Jiang Guoa,
Jun Longbc,
Daowei Dingb,
Qiang Wangd,
Yu Shane,
Ahmad Umarf,
Xin Zhangg,
Brandon L. Weeksg,
Suying Wei*b and
Zhanhu Guo*a
aIntegrated Composites Lab (ICL), Department of Chemical and Biomolecular Engineering, University of Tennessee, Knoxville, TN37996, USA. E-mail: zguo10@utk.edu
bDepartment of Chemistry and Biochemistry, Lamar University, Beaumont, TX 77710, USA. E-mail: suying.wei@lamar.edu
cSchool of Chemical Engineering and Technology, Harbin Institute of Technology, Harbin, Heilongjiang 150001, China
dEnvironmental Functional Nanomaterials (EFN) Laboratory, College of Environmental Science and Engineering, Beijing Forestry University, Beijing 100083, P. R. China
ePhysical Education Department, South China Agriculture University, Guangzhou 510642, P. R. China
fDepartment of Chemistry, Faculty of Science and Arts and Promising Centre for Sensors and Electronic Devices (PCSED), Najran University, P. O. Box: 1988, Najran 11001, Kingdom of Saudi Arabia
gDepartment of Chemical Engineering, Texas Tech University, Lubbock, TX 79409, USA
First published on 12th February 2016
The polyaniline (PANI)/epoxy nanocomposites with enhanced mechanical and electrical properties were prepared by three different techniques. Fourier transform infrared (FT-IR) spectroscopy and scanning electron microscopy (SEM) were used to study the chemical structure and surface morphology of the PANI nanoparticles, which were synthesized by the oxidation polymerization method. The effects of PANI loading and preparation method on the mechanical and electrical properties of PANI/epoxy nanocomposites were comparatively studied. The SEM images of the PANI/epoxy nanocomposites after doing the tensile test were used to study the dispersion of PANI nanoparticles in the epoxy matrix. The tensile strength of 5.0 wt% PANI/epoxy nanocomposites (107.27 MPa) was much higher than that of our previous PANI/epoxy nanocomposites (about 60.0 MPa) with the same PANI loading. The volume resistivity of the PANI/epoxy nanocomposites was also decreased compared to the reported literature. The toughness and Young's modulus of the PANI/epoxy nanocomposites were also studied and presented in this paper.
Conductive polymers have attracted great attention due to their low cost, easy synthesis, flexibility, high capacitance and good environmental stability.12 Among all the conductive polymers, polyaniline (PANI) is one of the most studied one because of its high conductivity, good stability, low cost, light weight, easy doping and de-doping, etc.5,13 PANI could be applied in different fields including supercapacitors, environmental remediation and coupling agent between epoxy and nanofillers.13,14 In our previous work, the chemical bonding between PANI and epoxy has been formed and improved the mechanical property. After adding the PANI nanoparticles, the electrical conductivity of epoxy was increased without reducing other properties.5,15 The dispersion quality of the nanoparticles in the epoxy matrix is a great challenge for enhancing the properties of the epoxy nanocomposites.5 In order to reach high quality dispersion, the nanofillers were mixed with epon resin under stirring, and the curing agent was added into the mixture for curing the epoxy nanocomposites. However, the fabrication procedure effect on the properties of cured epoxy nanocomposites has not been reported.
In this work, the PANI nanoparticles synthesized with an oxidation polymerization method were used as nanofillers to prepare epoxy nanocomposites with three different methods. The Fourier transform infrared spectroscopy (FT-IR), X-ray diffraction (XRD), and scanning electron microscope (SEM) were used to characterize the chemical structure, crystallization, and morphology of the synthesized PANI nanoparticles. The effects of fabrication procedure and PANI loading on the mechanical property and electrical conductivity were studied. To study the dispersion of PANI nanoparticles in the epoxy matrix, the fracture surface of the PANI/epoxy nanocomposites after doing the tensile test was studied by the SEM images as well.
:
APS
:
PTSA = 6
:
3
:
5. For solution 1, PTSA (30 mmol) and APS (18 mmol) were dissolved in deionized water (200 mL) in a beaker, which was treated by sonication (Branson 8510) in the ice water bath for 1 hour mechanical stirring (SCILO-GEX OS20-Pro LCD Digital Overhead Stirrer 300 rpm). Solution 2 was aniline (36 mmol) dissolved in deionized water (50 mL). Solution 2 was then added into solution 1, and the mixture was sonicated for an additional 1.5 hour mechanical stirring (300 rpm) in the ice water bath for polymerization of aniline. Finally, the product was vacuum filtered and washed with deionized water and massive acetone for 3 times.
