Elsevier

Electrochimica Acta

Volume 367, 20 January 2021, 137473
Electrochimica Acta

Role of electrolytes on the electrochemical characteristics of Fe3O4/MXene/RGO composites for supercapacitor applications

https://doi.org/10.1016/j.electacta.2020.137473Get rights and content

Highlights

  • Hybrid composite Fe3O4/MXene/RGO (FMR) is fabricated by a simple chemical process.

  • FMR, FMX and F worked in the potential window -1.0 to 0 V.

  • The order of supercapacitor performance is 5 M LiCl > 1 M Na2SO4 > 1 M KOH.

  • FMR electrode exhibits 82.1 % of cyclic stability even after 5000 cycles.

Abstract

This study aims at developing hybrid composite materials consisting of iron oxide (Fe3O4) /MXene /reduced graphene oxide (RGO) without any impurities using optimized experimental parameters to be utilized in next-generation supercapacitor applications and the searching of suitable electrolyte for the developed hybrid electrode materials. We have generated Fe3O4-decorated MXene nanosheets on RGO by a simple chemical oxidation method. The initial grain size of Fe3O4 of about 43 nm is further reduced to 30 nm when prepared with MXene nanosheets. The as-prepared samples are used as a negative electrode material and their capacitive performance is analyzed in potassium hydroxide (KOH), sodium sulphate (Na2SO4) and lithium chloride (LiCl) electrolytes. Fe3O4/MXene/RGO nanocomposites showed the best performance. Regarding the electrolytes, the following order has been obtained 5 M LiCl > 1 M Na2SO4 > 1 M KOH, which matches well with the bare ion size order. Moreover, Fe3O4/MXene/RGO electrode exhibits an 82.1% of cyclic stability up to 5000 charge/discharge cycles at a current density of 5 A g-1 demonstrating the best performance.

Introduction

Two-dimensional (2D) materials have various applications in the area of materials science such as energy storage, dielectrics, optical modulation, optoelectronics, electrocatalysis and sensors [1], [2], [3], [4], [5], [6], [7]. Among 2D materials, MXene nano-sheets can be considered as a novel class of 2D materials with an outstanding performance in several fields such as metal ion batteries, supercapacitors, water splitting, photocatalysis, lubrication and electronics [8], [9], [10], [11], [12], [13], [14]. MXene nano-sheets are typically synthesized based upon MAX-phases, which are three-dimensional layered ternary metal nitrides, carbides and any combination of them [15]. An increasing number of members of the MXene family with different early transition metal and variable stoichiometry has been recently observed and a greater number of members can be expected in the near future [16]. MXene nano-sheets have been used for electrochemical supercapacitor applications due to their enhanced volumetric capacitance, which helped to improve the electronic conductivity, active intercalation sites, and surface area [17,18]. Among the MXene family, the most studied and prominent member is Ti3C2Tx, for which TX stands for potentially existing surface terminations including -O2, -(OH)2 and -F2 functional groups. Ti3C2Tx nano-sheets have been utilized for electrochemical energy storage applications [19], [20], [21], [22]. Owing to the existence of these surface terminations, Ti3C2Tx nano-sheets have proven to demonstrate an enhanced electronic conductivity. In this context, high purity Ti3C2Tx nano-sheets showed a conductivity of around 6500 S cm-1, and even Ti3C2Tx prepared by HF etching presented a conductivity of about 1000 S cm-1 [22], [23], [24]. The theoretical capacity of the MXene nano-sheets is predicted to be 615 C g-1 [25]. It has been reported that the capacitance of MXene nano-sheets could be enhanced by proper cation interaction and suitable surface modifications [26]. Few composites using MXene nano-sheets have been developed to improve the electronic and surface characteristics of MXene with Ag, MnO2, Fe2O3, Mn3O4, Bi2MoO6, carbon nanotubes (CNTs) and reduced graphene oxide (RGO) [27], [28], [29], [30], [31], [32], [33]. Concerning metal oxides, Fe3O4 magnetic nanoparticles (MNPs) seem to be interesting to be used as a negative electrode material for supercapacitor applications due to their high theoretical capacitance, which has not been experimentally achieved so far [34]. Magnetite stems from the ferrite family with an inverse spinel structure [35] can be easily prepared by chemical processes using low-cost chlorides. The formation of composites with Fe3O4 and carbon materials is promising due to their good chemical stability, better electrical conductivity, high electron mobility, larger surface area and tunable magnetic properties [36], [37], [38]. Regarding carbon-based materials, RGO is of special interest due to its superior electrochemical properties required for excellent electrode materials for electrochemical applications [39], [40], [41]. Various metal oxides along with RGO have been used to develop hybrid electrode materials. An improvement of the capacitive performance of the electrode materials with the addition of RGO has been verified [42], [43], [44], [45], [46], [47], [48], [49], [50], [51].

