Lu Liabc,
Xia Liao*a,
Xingyue Shengb,
Zengheng Hao*bc,
Leilei Heb,
Pan Liub,
Hongbin Quanb and
Yi Zhangb
aCollege of Polymer Science and Engineering, State Key Laboratory of Polymer Materials Engineering, Sichuan University, Chengdu 610065, Sichuan, China. E-mail: xliao@scu.edu.cn
bChongqing Zhixiang Paving Technology Engineering Co., Ltd., Chongqing 401336, China. E-mail: haozengheng@cmhk.com
cChina Merchants Chongqing Communications Research & Design Institute Co., Ltd., Chongqing 400067, China
First published on 26th April 2019
In this paper, carboxylic multi-walled carbon nanotubes (MWCNTs-COOH) were modified by a series of hyperbranched polyesters (HBP) with different molecular structures (different branching degree) through surface grafting, and then the epoxy resin (EP)/carbon nanotube composites were prepared to explore the influences of structure regulation of HBP modified carbon nanotubes on the toughening performance of the composites. The results of Fourier transform infrared spectroscopy (FTIR), transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), and thermogravimetric analysis (TGA) of various HBP grafted carbon nanotubes confirmed that the HBP were successfully grafted onto MWCNTs-COOH via an esterification reaction between the carboxyl groups of MWCNTs-COOH and the hydroxyl groups of HBP, meanwhile, the higher the branching degree of the HBP, the higher its grafting ratio onto carbon nanotubes. Furthermore, the outcome of dynamic thermal mechanical analysis (DMA) indicated that the addition of MWCNTs-COOH increased the storage modulus and glass transition temperature (Tg) of the pure EP, and surface grafting of various HBP onto MWCNTs-COOH decreased the Tg and peak height of mechanical loss of composites. And as the branching degree of HBP increased, the interfacial bonding between MWCNTs and the EP matrix became stronger. The results of mechanical performance and morphology analysis also revealed that the addition of HBP grafted MWCNTs-COOH significantly improved its dispersion and interfacial bonding in the EP matrix, resulting in better performance in the enhancement of toughness of the composites. In addition, it was found that the higher the branching degree of HBP, the better the toughening performance of the composites.
Toughness, achieved through various deformation mechanisms before failure occurs, implies energy absorption. In past years, great efforts have been made to improve the toughness of epoxy thermosets. One effective mechanism to increase toughness is the addition of a second phase (elastomers), however, at the expense of its other performance such as thermal resistance and strength.5,7,9–11
Through the introduction of inorganic fillers to improve the toughness of epoxy resin without sacrificing other properties has been found recently.9,12–14 The multi-walled carbon nanotubes (MWCNTs) are ideal fillers for polymer composites due to their high Young's modulus as well as good electrical and thermal conductivity.5,8,15–17 Once added with a small amount of MWCNTs, the electrical, thermal and mechanical properties of the polymer matrix can be strongly improved, resulting the composites with good processability, such as balanced stiffness, toughness and other functional properties. However, due to their insolubility, non-melting, easy to tangle and agglomerate, and lack of surface functional groups, carbon nanotubes are difficult to process, as well as poor dispersibility and stability, poor compatibility with epoxy matrix materials limiting their application areas.14,18–21 An effective way to improve the dispersion and interfacial bonding properties of carbon nanotubes in epoxy matrix is surface chemical modification of carbon nanotubes.5,13,15,22
Jin et al.23 acidified P-MWCNTs (pure carbon nanotubes) to obtain A-MWCNTs (acidified carbon nanotubes). Then A-MWCNTs were amine treated (D-MWCNTs) and added to bisphenol A epoxy resin (DGEBA). DGEBA/MWCNTs matrix composites were prepared. Compared with pure DGEBA in mechanical properties, it was found that the interface between MWCNTs and DGEBA was well bonded after modification, which effectively improved the interface between MWCNTs and DGEBA. The dispersibility in bulk resin improves the fracture toughness of DGEBA. Spitalsky et al.24 also used acidification and amination treatment, and obtained similar conclusions. However, the traditional acidification and amination are relatively simple surface chemical modification, which makes it difficult to quantitatively control the surface groups of MWCNTs, and the damage to the structure of MWCNTs is obvious. Therefore, it is of great significance to find new surface modification methods for MWCNTs in toughening epoxy resins.
