# Porous Activated Carbons Derived fromPleurotus eryngii for Supercapacitor Applications

Authors: Yudan Yuan; Ruowei Yi; Yi Sun; Jianqiao Zeng; Jiaqi Li; Jiahao Hu; Yinchao Zhao; Wei Sun; Chun Zhao; Li Yang; Cezhou Zhao
Journal: Journal of Nanomaterials
 (2018)

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## Abstract

Varieties of natural biomass have been utilized to prepare porous carbon materials for supercapacitor applications. In this work, porous activated carbons derived fromPleurotus eryngii were prepared by carbonization and KOH activation. The activated carbons presented a large specific surface area of 3255 m2·g−1 with high porosity. The as-prepared electrode exhibited a maximal specific capacitance of 236 F·g−1 measured in a three-electrode cell system. Furthermore, the assembled symmetric supercapacitor showed a specific capacitance of 195 F·g−1 at 0.2 A·g−1 and a superior specific capacitance retention of about 93% after 15000 cycles. The desirable capacitive behavior suggests that Pleurotus eryngii is an attractive biomass source of carbon materials for the potential supercapacitor applications.


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## Body

## 1. Introduction

A supercapacitor is considered a promising energy storage device due to its unique merits of high specific power, high cycle stability, and rapid charge-discharge performance [1]. Owing to these features, a supercapacitor has been widely involved in various application fields, such as electric vehicles, consumer electronics, and industrial energy management [2, 3].A large amount of electrode materials for supercapacitors has been investigated so far, including carbon materials [4–6], metal oxides [7, 8], and conducting polymers [9, 10]. In recent years, two-dimensional (2D) nanomaterials [11] and hybrid materials [12] have attracted great interests. However, the synthesis of 2D nanosheets and hybrid materials is commonly involved with methods like arc-discharge synthesis, chemical vapor deposition, and microwave radiation, which are expensive, complicated, and sometimes harmful to the environment [13–15]. Now, the trend is to use biomass as a convenient and economical method for supercapacitors. Porous carbon material derived from biomass is regarded as one of the most promising candidates due to its high surface areas, good electrical conductivity, low cost, and renewability [16, 17].Recently, varieties of natural biomass have been utilized as starting materials to prepare porous carbon materials for supercapacitor [18–20]. It was reported that willow catkins activated by KOH present large three-dimensional interconnected micrometer-level pores composed of sheet-like primary particles [20]. Five types of tea leaves prepared by high-temperature carbonization and activation with KOH show typical amorphous and porous structures with a high specific surface [21]. Furthermore, N-doped porous carbon microsphere materials, synthesized from fermented rice, offer high porosity and high capacitance [22].Mushrooms, rich in carbon and oxygen, are widely distributed around the world. They are abundant, economical, and environmentally friendly. In this regard, many kinds of mushrooms have been used in supercapacitor applications [23, 24]. Pleurotus eryngii, a kind of mushrooms, has been commercially produced by the industrial process for decades with a considerable yield. This endows the Pleurotus eryngii with low price which helps it stand out among other biomass resources. Here, we reported a new facile way to synthesize the electrode materials with Pleurotus eryngii as a precursor.In this work, a facile fabrication of porous activated carbons derived fromPleurotus eryngii, followed by carbonization and KOH activation, has been demonstrated. The obtained materials present a high specific surface area of 3255 m2·g−1. In a three-electrode cell system, the prepared electrode offers a maximal specific capacitance of 236 F·g−1. Furthermore, the assembled symmetric supercapacitor shows a specific capacitance of 195 F·g−1 at 0.2 A·g−1 and a superior specific capacitance retention of about 93% after 15000 cycles. This work highlights the attractive features of Pleurotus eryngii in a supercapacitor which might inspire their future development in new energy storage device prototypes.


## 2. Experiments

### 2.1. Material Synthesis

Pleurotus eryngii was firstly washed with ethanol and dried at 60°C overnight. Secondly, the dried Pleurotus eryngii was carbonized under a nitrogen atmosphere at 500°C for 12 hours. And then, the carbonized Pleurotus eryngii was mixed with KOH solution in a 1 : 3 weight ratio and dried at 120°C overnight in a vacuum oven. The mixture was subsequently activated under a nitrogen atmosphere at 600, 700, and 800°C, respectively. Finally, the activated sample was washed with hydrochloric acid solution and excessive distilled water to remove the impurities. The products were denoted as APE-X, where X was the activation temperature.


