Lu Gan,
Songmin Shang*,
Chun Wah Marcus Yuen and
Shou-xiang Jiang
Institute of Textiles and Clothing, The Hong Kong Polytechnic University, Hong Kong. E-mail: shang.songmin@polyu.edu.hk; Fax: +852 2773 1432; Tel: +852 3400 3085
First published on 19th January 2015
Chemically functionalized graphene has been synthesized by covalently grafting D-glucose on graphene for the first time through an esterification reaction. The D-glucose functionalized graphene was further applied in the preparation of poly(vinyl alcohol) and poly(methyl methacrylate) nanocomposites. The thermal and mechanical properties of the prepared nanocomposites were then investigated. It was demonstrated that the D-glucose was grafted on the surface of the graphene through a covalent attachment. The chemically functionalized graphene had better dispersibility in both water and dimethylformamide than the pristine graphene. The better dispersion of the functionalized graphene in both aqueous and organic solvents simplified the preparation of the polymer nanocomposites. It was found that the D-glucose grafted graphene dispersed homogeneously in both poly(vinyl alcohol) and poly(methyl methacrylate) matrices, increasing the thermal and mechanical properties of the polymers at the same time. The phenomena were ascribed to the introduction of the D-glucose, which induced strong hydrogen bonding interactions between the functionalized graphene and the polymers. The results of this study indicate that this is an effective approach for preparing well-dispersed graphene-based polymer nanocomposites by covalently attaching functional molecules on the surface of graphene.
For this reason, researchers are exploring the possibility of chemical functionalization of graphene. As a significant precursor and derivative of graphene, graphene oxide (GO) tends to be more compatible with some solvents13 and polymers14 because GO consists of many oxygen containing groups compared with graphene.15 These groups further facilitate the chemical modifications on the GO. Through simple organic reactions, the GO is able to covalently bind with some small molecules16 or polymers,17,18 and these chemically functionalized graphene (CFG) molecules are more dispersible in aqueous19 and organic20 solvents, and polymer matrixes.21 Moreover, the CFGs are more easily incorporated into the polymer without losing the inherent properties of the CFGs and the prepared nanocomposites.22 Recently, considerable interest has arisen towards synthesizing solvent dispersible or soluble CFGs.23,24 Long time stable CFG dispersions simplify the fabrication of the polymer composites through solvent mixing approaches.
As a most common and simple monosaccharide, D-glucose has been widely used in biology, pharmacy and clinically related areas for centuries.25 It is also the basic nutrient for almost all organisms. More significantly, D-glucose has numerous hydroxyl and aldehyde groups along its backbone and is soluble in water and many organic solvents such as dimethylformamide (DMF) and pyridine. If D-glucose could be covalently grafted on the graphene,26 the D-glucose grafted CFG is expected to have better dispersion in both aqueous and organic solvents, which is very important for preparing polymer nanocomposites. Compared with those CFGs, which can only be dispersed in either aqueous or organic solvents, the D-glucose grafted CFG has wider application potential for more polymer matrices. Moreover, this D-glucose grafted CFG is expected to have stronger interactions with the polymers, especially those with oxygen containing groups, such as poly(vinyl alcohol) (PVA) and poly(methyl methacrylate) (PMMA), because the existence of the D-glucose will facilitate the hydrogen bonding interactions between the CFG and the polymers.
Herein, we report for the first time, the attachment of graphene and D-glucose through covalent grafting. The D-glucose grafted graphene, named Glu-G, was further incorporated into PVA and PMMA to prepare their nanocomposites. Fourier transform infrared (FTIR) spectroscopy, thermogravimetric analysis (TGA), Raman spectroscopy and X-ray diffraction (XRD) were used to confirm the structure of the Glu-G. The dispersions of the Glu-G in water and DMF were also investigated. To study the reinforcing effect of Glu-G to polymers and the interaction between the fillers and the matrices, PVA/Glu-G and PMMA/Glu-G nanocomposites were characterized by morphological, mechanical and thermal properties.
000–85
000, ∼87–89% alcoholized) was purchased from Accuchem (Canada). PMMA (mass density 1.19 g cm3, hardness ∼ 148 N mm−2) was purchased from International Laboratory (America). D-glucose was purchased from Unichem (China). All the other agents and solvents were of analytical grade and used as received. Deionized distilled water (DDW) was used exclusively in this study.
O stretching vibration) appeared and the intensity of the original peak at 1705 cm−1 became weaker, indicating that some carboxylic acid groups present in the GO had been converted to the ester groups. After the Glu-GO was reduced to Glu-G, the peak at 1705 cm−1 disappeared and that at ∼1100 cm−1 (C–O–C stretching vibration) became weaker, indicating the unreacted –COOH groups and the epoxy groups were eliminated by the hydrazine (see Fig. 1). Besides, the intensity of the two peaks at around 2900 cm−1 (–CH– stretching vibration) increased significantly, indicating that the resulting product contained more CH groups (on the glucose backbone). The peak intensity at around 3100–3500 cm−1 (–OH stretching vibration) was still relatively strong, indicating that the grafted D-glucose was not considerably affected by hydrazine.