Hyperbranched polymers have a lower branching efficiency than dendrimers while possessing many useful properties.5,6,25,26 The highly branched architecture minimizes chain–chain ability and low melt viscosity to these polymers, which is compatible with epoxy thermosets. The presence of plenty of functional groups (–OH) provides high reaction activity with inorganic filler, providing us a possibility to be desirable macromolecular surface modifier for MWCNTs, to further enhance the compatibility and dispersion in epoxy resin. On the other hand, research on toughening epoxy resin with hyperbranched polymers is also increasing. J. Yang27 used hyperbranched polymer H30 as toughening agent of epoxy resin, the results showed that H30 can significantly improve the tensile properties, ductility and impact toughness of epoxy resin at low temperature. Jorg Frohlich28 developed a new type of epoxy resin with polyether core–shell hyperbranched structure. The results of tensile test, impact toughness and DMA test showed that the toughness of epoxy resin was significantly improved.
Therefore, we believe that the preparation of hyperbranched polymer grafted carbon nanotubes modified epoxy resin can not only improve the dispersion and interfacial bonding of carbon nanotubes (MWCNTs) in epoxy resin (EP) matrix by using a large number of active end groups of hyperbranched polymer, but also further toughen epoxy resin on the basis of EP/MWCNTs. In the previous study,5 we had successfully prepared hyperbranched polyester (H202) grafted MWCNTs, and had applied it in the toughening of epoxy resin cured by diethyltoluene diamine. Results showed that the hyperbranched polyester grafted MWCNTs received a better dispersion in the epoxy prepolymer compared with the raw MWCNTs, which further decreased the glass transition temperature of the EP/MWCNTs composites and exhibited better performance in the enhancement in toughening EP.
Novel method to prepare high performance EP/MWCNTs composites had been provided in the previous study, achieving only investigating one kind of molecular structure of hyperbranched polyester grafted MWCNTs in the system. Still the surface modification of MWCNTs using hyperbranched polyester with different molecular structure might greatly influence the toughening performance, which has not been investigated before. This study aims to comparatively explore the role of hyperbranched polyesters with different branching degrees surface modification of MWCNTs in the toughening performance of the EP/MWCNTs composites.
Hyperbranched polyester H201 (Mw = 600 g mol−1, hydroxyl number = 550 mg KOH/g polymer), H202 (Mw = 1200 g mol−1, hydroxyl number = 520 mg KOH/g polymer), H203 (Mw = 2600 g mol−1, hydroxyl number = 500 mg KOH/g polymer), H204 (Mw = 5400 g mol−1, hydroxyl number = 490 mg KOH/g polymer) was purchased from Wuhan Hyperbranched Polymer Resins Science & Technology Co. Ltd. (China), and was used as received. Diglycidyl ether of bisphenol A (DGEBA, KE-133L, Chengdu Kemmett Technical Co., Ltd.) (epoxide equivalent: 182 g mol−1) was dried under vacuum at 80 °C for 8 h before use. Diethyltoluene diamine (DETDA) and N,N-dimethylformamide (DMF) were purchased from Sinopharm Chemical Reagent Beijing Co., Ltd., China, and were used as received.
The chemical structures of the MWCNTs-COOH and Hyper H201, H202, H203, H204 are shown in Scheme 1.
Fig. 1 FT-IR spectra of (a) hyper-branched polyester with different branching degrees and (b) different grafted MWCNTs-COOH. |
For FT-IR spectra of different branching degrees of hyper-branched polyester modified carbon nanotubes, it can be observed from Fig. 1b, compared with the pre-grafting (MWCNTs-COOH), the absorption peak of carbon nanotubes at the wave numbers of 2921.9 cm−1 and 2888.5 cm−1 were added after four different branching degrees of hyperbranched polyester grafting modifications, corresponding to the antisymmetric and symmetric stretching vibration of methyl and methylene, respectively. And the higher the branching degree of hyperbranched polyester increased, the stronger the absorption peak strength was. Since hyperbranched polyester contains large amounts of methyl and methylene in their molecular structure, it can be inferred from Fig. 1b that all four kinds of hyperbranched polyesters with different branching degrees have been successfully grafted onto carbon nanotubes. Moreover, it can also be seen from Fig. 1b that the intensity of the absorption peak at 1729.9 cm−1 representing the stretching vibration of carbonyl decreases obviously after grafting. This is because when carbonyl exists in the form of carboxylic acid, the absorption peaks are generally stronger due to hydrogen bonding. When carboxyl groups on carbon nanotubes surface are esterified with hydroxyl-terminated hyperbranched polyesters, the carbonyl absorption peaks will be significantly decreased.
Since the residual hyperbranched polyesters of each group of carbon nanotubes have been washed away by acetone before the infrared spectroscopy test, the above results suggest that the grafting reaction of hyperbranched polyesters of different branched degrees with carboxylated carbon nanotubes has occured, and the reaction principle is the esterification reaction between carboxyl groups on the surface of carbon nanotubes and hydroxyl groups of different hyperbranched polyesters.
