 1, confirm nanosheet morphology and the adjacent sheets are attached to one another to form the stacks. The MoS2 sheets have a smooth and slightly wrinkled surface found below 809 nm. The analysis of energy-dispersive X-ray spectroscopy (EDS) [Made QUANTAX 200 BRUKER] of MoS2, as shown in Figure 1, reveals the presence of molybdenum and sulfur. The FESEM micrograph of the filler h-BN, as evident in Figure 2, displays conical morphology and a rod-like structure. The thickness of the h-BN particles varies from 165 to 361 nm with an average value of 258 nm. The average filler length was found to be 1.13 µm as identified by the Image-J software. The EDS graph of the h-BN, in Figure 2, reveals the presence of boron and nitrogen atoms.

Figure 1
Images of FESEM of pristine MoS2 particles (a) high magnification; (b) low magnification; (c) EDS graph.
Figure 2
Images of FESEM of pristine h-BN particles (a) high magnification; (b) low magnification; (c) EDS graph.

3.2. Raman spectroscopic analysis

Raman spectroscopy characterization has proven to be a valuable tool for identification of chemical groups and vibrational/rotational modes of molecular bonds present in the composite. The interaction of incident laser photon signal with the test material produces electric dipole moment and causes vibrations of the molecules which is the basis for Raman light scattering4444 Weber WH, Merlin R. Raman scattering in materials science. Berlin, Heidelberg: Springer; 2000.. The constituents in the composite scatter photons at different proportions due to change in polarizability and exhibit a unique chemical “fingerprint” at a definite frequency. The location of active Raman band based on the group frequency and associated mode of molecular vibration was identified for each element in composites and compared with the standard.

The Raman spectrum of the CEC loaded with the filler and neat CEC is presented in Figure 3. It shows the Raman signal peak at 826 cm-1 resulting from the symmetric stretch vibration of CH2 group4545 Socrates G. Infrared and Raman characteristic group frequencies: tables and charts. 3rd ed. Hoboken: John Wiley & Sons, Inc.; 2004.. Similarly, the Raman peak intensity between the wavenumber 1227-1231 cm-1 corresponds to the epoxide group i.e. C-O stretching and C-O-C ether stretching mode of DGBA epoxy, where two bands overlap4545 Socrates G. Infrared and Raman characteristic group frequencies: tables and charts. 3rd ed. Hoboken: John Wiley & Sons, Inc.; 2004.,4646 Farquharson S, Smith W, Rose J, Shaw M. Correlations between molecular (Raman) and macroscopic (rheology) data for process monitoring of thermoset composite. J Process Anal Chem. 2002;7:45-53.. However, the weaker Raman intensity of epoxide group possibly due to the ring-opening reaction. The peak at 1190 cm-1 in the Raman spectra was related to twisting deformation and vibration of CH2 group4545 Socrates G. Infrared and Raman characteristic group frequencies: tables and charts. 3rd ed. Hoboken: John Wiley & Sons, Inc.; 2004.. The sharp peak at 1296 cm-1 belonged to the D-band of carbon fiber signifies A1g mode (singly degenerate 1-D vibration) results from the amorphous and disordered carbon structure. The Raman signal peak at 1605 cm-1 was caused due to the G-band of carbon fiber which represents the stretching of hexagonally arranged carbon-carbon lattice structure in E2g mode (doubly degenerate 2-D vibration). The D-band Raman intensity lesser as compared to G-band signifies fewer structural disorder of carbon. The ratio of the D-band to the G-band intensities (ID/IG) found to be less than unity for all the composites. In the same way, Jang et al.4747 Jang D, Lee DS, Lee A, Joh H-I, Lee S. Opto-thermal technique for measuring thermal conductivity of polyacrylonitrile based carbon fibers. J Ind Eng Chem. 2019;78:137-42. http://dx.doi.org/10.1016/j.jiec.2019.06.025.
http://dx.doi.org/10.1016/j.jiec.2019.06...
reported two distinct Raman bands at the wavenumber 1350 and 1600 cm-1 for Toray 300 carbon fiber. The G-band of carbon fiber may overlap with the phenyl aromatic band stretching between 1604 and 1610 cm-1. The Raman signal peak intensity at 2937 cm-1 associated with the stretch of terminal epoxide=CH2. The low intensity of terminal hydroxy group (3340 cm-1) is due to cure reaction. Asymmetric stretching of C-H group at 3065 cm-1 was due to the DGBA reaction with curing agent4646 Farquharson S, Smith W, Rose J, Shaw M. Correlations between molecular (Raman) and macroscopic (rheology) data for process monitoring of thermoset composite. J Process Anal Chem. 2002;7:45-53..

Figure 3
The Raman spectrum (a) the CEC loaded with MoS2 and the neat CEC; (b) the CEC loaded with h-BN and the neat CEC.

