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Electrochemical Properties of Coumarin 500 Encapsulated in a Liquid Crystal Guided Electrospun Fiber Core and Their Supercapacitor Application

Cite this: ACS Appl. Energy Mater. 2022, 5, 10, 12078–12089
Publication Date (Web):September 20, 2022
https://doi.org/10.1021/acsaem.2c01287

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Abstract

Here, we first report a study on coumarin 500 and liquid crystal including polyacrylonitrile nanofibers in terms of synthesis, characterizations, and supercapacitor performances. SEM, POM, FTIR, and DSC measurements showed that liquid crystal was inserted into the fine polyacrylonitrile nanofibers successfully. Because a strong molecular interaction took place between coumarin 500 and liquid crystal and coumarin 500 was sensitive to the polarity of the medium, the liquid crystal behaved as a guide material for coumarin 500, and it was expected that coumarin 500 was oriented by the director of the liquid crystal along the core of the fiber. The average polyacrylonitrile nanofiber size was between 0.19 to 0.25 μm, and liquid-crystal-doped and liquid-crystal+coumarin-500-doped fibers exhibited a similar distribution, which is approximately in the 0.30 to 0.60 μm interval. This proved that the fibers maintained their structure after modifications. Electrochemical evaluation of the different composite nanofibers showed that there was not a significant current increase upon liquid crystal addition into polyacrylonitrile nanofibers at voltammograms. Cs values were enhanced after the coumarin 500 addition into liquid-crystal-doped nanofiber and obtained as 410.60 F/g with a specific energy value of 57.03 Wh/kg. Additionally, the long-term charge–discharge test of the liquid-crystal+coumarin-500-doped polyacrylonitrile graphite electrode showed a very steady distribution between 100th and the 2500th cycles with a 14.12% Cs deviation. This is attributed to the stable and robust network of the PAN nanofiber and the synergetic effect between liquid crystal and coumarin 500 in the nanofiber net.

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1. Introduction

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Coumarin (2H-1-benzopyran-2-one) is known as a lactone and provides extremely interesting electrochemical and spectro-electrochemical features due to its benzopyrone structure. (1) The adjacent hydrogen atoms and both of the oxygen atoms, which host very active lone electron pairs, easily undergo reduction or oxidation under an electrochemical process or can serve as a useful modifier for conductive polymers. (2,3) Coumarin or its derivatives can be synthesized by Perkin, Pechman, or Kostanecki reactions, and it is naturally produced by a lactonization reaction in various plants. (4) Its odor and taste serve as an allelopathy agent for animals, and a wide range of foods have coumarin. (5) It has been used in medical applications with the name of warfarin as an anticoagulation agent, (6) in the rodenticide industry as 4-hydroxycoumarin to avoid predators such as rats, (7) and used as flavor or to aromatize food or perfumes due to its odor being very like vanilla, (5) but high concentrations of coumarin cause many defects in living organisms. (8,9) The main applications of coumarin are intensively based on the dye laser industry (10) and especially solar energy panels and OLEDs because of the high chromogenic structure it has. (11,12)
To the best of our knowledge, there has not been reported any study about the supercapacitor application of coumarin. Several utilizations were examined, but solely coumarin or its derivatives have never been studied in terms of energy storage applications. Here we tried to create a synergetic effect with another functional molecule between polyacrylonitrile nanofibers and liquid crystals (LCs). LCs are very specific materials which exhibit an intermediate state between isotropic liquids and solid crystals. Both the rheological properties of isotropic liquids and the crystalline order properties of solid crystals are simultaneously represented by LCs in a certain temperature range, namely in a mesophase. Considered the simplest among the mesophases, the nematic (N) mesophase has a weak orientational order where the molecules are arranged on an average along an n-direction vector. These materials are very responsive to external fields such as temperature, electrical, etc., because of having anisotropy. Dielectric properties of LCs are related to their molecular properties such as the orientational order, number density, and any interactions between molecules. The dielectric behavior of liquid crystals conveys the aggregate response of mesogens─meaning the type of liquid crystal exhibiting a particular mesophase─as well as their molecular properties, and there is a relation between the macroscopic polarization and the molecular response via the internal electric field. (13−15) LCs could be mixed with polymers that play the role of host material for example in electrospun fibers. Lagerwall’s research group is one of the leading groups to investigate the coaxial electrospun LC/polymer structures and their potential applications. Lagerwall et al. have generated the coaxial electrospun fibers using a thermotropic nematic LC as a core material and poly(vinylpyrrolidone)/TiO2 mixture as a sheath material. (16) Also, scientists have investigated some potential applications of LC/polymer electrospun fibers such as gas sensors. (17−19) Single-needle electrospinning is a different version of electrospinning apart from the coaxial electrospinning method to generate phase-separated LC/polymer electrospun fibers. Not only the authors (20−23) but also other scientists have reported such fibers containing LCs were formed by a single-needle electrospinning of a precursor of liquid crystal and polymer, and these could be used in various applications. (24−26)
Here, the chemical, optical, and energy storage capabilities of a combination of a nematic LC with the coumarin species in polyacrylonitrile nanofibers are reported for the first time. The study was based on the superior electroactive structure of the coumarin, and the electrocapacitive charge–discharge capability of the electrode was enhanced. The electrode structure is composed of a moderately conductive LC and polyacrylonitrile structures, but the electrochemical catalytic effect of the coumarin is indicated well by using cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS) results. It has been reported another photocatalytic structure added polyacrylonitrile nanofiber as a supercapacitor application, successfully. (27,28) Here again another spectro-electrochemically active large bandgap providing material, coumarin, was utilized as a composite material and examined. The LC and the coumarin were entrapped in the polyacrylonitrile nanofibers by simultaneous electrochemical electrospinning. There is a strong molecular interaction between LCs and azo-dyes, and azo-dyes have intense sensitivity to the polarity of the medium. Thus, LCs behave as a guide material for azo-dyes, and azo-dyes can be oriented by the director of LCs. (29−33) It was shown by the authors (20,21) and even other scientific groups (24−26) that LCs could be encapsulated as a core–sheath structure utilizing the high electric field of single-needle electrospinning. In the case the coumarin is electrospun alone, there might be a possibility that the coumarin may not be fully encapsulated in the core and it may be distributed along the radius of fiber. Therefore, during the electrochemical measurement, some of the coumarin may be dissolved in measurement medium. Then, the possible time-dependent diminishment in the coumarin concentration of fiber may affect the results of long-term electrochemical measurements. The aim was that the coumarin was encapsulated within the core of the spun fibers, so an LC was used as a guide in the present work. Therewithal, the LC was used to supply an electron tunneling effect between nanofibers and coumarin molecules on the pencil graphite electrode (PGE) surface. The electrochemical characterizations are used as initial tests prior to the supercapacitor measurements. Here, the main point is that coumarin was first utilized in a supercapacitor study, and the results exhibited significant Cs values.
In this paper, the preparation of the fiber precursor and fabrication of the modified PGE electrode are presented. The fabricated nanofiber net has been characterized by DSC, POM, SEM, and FTIR. The electrochemical and the supercapacitor measurements revealed the potential of the coumarin and liquid crystal + polyacrylonitrile modified electrode.

