1. Introduction
Carbon nanofibers are a class of nanomaterials that have recently been widely investigated for their utility in energy storage devices [
1]. They can be applied as electrodes in lithium ion, sodium ion or metal–air batteries without the necessity of binders, as electrodes in supercapacitors, or as separators in supercapacitors, etc., [
2,
3]. In most applications, freestanding and ideally even flexible nanofiber mats with sufficient structural stability in addition to high porosity are preferred as electrodes. In many cases, PAN is used as the base material for electrospinning due to its outstanding carbon yield during carbonization [
4]. After prior stabilization and subsequent carbonization, however, carbon nanofiber mats from pure PAN tend to be brittle and to break even under small mechanical loads. Because of this, several research groups investigate different possibilities to increase the flexibility of carbon nanofiber mats by optimizing spinning, stabilization, and carbonization parameters, as well as by adding diverse nanomaterials, such as graphene to increase the spinning solution’s conductivity, ZnO, TEOS, or others [
5,
6,
7].
In this work, we demonstrate the benefits of such nanoparticles (NPs) on PAN/NP electrospun nanofiber mats on the flexibility after stabilization and carbonization, comparing the physical and chemical properties of these nanofibrous mats. We show that nanoparticular additives, especially ZnO, can significantly improve the flexibility of the carbon nanofiber mats, which is already noticeable after the stabilization process.
2. Materials and Methods
Electrospinning was performed using a wire-based machine, “Nanospider Lab” (Elmarco, Czech Republic). Spinning was performed for 50–60 min with a nozzle diameter of 0.9 mm, a carriage speed of 100 mm/s, a wire–substrate distance of 240 mm, and a substrate–ground electrode distance of 50 mm.
Table 1 gives an overview of the spinning solutions prepared from PAN (X-PAN copolymer, Dralon, Dormagen, Germany) in dimethyl sulfoxide (DMSO, min. 99.9%, obtained from S3 chemicals, Bad Oeynhausen, Germany) and spinning parameters optimized for the respective samples.
Parts of the samples were stabilized in a muffle oven B150 (Nabertherm, Lilienthal, Germany) at a temperature of 280 °C for 1 d, approached with a heating rate of 1 K/min. Carbonization was performed in a tube furnace CTF 12/TZF 12 (Carbolite Gero Ltd., Sheffield, UK) at 500 °C for 1 h under constant nitrogen flow of 160 mL/min, approached with a heating rate of 1 K/min.
Characterization of the samples was performed by scanning electron microscopy (SEM, Phenom ProX G3 Desktop SEM, Thermo Fisher Scientific, Waltham, MA, USA), X-ray diffractometry (XRD, X’Pert Pro MPD PW3040-60 diffractometer, Malvern Panalytical GmbH, Kassel, Germany), thermogravimetric analysis (TGA, Hi-Res TGA 2950 Thermogravimetric Analyzer from TA Instruments, New Castle, DE, USA), and Fourier transform infrared (FTIR) spectrometry (Excalibur 3100, Varian Inc., Palo Alto, CA, USA) in attenuated total reflection mode (ATR-FTIR).
3. Results and Discussion
The surface of the as-spun samples is shown in
Figure 1, followed by the stabilized (
Figure 2) and carbonized samples (
Figure 3). PAN, PAN/TEOS, and PAN/ZnO show common nanofiber mats, with small particles visible on the PAN/ZnO nanofiber mat which apparently stem from ZnO agglomerations. PAN/nickel ferrite is mostly non-fibrous, which may be attributed to the high relative humidity of 35% during spinning. No significant deviations from the original morphology were observed for the stabilized and carbonized samples.
The nanofiber diameter distribution for the three fibrous samples is depicted in
Figure 4a. PAN/TEOS keeps the diameter mostly constant, which seems to make it advantageous for stabilization and carbonization. TGA measurements (
Figure 4b) show a steep decrease in sample mass due to the cyclization of nitrile groups at around 300 °C, which is increased by TEOS and reduced by ZnO. XRD measurements of the as-spun nanofiber mats (
Figure 4c) reveal, besides the PAN diffraction peak at 17°, no contribution from the amorphous TEOS and the typical sharp peaks of ZnO nickel ferrite, respectively.
FTIR measurements of all samples are depicted in
Figure 5. While raw PAN shows typical C-H
2 bending and stretching (1451 cm
−1, 1363 cm
−1), the Si-O-Si peak of TEOS at 1083 cm
−1 only becomes visible after stabilization, along with common peaks of stabilized PAN [
6]. Large peaks after carbonization indicate a lower degree of carbonization [
6].
Bending tests on stabilized samples revealed the expected brittle behavior of carbon nanofiber mat from pure PAN, while the other samples, especially PAN/ZnO, were much more flexible. This underlines that adding nanoparticles to PAN nanofiber mats is a promising approach to improve the flexibility of the resulting carbonized nanofiber mats.
Author Contributions
Conceptualization, C.H., T.G. and A.E.; methodology, C.H., T.G. and A.E.; formal analysis, A.E.; investigation, B.B., C.H., T.G., U.G., J.L.S., A.E. and M.W.; writing—original draft preparation, A.E.; writing—review and editing, All authors; visualization, U.G. and A.E. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
All data are included in this paper.
Conflicts of Interest
The authors declare no conflicts of interest.
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