The Raman spectrum of the CEC loaded with the MoS2 is presented in Figure 3a. Apart from the carbon fiber and epoxy resin characteristic peaks, the MoS2 functional group exhibited a signature peak between the wavenumbers 389 and 411 cm-1 indicative of the in-plane (E′2g) and out-of-plane directions (A1g) intra-layer vibration. The E′2g peak appeared as a result of internal vibration of sulfur atoms relative to the molybdenum layer, A1g peak related to out-of-layer vibration of sulfur atoms4848 Frey GL, Tenne R, Matthews MJ, Dresselhaus MS, Dresselhaus G. Raman and resonance Raman investigation of MoS2 nanoparticles. Phys Rev B Condens Matter Mater Phys. 1999;60(4):2883-92. http://dx.doi.org/10.1103/PhysRevB.60.2883.
http://dx.doi.org/10.1103/PhysRevB.60.28...
. Likewise, Frey et al.4848 Frey GL, Tenne R, Matthews MJ, Dresselhaus MS, Dresselhaus G. Raman and resonance Raman investigation of MoS2 nanoparticles. Phys Rev B Condens Matter Mater Phys. 1999;60(4):2883-92. http://dx.doi.org/10.1103/PhysRevB.60.2883.
http://dx.doi.org/10.1103/PhysRevB.60.28...
observed Raman peaks at 383 and 408 cm-1 for MoS2 particles when considering laser excitation wavelength of 500 nm i.e. different from the wavelength of the present study (532 nm). This difference in excitation wavelength lead to a slight variation in the location of Raman peak intensity compared to the published literature since the incident laser wavelength has a notable effect on the dipole moment, in turn on Raman active mode4949 Ferraro JR, Nakamoto K, Brown CW. Introductory Raman spectroscopy. 2nd ed. USA: Elsevier; 2003.. The composites loaded with 4 and 6 Wt.% MoS2 showed a larger MoS2 characteristic peak intensity. Also, the two Raman peaks (E′2g and A1g) in MoS2 loaded CEC appeared at a nearly constant wavenumber gap (26 cm-1) signified several layers of MoS2 filler present in the composite. Figure 3b displays the Raman spectrum associated with the h-BN loaded CEC series. It reveals the Raman scattering near 1370 cm-1 wavenumber and infers the E2g phonon band due to the presence of a functional group of h-BN. In the same way, the researchers Nemanich et al.5050 Nemanich RJ, Solin SA, Martin RM. Light scattering study of boron nitride microcrystals. Phys Rev B Condens Matter. 1981;23(12):6348-56. http://dx.doi.org/10.1103/PhysRevB.23.6348.
http://dx.doi.org/10.1103/PhysRevB.23.63...
reported Raman peak for h-BN at wavenumber 1366 cm-1. The Raman spectra in both types of hybrid filler loaded composites containing a filler with 4, 6 Wt.% exhibited a larger G-band intensity. Hence, it confirms improved matrix to fiber stress transfer. The shorter bond length h-BN (1.45 Å) shows the Raman characteristic peak at a higher wavenumber than the MoS2 (2.43 Å). The Raman spectra peak at low frequency (< 100 cm-1) is due to a highly reflective sample and therefore the intensity is too strong for the notch filter.

3.3. Dynamic mechanical analysis

The dynamic mechanical analysis (DMA) provides information on the softening temperature, the maximum operative temperature, the change in stiffness and the damping properties of composites due to the synergetic effect of cyclic bending load and temperature rise5151 ASTM International. ASTM D7028-07. Standard test method for glass transition temperature (Tg) of polymer matrix composites by dynamic mechanical analysis (DMA). West Conshohocken: ASTM International; 2015..

The dynamic properties were measured as per ASTM D 7028-075151 ASTM International. ASTM D7028-07. Standard test method for glass transition temperature (Tg) of polymer matrix composites by dynamic mechanical analysis (DMA). West Conshohocken: ASTM International; 2015. at a loading frequency 1 Hz, heating rate 5°C.min-1 by varying the temperature from ambient to 200°C. The dimension of the test sample was 57 mm × 13 mm × 4 mm. The cyclic deformation of amplitude 20 µm was applied at the center of the test sample with their ends being clamped (dual cantilever beam flexural setup). The E′, E′′, and tan δ were the responses determined as a function of temperature. The typical variation of elastic modulus with temperature is presented in Figure 4.

Figure 4
An ideal graph of elastic modulus versus temperature of FRP composite.