2. Experimental Section

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2.1. Chemicals and Apparatus

4′-Heptyl-4-biphenyl carbonitrile (7cb), which is a member of 4-cyano-4′-alkylbiphenyls (nCB) liquid crystals has a rod-like shape with a length of almost 20 Å. (34)Figure 1a demonstrates the molecular formula of 7cb. It was purchased from TCI Inc. and was used as an LC dopant for electrospun fibers. nCBs are one of the well-known liquid crystalline fragments, where the n symbolizes the numbers of carbon atoms in the alkyl chain. 7cb exhibits a nematic (N) mesophase between 20.10 to 39.60 °C in the bulk state. It becomes an isotropic phase and solid crystalline phase above 39.60 °C and below 20.10 °C, respectively. Phase transition temperatures might change depending on research conditions. Due to the presence of a strong dipole moment, good chemical stability, and a convenient temperature range of the liquid crystalline phase, 7cb is a favorable material for LC/polymer composites. (35,36)

Figure 1

Figure 1. Chemical structure of (a) 7cb and (b) c500. (c) Schematic diagram of the electrospinning diagram. (d) A picture of the nanofiber-coated electrode.

Potassium dihydrogen phosphate (KH2PO4), potassium chloride (KCl), nitric acid HNO3 (99.9%), potassium hydroxide (KOH), sodium nitrate NaNO3(aq), sodium hydroxide NaOH (98.00%), polyacrylonitrile (PAN) (Mw ≈ 150 000), and N,N-dimethylformamide (DMF) (99.80%) were bought from Sigma-Aldrich. Scanning electron microscopy (SEM) with energy dispersive spectroscopy analyzes (EDS) monitored with JEOL, JSM-7600F. Fourier transform infrared spectroscopy (FTIR) measurements were performed with a PerkinElmer-ATR supported FTIR analyzer. Thermogravimetric measurements were recorded with a PerkinElmer-Pyris 6 TGA analyzer for a 4.8 mg sample under 20 mL/min of 2.5 bar of nitrogen gas flow. An Autolab PGSTAT 204 potentiostat/galvanostat (Metrohm) was utilized for electrochemical measurements. NOVA 2.1.4 software was used for the electrochemical measurements.