### 2.2. Material Characterization

The samples were examined under a scanning electron microscope (SEM, Hitachi S4700). The morphology images were recorded on a transmission electron microscope (TEM, FEI Tecnai G2 F20 S-twin TEM system). X-ray diffraction (XRD) patterns were measured on a Bruker D8 ADVANCE diffractometer. Raman spectra were examined by a Renishaw inVia Raman microscope. X-ray photoelectron spectroscopy (XPS) analysis was carried out on a Thermo Scientific XPS system. Specific surface areas of the samples were measured by the Brunauere-Emmette-Teller (BET) method on a Beishide 3H-2000PS2 specific surface and pore size analysis instrument.


### 2.3. Electrochemical Measurements

The electrochemical performance of the active materials was measured in both three-electrode and two-electrode systems with 6 M KOH aqueous solution used as the electrolyte. In the three-electrode system, the counter electrode and reference electrode were platinum foil and saturated Ag/AgCl. The working electrode was prepared by mixing the active materials (80 wt%), polyvinylidene fluoride (10 wt%), and carbon black (10 wt%) in a few drops of N-methyl-2-pyrrolidone solvent. Subsequently, the resulting mixture was coated on a nickel foam substrate and dried at 80°C vacuum for 24 hours [25]. The mass loading of the active material for each electrode was about 5 mg·cm−2. In the two-electrode system, the symmetric supercapacitor was assembled by employing two APE-700 electrodes with a separator. The cyclic voltammetry (CV), galvanostatic charge/discharge (GCD), and electrochemical impedance spectroscopy (EIS) measurements were carried out on a Metrohm Autolab PGSTAT302N electrochemical workstation. The specific capacitance Cm (F·g−1) was calculated according to the discharge curve by the following equation [18, 26]:
(1)Cm=kIΔtmΔV.where I (A) is the discharge current, ∆t (s) is the discharge time, ∆V (V) is the discharge voltage window excluding the IR drop, m (g) is the mass of active materials in a single electrode, and k is a constant (k=1 for a three-electrode system and k=2 for a two-electrode system).


## 2.1. Material Synthesis

Pleurotus eryngii was firstly washed with ethanol and dried at 60°C overnight. Secondly, the dried Pleurotus eryngii was carbonized under a nitrogen atmosphere at 500°C for 12 hours. And then, the carbonized Pleurotus eryngii was mixed with KOH solution in a 1 : 3 weight ratio and dried at 120°C overnight in a vacuum oven. The mixture was subsequently activated under a nitrogen atmosphere at 600, 700, and 800°C, respectively. Finally, the activated sample was washed with hydrochloric acid solution and excessive distilled water to remove the impurities. The products were denoted as APE-X, where X was the activation temperature.


## 2.2. Material Characterization

The samples were examined under a scanning electron microscope (SEM, Hitachi S4700). The morphology images were recorded on a transmission electron microscope (TEM, FEI Tecnai G2 F20 S-twin TEM system). X-ray diffraction (XRD) patterns were measured on a Bruker D8 ADVANCE diffractometer. Raman spectra were examined by a Renishaw inVia Raman microscope. X-ray photoelectron spectroscopy (XPS) analysis was carried out on a Thermo Scientific XPS system. Specific surface areas of the samples were measured by the Brunauere-Emmette-Teller (BET) method on a Beishide 3H-2000PS2 specific surface and pore size analysis instrument.


## 2.3. Electrochemical Measurements

The electrochemical performance of the active materials was measured in both three-electrode and two-electrode systems with 6 M KOH aqueous solution used as the electrolyte. In the three-electrode system, the counter electrode and reference electrode were platinum foil and saturated Ag/AgCl. The working electrode was prepared by mixing the active materials (80 wt%), polyvinylidene fluoride (10 wt%), and carbon black (10 wt%) in a few drops of N-methyl-2-pyrrolidone solvent. Subsequently, the resulting mixture was coated on a nickel foam substrate and dried at 80°C vacuum for 24 hours [25]. The mass loading of the active material for each electrode was about 5 mg·cm−2. In the two-electrode system, the symmetric supercapacitor was assembled by employing two APE-700 electrodes with a separator. The cyclic voltammetry (CV), galvanostatic charge/discharge (GCD), and electrochemical impedance spectroscopy (EIS) measurements were carried out on a Metrohm Autolab PGSTAT302N electrochemical workstation. The specific capacitance Cm (F·g−1) was calculated according to the discharge curve by the following equation [18, 26]:
(1)Cm=kIΔtmΔV.where I (A) is the discharge current, ∆t (s) is the discharge time, ∆V (V) is the discharge voltage window excluding the IR drop, m (g) is the mass of active materials in a single electrode, and k is a constant (k=1 for a three-electrode system and k=2 for a two-electrode system).