Fig. 3 XPS survey spectra of (a) MWCNTs-H201, (b) MWCNTs-H202, (c) MWCNTs-H203, (d) MWCNTs-H204, (e) MWCNTs-COOH. |
As can be seen from Fig. 3, the C1s and O1s peaks of all carbon nanotube samples are shown by X-ray photoelectron spectroscopy. For the original carboxylated carbon nanotubes, the weak O1s peaks are mainly attributed to the oxygen atoms contained in the carboxyl groups on the surface of carbon nanotubes. For hyperbranched polyester modified carbon nanotubes with different branching degrees, the O1s peak increased significantly, and along with the increase of branching degree in the molecular structure of hyperbranched polyester, the intensity of O1s peak increased, proving that hyperbranched polyesters with different branching degrees did exist on the surface of carbon nanotubes.
Furthermore, the C1s and O1s fine spectral peaks of each group of samples were analyzed. It can be seen from the fine spectrum of O1s peaks (as shown in Fig. 4b). Compared with unmodified carboxylated carbon nanotubes, the intensity of O1s peaks of different hyperbranched polyester modified carbon nanotubes increased significantly. The order of strength is MWCNTs-H204 > MWCNTs-H203 > MWCNTs-H202 > MWCNTs-H201 > MWCNTs-COOH. This is because the higher the degree of branching of hyperbranched polyester increases, the more hydroxyl end groups are introduced into carbon nanotubes, which gradually enhances its O1s peak strength.
At the same time, it can be seen from the fine spectrum of C1s peak (as shown in Fig. 4a) that the strength order of C1s peak is opposite to that of O1s peak. This phenomenon may be due to a series of chemical treatments in the process of surface hyperbranching of carbon nanotubes. Semi-quantitative X-ray photoelectron spectroscopy analysis of surface elements for each group of samples is shown in Table 1. From Table 1, it can be seen that the changes of atomic percentage of C and O on the surface of hyperbranched polyester modified carbon nanotubes and carboxylated carbon nanotubes with different branching degrees are consistent with the results of qualitative discussion.
Samples | C1s (%) | O1s (%) | nO/nC |
---|---|---|---|
MWCNTs-H201 | 25.06 | 74.94 | 0.33 |
MWCNTs-H202 | 33.10 | 66.90 | 0.49 |
MWCNTs-H203 | 34.19 | 65.81 | 0.52 |
MWCNTs-H204 | 39.66 | 60.34 | 0.66 |
MWCNTs-COOH | 10.80 | 89.20 | 0.12 |
To further explore the effect of surface modification of hyperbranched polyester on carbon nanotubes, the C1s peaks were separated according to the binding energy of different valence states of each element, as shown in Fig. 5. For the original carboxylated carbon nanotubes (Fig. 5e), the C1s peak can be decomposed into three single peaks, in which the binding energy 284.6 eV is the main peak formed by sp2 hybrid C atom in the coiled graphite layer of carboxylated carbon nanotubes, and the binding energy 285.6 eV is the characteristic peak formed by a small number of structural defects in the preparation process of carboxylated carbon nanotubes. The energy 289.0 eV was the characteristic peak of C atom in –COOH on the surface of carboxylated carbon nanotubes. The hyperbranched polyester modified carbon nanotubes with different branching degrees showed that a new single peak appeared at the binding energy 286.8 eV of the four groups of samples, which represented the characteristic peak of C atom contained in the terminal hydroxyl C–OH in the molecular structure of hyperbranched polyester.
Fig. 5 The C1s peak separation of (a) MWCNTs-H201, (b) MWCNTs-H202, (c) MWCNTs-H203, (d) MWCNTs-H204, (e) MWCNTs-COOH. |
In conclusion, it is strongly proved that hydroxyl-terminated hyperbranched polyesters with different branching degrees are grafted onto the surface of carbon nanotubes in the form of covalent bonds rather than simple adsorption.
The TGA curves of different degrees of hyperbranched polyester modified carbon nanotubes are plotted in Fig. 7.
For MWCNTs-COOH, there was no obvious mass loss in the temperature range of 30–800 °C. A small amount of mass loss was due to the carboxyl functional groups on the surface of carbon nanotubes and a small amount of impurities. However, when the temperature of MWCNTs-COOH grafted with four different hyperbranched polyesters was increased to 300 °C, all TGA curves showed obvious inflection points and the decomposition rate increased significantly, respectively.