2.2. Preparation of the Coumarin and LC Composite PAN Nanofibers

The electrospinning method is performed by using several setups including either a collector or needle. One method uses a flat stationary collector depositing the fiber in any orientation. The other specific designs for the collector are to produce fibers aligned in a preferred orientation. (37−39) Here, a rod-shaped electrode collector was used and rotated about an axis parallel to the E-field.
Before the electrospinning process, precursors were prepared with various contents. For electrospinning all fiber types, first, precursor-1 was prepared, for which 7.6 wt % polyacrylonitrile was dissolved in DMF, in accordance with the authors’ previous work, where a fine LC/PAN fiber was obtained. (20) In order to electrospin pure PAN fibers, precursor-1 was used. Then, 7cb was added to the precursor-1 in a 1:1 mass ratio with polyacrylonitrile, and so, precursor-2, which was used for generating the PAN/7CB fibers, was obtained. The last solution, which was named as precursor-3, was prepared by adding c500, individually weighed to 0.27, 0.37, 0.56, 0.65, and 0.75% by mass of 7cb and polyacrylonitrile, to precursor-2. All precursors were gently stirred for 24 h over a magnetic stirrer.
Fibers were electrospun by using the Inovenso S1 electrospinning device, which is schematically given in Figure 1. The device is equipped with a programmable syringe pump of 0.001 mL/h accuracy, a 30.0 kV high voltage source, and a syringe needle of 0.8 mm outer and 0.5 mm inner diameter. In the experimental setup, the syringe needle and the collector were adjusted as the positive pole and negative pole, respectively. The electrode is connected through a conductive shaft to the negative pole. The advantage of the rotating rod method is to maintain that the nanofiber covers the entire electrode surface (Figure 1d). The distance between the needle and the PGE, z, was set and kept constant at 23.0 cm during the electrospinning processes. All fiber types were electrospun under a constant 12.0 kV voltage corresponding to a 522.0 V/cm electric field and were carried out at room temperature with a relative humidity of about 15–20%. Throughout the electrospinning process of the nanofibers, to acquire a fine-electrospinning jet, the feeding rate of precursor was adjusted from 0.13 to 0.25 mL/h depending on the type of the precursor.

2.3. Electrochemical Measurements

Electrochemical measurements of PGE and nanofiber-coated composite electrodes were examined using CV and EIS methods. A 3.00 mL aliquot of 3.00 M KOH (pH 7.20) solution was placed as the electrolyte in the electrochemical cell using the triple-electrode system. In the system where the examined electrode is used as the working electrode, the reference and counter electrodes were Ag/AgCl (containing 3.0 M KCl, CHI115) and a Pt wire electrode (CH Instruments Inc. CHI 111), respectively. CV measurements were performed in the range of −1.00 to 0.0 V, using various scan rates changing from 5 to 100 mV/s scan rate. The frequency range used in EIS measurements is 10–1 to 10–4 Hz. In EIS measurements, 6.00 M KOH solution was used as the electrolyte medium.
Specific capacitance (Cs) (F/g) and specific energy (E) (Wh/kg) values were calculated for composite electrodes using the following equations. (40) Here, m is the mass of electroactive substance on the electrode surface (mg), ΔV is the applied charge–discharge potential (V), S is the scan rate (mV/s), and I refers to the current value (A) obtained from the electrode. The Cs value obtained by using these data was used in the calculation of E.
(1)
(2)
Prior to the characterization and supercapacitor measurements, the amount optimization was conducted for c500 modified electrodes by CV method. As obviously seen in Figure 2, the highest electrochemical signal was obtained for 0.65% c500-containing composite structure. Therefore, it was determined as the optimum c500 amount for further measurements.

Figure 2

Figure 2. Electrochemical evaluation of the c500 amount in the composite electrode structure. Cyclic voltammograms of (a) 0.27, (b) 0.37, (c) 0.56, (d) 0.65, and (e) 0.75%-added electrodes.

Electrospun fiber precursors were prepared in three different compositions of 7cb, PAN, and c500, and called as samples 1 to 7, tabulated in Table 1. According to the result of amount optimization, so as to become comprehensible, sample-1, sample-2, and sample-6, whose characterization and supercapacitor measurements were carried out, were encoded as PAN, PAN/7CB, and PAN/7CB/C500, respectively.
Table 1. Composition of Each Sample
specimen PAN:DMF (wt %) 7cb:PAN (wt ratio) c500:7cb+PAN (wt ratio) codes of fibers
sample-1 7.6% - - PAN
sample-2 7.6% 1:1 - PAN/7CB
sample-3 7.6% 1:1 0.27:99.73 -
sample-4 7.6% 1:1 0.37:99.63 -
sample-5 7.6% 1:1 0.56:99.44 -
sample-6 7.6% 1:1 0.65:99.35 PAN/7CB/C500
sample-7 7.6% 1:1 0.75:99.25 -

