PANI Incorporated Fe-MOF: As an Electrode Material for
Supercapacitor
Manish Kumar, Shubhra Sinha, Rajiv Nayan, Manmohan L. Satnami, Manas
Kanti Deb, Kallol K. Ghosh, Shamsh Pervez, Kamlesh K. Shrivas, Vaibhav Dixit
and Indrapal Karbhal*
School of Studies in Chemistry, Pt. Ravishankar Shukla
University, Raipur (C.G.) India
Abstract
A
novel composite of Fe-metal organic framework (Fe-MOF) and polyaniline (PANI)
was synthesized using a cost-effective and rapid hydrothermal method.
Structural characterization confirmed the successful incorporation of granular
PANI over the Fe-MOF surface, which was examined through X-ray diffraction
(XRD), scanning electron microscopy (SEM), and Raman spectroscopy. The
Fe-MOF@PANI electrode demonstrated a high specific capacitance of 234.6 F g⁻¹
at 1 A g⁻¹ and 87% capacitance retention after 400 cycles at 10 A g⁻¹. Key
features of the synthesized nanocomposite include scalability, high porosity,
long-term stability, good conductivity, low charge transport resistance, and a
fast charge-discharge rate. This study highlights Fe-MOF@PANI as a promising
electrode material for supercapacitors.
Keywords:
Metal
organic framework; Energy storage; Supercapacitor, Polyaniline, Stability.
Introduction
Energy is a fundamental concept in both
scientific inquiry and everyday life, with the majority of it ultimately
derived from the sun and often harnessed through various chemical reactions.
For instance, gasoline used to power vehicles, electricity supplied to homes,
and the food consumed in diets all rely on chemical reactions to either release
or generate energy. Gasoline and food undergo specific chemical processes to
release energy, while electricity production, with about 50% generated by
burning coal, is a result of complex chemical reactions. This intrinsic
connection makes the study of energy an integral part of chemistry. In recent
years, the global demand for energy has surged dramatically and is anticipated
to escalate further due to a combination of population growth, economic
expansion, and technological advancements. This rising demand, coupled with
environmental concerns and the intricate nature of power distribution systems,
has driven an urgent shift towards renewable and sustainable energy sources,
such as wind and solar energy (Karbhal et al., 2023; Karbhal et al., 2022;
Thakur et al., 2017). The efficient utilization of these new energy sources is
crucial, given their non-constant power generation capabilities, necessitating
advancements in energy storage and distribution technologies to ensure a stable
and reliable energy supply (Patrike et al., 2023; Tan et al., 2023;
Sadiq et al., 2022; Deshmukh et al., 2018).
Metal-organic
frameworks (MOFs) have unique qualities such as increased surface area, porous
structure, high thermal and mechanical stability, active redox sites, making
them a promising solution for such applications (Shaheen et al., 2023). MOFs
are highly structured materials made up of metal ions or clusters (nodes)
connected by organic ligands (linkers), creating unique and customizable porous
architectures. Using metal cores as electrodes in supercapacitors can improve
energy storage through pseudo-capacitance. MOFs are characterized by their high
porosity and surface area, akin to tiny sponges with up to 90% of their volume
being space. Unlike some other porous materials, MOFs offer exceptional control
over their pore size and functionality. By carefully selecting the metal
clusters and organic linkers used in their synthesis, scientists can design
MOFs with pores of specific sizes and chemical properties, allowing for
targeted applications like separating specific gas molecules or capturing
pollutants (Sinha et al., 2024; Niu et al., 2022; Devi et al., 2020;
Wang et al., 2020). MOFs possess a highly ordered crystalline structure,
contributing to their stability and predictability, which simplifies their
study and engineering for specific purposes. The organic linkers in MOFs can be
modified with various functional groups, enabling researchers to tailor the
MOF's surface chemistry for specific applications such as catalysis or drug
delivery. Many MOFs exhibit remarkable thermal stability, capable of
withstanding high temperatures without decomposition, making them suitable for
applications requiring harsh operating conditions. The combination of high
porosity, tunable pores, and functionalizability allows scientists to design materials
with a wide range of properties, making them highly versatile materials with
the potential to revolutionize various fields (Sinha et al., 2024; Sinha et
al., 2023). Additionally, certain MOFs possess inherent electrical and optical
properties, such as conductivity, luminescence, and nonlinear optical behaviour,
which have implications for applications in electronics, photonics, and
optoelectronics (Zhang et al., 2017). They may have limited
applicability due to their unpredictable orientation, low conductivity, and
inclination to agglomerate (Hussain et al., 2022). To improve the structure and
properties of MOFs, researchers have focused on developing better preparation
processes. MOFs have gained tremendous research attention in recent years for
their versatile applications in a wide variety of fields, including their
potential use in supercapacitors due to their high surface area, tunable
porosity, and unique electrical properties.
The
current research aims to overcome constraints in MOFs and maximize their
potential as energy storage devices. It is noteworthy that, understanding MOF
materials requires analysing their crystallographic data, such as unit cell
diameters, space group symmetry, and atomic positions inside the crystal
lattice. MOFs physical and chemical properties are influenced by the
arrangement of their atoms or molecules, as revealed by structural information.