The doping and surface modification of graphene based carbon materials are evaluated for the energy storage and conversion processes [52,53]. The process of making RGO is also important as the final product properties, depending on the synthesis process [54]. Graphene, graphene derivative, 2D analogous materials and their composites are also attempted and found some improvement in the electrochemical applications [55,56]. Excellent capacitance retention has been showed by developing the graphene oxide sheets with simultaneous reduction and covalent grafting of polythiophene on graphene oxide sheets [57]. The addition of inorganic materials such as NiO, MnO2, ZnO, Mn3O4, Fe2O3, Fe3O4 and MoS2 along with graphene based carbon materials showed the improved physicochemical characteristics [58], [59], [60], [61].

Apart from the electrode material, the electrolyte is important regarding the resulting electrochemical performance. Only a limited number of studies have tried to address the effect of the electrolyte and the electrolyte's concentration on the electrochemical characteristics of the materials [62], [63], [64], [65]. However, the electrochemical response of each electrode material would depend on the respective electrolyte and their compatibility. Therefore, it is important to evaluate the performance of the electrode materials in different electrolytes.

This study aims at developing hybrid composite materials consisting of Fe3O4/MXene/RGO to be used in next-generation supercapacitor applications. We have generated Fe3O4-decorated MXene nano-sheets on RGO by a relatively simple chemical oxidation method. The structural, morphological, and magnetic characteristics of the Fe3O4/MXene/RGO composites have been assessed. The electrochemical characteristics of these novel composite electrode materials have been studied using three different electrolytes including KOH, Na2SO4 and LiCl to understand the role of the electrolyte on the electrochemical performance of the Fe3O4/MXene/RGO hybrid nanocomposites.

Fe3O4 MNPs were synthesized by chemical oxidation using NaOH and KNO3 as additives [66]. RGO was prepared by a microwave-assisted synthesis process using l-ascorbic acid [67]. Regarding the synthesis of MXene nano-sheets, the initial Ti3AlC2-powder was purchased from FORSMAN SCIENTIFIC Co. Ltd., Beijing (China). In order to create multi-layer Ti3C2Tx-nano-sheets, 10 g of Ti3AlC2-powder were immersed in 100 ml of a 40% hydrofluoric acid solution. The mixture was stirred for three minutes and, then kept at room temperature for two hours. The as-prepared suspension was then washed using deionized water several times until reaching a pH above 6 and, subsequently, centrifuged to separate the powder. Afterward, the washed powder was filtered under vacuum conditions and dried at room temperature for 24 hours. Optimized amounts of ferrous chloride were dissolved in 100 ml of double distilled water and heated to 60 °C. Then, 200 mg of MXene nano-sheets dispersed in water were added to the solution to decorate the ferrous ions on the layered structure of MXene nano-sheets. In another experimental batch, ferrous ions were mixed with a MXene (200 mg) / RGO (100 mg) dispersion. Afterward, appropriate amounts of NaOH and aqueous KNO3 were added to the solution. The chemical reaction was going on for 2 hours at 90 °C before cooling the reactor down to room temperature. The formed MNPs were washed several times with double distilled water thus removing the unreacted initial species. During washing, a magnetic bar was used to allow a fast separation of magnetic materials from unreacted species (excess of non-magnetic MXene and RGO). The synthesis process of the Fe3O4/MXene/RGO hybrid nanocomposites is schematically shown in Fig. 1. Bare Fe3O4, Fe3O4/MXene and Fe3O4/MXene/RGO samples are abbreviated as F, FMX and FMR.

X-ray diffraction (XRD) patterns were recorded using a Bruker D8 X-ray diffractometer equipped with a Cu- radiation source for phase analysis. Fourier Transform Infra-Red spectroscopy (FTIR) was performed using a Perkin Elmer FTIR spectrophotometer. A vibrating sample magnetometer (VSM) (Model 7404, Lakeshore, USA) was utilized to record the magnetic hysteresis loop at room temperature. The morphology of the bare and composite materials was examined by field emission scanning electron microscopy (FESEM) (FEI Quanta 250 FEG) and transmission electron microscopy (TEM) (Tecnai F20 FEG TEM with 200 kV accelerating voltage).

