Zhimei Weia,
Minle Penga,
Fang Qiua,
Xiaojun Wang*b,
Shengru longb and
Jie Yang*bc
aCollege of Polymer Science and Engineering, Sichuan University, Chengdu, 610065, China
bInstitute of Materials Science and Technology, Sichuan University, Chengdu, 610064, China. E-mail: ppsf@scu.edu.cn; wangxj@scu.edu.cn; Fax: +86-28-85412866; Tel: +86-28-85412866
cState Key Laboratory of Polymer Materials Engineering (Sichuan University), 610065, China
First published on 22nd April 2015
Conductive electrospun fibers have attracted widespread interest in the field of electromagnetics. However, the problem of how to effectively improve the electrical conduction of electrospun fibers has still not been adequately addressed. In this study, a new, simple and effective method was introduced to significantly improve the conductive properties of fibers. PES/PVA fibers with previous addition of 20 wt% PVA were chosen as a matrix due to the large parallel porous structure. The carbon nanotubes (CNTs) were first absorbed by the PES/PVA fibers, and then a thin polymer/CNTs composite layer was self-formed on the surface of the porous fibers by vapor treatment. Most importantly, a CNTs network structure was also formed in this vapor process, which easily gave the porous fibers a significant enhancement in conductivity with only a small amount of CNTs. Electrical conduction tests showed that the conduction of the fibers increased with increasing CNT content, and attained the maximum value when the amount of CNTs was around 7 wt%. The adsorption time and the DMSO vapor treatment time were optimized to obtain the best thin polymer/CNT composite layers. The surface microstructure of the composite layer was observed using scanning electron microscopy (SEM) and TGA. The results showed that this novel, powerful method could potentially be used to prepare novel types of conductive polymer fibers.
At present, the traditional way to make electrical conductive ultrafine fibers is by directly electrospinning electrical conductive polymers, e.g. polyacetylene,7 polypyrrole,8 and polyaniline.9 Fibers produced by this method have good conductivities and the preparation step is relatively simple. However, most known polymers are not electrical conductive polymers,10–12 so it is desirable to improve their electrical conductivity. However, this method is not appropriate for such types of polymer ultrafine fibers. Much research has been done on this topic. To date, two approaches were used to improve the electrical conductivity of electrospun non-electrical conductive polymer fibers. One was high temperature carbonization, which resulted in the formation of carbon atoms in the macromolecules' main chains, which significantly improved their electrical conductivity properties. The best example was the carbon nanofibers prepared by the carbonization of electrospun polyacrylonitrile (PAN) nanofibers.13–15 Fibers produced by this method had good conductivities but the cost of preparation was high and the preparation step was relatively complex. The other route employed was by adding conductive additives into the electrospun solution to prepare composite ultrafine fibers16,17 such as carbon nanopowders,18,19 carbon nanotubes,20–22 and metals. This method was the universal method used to improve the conductivity of electrospun fibers. However, for applications using different types of polymer, the amount of conductive additives was high. According to previous reports,23,24 the electrical conductivity of the fibers would be improved only with a large mass of CNTs (40%) by this method. Large amounts of conductive additives would not only cause the cost of preparation to increase25–26 but also make the weight of fibers increase thereby losing the advantages of light weight. Moreover, most CNTs are dispersed in the matrix, only few27–28 CNTs could connect with each other to make a contribution to the conductivity of the fibers. These factors would slow down the development of this method; only 20 publications reported this method by the end of 2014. Therefore, it was necessary and of interest to develop a novel method to improve the electrical conductivity of electrospun ultrafine fibers, which was easier and also needs less amounts of additives than the reported methods in order to obtain high electrical conductivity.
In this study, polyethersulfone (PES) and PES/PVA porous ultrafine fibers were first prepared by electrospinning. Then, they were used as matrix materials to absorb the electrical conductive additive material of CNTs. The CNTs will detach because of the weak non-covalent interactions between the electrical conductivity additives and the fiber matrix. To avoid this, vapor treatment was used to anchor the CNTs. In this way, small amounts of CNTs connect with each other and form the network on the surface of the fibers thereby improving the electrical conductivity in a highly efficient way. At the same time, vapor treatment was simple and could be universally applied to most polymers. The most suitable conditions such as a porous structure for adsorption and the solvent vapor treatment parameters were investigated. Finally, after the preparation of the electrically conductive fibers, the electrical conductivity of fibers with different amounts of CNTs was investigated.