During the preparation of samples, the reaction products were washed repeatedly by acetone, and the unreacted residual hyperbranched polyesters on the surface of carbon nanotubes were removed as far as possible. Therefore, it can be inferred that the rapid decline of TGA curves of each group of samples was due to the grafting of carbon nanotubes. The rapid decomposition of hyperbranched polyesters in this temperature range also proved that hyperbranched polyesters with different branching degrees had been successfully grafted onto carbon nanotubes.
Since the TGA curve directly reflects the grafting amount of hyperbranched polyesters on the surface of carbon nanotubes, the four different hyperbranched polyesters begin to decompose at about 300 °C, and almost completely decompose at about 600 °C. Therefore, the grafting amount of hyperbranched polyesters with different branching degrees on carbon nanotubes can be calculated by the following formula.
Fwt = ΔMH − ΔMCOOH | (1) |
Among the formula, Fwt is the grafting amount of hyperbranched polyester onto carbon nanotubes, ΔMH is the weight loss percentage of hyperbranched polyester modified carbon nanotubes at 600 °C, and ΔMCOOH is the weight loss percentage of carboxylated carbon nanotubes at 600 °C.
As shown in Table 2, the grafting content of hyperbranched polyesters with different branching degrees on carbon nanotubes was calculated, respectively.
Samples | Fwt |
---|---|
MWCNTs-H201 | 5.90% |
MWCNTs-H202 | 6.05% |
MWCNTs-H203 | 17.40% |
MWCNTs-H204 | 18.10% |
Fig. 8 shows the DMA patterns of the storage modulus to temperature of different epoxy/carbon nanotube composites. It can be seen from the figures that the storage modulus of the composites is obviously improved by adding MWCNTs-COOH without hyperbranched polymer modification compared with pure epoxy resin. This is because MWCNTs-COOH are rigid inorganic carbon nanomaterials with high aspect ratio, high strength and stiffness, and MWCNTs-COOH play a role of physical crosslinking point in epoxy resin, which reduces the mobility of molecular chains, so the storage modulus of epoxy resin filled with carbon nanotubes is greatly increased. However, after modification with hyperbranched polyester, the storage modulus of epoxy composites decrease obviously, and with the increase of the branching degree of hyperbranched polyester, the storage modulus decrease more obviously. The possible reason for this phenomenon is that there are a large number of molecular branched chains in the molecular structure of hyperbranched polyester which distribute in the resin matrix. For the reason that the hyperbranched structure of internal molecular chains does not cross-link, the uncrossed hyperbranched structure acts as a “flexible segment” in the matrix and becomes a part of the epoxy resin cross-linking network,39 which providing greater mobility for the low-level kinematic units of epoxy resin molecules smaller than chain segments. Thus the storage modulus of epoxy composites decreases, as the higher the branching degree increased, the higher the content of the “flexible segment” and the more obvious the reduction of the storage modulus were.
Fig. 9 shows the DMA spectrum of mechanical loss of epoxy resin/carbon nanotube composites. It can be seen from the diagram that all the tested samples are homogeneous systems with only one glass transition temperature (Tg). Compared with pure epoxy resin, the glass transition temperature of MWCNTs-COOH without hyperbranched polymer modification increases significantly after adding epoxy resin matrix. However, after the modification of MWCNTs-COOH with hyperbranched polymers, the Tg of the resin matrix decreases significantly, and with the increase of branching degree, the Tg decreases more obviously, but when the branching degree increases to a certain extent, the Tg value does not change. It is noteworthy that after grafting modification of carbon nanotubes with hyperbranched polymers, the loss peak height also shows a significant downward trend with the increase of branching degree of hyperbranched polymers. This is due to the good compatibility and chemical bonding force between hyperbranched polymers and epoxy resin matrix,39 which increases the interfacial bonding between carbon nanotubes and matrix. And with the increase of branching degree, the stronger the interfacial bonding, the more uniformly dispersed MWCNTs-COOH hinder the movement of polymer chains, so the loss peak height is reduced.
Samples | Tensile strength (MPa) | Elongation at break (%) | Charpy impact strength (kJ m−2) | Barcol hardness |
---|---|---|---|---|
EP | 28.9 | 16.5 | 4.76 | 41.2 |
EP/MWCNTs-COOH | 35.2 | 12.8 | 10.2 | 48.2 |
EP/MWCNTs-H201 | 34.3 | 15.9 | 12.17 | 46.1 |
EP/MWCNTs-H202 | 35.1 | 20.2 | 13.24 | 42.9 |
EP/MWCNTs-H203 | 36.9 | 24.7 | 19.94 | 40.8 |
EP/MWCNTs-H204 | 35.8 | 31.3 | 21.07 | 39.7 |
The tensile strength is the stress at which a material breaks or permanently deforms. As an intensive property, it does not depend on the size of the test specimen. In addition, Charpy impact strength is a standardized high strain rate test that determines the amount of energy absorbed by a sample during fracture. The absorbed energy is a measure of a given material's toughness. Barcol hardness is used to determine the hardness of both reinforced and non-reinforced rigid plastics. The specimen is placed under the indentor of the Barcol hardness tester and uniform pressure is applied to the specimen until the dial indication reaches a maximum. The depth of the penetration is converted into absolute Barcol numbers.