3.3.1. Effect of filler on storage modulus (E′)

The strength of the intermolecular forces, the packing, and the mobility of the polymer chains decide the E′. As the temperature increased, the composite experiences a relaxation mainly due to the cooperative movement of polymer chain segments. The easier polymer chain motion and energy dissipation in the relaxation process reduce the effective stress transfer between the constituents, which, in turn, lower the stiffness and the E′. The E′ of the material drops by more than one order at the Tg5252 Stark W. Investigation of the curing behaviour of carbon fibre epoxy prepreg by dynamic mechanical analysis. Polym Test. 2013;32(2):231-9. http://dx.doi.org/10.1016/j.polymertesting.2012.11.004.
http://dx.doi.org/10.1016/j.polymertesti...
. The E′ variation with the temperature at different filler concentrations is presented in Figure 5. Both the h-BN and MoS2 have positive effects on the E′ in glassy as well as rubbery regions up to 6 Wt.%. The E′ was greatly affected by filler concentration below Tg. A similar effect was elucidated by Loos et al.3434 Loos MR, Coelho LAF, Pezzin SH, Amico SC. Effect of carbon nanotubes addition on the mechanical and thermal properties of epoxy matrices. Mater Res. 2008;11(3):347-52. http://dx.doi.org/10.1590/S1516-14392008000300019.
http://dx.doi.org/10.1590/S1516-14392008...
for CNTs loaded epoxy composite. The filler loaded epoxy resin forms a polymer-filler continuous network and modifies the epoxy matrix-carbon fiber interaction. The MoS2 as well as h-BN fillers possibly occupied the free matrix volume and lowered the segmental mobility of the polymer chains due to chemical crosslinks. The maximum E′ of 14067 MPa was noticed for 6MSCEC at 35°C and it represents 70% larger than the neat CEC having a value of 8256 MPa. The MoS2 at 6 Wt.% perhaps creates a stiffer MoS2/epoxy chain network, and higher crosslinks between the surfaces of the fibers/fillers. Hence, a greater level of stress transfer was possible and improved E′. A similar effect reported by Azimpour-Shishevan et al.5353 Azimpour-Shishevan F, Akbulut H, Mohtadi-Bonab MA. Synergetic effects of carbon nanotube and graphene addition on thermo-mechanical properties and vibrational behavior of twill carbon fiber reinforced polymer composites. Polym Test. 2020;90:106745. http://dx.doi.org/10.1016/j.polymertesting.2020.106745.
http://dx.doi.org/10.1016/j.polymertesti...
for soft fillers (CNTs/graphene) strengthened CEC. The next highest E′ of 12295 MPa was observed for 6BNCEC. However, the composites reinforced beyond 6 Wt.% filler have the lower E′ signifying the detrimental effect of filler at the higher concentration causing stress accumulation. The lower E′ of the composite is also associated with the slip of filler in the epoxy matrix under dynamic loading.

Figure 5
The plot of storage modulus versus temperature (a) the CEC loaded with MoS2 and the neat CEC; (b) the CEC loaded with h-BN and the neat CEC.

The various scholars incorporated filler such as B4C1818 Muralidhara B, Babu SPK, Suresha B. Studies on dynamic mechanical and thermal properties of boron arbide filled carbon fiber/epoxy composites. Mater Today Proc. 2021;46(Pt 19):9145-9. http://dx.doi.org/10.1016/j.matpr.2019.12.204.
http://dx.doi.org/10.1016/j.matpr.2019.1...
, SiC3030 Kumaresan K, Chandramohan G, Senthilkumar M, Suresha B. Dynamic mechanical analysis and three-body wear of carbon–epoxy composite filled with SiC particles. J Reinf Plast Compos. 2012;31(21):1435-48. http://dx.doi.org/10.1177/0731684412459250.
http://dx.doi.org/10.1177/07316844124592...
, SiO21919 Divya GS, Suresha B, Somashekar HM, Jamadar IM. Dynamic mechanical analysis and optimization of hybrid carbon-epoxy composites wear using taguchi method. Tribol Ind. 2020;43(2):298-309., clay2020 Chowdhury FH, Hosur MV, Jeelani S. Investigations on the thermal and flexural properties of plain weave carbon/epoxy-nanoclay composites by hand-layup technique. J Mater Sci. 2007;42(8):2690-700. http://dx.doi.org/10.1007/s10853-006-1370-3.
http://dx.doi.org/10.1007/s10853-006-137...
,2121 Zhou Y, Hosur M, Jeelani S, Mallick PK. Fabrication and characterization of carbon fiber reinforced clay/epoxy composite. J Mater Sci. 2012;47(12):5002-12. http://dx.doi.org/10.1007/s10853-012-6376-4.
http://dx.doi.org/10.1007/s10853-012-637...
,3333 Tareq MS, Zainuddin S, Woodside E, Syed F. Investigation of the flexural and thermomechanical properties of nanoclay/graphene reinforced carbon fiber epoxy composites. J Mater Res. 2019;34(21):3678-87. http://dx.doi.org/10.1557/jmr.2019.302.
http://dx.doi.org/10.1557/jmr.2019.302...
, graphene platelets2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
http://dx.doi.org/10.1007/s40033-020-002...
,2323 Hossain MK, Chowdhury MMR, Bolden NW. Evaluation of thermo-mechanical properties of carbon/epoxy amino-functionalized graphene nanoplatelet composite. Glob J Eng Sci. 2020;4(4):1-10., GO3131 Adak NC, Chhetri S, Kim NH, Murmu NC, Samanta P, Kuila T. Static and dynamic mechanical properties of graphene oxide-incorporated woven carbon fiber/epoxy composite. J Mater Eng Perform. 2018;27(3):1138-47. http://dx.doi.org/10.1007/s11665-018-3201-5.
http://dx.doi.org/10.1007/s11665-018-320...
and concluded that their presence favorable for improving E′ of CEC. Likewise, the previous studies showed that E′ of epoxy was improved by the inclusion of h-BN2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
http://dx.doi.org/10.1039/C9NJ05834F...
, graphene2424 Cai L, Al Ostaz A, Li X, Drzal LT, Rook BP, Cheng AHD, et al. Processing and mechanical properties investigation of epoxy-impregnated graphene paper. J Nanomech Micromech. 2016;6(3):04016005. http://dx.doi.org/10.1061/(ASCE)NM.2153-5477.0000108.
http://dx.doi.org/10.1061/(ASCE)NM.2153-...
, and GO3232 Wan YJ, Gong LX, Tang LC, Wu LB, Jiang JX. Mechanical properties of epoxy composites filled with silane-functionalized graphene oxide. Compos, Part A Appl Sci Manuf. 2014;64:79-89. http://dx.doi.org/10.1016/j.compositesa.2014.04.023.
http://dx.doi.org/10.1016/j.compositesa....
filler. However, very few research works available describing the effect of MoS2, h-BN filler on E′ of the CEC that too available only in the higher filler Wt.% and not in the wider range. In the present study E′ improved up to 70% for 6 Wt.% MoS2 reinforced CEC and 49% for 6 Wt.% h-BN reinforced CEC.