3. Results and Discussion

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3.1. SEM Analysis

High-resolution SEM images of all samples electrospun under 12.0 kV electrospinning voltage are given in Figure 33. All the fibers had no beads, which means inhomogeneity along the fiber. As seen in Figure 3a, the thinnest fibers existed in PAN fibers, which were composed of pure polyacrylonitrile. In the literature, it is given that some electrospinning parameters, which are the viscosity of precursor, the net charge density carried by the electrospinning jet, feeding rate, and the surface tension of precursor, affect the bead formation in electrospun fibers. (41−48) The fibers without beads might be obtained with a rise in surface tension, although beads might exist in fibers with rising in precursor viscosity and charge density. (47)7cb LC was surrounded by a polymer sheath as seen in Figure 3b,c. The thickness distribution of fibers for all samples was examined from 10 000× magnification SEM images by means of the ImageJ analyzing program. Figure 3d–f represents the distribution of the fiber thickness of PAN, PAN/7CB, PAN/7CB/C500, respectively. In the figure, blue columns give the distribution of fiber thickness, and red lines show the Gaussian distribution. A total of 100 different fibers were evaluated at a minimum for each distribution plot. As indicated above, the thinnest fibers were observed for PAN as 0.19 to 0.30 μm despite the substantial distribution between 0.19 to 0.25 μm. The fibers of PAN/7CB and PAN/7CB/C500 have exhibited a similar distribution, which is approximately 0.30 to 0.60 μm (Figure 3e,f); it means that there is not an important effect of the addition of c500 in the change of thickness of fibers, even if c500 is added to precursor at a very low weight. Regarding the enlargement of fiber diameter, it increases with the increase in viscosity of precursor at a fixed needle-to-collector distance, feeding rate, and electrospinning voltage. In a similar vein, average fiber diameter increases with an increase in feeding rate at a fixed needle-to-collector distance, viscosity, and electrospinning voltage. (48) Before PAN/7CB was electrospun, the viscosity of the precursor-2 became a little less than precursor-1 because of adding the LC. As a consequence, it was expected that the thickness of PAN/7CB and PAN/7CB/C500 would be wider than PAN. However, in order to supply a fine fiber jet, the feeding rates for each precursor were 0.13, 0.21, and 0.21 mL/h for precursor-1 to -3, respectively. Considering the change in feeding rate, it was expected that the fiber thickness of PAN was less than PAN/7CB and PAN/7CB/C500 and also the fiber thickness of PAN/7CB and PAN/7CB/C500 was approximately closer to each other, as it has been observed. Here, one might say that the change in feeding rate was more dominant than the change in viscosity of precursor for the variation of the fiber thickness. Besides, the effort of LCs to self-assemble along the fiber axis as a core due to the high electric field might be the reason why PAN/7CB and PAN/7CB/C500, which had LCs in their compositions, existed as thicker fibers.

Figure 3

Figure 3. SEM images of fibers which belong to (a) PAN, (b) PAN/7CB, and (c) PAN/7CB/C500; the thickness distribution of the fibers of (d) PAN, (e) PAN/7CB, and (f) PAN/7CB/C500.

Fibers were electrospun at a 12.0 kV electrospinning voltage and a 23.0 cm needle-to-collector distance. The scale bar represents 1 μm. The thickness of fibers was analyzed from SEM images. PAN, PAN/7CB, and PAN/7CB/C500 correspond to Figure 3(d–f), respectively. Blue columns give the distribution of fiber thickness, and red lines point out Gaussian distribution. The scale bar in SEM images represents 1 μm.

3.2. POM Analysis

Fiber morphology was investigated using POM aside from SEM, and relative images are given in Figure 4. In accordance with SEM results, it has obviously occurred that the thickness of PAN fiber was narrower than the others (Figure 4a). Similarly, fiber structures appeared quite homogeneous, i.e., beadless or barely beads, accordingly in SEM images. Images were shot under crossed polarizers with and without an optical retarder so as to show the presence of LCs in the fiber structure utilizing the difference between the birefringence of polyacrylonitrile and 7cb, which is almost 0.01 (49) and 0.25 (50) at 23.0 °C, respectively. As seen in Figure 4a,b, PAN fibers were clearly seen by means of an optical retarder, but the fibers were not appearing under crossed polarizers as polyacrylonitrile had low birefringence. On the contrary, PAN/7CB and PAN/7CB/C500 fibers appeared under crossed polarizers both with and without an optical retarder as shining stripes (Figure 4d–f). The shining magnitude of LCs depends on the plenary angle of fiber with respect to one of the polarizers in straight aligned LCs. (51) The authors have reported in their previous work that a low-molecular-weight LC was planarly self-ordered within the core of the polymer sheath owing to the large ordering force during the electrospinning. (20) The fiber stripes, which include 7cb, appear brighter as the stripes approach an angle of 45° as to the polarizer, whereas the stripes appear darker as they approach 0°.

Figure 4

Figure 4. POM images of fibers cumulated on microscope slides are presented in (a,c,e) between crossed polarizers with a 137 nm optical retarder and in (b,d,f) without any retarder. (a,b), (c,d), and (e,f) are associated with PAN, PAN/7CB, and PAN/7CB/C500, respectively. Fibers were electrospun at a 12.0 kV application voltage and a 23.0 cm needle-to-collector distance. The scale bar represents 100 μm.