## 3. Results and Discussions

As shown in the SEM image of Figure1(a), the Pleurotus eryngii presents three-dimensional porous network structure with micrometer-level pores. Figures 1(b) and 1(c) show the carbonized samples with different magnifications. The SEM image of the activated samples at 700°C is displayed in Figure 1(d). When comparing Figures 1(c) and 1(d), it is found that a higher roughness is observed on the surface of the activated samples after KOH activation. The TEM image of APE-700 as shown in Figure 2(a) indicates that numerous nanoparticles are stacked each other in different directions aggregating on the rough surface of the activated samples (Figure 1(d)). A high-resolution TEM (Figure 2(b)) image from APE-700 reveals that less than 1 nm abundant micropores are created after the activation.Figure 1
SEM images of (a)Pleurotus eryngii, (b, c) carbonized Pleurotus eryngii with different magnifications, and (d) as-prepared APE-700 electrode sample.
(a)
(b)
(c)
(d)Figure 2
(a, b) TEM images of APE-700 with different magnifications.
(a)
(b)The XRD patterns of various temperature-activated samples are shown in Figure3(a). All the APE samples exhibit two broad- and low-intensity peaks near 25°and 43°, corresponding to (002) and (100) planes of the graphite [25, 27]. The intensity of these two peaks decreases as the activation temperature increases, probably due to a lower graphitization degree [20]. Figures 3(b)–3(d) are the Raman spectra of APEs. Two broad bands centered at 1350 cm−1 (D-band) and 1584 cm−1 (G-band) are clearly observed [20, 25]. The relative intensity ratios of D-band to G-band (ID/IG) of APE-600, APE-700, and APE-800 are 2.9, 3.3, and 3.6, respectively. As the D-band is induced by the defects in the graphite lattice and the G-band is generated by the sp2 carbon atomic pair stretching, APE-800 exhibits the lowest graphitization degree [28]. This can be ascribed to the higher temperature facilitating the erosion reaction between carbonaceous material and KOH, which may decrease the graphitization degree of the APE materials. The results are consistent with those of the XRD analysis in Figure 3(a).Figure 3
(a) XRD patterns of APEs obtained at various activation temperatures. Raman spectra of APE-600 (b), APE-700 (c), and APE-800 (d).
(a)
(b)
(c)
(d)XPS measurement was used to further confirm the surface chemical properties and atomic compositions of as-prepared APEs. The wide XPS spectra in Figure4(a) display two peaks at 284 and 533 eV, corresponding to C 1s and O 1s, respectively. There are oxygen-containing functional groups in all the activated samples [25]. The atomic percentage of oxygen decreases from 17.33 to 8.91 atom% (see Table 1) when the activation temperature has been changed from 600°C to 800°C. The C 1s spectra of APEs in Figures 4(b)–4(d) could be approximately fitted into three peaks, which can be assigned to sp2 C=C bond in graphitic carbon (284.6 eV), sp3 C-C hybridization (285.4 eV), and -C=O/-COO- bond (288.6 eV) [25, 29]. The relative intensity of sp3 C-C hybridization peaks (the purple peaks in Figures 4(b)–4(d)) increases as the temperature raises from 600 to 800°C. The increasing intensity in the C-C bond corresponds to the reduction of the graphitization degree for APE samples at higher temperature. The most probable reason is that the KOH is more reactive with carbonaceous materials, which causes more lattice defects in the activation process.Figure 4
(a) XPS spectra of APEs activated at different temperatures. High-resolution C 1s spectra of APE activated at 600°C (b), 700°C (c), and 800°C (d).
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(b)
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(d)Table 1
Chemical compositions of as-prepared APEs by XPS analysis.
Element
APE-600
APE-700
APE-800
C (atom%)
82.67
88.96
91.09
O (atom%)
17.33
11.04
8.91The nitrogen adsorption-desorption isotherms of APEs activated at 600°C, 700°C, and 800°C are shown in Figure5(a). An abrupt increase occurs at very low relative pressure (less than 0.1) according to isotherms, followed by a smooth increase at the high relative pressures. From those results, it implies that the APEs have abundant micropores with a narrow pore size distribution [30]. At the relative pressures from 0.4 to 1.0, the subtle hysteresis loops provide evidence for forming a small amount of mesopores in the samples [31].Figure 5
(a) Nitrogen adsorption-desorption isotherms of APEs activated at 600°C, 700°C, and 800°C, respectively. (b) Pore size distribution curves of the APEs.