Based on the obtained result, the E′ of MoS2 composite series below Tg from the highest to the lowest level is in the order – 6MSCEC > 4MSCEC > 2MSCEC > 8MSCEC > CEC. The E′ of BN composite series below Tg from the highest to the lowest level is as follows – 6BNCEC > 4BNCEC > 2BNCEC > CEC > 8BNCEC. The glassy region (developed temperature < Tg) is characterized by high stiffness, E′ and restricted molecular chain motion. The E′ in all the composites above Tg (rubbery region) becomes low since the resin matrix loses its stability5454 Ghosh P, Bose NR, Mitra BC, Das S. Dynamic mechanical analysis of FRP composites based on different fiber reinforcements and epoxy resin as the matrix material. J Appl Polym Sci. 1997;64(12):2467-72.. Hence, the composite can store more energy at a temperature below Tg (glassy state).

3.3.2. Effect of filler on loss modulus (E′′)

When the cyclic load is applied to the composite, the filler along with fiber reinforcement tries to hold the laminate in place. However, certain activation energy is essential to deform the sample and overcome the barrier for molecular motions5555 Goertzen WK, Kessler MR. Dynamic mechanical analysis of carbon/epoxy composites for structural pipeline repair. Compos, Part B Eng. 2007;38(1):1-9.. During this process, some amount of energy is dissipated. The E′′ is the measure of the internal heat energy dissipated from the composites related to the internal friction of filler/fiber-matrix caused by the phase transformation under dynamic loading. The viscoelastic lag between stress and strain is denoted by E′′. The variation of E′′ with temperature is indicated in Figure 6. The E′′ attains a peak value at the Tg where the onset of segmental motion of epoxy polymer chains occurs. The h-BN fillers have excellent thermal conductivity (Table 2) and therefore it facilitates in the larger improvement of the composite thermal conductivity than the MoS2. Hence, the h-BN reinforced CEC enhances heat dissipation leading to the higher E′′. The enhancement of E′′ was observed up to 6 Wt.% h-BN (33% improved) and 4 Wt.% MoS2 reinforced CEC (9% improved), and later it was reduced compared to neat CEC. This observation agree with the work of Apsarraj et al.4242 Apsarraj AD, Suresha B. Dynamic mechanical analysis and abrasive wear behavior of carbon-epoxy with molybdenum disulfide. In: International Conference on Innovations and Emerging Trends in Mechanical Engineering (IIETME-2014); 2014; Bangalore. Proceedings. Bangalore, India: Department of mechanical engineering, Nagarjuna college of engineering & technology; 2014. who reported a declining trend for E′′ at 5 and 10 Wt.% MoS2 (size: 25µm) reinforced unidirectional CEC. The maximum E′′ of 1775 MPa was noticed for 6BNCEC at 88°C (Tg) and related the broadening of E′′ peak to the inhibition of relaxation process. The next highest E′′ of 1530 MPa was observed for 4BNCEC at 92°C (Tg). The higher E′′ conveys better filler-epoxy matrix interaction and strong internal friction. Beyond the respective Tg it reduced the E′′.

Figure 6
The plot of loss modulus versus temperature (a) the CEC loaded with MoS2 and the neat CEC; (b) the CEC loaded with h-BN and the neat CEC.

The earlier research studies depicted improvement in E′′ of CEC with the inclusion of B4C1818 Muralidhara B, Babu SPK, Suresha B. Studies on dynamic mechanical and thermal properties of boron arbide filled carbon fiber/epoxy composites. Mater Today Proc. 2021;46(Pt 19):9145-9. http://dx.doi.org/10.1016/j.matpr.2019.12.204.
http://dx.doi.org/10.1016/j.matpr.2019.1...
, SiC3030 Kumaresan K, Chandramohan G, Senthilkumar M, Suresha B. Dynamic mechanical analysis and three-body wear of carbon–epoxy composite filled with SiC particles. J Reinf Plast Compos. 2012;31(21):1435-48. http://dx.doi.org/10.1177/0731684412459250.
http://dx.doi.org/10.1177/07316844124592...
, SiO21919 Divya GS, Suresha B, Somashekar HM, Jamadar IM. Dynamic mechanical analysis and optimization of hybrid carbon-epoxy composites wear using taguchi method. Tribol Ind. 2020;43(2):298-309., clay2020 Chowdhury FH, Hosur MV, Jeelani S. Investigations on the thermal and flexural properties of plain weave carbon/epoxy-nanoclay composites by hand-layup technique. J Mater Sci. 2007;42(8):2690-700. http://dx.doi.org/10.1007/s10853-006-1370-3.
http://dx.doi.org/10.1007/s10853-006-137...
, graphene2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
http://dx.doi.org/10.1007/s40033-020-002...
,2323 Hossain MK, Chowdhury MMR, Bolden NW. Evaluation of thermo-mechanical properties of carbon/epoxy amino-functionalized graphene nanoplatelet composite. Glob J Eng Sci. 2020;4(4):1-10.,3333 Tareq MS, Zainuddin S, Woodside E, Syed F. Investigation of the flexural and thermomechanical properties of nanoclay/graphene reinforced carbon fiber epoxy composites. J Mater Res. 2019;34(21):3678-87. http://dx.doi.org/10.1557/jmr.2019.302.
http://dx.doi.org/10.1557/jmr.2019.302...
, and GO3131 Adak NC, Chhetri S, Kim NH, Murmu NC, Samanta P, Kuila T. Static and dynamic mechanical properties of graphene oxide-incorporated woven carbon fiber/epoxy composite. J Mater Eng Perform. 2018;27(3):1138-47. http://dx.doi.org/10.1007/s11665-018-3201-5.
http://dx.doi.org/10.1007/s11665-018-320...
.