3.3. DSC Analysis

To prove the existence of the 7cb LC within the fiber, DSC measurement was performed as well. DSC is a beneficial technique that enables information about the phase transition region of LCs. (20,26,52) DSC thermographs of bulk PAN, bulk 7cb, and PAN/7CB fiber for both heating and cooling were merged in Figure 5. Measurements were carried out from 32.0 to 50.0 °C for all specimens with a 5.0 °C/min scanning rate. As seen in Figure 5, bulk polyacrylonitrile did not exhibit any peak during both heating and cooling; namely, there was not any phase transition in this temperature interval. However, for 7cb, a small endothermic peak and a small exothermic peak were taken place at 39.5 and 38.5 °C; the peaks stood for nematic–isotropic (N–I) and isotropic–nematic (I–N) phase transitions, respectively. These peaks pointed out a weak first order phase transition between N and I phases. (53) Comparably, a few weak peaks rose at 41.1 °C for heating and 40.0 °C for cooling in the DSC thermograph of PAN/7CB(Figure 5). These peaks were associated with phase transition between the N and I phase and were due to the presence of 7cb in the composite. In Figure 5, N–I and I–N phase transition peaks did not point at the same temperature for both bulk 7cb and PAN/7CB that included 7cb. For LCs, temperature shifts at phase transitions during heating and cooling like this, which are due to superheating and supercooling of LC, represent thermal hysteresis that means a first-order phase transition and is a characteristic behavior for such LCs. (54−58) Thereafter, the existence of 7cb within the fiber could be verified with the results of DSC. It is crucial to state that showing the DSC analyses of c500-doped fiber (PAN/7CB/C500) was found unnecessary here since the c500 does not possess any phase transition at the scanning temperature interval in which the DSC analysis was done.

Figure 5

Figure 5. DSC thermographs of bulk 7cb, bulk polyacrylonitrile, and the PAN/7CB fiber.

3.4. FTIR Analysis

The IR analysis has been carried out in the range of 4000–600 cm–1 presented in Figure 6. The IR spectra of bulk polyacrylonitrile, 7cb, and c500 have been analyzed in comparison with that of their fibers, PAN/7CB and PAN/7CB/C500. Basically, it has been found the fibers of PAN/7CB and PAN/7CB/C500 reflect the absorption of its compositions. Being a rigid chain, the PAN fiber showed slight absorption in its IR spectra in a comparison with that of its PAN/7CB and PAN/7CB/C500 fibers. 7cb and c500 exhibit characteristic and strong absorptions in both IR spectra of 7cb and c500, and these peaks are maintained in the PAN/7CB and PAN/7CB/C500 fibers. Some of the absorptions are tabulated in Table 2.
Table 2. Some Distinguishing Vibration Frequencies of the Samples
  mode PAN 7CB PAN/7CB PAN/7CB/C500
wavenumber (cm–1) υ(C≡N) 2243 2227 2227 2227
υ(C=C) --- 1605 1606 1605
υ(C–F) --- --- --- 1113

Figure 6

Figure 6. FTIR spectra of PAN, 7cb, c500, and their nanofiber composites.

3.5. Electrochemical Measurement Results

A series of electrochemical characterizations were carried out to evaluate the electroactivity of both 7cband c500in PAN nanofiber on the PGE electrode surface for further supercapacitor measurements. Voltammetric measurements and impedance spectra of PGE/PAN, PGE/PAN/C500, PGE/PAN/7CB, and PGE/PAN/7CB/C500 electrodes were examined in terms of peak current changes and Nyquist plots (Figure 7a–c). In general, the coating of the active PGE surface creates an electron hindrance effect, and the current value of the PGE electrode decreases. (22) However, the point is that using electron tunneling and the host effect of these fine PAN nanofibers is an exciting area and needs to be explored. (59) There has been reported plenty of supercapacitors with excellent outputs, (60−63) and the contribution of these nanofibers can contribute to the responses significantly. Here, the electrochemical contributions of the individual modifiers (7cb and c500) to the PAN-coated PGE was evaluated. It has seen that both 7cb and c500 increased the electrochemical response of the PGE/PAN electrode as given in Figure 7a,b. A detailed comparison of the voltammograms obtained from PGE/PAN and PGE/PAN/7CB electrodes is shown in Figure 7b. In this figure, one can conclude that there has been no significant current increase after the 7cb addition into the PAN nanofiber structure. This behavior is attributed to the long neutral chain of the 7cb ionic liquid structure, and it is used for the remote and the entrapment of c500 molecules, which are really abundant in electron donor groups. Apparently, c500 addition into the electrode structure made a significant increase at the peaks even higher than that of the PGE/PAN/C500 electrode. The peak current increased 10-fold (Figure 7a) after the c500 addition, due to the chromogenic groups that c500 has exhibited excellent electroactive performance. And the current increment between PGE/PAN/C500 and PGE/PAN/7CB/C500 electrodes is related to the host and rotating effect of the IL structure on the c500 molecules, which give a healthy gate through the electrode surface. Such electron wiring and tunneling effects have been used for decades by many electrochemists for triggering diffusion of the electrons. (64,65) When the Nyquist plots are examined, they are observed as linear spectra, and the best fitting circuit was found as [RCW] indicating Warburg’s impedance process. Here, the circuit elements are referring to Rct, the charge transfer resistance, C, the capacitance, W, the Warburg’s impedance; corresponding parameter values are indicated on the Figure 7d. Also, chi-square value is observed as 0.054, which indicates high correlation with the fitting curve. The electron transfer capability of the electrode surface increases proportionally with the slopes of these linear parts of Nyquist plots. Therefore, PGE/PAN, PGE/PAN/C500, PGE/PAN/7CB, and PGE/PAN/7CB/C500 electrodes showed compatible spectra with the current value increments obtained from CV results. Here, c500 showed the maximum slope value, and then, the 7cb-added electrode has a lower slope, and the PGE/PAN electrode showed the minimum slope (Figure 7c).