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| Fig. 2 (a) FTIR spectra; (b) TGA curves (under nitrogen); (c) Raman spectra and (d) XRD patterns of GO, Glu-GO and Glu-G. | ||
TGA carried out in a nitrogen atmosphere was then used to investigate the grafting rate of Glu-G, as shown in Fig. 2(b). It can be seen from the curves that the percentage weight loss was about 40% for GO and 52% for Glu-GO at 600 °C. Based on this result, it was calculated that there was about 23 wt% of glucose and 77 wt% of GO in the Glu-GO. After the Glu-GO was reduced to the Glu-G, the weight loss percentage of the Glu-G at 600 °C was about 25%. Because the oxygen containing groups had been eliminated through the reducing process,28 the weight loss of the Glu-G was mainly due to the loss of D-glucose. Because the weight content of the D-glucose obtained from the results of Glu-GO and Glu-G were similar, it was confirmed that D-glucose was grafted on the graphene and the grafting rate was ∼20%.
It is well-known that the oxidation of graphite partially destroys its sp2 structure. Thus, Raman spectroscopy was conducted to detect the structure deformation and Fig. 2(c) presents the Raman spectra of the GO, the Glu-GO and the Glu-G. It can be observed that all three materials had two characteristic peaks at around 1350 cm−1 and 1580 cm−1, which were generally named as the D band and G band, respectively. The D band indicates the carbons with sp3 hybridization, while the G band represents sp2 hybridized carbons. The intensity ratio of these two bands (ID/IG) is often introduced to speculate the degree of the structure defect. From Fig. 2(c), ID/IG for GO was calculated to be about 0.86. After the D-glucose was covalently attached to the GO, the G band red shifted to 1572 cm−1 and the ID/IG for the Glu-GO was lower (0.80) compared to that of the GO. The sp2 domains increased during the reaction process, resulting in the decrease of the ID/IG ratio. When Glu-GO converted to Glu-G after the reduction process, an increase of ID/IG (1.09) was observed, indicating that the reduction decreased the topological disorder of the graphene due to the removal of the oxygen groups.29 The peaks at around 2700 cm−1 are known as the 2D band of the carbon materials. It was also observed from Fig. 2(c) that although the peak position of the Glu-G at the 2D band shifted a little, the peak intensity of the Glu-G was almost the same as the GO, indicating that Glu-G could also be exfoliated to a few layers in the solvents.
Fig. 2(d) shows the XRD patterns of graphite, GO, Glu-GO and Glu-G. It can be seen that the graphene had a characteristic peak at ∼26° (002) with a d spacing of 0.34 nm.30 After oxidation, GO had a characteristic peak at ∼11° (001) with a much larger d spacing of 0.81 nm due to the existence of the oxygen groups. After D-glucose was grafted on the GO, the peak of the Glu-GO shifted to a lower value, indicating that the introduction of the D-glucose gave rise to the interlayer spacing of the graphene sheet. The Glu-G had a broad peak at ∼24° (002), which implied that the covalent attachment of the D-glucose did not destroy the crystalline structure of the graphene.
Fig. 3(a) and (b) show the TEM images of the Glu-G. It can be observed that the Glu-G was able to be exfoliated to very few layers. The selected area electron diffraction (SAED) pattern of the Glu-G showed well-defined diffraction spots, indicating a crystalline structure of the reduced Glu-G. Fig. 3(c) presents the UV absorption spectra of GO and Glu-G in water (with the concentration of 0.05 mg mL−1). It is well known that the absorption peak λmax represents the π conjugation of the investigated material. Compared with that of GO (∼220 nm), the λmax of Glu-G (∼280 nm) red-shifted to a higher value, indicating that the conjugation system of the Glu-G was restored after the reduction process.31
The introduction of the D-glucose on the surface of the graphene also affects the dispersibility of the functionalized graphene. Because the D-glucose contains a number of oxygen containing groups along its backbone, Glu-G has a much better dispersibility than GO in both aqueous and organic solvents. As shown in Fig. 3(d), Glu-G was able to be dispersed in water and DMF homogeneously without aggregation for more than 2 months. The UV-vis spectra of the Glu-G in water and DMF are shown in Fig. 3(e) and (f). From the inset figures, it can be seen that the Glu-G solution in both water and DMF obeys Beer's law. Following Beer's law, the extinction coefficient for the Glu-G in water was 36.4 mL mg−1 cm−1, with a maximal solubility of 0.58 mg mL−1, and the extinction coefficient for Glu-G in DMF was 42.2 mL mg−1 cm−1, with a maximal solubility of 0.61 mg mL−1. The good dispersion of Glu-G in both aqueous and organic solvents facilitates the fabrication of the Glu-G based nanocomposites for both aqueous soluble and organic soluble polymers.