3.3.3. Effect of filler on loss factor

We evaluated the tangent of the phase angle (δ) based on the ratio of the E′′ to E′. It signified balance between the elastic and the viscous phases of polymer composites5656 Murugan R, Ramesh R, Padmanabhan K. Investigation on static and dynamic mechanical properties of epoxy based woven fabric glass/carbon hybrid composite laminates. Procedia Eng. 2014;97:459-68. http://dx.doi.org/10.1016/j.proeng.2014.12.270.
http://dx.doi.org/10.1016/j.proeng.2014....
. The tan δ indicated how good a material dissipated energy under a cyclic load, which depends on the bond rotation and intermolecular friction. The peak position of loss factor curve illustrated the high damping owing to the chain motion5353 Azimpour-Shishevan F, Akbulut H, Mohtadi-Bonab MA. Synergetic effects of carbon nanotube and graphene addition on thermo-mechanical properties and vibrational behavior of twill carbon fiber reinforced polymer composites. Polym Test. 2020;90:106745. http://dx.doi.org/10.1016/j.polymertesting.2020.106745.
http://dx.doi.org/10.1016/j.polymertesti...
.

The graphical variation of the tan δ with temperature for various composites is shown in Figure 7. When the temperature was below Tg the molecules in the composite packed closely and the chain segments in a frozen state causing low tan δ. The tan δ reached the maximum at Tg where the resin molecules attained high mobility5656 Murugan R, Ramesh R, Padmanabhan K. Investigation on static and dynamic mechanical properties of epoxy based woven fabric glass/carbon hybrid composite laminates. Procedia Eng. 2014;97:459-68. http://dx.doi.org/10.1016/j.proeng.2014.12.270.
http://dx.doi.org/10.1016/j.proeng.2014....
. At the transition regime, the maximum molecular chain participated in the micro-Brownian movement (conjunctive diffusion), and hence energy dissipation causes maximal damping5757 Hameed N, Sreekumar PA, Valsaraj VS, Thomas S. High-performance composite from epoxy and glass fibers: morphology, mechanical, dynamic mechanical, and thermal analysis. Polym Compos. 2009;30(7):982-92. http://dx.doi.org/10.1002/pc.20644.
http://dx.doi.org/10.1002/pc.20644...
. Beyond Tg, the tan δ started decreasing. With the increase in temperature, the happening of filler-matrix interface slippage might also dissipate the energy88 Chung DDL. Composite materials: functional materials for modern technologies. In: Derby B, editor. Engineering materials and processes. London: Springer; 2003.,5858 Chartoff RP, Menczel JD, Dillman SH. Dynamic mechanical analysis (DMA). In: Menczel JD, Prime RB, editors. Thermal Analysis of Polymers. Hoboken, USA: John Wiley & Sons, Inc.; 2008. http://dx.doi.org/10.1002/9780470423837.ch5
http://dx.doi.org/10.1002/9780470423837....
. The low tan δ recorded for 6MSCEC sample (36%↓) implied a more constrained region due to the larger filler contact area with the epoxy, indicated effective filler dispersion in the epoxy networks that stiffen the composites. Apsarraj et al.4242 Apsarraj AD, Suresha B. Dynamic mechanical analysis and abrasive wear behavior of carbon-epoxy with molybdenum disulfide. In: International Conference on Innovations and Emerging Trends in Mechanical Engineering (IIETME-2014); 2014; Bangalore. Proceedings. Bangalore, India: Department of mechanical engineering, Nagarjuna college of engineering & technology; 2014. as well reported tan δ decrement for 5 and 10 Wt.% MoS2 reinforced unidirectional CEC. In the same way, tan δ peak height of h-BN loaded CEC lowered until 6 Wt.% (11%↓) due to stiffness enhancement and mobility restriction of the h-BN blend epoxy. A similar effect confirmed by Joy et al.2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
http://dx.doi.org/10.1039/C9NJ05834F...
for nano h-BN loaded epoxy resin. Among the filler loaded composites, the maximum tan δ of 0.687 (h-BN) and 0.611 (MoS2) were observed for the filler loading of 8 Wt.% at Tg.

Figure 7
The plot of tan δ versus temperature (a) the CEC loaded with MoS2 and the neat CEC; (b) the CEC loaded with h-BN and the neat CEC.