:
hexahydro-4-methylphthalic anhydride
:
2-ethyl-4-methylimidazole = 25 g
:
19.75 g
:
0.25 g. The PANI/epoxy nanocomposites with 1.0 and 5.0 wt% PANI nanoparticles were synthesized by this method. The samples were named as 1.0 wt% PANI/epoxy-1 and 5.0 wt% PANI/epoxy-1, respectively.
C stretching vibration of the quinoid and benzenoid rings of the PANI polymer backbone, respectively.16 The peak at 1285 cm−1 is due to the C–N stretching vibration of the benzenoid unit, and the peak at around 1232 cm−1 is assigned to the C–H stretching vibration of the quinoid rings.17 The peak at 789 cm−1 corresponds to the out-of-plane bending of C–H in the substituted benzenoid ring. These prove that the PANI nanoparticles are the emeraldine salt form.12 The two broad diffraction peaks at 2θ = 20.1 and 25.3°, Fig. 1(b), correspond to the (100) and (110) crystallographic plane of the partially crystalline PANI nanoparticles.17 Fig. 1(c) shows the SEM image of the PANI nanoparticles. The PANI nanoparticles have a rough surface with an average diameter of 110 nm measured by the nano measurer software. All the results indicate that the PANI nanoparticles have been successfully synthesized.
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| Fig. 1 (a) FT-IR spectrum, (b) XRD pattern and (c) SEM microstructures of the synthesized PANI nanoparticles. | ||
Fig. 2 shows the curve of tensile stress as a function of tensile strain for the cured pure epoxy and PANI/epoxy nanocomposites with different fabrication methods. The tensile strength of cured pure epoxy is 80.87 MPa, a little lower than that of pure epoxy with curing agent Epicure W.2 The PANI/epoxy nanocomposites with a PANI loading of 5.0 wt% show an enhanced tensile strength compared with that of cured pure epoxy, which is due to the covalent bondings formed between PANI nanoparticles and epoxy matrix.15,18 And the PANI/epoxy-3 nanocomposites show much higher tensile strength (107.27 MPa) than PANI/epoxy-2 (96.35 MPa) and PANI/epoxy-1 (88.81 MPa).
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| Fig. 2 Stress–strain curves of cured pure epoxy, 5.0 wt% PANI/epoxy-1, 5.0 wt% PANI/epoxy-2, 5.0 wt% PANI/epoxy-3, and 8.0 wt% PANI/epoxy-3, respectively. | ||
However, the tensile strength of 8.0 wt% PANI/epoxy-3 nanocomposites was decreased to 62.93 MPa, which is induced by the agglomeration of the PANI nanoparticles.5 The Young's modulus is the slope of the stress–strain curve at elastic portion. And the toughness can be determined by integrating the stress–strain curve. The Young's modules and toughness of pure epoxy and PANI/epoxy nanocomposites are summarized in Table 1. Adding the PANI nanoparticles into the epoxy matrix would reduce the toughness of epoxy but enhance the Young's modulus of the epoxy. These results indicate that the stiffness is improved by sacrificing the toughness, which is consistent with the results in magnetic epoxy nanocomposites and layered silicates/epoxy nanocomposites.19,20
| Toughness (J m−3 104) | Young's modulus (GPa) | |
|---|---|---|
| Pure epoxy | 406.0 | 1.6 |
| 5.0 wt% PANI/epoxy-1 | 395.0 | 2.2 |
| 5.0 wt% PANI/epoxy-2 | 387.0 | 2.3 |
| 5.0 wt% PANI/epoxy-3 | 331.0 | 3.1 |
| 8.0 wt% PANI/epoxy-3 | 83.0 | 2.6 |