Figure 7

Figure 7. Electrochemical characterizations of developed electrodes. (a) Cyclic voltammogram of (a) all nanofiber modified PGE electrodes, (b) detailed CV presentation of the PGE/PAN and PGE/PAN/7CB electrodes, (c) Nyquist plot of the nanofiber modified PGE electrodes, and (d) Nyquist plot of the 7cb-c500 nanofiber modified PGE electrode and its equivalent circuit.

3.6. Electrochemical Supercapacitance Measurements

After the CV and EIS characterizations of the developed nanofibers, it has been evaluated that c500 made the highest electrochemical contribution to the composite nanofiber structure. Then, the supercapacitive performances of the different nanofibers were evaluated in the 3.00 M KOH (pH 7.20) solution for different scan rates given in Table 3 with the corresponding Cs values. The results showed that the capacitance of the PGE/PAN electrode was decreased after 7cb addition into the structure. Cs values of the PGE/PAN were obtained higher than the PGE/PAN/7CB for all scan rates even at the best scan rate performances (15.77 F/g for PGE/PAN and 11.85 F/g for PGE/PAN/7CB). This is attributed to the electrochemical inhibition effect of the 7cb structure, which does not provide free and active polar and electroactive pairs or functional groups’ instead, it has nonpolar rings and a long alkane chain. So, the charge–discharge capability of the nanofiber is hindered; hence, the structure has two ends. The one end is nonpolar, and it is easy to penetrate the pores of the nonpolar PAN nanofiber, but the CN end is very likely to act as a Lewis acid toward c500 molecules. Thereafter, the Cs values obtained from the PGE/PAN/7CB/C500 electrode showed a significant increase due to most probably this Lewis acid–base interaction between the very reactive O and CN groups of c500 and 7cb. Also, the specific energy value was obtained as 57.03 Wh/kg. Here, the main point is the presence of PAN nanofiber as a supporting backbone. In Figure 8, the current density–potential results are overlapped, and the best Cs values obtained from different scan rate measurements are indicated on each electrode configuration. Here, the synergetic effect of the polyacrylonitrile, 7cb, and c500 structures can be indicated more clearly. As the peak resolutions and the current density values were examined with the corresponding Cs values given in Table 3, it can be clearly concluded that the electron controlling mechanism is enhanced by the combination of 7cb with c500 in those PAN nanofiber cores (Table 3).
Table 3. Cs Values of the PAN, PAN/7CB, and PAN/7CB/C500 Modified PGE Electrodes for Different Scan Rates
  specific capacitances of electrodes (F/g)
scan rate (mV/s) PGE/PAN PGE/PAN/7CB PGE/PAN/7CB/C500
5 10.88 9.69 24.56
10 10.03 10.03 39.70
20 15.77 9.35 52.63
50 3.80 11.85 86.54
100 1.18 10.79 410.60

Figure 8

Figure 8. Cyclic voltammograms of (a) PGE/PAN, (b) PGE/PAN/7CB, and (c) PGE/PAN/7CB/C500 electrodes at scan rate from 5 to 100 mV/s.

In Figure 9a, the charge–discharge cycling behavior of PGE/PAN/7CB/C500 electrode, and the long-term specific capacitance stability of the electrode are given in Figure 9b. Since the best Cs value was observed at the 100 mV/s scan rate for PGE/PAN/7CB/C500, the long-term measurements were recorded at 100 mV/s for 2500 cycles. Obtained Cs values were as 410.60 F/g for the first cycle and 597.13 F/g for the 2500th cycle. Due to the electron transfer and diffusion of the electrons controlled by multiple mechanisms─especially in the presented electrode composition─the Cs values were stabilized after the 100th cycle, and the obtained recoveries were given in Figure 9b for every 100th measurement. This is attributed to the relatively low stabilization behavior of the carbonaceous materials in high charge–discharge occurrence. (66) The results showed a very steady distribution among 100% values, and the difference between the 100th and the 2500th Cs values was observed as 86.00%.

Figure 9

Figure 9. Cyclic stability of the PGE/PAN/7CB/C500 electrode. (a) Plots of 1st and 2500th cycles, and (b) Cs values of each 100th measurement and their correlation.