The overall supercapacitor performance is mainly based on the interaction between the electrode and electrolyte, which is a crucial function apart from the operating voltage. The electrolyte plays a significant role in the electrochemical parameters including cycling stability, operating temperature, power density, equivalent series resistance and self-discharge rate of the supercapacitors. Therefore, it is highly important to investigate the electrochemical performance of the as-prepared materials in different electrolytes. Herein we have studied the electrochemical performance of as-prepared materials in different electrolyte ion size including 5 M LiCl, 1 M Na2SO4 and 1 M KOH. All electrochemical experiments were done using a PARSTAT MC-1000 electrochemical workstation with a VERSA STUDIO software. The electrochemical characterizations included cyclic voltammetry (CV), galvanostatic charge-discharge (GCD) and electrochemical impedance spectroscopy (EIS). All experiments were done for three electrode systems, for which the synthesized composites, Hg/HgO or Ag/AgCl and platinum electrodes were used as working electrode, reference electrode and counter electrode respectively. In the case of electrolyte of 1 M KOH, Hg/HgO was used as a reference electrode, whereas Ag/AgCl was utilized for this purpose for 1 M Na2SO4 and 5 M LiCl electrolytes.

The electrodes were prepared based upon a binder approach. The active material, PVDF (as a binder) and carbon black (as conductive agent) were used in mass ratios of 75:15:10 and grounded finely using a mortar pastel to form a smooth slurry. The slurry was coated over an area of 1cm2 of pre-cleaned stainless steel (SS) substrates of a total area of 2 cm × 1 cm. In order to circumvent the insulating effect of the binder, a conducting agent was used during the preparation of the slurry. In order to mix the slurry, N-methyl pyrrolidone (NMP) was used as a solvent and the coated electrodes were kept at 80 °C overnight. After drying, the mass of the electrodes was measured. The active mass of the electrode was obtained by subtracting the final mass of the coated SS substrate from the original mass of SS substrate.

Based upon the CV and GCD analysis, the specific capacitance of the as-prepared electrodes was calculated using the following equations:FromCV,Cs=IdV2mΔVνFromGCD,Cs=IΔtmΔVwhere, IdV is the area under the CV curve (A V), m is the active mass of the electrode (gm), ΔV is the working potential window (V), ν is the scan rate (mV s-1), Δt is the discharge time (s) and I is the discharge current (A).

The CV and GCD analyses were accomplished in the potential window between -1.0 and 0 V. For CV, the electrodes were tested with various scan rates ranging from 5 to 125 mV s-1. Similarly, GCD profiles were obtained for various current densities ranging from 0.2 to 1 A g-1.

Section snippets

Results and discussion

The single phase of Fe3O4 in bare, MXene and MXene/RGO composites is confirmed from the XRD pattern with reference to the JCPDS card no 82-1533 as shown in Fig. 2. The average grain size of the bare Fe3O4 MNPs was estimated to be 43 nm based upon the Scherrer's equation [68]. When introducing MXenes in the composite, the average grain size reduced to 30 nm. The reduction of the average grain size of Fe3O4 in FMX might be due to the distribution of nucleation seeds over the MXene surface. It is

Conclusions

Magnetic nanocomposites consisting of Fe3O4/MXene and Fe3O4/MXene/RGO were generated by chemical oxidation without any impurities. The saturation magnetization of bare Fe3O4 was about 89 emu g-1 and decreased to 70 and 62 emu g-1 due to the addition of MXene and MXene/RGO, respectively. A detailed analysis of the resulting morphologies showed the sheet-like morphology of MXene decorated with Fe3O4. The Fe3O4-decorated MXenes and bare Fe3O4 MNPs were decorated on RGO sheets to generate

Credit author statement

Thirumurugan Arun- Conceptualization, Methodology, Investigation and Writing - Original Draft

Ankita Mohanty- Investigation and Writing - Original Draft

Andreas Rosenkranz- Writing - Original Draft

Bo Wang-Resource

Jinhong Yu-Resource

Mauricio J. Morel-Resource

R. Udayabhaskar- Investigation and Resource

Samuel A. Hevia- Investigation and Resource

Ali Akbari-Fakhrabadi-Resource

R.V. Mangalaraja-Resource

Ananthakumar Ramadoss- Investigation, Resource and Writing - Original Draft

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgement

Arun Thirumurugan gratefully acknowledges the University of ATACAMA for the financial support. The authors also express their gratitude to Dr. R. Justin Joseyphus (Department of Physics, National Institute of Technology, Tamil Nadu, India) for the VSM measurements. A. Rosenkranz gratefully acknowledges the financial support given by ANID-CHILE within the project Fondecyt 11180121 as well as the VID of the University of Chile in the framework of “U-Inicia UI013/2018”. A. Rosenkranz and B. Wang

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