Several scholars revealed that filler such as SiC3030 Kumaresan K, Chandramohan G, Senthilkumar M, Suresha B. Dynamic mechanical analysis and three-body wear of carbon–epoxy composite filled with SiC particles. J Reinf Plast Compos. 2012;31(21):1435-48. http://dx.doi.org/10.1177/0731684412459250.
http://dx.doi.org/10.1177/07316844124592...
, SiO21919 Divya GS, Suresha B, Somashekar HM, Jamadar IM. Dynamic mechanical analysis and optimization of hybrid carbon-epoxy composites wear using taguchi method. Tribol Ind. 2020;43(2):298-309. lowered tan δ whereas B4C1818 Muralidhara B, Babu SPK, Suresha B. Studies on dynamic mechanical and thermal properties of boron arbide filled carbon fiber/epoxy composites. Mater Today Proc. 2021;46(Pt 19):9145-9. http://dx.doi.org/10.1016/j.matpr.2019.12.204.
http://dx.doi.org/10.1016/j.matpr.2019.1...
, GNP2323 Hossain MK, Chowdhury MMR, Bolden NW. Evaluation of thermo-mechanical properties of carbon/epoxy amino-functionalized graphene nanoplatelet composite. Glob J Eng Sci. 2020;4(4):1-10., GO3131 Adak NC, Chhetri S, Kim NH, Murmu NC, Samanta P, Kuila T. Static and dynamic mechanical properties of graphene oxide-incorporated woven carbon fiber/epoxy composite. J Mater Eng Perform. 2018;27(3):1138-47. http://dx.doi.org/10.1007/s11665-018-3201-5.
http://dx.doi.org/10.1007/s11665-018-320...
increased tan δ of CEC. In addition to that, some studies showed that clay2020 Chowdhury FH, Hosur MV, Jeelani S. Investigations on the thermal and flexural properties of plain weave carbon/epoxy-nanoclay composites by hand-layup technique. J Mater Sci. 2007;42(8):2690-700. http://dx.doi.org/10.1007/s10853-006-1370-3.
http://dx.doi.org/10.1007/s10853-006-137...
,2121 Zhou Y, Hosur M, Jeelani S, Mallick PK. Fabrication and characterization of carbon fiber reinforced clay/epoxy composite. J Mater Sci. 2012;47(12):5002-12. http://dx.doi.org/10.1007/s10853-012-6376-4.
http://dx.doi.org/10.1007/s10853-012-637...
, graphene2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
http://dx.doi.org/10.1007/s40033-020-002...
increased tan δ of CEC but lowered tan δ when it was added to the epoxy2121 Zhou Y, Hosur M, Jeelani S, Mallick PK. Fabrication and characterization of carbon fiber reinforced clay/epoxy composite. J Mater Sci. 2012;47(12):5002-12. http://dx.doi.org/10.1007/s10853-012-6376-4.
http://dx.doi.org/10.1007/s10853-012-637...
,2424 Cai L, Al Ostaz A, Li X, Drzal LT, Rook BP, Cheng AHD, et al. Processing and mechanical properties investigation of epoxy-impregnated graphene paper. J Nanomech Micromech. 2016;6(3):04016005. http://dx.doi.org/10.1061/(ASCE)NM.2153-5477.0000108.
http://dx.doi.org/10.1061/(ASCE)NM.2153-...
. Hence, increased tan δ of filler loaded CEC might be due to the inherent damping properties of carbon fiber which reduced intermolecular friction and improved energy dissipation.