The content of CNTs in the PES-based porous ultrafine fibers samples were estimated using the following formula:
ωc = CC − CB | (1) |
The thermal properties of the PES-based porous ultrafine fibers with and without CNTs were explored by differential scanning calorimetry (DSC). DSC experiments were performed on a Netzsch DSC 200 PC thermal analysis instrument (Netzsch, Selb, Germany). All experiments were conducted in the temperature range from 30 to 300 °C with a constant heating and cooling rate of 10 K min−1 and a waiting period of 2 minutes at the minimum temperature. Glass transition temperatures (Tg) were determined from the first heating run.
Thereafter, the capacities of pure PES and PES/PVA porous fibers for CNTs adsorption were investigated. Three types of porous fibers, PES porous fibers, PES/PVA porous fibers prepared with previous additional amounts of 10 wt% and 20 wt% PVA, were prepared as the CNTs adsorbing medium in this study. As seen in Fig. 2a, very small amounts of CNTs could be observed on the surface of pure PES porous fibers. Compared with the pure PES porous fibers, there were more CNTs absorbed on the surface of the PES/PVA porous fibers prepared with a previous additional amount of 10 wt% PVA. This indicated that the larger pores would absorb better compared to the smaller porous structure. Furthermore, when increasing the amount of PVA to 20 wt%, many more CNTs were absorbed on the surface as a larger porous structure was formed. This suggests a better possibility to form a continuous conductive surface layer for the large and parallel porous structure. In this case, the PES/PVA porous fibers prepared with a previous additional amount of 20 wt% PVA were considered to be the most suitable fibers to absorb the CNTs in this study and were used as the matrix porous fibers in all the following study.
To immobilize the CNTs on the surface of the fibers, DMSO vapor treatment was applied. The DMSO vapor could slightly dissolve the polymer on the surface of the fibers. Because of the surface tension of the dissolved fibers' surface, the porous structure on the fibers surface would be closed and the CNTs would be anchored on the surface porous structure. The vapor treatment time would have a large influence on the formation of the conductive surface layer. The PES-based porous fibers would be destroyed if the treatment time was too long, while if the treatment time was not long enough, the CNTs would not be effectively embedded and immobilized. Fig. 3 shows the SEM images of DMSO vapor treated PES/PVA/CNTs porous ultrafine fibers for 0, 1.5, and 2 hours. The results show that with increasing time of vapor treatment, less amount of CNTs on the surface of fibers could be observed and the surface porous structure disappeared. Because there were only few CNTs on the surface of the fibers after 2 h of vapor treatment, the maximum vapor treatment time was taken as 2 h in this study. There would be two possible reasons for this phenomenon. One is that the CNTs were rinsed off from the surface of the fibers after the porous structure was closed. While the other is that the CNTs were embedded into the surface layer and formed a thin conductive layer around the fibers.
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Fig. 3 SEM images of DMSO vapor treatment of PES/PVA porous fibers after the adsorption of CNTs with time of 0 (a), 1.5 (b), and 2 h (c). The magnification of all the images is 50![]() |
As shown in Fig. 4, there were almost no CNTs on the internal fibers and only some could be observed on the surface; this indicates that the un-immobilized CNTs on the fibers mats were removed by the ethanol washing process. The cross-section SEM images of the PES/PVA porous fibers show that there were no CNTs in the inner porous structure, while in the surface layer some CNTs could be observed. Therefore, this result indicates that when the surface porous structure was closed, some CNTs were also enclosed into the porous structure.