Fig. 3 shows the SEM images of the fracture surface of the cured pure epoxy and PANI/epoxy nanocomposites with different synthesized methods and PANI loadings. A relatively smooth fracture surface with “river-like” patterns is observed in the SEM images of pure epoxy, Fig. 3(a), indicating a brittle failure because of the rapid crack propagation.21 Adding the PANI nanoparticles into the epoxy matrix, the fracture surface of the PANI/epoxy nanocomposites becomes much rougher, Fig. 3(b–e). However, compared with 5.0 wt% PANI/epoxy-1 and 5.0 wt% PANI/epoxy-2 nanocomposites, Fig. 3(b and c), the fracture surface of 5.0 wt% PANI/epoxy-3 nanocomposites is relatively smoother, indicating that the PANI nanoparticles have a good dispersion in the epoxy matrix, Fig. 3(d). Due to the good nanoparticle dispersion in the epoxy matrix and the covalent bondings formed between PANI nanoparticles and epoxy matrix,18 the tensile strength (107.27 MPa) of 5.0 wt% PANI/epoxy-3 nanocomposites is much higher than previously reported PANI/epoxy nanocomposites (about 60.0 MPa) at the same PANI loading.5 The agglomeration of the PANI nanoparticles is observed in the fracture surface of 8.0 wt% PANI/epoxy-3 nanocomposites, Fig. 3(e), and leads to a decreased tensile strength (62.93 MPa). However, the 8.0 wt% PANI/epoxy-3 nanocomposites still show higher tensile strength (62.93 MPa) than previously reported PANI nanocomposites with 10.0 wt% PANI loading (about 55 MPa).5
Fig. 4 depicts the volume resistivity of the cured pure epoxy and its PANI nanocomposites with different fabrication methods. The volume resistivity of cured pure epoxy is about 1.1629 × 1016 Ω cm. The volume resistivity is decreased by adding the conductive PANI nanoparticles into the epoxy matrix. When the PANI loading is 5.0 wt%, the volume resistivity of the nanocomposites is decreased to 2.06785 × 1012 Ω cm for PANI/epoxy-1 nanocomposites, 2.3913 × 1012 Ω cm for PANI/epoxy-2 nanocomposites. However, for the 5.0 wt% PANI/epoxy-3 nanocomposites, the volume resistivity is decreased to 3.0928 × 1011 Ω cm, indicating that the PANI nanoparticles are well dispersed in the epoxy matrix, which is consistent with the SEM observation of the fracture surface of PANI/epoxy nanocomposites. When increasing the PANI loading to 8.0 wt%, the volume resistivity of the PANI/epoxy-3 nanocomposites was decreased to 3.8017 × 1010 Ω cm, even lower than that of our previously reported PANI/epoxy nanocomposites with 10.0 wt% PANI nanoparticles (about 1.0 × 1011 Ω cm).5 Fig. 5 depicts the volume resistivity of PANI/epoxy-3 nanocomposites with different PANI nanoparticle loadings. When 1.0 and 2.0 wt% PANI nanoparticles were added into the epoxy matrix, the volume resistivity was decreased to 1.5576 × 1014, and 1.31943 × 1014 Ω cm for 1.0 wt% PANI/epoxy-3, and 2.0 wt% PANI/epoxy-3 nanocomposites, respectively. However, when the PANI loading was increased to 5.0 wt%, the volume resistivity of 5.0 wt% PANI/epoxy-3 nanocomposites was decreased significantly, almost 4 orders of magnitude lower than that of the cured pure epoxy (1.1629 × 1016 Ω cm). The variation of volume resistivity of the PANI/epoxy-3 nanocomposites with different loadings of PANI nanoparticles indicated the formation of percolated network. At lower PANI loading, the PANI nanoparticles rarely contact each other, which makes the electron hopping more difficult because of the large spacing between particles.22 When the particle loading was increased to higher percent, the percolation network was formed by nanoparticles in the epoxy matrix at a certain nanoparticle loading, making the electron hopping much easier between neighboring nanoparticles.23 Similar phenomenon is also observed the epoxy nanocomposites with iron-core–carbon-shell nanoparticles.4
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| Fig. 4 Volume resistivity of pure epoxy, 5.0 wt% PANI/epoxy-1, 5.0 wt% PANI/epoxy-2, 5.0 wt% PANI/epoxy-3, and 8.0 wt% PANI/epoxy-3, respectively. | ||
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| Fig. 5 Volume resistivity of pure epoxy, 1.0 wt% PANI/epoxy-3, 2.0 wt% PANI/epoxy-3, 5.0 wt% PANI/epoxy-3, and 8.0 wt% PANI/epoxy-3, respectively. | ||
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