3.3.4. Effect of filler on Tg

The heated composite material transformed from the glassy to rubbery state attributable to the mobility change of polymer chains at a temperature known as Tg5252 Stark W. Investigation of the curing behaviour of carbon fibre epoxy prepreg by dynamic mechanical analysis. Polym Test. 2013;32(2):231-9. http://dx.doi.org/10.1016/j.polymertesting.2012.11.004.
http://dx.doi.org/10.1016/j.polymertesti...
. The temperature that corresponded to the peak of tan δ curve was considered the Tg. Below the Tg, the polymer chains were locked as they do not have sufficient energy to cause structure transformation. When the temperature exceeds Tg, the polymer molecules could slide each other and the material turned flexible5858 Chartoff RP, Menczel JD, Dillman SH. Dynamic mechanical analysis (DMA). In: Menczel JD, Prime RB, editors. Thermal Analysis of Polymers. Hoboken, USA: John Wiley & Sons, Inc.; 2008. http://dx.doi.org/10.1002/9780470423837.ch5
http://dx.doi.org/10.1002/9780470423837....
. The Tg obtained depended on segmental mobility of the polymer chains and it, in turn, depended on the chain stiffness, steric hindrance, and availability of space for the molecular motion. The addition of the fillers MoS22727 Madeshwaran SR, Jayaganthan R, Velmurugan R, Gupta NK, Manzhirov AV. Mechanical and thermal properties of MoS2 reinforced epoxy nanocomposites. J Phys Conf Ser. 2018;991:12054. http://dx.doi.org/10.1088/1742-6596/991/1/012054.
http://dx.doi.org/10.1088/1742-6596/991/...
and h-BN2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
http://dx.doi.org/10.1039/C9NJ05834F...
affected the mobility of the epoxy chains and varied the Tg. Besides, the Tg was also affected by the crosslinking density, the dispersion of filler and its interaction with the epoxy resin3131 Adak NC, Chhetri S, Kim NH, Murmu NC, Samanta P, Kuila T. Static and dynamic mechanical properties of graphene oxide-incorporated woven carbon fiber/epoxy composite. J Mater Eng Perform. 2018;27(3):1138-47. http://dx.doi.org/10.1007/s11665-018-3201-5.
http://dx.doi.org/10.1007/s11665-018-320...
. With the 4 Wt.% h-BN incorporation in the CEC, the maximum Tg was attained i.e. an increase from 88.09 to 92.48°C. It was attributed to the increased chain rigidity and stronger fiber-polymer-filler interactions due to the improved filler dispersion. Therefore, the greater resistance to the motion of polymer molecules demanded more heat energy. Joy et al.2626 Joy J, George E, Thomas S, Anas S. Effect of filler loading on polymer chain confinement and thermomechanical properties of epoxy/boron nitride (h-BN) nanocomposites. New J Chem. 2020;44(11):4494-503. http://dx.doi.org/10.1039/C9NJ05834F.
http://dx.doi.org/10.1039/C9NJ05834F...
also reported Tg improvement for h-BN loaded epoxy. However, when the h-BN concentration exceeded 4 Wt.% the easy sliding between the h-BN particles became prominent, likely reduced the crosslinking points, and lowered the Tg. In contrast, the MoS2 filled CEC slightly lowered the Tg which might be due to anisotropy of thin wrinkled MoS2, barrier effect and tendency to lose brittleness with MoS2. It was recognized from the shift in the tan δ peak towards the lower temperature. The Tg reduction up to 1.74°C is noticed for 2MSCEC. A similar reduction of Tg was found in the literature for soft filler (graphene) loaded CEC2222 Muralidhara B, Babu SPK, Suresha B. Studies on the role of graphene nanoplatelets on mechanical properties, dynamic-mechanical and thermogravimetric analysis of carbon-epoxy composites. J Inst Eng India Ser D. 2020. http://dx.doi.org/10.1007/s40033-020-00219-0.
http://dx.doi.org/10.1007/s40033-020-002...
.

Based on the DMA, the degree of crosslinking was evaluated according to the Equation 1 5959 Hill L. Dynamic mechanical and tensile properties. In: Koleske J, editor. Paint and Coating Testing Manual. 15th ed. West Conshohocken, PA: ASTM International; 2012..

Crosslink density = E'r RT (1)

Where, E′r = Storage modulus (MPa) measured at the rubbery region, R = Universal gas constant (8.314 J.K-1.mol-1), T = temperature corresponding to the E′r (381°K).

The crosslink density has been expressed in the moles of elastically effective network chains per unit volume. The higher crosslink density witnessed for 4MSCEC and 6MSCEC in the order 0.262 and 0.221 mol.cm-3, respectively. In both the types of composites, filler concentration of 8 Wt.% caused a low crosslink density due to localized agglomeration which possibly lowered the filler entry into the inter chain spacing of polymer and decreased the polymer–filler crosslink. The result of the DMA is given in Table 4.

Table 4
Dynamic properties of the filler loaded CEC and the neat CEC.

3.4. Thermogravimetric analysis: ambient condition

The TGA provides information regarding the heat resistance and decomposition behavior of the polymeric material6060 Ralph E. Wright. Thermosets, reinforced plastics, and composites. In: Harper Charles A, editor. Handbook of plastics, elastomers, and composites. New York: McGraw-Hill; 2002.. The TGA under the oxygen atmosphere guarantees the complete decomposition of both the epoxy matrix and carbon fiber. The test comprises recording the change in weight of the composite once it was subjected to an increase in temperature. The test involves two-stage heating. Initially, the composite samples (5-10 mg) were heated from 50 to 600°C in a hermetic aluminum crucible at 20°C.min-1 and held at 600°C for 1 min. Secondly, the sample was heated to a temperature of 900°C at 20°C.min-1, and held at 900°C for 10 min.