The surface morphologies of GO and Glu-G were then investigated by AFM, as shown in Fig. 4. As can be seen from the height profile, GO had an average thickness of ∼1.0 nm, which was in accordance with the previous studies.32 Moreover, Glu-G sheet had an average thickness of ∼3.2 nm, which is much thicker than that of GO. This result was mainly ascribed to the introduction of the D-glucose on both sides of the graphene sheets.
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| Fig. 5 SEM images of the fractured surface of (a) PVA/Glu-G and (b) PMMA/Glu-G nanocomposites; (c) XRD patterns and (d) FTIR spectra of PVA, PMMA and their nanocomposites. | ||
To further investigate the structures of the nanocomposites, XRD analysis was conducted and the results are shown in Fig. 5(c). It was observed that pure PVA showed characteristic peaks at ∼20°, which corresponded to the crystalline phase of the PVA. The PMMA had two very broad peaks at ∼14.5° and ∼30°, revealing its amorphous structure.33 After Glu-G was incorporated, the peaks of the resulting nanocomposites were almost the same as the pristine polymers, suggesting that Glu-G sheets were fully exfoliated and well dispersed without any change the structure of the polymer matrices.
It was believed that strong interactions between the Glu-G and the polymers resulted in a uniform dispersion of the Glu-G, and the interactions were confirmed by the FTIR spectra, as shown in Fig. 5(d). Taking PVA and PVA/Glu-G as an example, it was seen that pure PVA had a wide band at ∼3455 cm−1, which was attributed to the stretching vibration of O–H bond. When Glu-G was incorporated in PVA, the peak became broader and shifted to a lower wavenumber at ∼3447 cm−1. This was due to the strong interactions between Glu-G and PVA. Because D-glucose has a number of oxygen containing groups, such as formyl and hydroxyl groups, Glu-G was able to form interactions through hydrogen bonding with –OH groups along the PVA chains, resulting in the shift of –OH in FTIR spectra. Analogously, Glu-G also formed hydrogen bonds with PMMA due to the existence of methyl ester groups within the PMMA backbone. It could be seen from the spectra that the intensity at ∼1728 cm−1 (C
O stretching vibration) in PMMA/Glu-G nanocomposite increased compared to that of the pristine PMMA, which might have resulted from the interactions between the –OH groups in the Glu-G and the COOCH3 groups in the PMMA. The schematic illustration of the interactions between the filler and the matrices are shown in Fig. 6. Unlike pristine graphene, because Glu-G contains D-glucose within its body, Glu-G is more dispersible in both solvents and polymers than the pristine graphene without the introduction of foreign compatibilizers. It is thus expected that the synthesized Glu-G will be good reinforcing filler for polymers with oxygen-containing and nitrogen-containing groups such as polyurethane (PU) and resin.
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| Fig. 7 DSC curves of (a) PVA, PVA/Glu-G nanocomposite, and (b) PMMA and PMMA/Glu-G nanocomposite; and TGA curves of (c) PVA, PVA/Glu-G nanocomposite, and (d) PMMA and PMMA/Glu-G nanocomposite. | ||
It is well-known that the mechanical properties of a polymer could be influenced tremendously by the nanofillers incorporated into its matrix.36,37 Therefore, a typical stress–strain test was conducted, with the results shown in Fig. 8(a) and (b) and Table 1. It was clearly observed that the incorporation of the Glu-G notably improved the mechanical strength of the PVA and PMMA. Although the elongation of the nanocomposites decreased slightly, the Young's modulus and the tensile stress of both the PVA and PMMA nanocomposites improved significantly compared to those of the pristine polymers (Table 1). The incorporation of the Glu-G decreased the crystallinity of the polymers. The decrease in polymer crystallinity made the prepared nanocomposites tougher and easier to be broken down, which caused a slight decrease in the elongation of the nanocomposites. However, the strong hydrogen bonding interactions between the Glu-G and the polymers facilitated an effective load transfer from the polymer matrices to the filler when the nanocomposites were under stretching force, resulting in the improvement in the Young's modulus and the tensile stress.
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| Fig. 8 Stress–strain curves of (a) PVA, PVA/Glu-G nanocomposite, and (b) PMMA and PMMA/Glu-G nanocomposite. | ||
| Samples | Tensile stress (MPa) | Tensile strain (%) | Modulus (MPa) |
|---|---|---|---|
| PVA | 18.4 | 71.7 | 526 |
| PVA/Glu-G 1.0 wt% | 25.1 | 70.3 | 808 |
| PMMA | 43.1 | 4.6 | 14.9 |
| PVA/Glu-G 1.0 wt% | 46.6 | 3.5 | 21.2 |
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