In Table 4, Cs values of materials investigated in recent studies are given. Comparing our study and the results in the literature, the Cs value of PGE/PAN/7CB/C500 is almost 2 times larger than those of the electrodes previously reported.
Table 4. Comparison of Cs Values Obtained from the Present Study and the Literature
supercapacitor composition specific capacitance value (F/g) measurement medium
PEDOT polymerized into cellulose paper matrix (67) 179 PVA
zirconia-based carbon nanofiber (68) 140 6 M KOH
nanocellulose cathode, HPC/NiCo2O4 (69) 235, 211, 196, 170, and 150 -
N-doped graphene obtained by microwave irradiation (70) 200 1 M H2SO4
N-doped graphene obtained by microwave irradiation (70) 130 6 M KOH
d-MOF-808@PANI at d-MOF/PANI (71) 188.00 1.0 M KOH
nitrogen-doped carbon foam was prepared on the basis of polyacrylamide gel (72) 224.4 3.0 M KOH
MnO2 nanoparticles with acetylene black and polyvinylidene fluoride electrode (73) 202 1 M Na2SO4
peanut-like Mn2O3/C, carbon black, and polytetrafluoroethylene (PTFE) (74) 158.8 1.0 M Na2SO4
Mn2O3@MnO2 composite nanofibers (75) 225.0 1 M Na2SO4
deep-eutectic solvent with porous nitrogen-doped carbon (76) 235.8 6 M KOH
PAN/7CB/C500 (present study) 410.60 6 M KOH
In our previously reported supercapacitor studies, original modifications of carbon-based electrodes have been investigated. It has to be underlined that there is an excellent improvement at the specific capacitance values. Our first supercapacitor study was about the modification of carbon paste electrodes with human-hair-sourced activated carbons with a very low Cs value of 26.88 F/g. (77) This value was improved with the addition of graphene-like hair fibers to the electrode structure, and the Cs value was obtained as 139.00 F/g. (78) In the most recent PAN nanofiber and TiO2 nanoparticle including paper, a 156.00 F/g value was reached. (27) This is very important in that TiO2 nanoparticles and PAN nanofibers created a synergetic effect, and here, the same effect is seen between 7cb and c500 in the nanofiber net. As it is always sought for recycled materials to contribute to the energy field, here, two radical structures such as 7cb and c500 were used in a supercapacitor application for the first time. This makes the presented examination very valuable.

4. Conclusions

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Here polyacrylonitrile, 7cb, and c500 were first combined in a nanofiber net and examined in terms of physical, chemical, and electrochemical properties and finally applied as an energy storage device. Therefore, SEM, POM, FTIR, and DSC measurements were carried out. Because of the strong molecular interaction between 7cb and c500 and the high sensitivitiy of c500 to the polarity of the medium, 7cb was used as a guide material in order to align the c500 molecules throughout the fiber core.
  • SEM results showed that fine and beadless nanofibers were achieved, and besides, the thinnest fibers were observed for PAN, as 0.19 to 0.30 μm, even though they were substantially distributed between 0.19 to 0.25 μm. Whereas, PAN/7CB and PAN/7CB/C500 exhibited a similar distribution, which is approximately 0.30 to 0.60 μm. Therefore, it means that there was not an important effect of 7cb and c500 in the change of thickness of PAN nanofibers.

  • POM and DSC measurements were carried out to explain 7cb presence in the PAN nanofibers. POM analysis shows that 7cb exists in the core of fibers considering the irradiance of images of PAN and 7cb, which possess different birefringence. Moreover, the thermic peaks for the fiber with 7cb (PAN/7CB), which are comparable with thermic peaks of bulk 7cb, are associated with phase transition between N and I phases, namely, DSC results proved the existence of 7cb in the PAN/7CB fiber.

  • FTIR measurements supported the existence of 7cb and c500 in the fiber net. The enhancement of the peak intensities of corresponding −CN, −CC, and −CF bonds proved that the modified PAN nanofibers were successfully produced.

  • Electrochemical evaluation of the different composite nanofibers showed that there was not a significant current increase upon 7cb addition into PAN nanofibers. Cs values were also lowered after 7cb addition. The main peak increment and the Cs value enhancement were seen after c500 addition into PAN/7CB nanofiber as 410.60 F/g, and the specific energy value was obtained as 57.03 Wh/kg. Additionally, a long-term charge–discharge test of the PAN/7CB/C500 modified PGE showed a very steady distribution among 100% value, and the difference between the 1st and the 2500th Cs values was observed as 145.43%. This is attributed to the stable and robust network of PAN nanofiber and the synergetic effect between 7cb and c500 in the nanofiber network.

Author Information

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  • Corresponding Author
  • Authors
    • Atilla Eren Mamuk - Department of Physics, Faculty of Science, Mugla Sitki Kocman University, 48050 Mugla, TurkiyeOrcidhttps://orcid.org/0000-0002-1524-3342
    • Sema Aslan - Department of Chemistry, Faculty of Science, Mugla Sitki Kocman University, 48050 Mugla, Turkiye
    • Derya Bal Altuntaş - Department of Bioengineering, Faculty of Engineering and Architecture, Recep Tayyip Erdogan University, 53100 Rize, Turkiye
  • Author Contributions

    A.E.M.: generating the electrospun-fiber-coated electrodes; analyzing and interpreting the POM, SEM, and DSC data; writing the paper. Ç.K.: generating the electrospun-fiber-coated electrodes; analyzing and interpreting the FTIR data; enhancing the rod-shaped electrode–collector setup; organizing the process. S.A.: performing the electrochemical measurements and analyzing the relevant data; writing the paper; interpreting the electrochemical properties of the electrodes. D.B.A.: performing the electrochemical measurements and analyzing the relevant data; interpreting the electrochemical properties of the electrodes.