The characteristics of the thermally stable material are the higher softening temperatures, the more residual mass, and the minimal deviations in the physical or chemical properties6161 Saba N, Jawaid M. A review on thermomechanical properties of polymers and fibers reinforced polymer composites. J Ind Eng Chem. 2018;67:1-11. http://dx.doi.org/10.1016/j.jiec.2018.06.018.
http://dx.doi.org/10.1016/j.jiec.2018.06...
. The thermograms of different composite samples are presented in Figure 8. At a very low temperature, the molecular chains are fixed, holding the filler/fiber with the matrix. However, the chains move freely at an elevated temperature and the interaction between the matrix and the filler/fiber becomes weak. This causes a reduction in the thermal stability. In the first stage, decomposition is related to the evaporation of moisture content and volatilization of the epoxy matrix (degradation because of chain scission)6262 Prime RB, Bair HE, Vyazovkin S, Gallagher PK, Riga A. Thermogravimetric analysis (TGA). In: Menczel JD, Prime RB, editors. Thermal analysis of polymers. Hoboken, USA: John Wiley & Sons, Inc.; 2008. http://dx.doi.org/10.1002/9780470423837.ch3.
http://dx.doi.org/10.1002/9780470423837....
starts near the temperature 260°C. Similarly, at this temperature there can be a small reduction in the content of oxygen present at the carbon fiber surface. Further, the combustion of residual carbon of epoxy resin occurs between 420 to 600°C6363 Yu C, Zhang J, Li Z, Tian W, Wang L, Luo J, et al. Enhanced through-plane thermal conductivity of boron nitride/epoxy composites. Compos, Part A Appl Sci Manuf. 2017;98:25-31. http://dx.doi.org/10.1016/j.compositesa.2017.03.012.
http://dx.doi.org/10.1016/j.compositesa....
besides carbon fiber experiences oxidation and turns into CO2 vapor6464 Grund D, Orlishausen M, Taha I. Determination of fiber volume fraction of carbon fiber-reinforced polymer using thermogravimetric methods. Polym Test. 2019;75:358-66. http://dx.doi.org/10.1016/j.polymertesting.2019.02.031.
http://dx.doi.org/10.1016/j.polymertesti...
. The decomposition temperatures of different composites evaluated at 25, 50, and 75% weight loss are displayed in Table 5. The thermal stability of both the h-BN reinforced CEC and MoS2 reinforced CEC are comparable. The decomposition temperature is shifted slightly to a higher temperature as a solid-lubricant filler is reinforced to the epoxy resin. Among all, 4MSCEC and 4BNCEC materials need the higher heat energy for the complete thermal decomposition and it is thermally stable. This improvement in the thermal stability is identified by the increase in decomposition temperature attributed to rigid MoS2 filler that restrains the mobility of the epoxy chains and barrier effect of MoS2 restricts the osmosis of heat consequently delay the oxidation (slow down heat and mass transfer)6565 Wang D, Zhou K, Yang W, Xing W, Hu Y, Gong X. Surface modification of graphene with layered molybdenum disulfide and their synergistic reinforcement on reducing fire hazards of epoxy resins. Ind Eng Chem Res. 2013;52(50):17882-90. http://dx.doi.org/10.1021/ie402441g.
http://dx.doi.org/10.1021/ie402441g...
and release of pyrolysis gas. Moreover, MoS2 oxidizes to molybdenum trioxide (MoO3) that potentially suppresses the smoke6565 Wang D, Zhou K, Yang W, Xing W, Hu Y, Gong X. Surface modification of graphene with layered molybdenum disulfide and their synergistic reinforcement on reducing fire hazards of epoxy resins. Ind Eng Chem Res. 2013;52(50):17882-90. http://dx.doi.org/10.1021/ie402441g.
http://dx.doi.org/10.1021/ie402441g...
. Similarly, h-BN filler also impedes the escape of decomposition products and delayed the evaporation of volatile matter promoting thermal stability.

Figure 8
Thermograms of composites (a) the CEC loaded with MoS2 and the neat CEC; (b) the CEC loaded with h-BN and the neat CEC.
Table 5
Temperature at different weight losses of various composites.

4. Conclusions

We investigated the dynamic mechanical properties and the thermal stability of carbon fabric reinforced epoxy with fillers – h-BN and MoS2 and arrived at the following conclusions:

  • The local filler networks at 6 Wt.% (MoS2/h-BN) in the carbon fabric-epoxy composite transferred the applied external load and improved the stiffness and the E′ of the composite. Particularly, MoS2 reinforced CEC improved E′ up to 70% as it promoted stiffening and crosslink density.

  • The internal heat energy dissipation was large for the maximum loss modulus witnessed in the 6BNCEC (improved by 33%) at the transition state temperature. The larger energy dissipation indicated more resistance towards the viscoelastic deformation of epoxy matrix due to better filler distribution in the matrix. Although, the height of tan δ peak lowered with solid lubricant filler (MoS2 as well as h-BN) loaded CEC, it did not reduce much like hard filler loaded composite in the published literature.

  • The 4MSCEC and the 4BNCEC showed superior thermal stability due to better filler-epoxy interaction with a low mass loss at an elevated temperature. The smoke suppressing characteristics and rigid filler (restrains the epoxy chains mobility) responsible for the delay of thermal decomposition.

  • The filler addition above the critical limit (6 Wt.%) reduced the adhesion of the reinforcement-matrix due to particle-particle interface and lowered the DMA properties.

  • The Raman spectrum of the filler reinforced CEC confirmed the presence of filler by showing its Raman signature at the wavenumber 389 and 411 cm-1 for MoS2 while 1370 cm-1 for h-BN apart from the carbon fiber and epoxy resin. The larger G-band Raman intensity of 4 and 6 Wt.% filler loaded CEC confirmed the improved matrix to fiber stress transfer via the filler.

  • From the present investigation, the optimum soft filler (h-BN/MoS2) addition in CEC caused noteworthy improvement of storage modulus, loss modulus, crosslink density, and thermal stability. Therefore, composites derived from such low-cost and abundantly available solid lubricant filler are a good choice for elevated temperature environments and are recommended for future studies.

5. Acknowledgments

The authors are grateful to Dr. Siddaramaiah, HOD, Polymer Science & Technology, SJCE, Mysuru for providing the DMA test facility. The authors are thankful to Mr. Sridhar T, Mr. Manohar R, Mr. Sandeep D for assisting to carry out tests.

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Publication Dates

  • Publication in this collection
    19 Nov 2021
  • Date of issue
    2021

History

  • Received
    04 May 2021
  • Reviewed
    17 July 2021
  • Accepted
    04 Aug 2021
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