(a)
(b)When the activation temperatures increase from 600°C to 700°C, the flat plateau of the isotherms, as shown in Figure5(a), moves to a higher position, revealing that more pores are produced and, as a result, a higher specific surface area is achieved [32]. However, it can be noted that the plateau is shifted down when increasing the activation temperature to 800°C. A collapse of the pore structure may probably happen due to the excessive temperature. The total BET specific surface area of APE-700 is 3255 m2·g−1 with respect to 2253 m2·g−1 for APE-600 and 2704 m2·g−1 for APE-800. The mechanism of KOH activation is shown in the following equation [23, 33]:
(2)6KOH+2C→2K+3H2+2K2CO3.During the KOH activation process, the carbon frameworks are etched by the redox reaction. After washing, metallic K and K compounds are removed and pores are created.The pore size distribution of the APEs measured by the H-K model (supplied by the Beishide 3H-2000PS2 specific surface and pore size analysis instrument) is shown in Figure5(b). The pore size of the APEs is mainly at a range of 0.5–1.0 nm, implying that massive micropores are present in the APEs. In the aqueous solution of KOH, the micropores with pore sizes larger than 2 nm are commonly considered too wide to form the double layer while pore sizes less than 0.5 nm are too small for the process [20]. Therefore, it is expected that the pore size of the APEs activated at different temperatures is suitable for the transport of electrolyte ions.Typical CV curves of the samples with different activation temperatures at the scan rate of 50 mV·s−1 are shown in Figure 6(a). It is clear that all CV curves display rectangular-like shapes with a characteristic feature of a good capacitor behavior, promising to be used as the electrode material of supercapacitors. Figure 6(b) presents the GCD curves of APEs measured at a current density of 2 A·g−1. It is found that the APE-700 has the largest integrated area in the CV curves and the longest charge-discharge time, suggesting the highest specific capacitance for APE-700. Its specific capacitance is calculated as 236 F·g−1. The Nyquist plots of APEs measured from 10 mHz to 100 kHz are shown in Figure 6(c). APEs display good capacitive behavior with a nearly vertical line at low frequencies, among which the slopes are much larger when the activation temperature decreases. At high frequencies, the intercept of plots with the real axis presents a low equivalent serial internal resistance of ~0.3 Ω, including the intrinsic resistance of activated materials, electrolyte and the contact resistance. The bode phase diagrams of all samples are shown in Figure 6(d). Compared with APE-800, the phase angles of APE-600 and APE-700 are ~85° and ~81°, respectively, which are closed to that of an ideal capacity (90°), indicating a good capacitive property.Figure 6
Electrochemical performance measured in a three-electrode system: (a) CV curves of APEs activated at 600°C, 700°C, and 800°C, respectively, at 50 mV·s−1; (b) GCD curves of the APEs at 2 A·g−1; (c) Nyquist plots of the APEs, an enlarged view in the high-frequency region is shown in the inset; (d) bode phase diagrams of the APEs; (e) CV curves of APE-700 at different scan rates from 5 to 100 mV·s−1; (f) GCD curves of APE-700 at different current densities from 2 to 20 A·g−1.
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(f)The electrochemistry properties of APE-700 have been investigated further in more detail. The CV curves of APE-700 are presented in Figure6(e) at scan rates from 5 to 100 mV·s−1. The rectangular-like shape is maintained even at a high scan rate of 100 mV·s−1, revealing low equivalent series resistance and fast charge transport capability [34]. The GCD curves of APE-700 (Figure 6(f)) show almost symmetrical and linear relationship at a series of current densities ranging from 2 to 20 A·g−1, which agreed well to a typical property of electrical double-layer capacitors. However, the rate capability of APE-700 is not high, due to abundant micropores and a small amount of mesopores generated by KOH activation. In general, at low current density, the ions of electrolyte are able to penetrate into the micropores. When the current density increases, the narrow micropores may hinder or restrict the ion diffusion due to the space limitations, leading to a moderate rate capability [1, 35].Table2 summarizes a comparison of our result with other biomass-derived carbon materials reported previously. It seems that the APE-700 presents a moderate specific capacitance due to its highest surface area. The main reasons are probably as follows: firstly, the specific capacitance is related not only to the surface area but also to the pore structure, interfacial wettability, and electrical conductivity. Secondly, the measurement and electrolyte of the materials listed in Table 2 are not exactly the same. In particular, the specific capacitance would decay when the current density increases.Table 2