  • Funding

    This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.

  • Notes
    The authors declare no competing financial interest.

Acknowledgments

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The authors acknowledge the technical support of The Center of Research Laboratories and Molecular Nano Materials Laboratory, which are incorporated with Mugla Sitki Kocman University.

Abbreviations

ARTICLE SECTIONS
Jump To

LC

liquid crystal

7cb

4′-heptyl-4-biphenyl carbonitrile (bulk)

nCB

4-cyano-4′-alkylbiphenyls

PAN

polyacrylonitrile (bulk)

c500

coumarin 500 (bulk)

POM

polarized optical microscopy

SEM

scanning electron microscopy

FTIR

Fourier transform infrared spectroscopy

DSC

differential scanning calorimetry

PAN

polyacrylonitrile fiber

PAN/7CB

7cb-doped polyacrylonitrile fiber

PAN/7CB/C500

7cb and c500-doped polyacrylonitrile fiber

PGE

pencil graphite electrode

PGE/PAN

polyacrylonitrile fiber coated over pencil graphite

PGE/PAN/7CB

7cb-doped polyacrylonitrile fiber coated over pencil graphite

PGE/PAN/7CB/C500

7cb and c500-doped polyacrylonitrile fiber coated over pencil graphite

CV

cyclic voltammetry EIS electrochemical impedance spectroscopy

References

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This article is cited by 2 publications.

  1. Melissa W. Williams, James Aaron Wimberly, Ratib M. Stwodah, Jimmy Nguyen, Paola A. D’Angelo, Christina Tang. Temperature-Responsive Structurally Colored Fibers via Blend Electrospinning. ACS Applied Polymer Materials 2023, 5 (4) , 3065-3078. https://doi.org/10.1021/acsapm.3c00222
  2. Zhibo Zhang, Andrey Bolshakov, Jiecai Han, Jiaqi Zhu, Kun-Lin Yang. Electrospun Core-Sheath Fibers with a Uniformly Aligned Polymer Network Liquid Crystal (PNLC). ACS Applied Materials & Interfaces 2023, 15 (11) , 14800-14809. https://doi.org/10.1021/acsami.2c23065
  • Abstract

    Figure 1

    Figure 1. Chemical structure of (a) 7cb and (b) c500. (c) Schematic diagram of the electrospinning diagram. (d) A picture of the nanofiber-coated electrode.

    Figure 2

    Figure 2. Electrochemical evaluation of the c500 amount in the composite electrode structure. Cyclic voltammograms of (a) 0.27, (b) 0.37, (c) 0.56, (d) 0.65, and (e) 0.75%-added electrodes.

    Figure 3

    Figure 3. SEM images of fibers which belong to (a) PAN, (b) PAN/7CB, and (c) PAN/7CB/C500; the thickness distribution of the fibers of (d) PAN, (e) PAN/7CB, and (f) PAN/7CB/C500.

    Figure 4

    Figure 4. POM images of fibers cumulated on microscope slides are presented in (a,c,e) between crossed polarizers with a 137 nm optical retarder and in (b,d,f) without any retarder. (a,b), (c,d), and (e,f) are associated with PAN, PAN/7CB, and PAN/7CB/C500, respectively. Fibers were electrospun at a 12.0 kV application voltage and a 23.0 cm needle-to-collector distance. The scale bar represents 100 μm.

    Figure 5

    Figure 5. DSC thermographs of bulk 7cb, bulk polyacrylonitrile, and the PAN/7CB fiber.

    Figure 6

    Figure 6. FTIR spectra of PAN, 7cb, c500, and their nanofiber composites.

    Figure 7

    Figure 7. Electrochemical characterizations of developed electrodes. (a) Cyclic voltammogram of (a) all nanofiber modified PGE electrodes, (b) detailed CV presentation of the PGE/PAN and PGE/PAN/7CB electrodes, (c) Nyquist plot of the nanofiber modified PGE electrodes, and (d) Nyquist plot of the 7cb-c500 nanofiber modified PGE electrode and its equivalent circuit.

    Figure 8

    Figure 8. Cyclic voltammograms of (a) PGE/PAN, (b) PGE/PAN/7CB, and (c) PGE/PAN/7CB/C500 electrodes at scan rate from 5 to 100 mV/s.

    Figure 9

    Figure 9. Cyclic stability of the PGE/PAN/7CB/C500 electrode. (a) Plots of 1st and 2500th cycles, and (b) Cs values of each 100th measurement and their correlation.

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