From Table 3 and Fig. 10 it can be seen that the tensile strength and elongation at break of pure EP are 28.9 MPa and 16.5% respectively. After adding MWCNTs-COOH, the tensile strength increases to 35.2 MPa and the elongation at break decreases to 12.8%. Moreover, after the addition of various hyperbranched polyester grafting carbon nanotubes, the tensile strength have little change compared with MWCNTs-COOH/EP, indicating that the branching degree of hyperbranched polyester has little effect on the tensile strength of EP composites. However, the elongation at break increase obviously.
On the other hand, the Charpy impact strength of MWCNTs-COOH/EP (10.2 kJ m−2) was about 114.3% higher than that of neat EP (4.76 kJ m−2), while that of various hyperbranched polyester grafting carbon nanotubes and EP composites was further improved. And with the increase of branching degree of hyperbranched polyester, the Charpy impact strength was increased obviously. The Barcol hardness of MWCNTs-COOH/EP (48.2) was about 17% higher than that of neat EP (41.2), but compared with MWCNTs-COOH/EP, after the addition of various hyperbranched polyester grafting carbon nanotubes, the Barcol hardness of EP composites decreased significantly, and the higher the branching degree increased, the more obvious the decline of Barcol hardness was.
The above results indicate that the addition of MWCNTs-COOH enhances the toughness of EP, and the further surface grafting of hyperbranched polyester onto MWCNTs-COOH can enhance the toughness of the composites to a larger extent. Two possible mechanisms are proposed: first, a large amount of –OH in hyperbranched polyester might form hydrogen bond with EP, which improved the interfacial bonding between epoxy resin and carbon nanotubes. And the higher the branching degree of hyperbranched polyester, the stronger the interfacial bonding. Second, the surface grafting enhances the dispersion of carbon nanotubes in the EP matrix.
From Fig. 11, it can be seen that the dispersion of carboxylated carbon nanotubes in epoxy resin matrix is not uniform, and there is a large area of reunion. Compared with MWCNTs-COOH, the area of reunion of MWCNTs-H201 and MWCNTs-H202 decreases and the dispersion improves. As shown in Fig. 11e–h, with the further increase of the degree of branching of hyperbranched polyesters, the samples of MWCNTs-H203/EP and MWCNTs-H204/EP composites did not find the aggregates of carbon nanotubes, which could basically be considered as nano-scale dispersion.
On the other hand, as shown in Fig. 11a and b, the impact section of pure epoxy resin is smooth, the phase state is uniform, the fracture stripes are straight and layered, and the orientation is orderly, showing typical brittle fracture characteristics. As shown in Fig. 11c and d, after adding 0.3% mass ratio of MWCNTs-COOH, the fracture surface becomes rough relatively, and the cracks are still linear and partially uniform and orderly. Although there are a few active groups on the surface of MWCNTs-COOH, the bonding energy between MWCNTs-COOH and epoxy resin is weak. When the resin matrix breaks, the carbon nanotubes do not exert too much force on the matrix, resulting in a large number of long strip-like ridges on the fracture surface, indicating that the carbon nanotubes are basically pulled out of the resin matrix.40,41 However, with the modification of carbon nanotubes by hyperbranched polyester, the long strip-shaped convex edges on the fracture surface are obviously reduced, as shown in Fig. 11e–l, and with the increase of branching degree, the pull-out phenomenon of carbon nanotubes is less. The surface of MWCNTs-H203 and MWCNTs-H204 are mostly coated with resin matrix materials (Fig. 11i–l), and the exposed part of carbon nanotubes is basically snap rather than pulled out, which indicates that carbon nanotubes and resin matrix form a very strong interface connection, and the higher the branching degree of hyperbranched polymer increases, the stronger the interfacial bonding is. Therefore, when the sample is impacted, the load acting on the resin matrix is transferred to the carbon nanotubes through the interface, which plays a role of bearing load and consuming fracture energy, and prevents the propagation of matrix cracks, greatly improving the strength and toughness of epoxy resin composites.
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