Comparison of the properties of biomass-derived carbon materials.
Biomass
SBET (m2·g−1)
Cm (F·g−1)
Measurement
Electrolyte
Ref.
Willow catkins
1533
298
0.5 A·g−1
6 M KOH
[16]
Tea leave
2841
330
1 A·g−1
2 M KOH
[21]
Glucose
757
260
0.5 A·g−1
6 M KOH
[17]
Coconut shell
1532
228
5 mV·s−1
6 M KOH
[19]
Corn starch
1167
162
0.625 A·g−1
6 M KOH
[18]
Cotton
1085
207
1 A·g−1
1 M H2SO4
[28]
Paulownia sawdust
1900
227
2 mV·s−1
6 M KOH
[36]
APE-700
3255
236
2 A·g−1
6 M KOH
This workIn order to investigate the practical electrochemical performance of APE-700, the symmetric supercapacitor was assembled and measured in 6 M KOH electrolyte. The CV and GCD curves are shown in Figures7(a) and 7(b). Good capacitive behaviors at different scan rates and current densities are seen. According to (1), the specific capacitance of APE-700 is calculated as 195 F·g−1 at a current density of 0.2 A·g−1. Furthermore, the cycling stability of APE-700 was performed by the GCD test at a constant density of 2 A·g−1. As shown in Figure 7(c), the specific capacitance retention is about 93% with a slight fluctuation after 15000 cycles, exhibiting excellent long-term cycle stability and great potential for energy storage devices.Figure 7
Electrochemical performance of APE-700 measured in a two-electrode system: (a) CV curves at different scan rates from 5 to 100 mV·s−1; (b) GCD curves at different current densities from 0.2 to 10 A·g−1; (c) cycle stability at a current density of 2 A·g−1 in 6 M KOH solution; (d) EIS before and after the cyclic stability test, an enlarged view in the high-frequency region is shown in the inset.
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(b)
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(d)Figure7(d) shows the electrochemical impedance spectra of APE-700. It is noted that the equivalent serial internal resistance increases after 15000 cycles, which may be attributed to the abscission of the activated material or the variation of oxygen-containing functional groups. The semicircle loop (nearly 1 Ω), an indicator of the charge-transfer resistance between electrolytes and electrode, represents good and stable ionic conductivity of the two samples. The SEM images of APE-700 before and after the cyclic stability test are shown in Figures 8(a) and 8(b). No obvious difference is observed between the two samples.Figure 8
SEM images of APE-700 (a) before the cyclic stability test and (b) after the cyclic stability test.
(a)
(b)In summary,Pleurotus eryngii activated at 700°C presents a high electrochemistry performance, which may be attributed to the following properties: (a) high specific surface area, which is much more favored to form considerable electrochemical double layers; (b) suitable pore size, which could facilitate ion transport resulting in an effective improvement in the charge-discharge process; (c) high graphitization degree, leading to a good electrical conductivity; and (d) the existence of oxygen-containing functional groups, which not only provides extra pseudo-capacitance but also improves the hydrophilicity and wettability of the porous carbon materials.


## 4. Conclusion

Porous activated carbons derived fromPleurotus eryngii were synthesized by carbonization firstly and then KOH activation. The porous carbons activated at 700°C, among other activation temperatures, exhibit the highest specific surface area of 3255 m2·g-1, and the prepared electrode offers a maximal specific capacitance of 236 F·g−1 measured in a three-electrode cell system. Furthermore, the assembled symmetric supercapacitor shows a specific capacitance of 195 F·g−1 at 0.2 A·g−1 and excellent long-term cycle stability with a capacitance retention of 93% after 15000 charge/discharge cycles at a current density of 2 A·g−1. This work highlights the attractive capacitive features of the Pleurotus eryngii as a readily available biomass source, which might inspire their future development as a new resource of porous activated carbons for supercapacitors and other energy storage devices.



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