The TGA results could further prove this result. As seen in Fig. 5, CNTs are not degraded in the N2 atmosphere until 800 °C. For both PES/PVA porous ultrafine fibers and PES/PVA porous ultrafine fibers with the surface adsorption of CNTs, there were two regions in their weight loss trace. The first weight loss is attributed to the decomposition of PVA, while the second weight loss is that of PES, which showed that there was still some PVA left in the fiber matrix. The decomposition temperatures of the PES and PVA components were 495.8 °C and 220.5 °C, respectively. With the addition of CNTs, the thermal stability of electrospun porous PES/PVA porous ultrafine fibers increased. The start decomposition temperature of the PES/PVA porous fibers was about 150 °C, while it increased to 260 °C for the fibers after the surface adsorption of CNTs. Based on eqn (1), the content of CNTs in the PEA/PVA porous fibers was about 11 wt%. Based on the SEM characterization results, there were quite few CNTs on the surface and none in the insides of the fibers. Therefore, in this case, the only place for the presence of CNTs was the surface layer of the fibers, which makes the conductive layer on the surface of the fibers and could improve the conductivity properties of fibers with the very least amounts of CNTs.
To easily understand the entire procedure, a scheme is provided in Fig. 6. The CNTs were absorbed on the surface and surface porous structure. After the vapor treatment, the porous structure on the surface of fibers would disappear and thus the CNTs were embedded, forming a thin polymer/CNTs composite layer around the ultrafine fibers. During the electrospinning process, the fibers formed interweaved structures and the thin conductive composite layer could significantly improve the conductivity of the fiber mats.
As can be seen in Table 1 and Fig. 7, with the content of the CNTs increasing, the surface resistance of fiber mats reduced significantly at the beginning, which means an obvious improvement for the conductive properties of PES/PVA porous ultrafine fibers. When the concentration of the suspension of CNTs reached 3.0 × 10−3 g L−1, the surface resistance decreased to 10.98 R sq−1 and with further increase in the concentration, the surface resistance did not changed. This suggests that the formation of the CNTs network in the thin composite layer was fulfilled at this concentration. The CNTs formed networks to make electric charge move freely. With further increasing the concentration, the content of CNTs in the conductive thin composite layer should be increased. However, the additional content offers no contribution to the improvement of the conductivities of the mats. As Table 2 shows, the TGA results of PES/PVA porous ultrafine fibers with different contents of CNTs are different. The TGA results showed that the real content of the CNTs in the PES/PVA porous ultrafine fiber mats was about 7 wt% when the concentration of suspension of CNTs was 3.0 × 10−3 g L−1. This means that only a content of 7 wt% of CNTs was required to fulfill the formation of the continuous conductive layer. Therefore, a low content of CNTs could result in a good conductivity for the fiber mats (Fig. 8).
No. | 0# | 1# | 2# | 3# | 4# | 5# |
---|---|---|---|---|---|---|
C (g L−1) × 10−2 | 0 | 0.03 | 0.2 | 0.3 | 0.6 | 2.4 |
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Fig. 7 The electrical conductivity of PES/PVA porous ultrafine fibers with different contents of CNTs. |
Samples | a | b | c | d | e | f |
---|---|---|---|---|---|---|
Content (%) | 0 | 4.08 | 5.56 | 6.99 | 12.69 | 15.00 |
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Fig. 8 The DSC curves of PES based with different contents of CNTs 0% (a), 4.08% (b), 5.56% (c), 6.99% (d), 12.69 (e), 15.00% (f). |
The influence of surface polymer/CNTs composite layers on thermal properties of PES-based ultrafine fibers was assessed by DSC investigations. As displayed in Fig. 7, no melting peak but only the glass transition region could be observed in the DSC heating curves for all PES-based porous fibers, which indicated that the PES was an amorphous polymer. The glass transition temperatures (Tg) determined for PES-based porous ultrafine fibers with different surface CNTs contents ranged from 228–231 °C. All of them were larger than that of the pure PES ultrafine fibers (220 °C). This might be due to the restrictive movement of macromolecular chains by the incorporation of CNTs in the fibers' surface layers (Table 3).
No. 1 | a | b | c | d | e | f |
---|---|---|---|---|---|---|
Tg (°C) | 220 | 229 | 230 | 231 | 231 | 231 |
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