To improve supercapacitor performance, MOFs can be combined with aqueous
electrolytes, doped with conductive materials, or fabricated using various
processes. MOFs as electrode materials can improve supercapacitor performance,
especially when paired with aqueous electrolytes (Nagaraju et al., 2022). Hence,
a composite of Fe-MOF with conducting polymer, polyaniline (PANI), i.e.,
Fe-MOF@PANI has been synthesized in the present work and has been employed as a
supercapacitor electrode material. It was observed that Fe-MOF@PANI electrode exhibited
a high specific capacitance of 234.64 F g-1 at a current density of
1 A g-1. Moreover, it shows 87% capacitance retention after 400
cycles at a current density of 10 A g-1.
Experimental Section
Chemicals
and Reagents
Trimesic acid
(95%) and aniline were purchased from Sigma Aldrich. Ammonium persulfate (APS)
and ferric chloride were purchased from Qualigens, N, N-Dimethylforamide (99.80%)
and acetone were purchased from Merck. Concentrated HCl and other reagents were
of analytical grade and were used without any further purification. Deionized
(DI) water was used during all the experiments.
Synthesis
of Fe-MOF@PANI
To
synthesize the Fe-MOF, solvothermal method was selected. The solvothermal
synthesis process uses aqueous or non-aqueous solvents to create ferrite
materials with exact control over size distribution, shape, and crystalline
phases. Initially, trimesic acid (0.420 g)
and ferric chloride (0.324 g) were taken in a 100 ml beaker and 1:4 solution of
DMF and water respectively were added and stirred in a magnetic stirrer for 10
mins. The obtained solution is further kept in an autoclave for heating in a vacuum
oven at 130°C for 24 hr. After cooling down filtration process is performed
along with washing with acetone and deionized water and dried in a vacuum oven
at 90°C. Figure 1 represents the schematic representation of the above-mentioned
synthesis procedure.
Figure 1.
Preparation of Fe-MOF
For the synthesis
of Fe-MOF@PANI (0.1 M), Fe-MOF (100 mg) was taken
in 0.1 M HCl solution in a round bottom flask then, 0.1 M aniline was added to
the same. After stirring for 15 minutes, 0.125 M APS was added dropwise to the
solution. It was observed that the colour of the solution slowly changed to
emerald green. The synthesized product was then stored at 10°C for 24 hours to
facilitate the formation of the PANI granules. Later, it was taken out and
dried in a vacuum oven at 90°C (Nayan et al., 2024). The synthesis
procedure has been illustrated schematically in figure 2.
Electrolyte Preparation
For
the entire period of electrode testing, a 1 M H2SO4
solution was prepared and used as the electrolyte.
Figure 2. Synthesis
procedure for PANI integrated Fe-MOF
Results
and Discussion
SEM
Analysis
The
morphological characteristics of Fe- MOF and Fe- MOF@PANI were determined
through FESEM micrographs, as depicted in figure 3. The figure 3 (a) and (b)
are the FE-SEM images of the Fe-MOF and it can be seen the typical octahedral
morphology of Fe-MOF, whereas figure 3 (c) and (d) validate the successful
incorporation of PANI. The integration of PANI with provided a high surface
area and more diffusion sites (Villenoisy et al., 2021).

Figure
3. (a) & (b) SEM images Fe-MOF and (c) & (d) PANI incorporated Fe-MOF
XRD Analysis
The
X-ray diffractograms of the pure Fe-MOF, and PANI
integrated Fe-MOF composite are displayed in Figure 4 (a). The peaks at
9-10° (002), 15° (101), and 18-20° (201) confirm the formation of pristine
Fe-MOF, peaks 43-45° (110) and 65° (200), While additional peaks can be
observed in the pattern of PANI-integrated Fe-MOF peaks 15° (011), 20-30°
(020), 30-40° (200) and 65° (200). The supplementary peaks correspond to PANI,
confirming the successful integration of PANI in Fe-MOF (Tian et
al., 2021; Chu et al., 2020).

Figure
4. (a) XRD and (b) Raman spectrum of Fe-MOF and Fe-MOF@PANI
Raman Analysis
In
order to carry out the structural investigation of the synthesized materials,
Raman spectroscopy was employed. The Raman spectra for Fe-MOF/PANI and Fe-MOF
have been displayed in figure 4 (b). The peaks around 1328 cm-1 and
1561 cm-1 are related to the D, and G bands respectively. Generally,
the D band is associated with disordered of sp3 carbon network. It
is associated with the degree of defect in the material, while the G band is a
result of in-plane stretching of sp2 carbon bond. Similar results
were observed in case of Fe-MOF, depicting the D and G bands at 1350 cm-1
and 1580 cm-1, respectively (Jeong et al., 2023).
Electrochemical
measurements were conducted using the CH instrument with a 1M H2SO4
aqueous electrolyte. Figure 5 (a) represents the galvanic charge discharge (GCD)
curves of 0.1 M Fe-MOF@PANI at a current density of 1, 2, 3, 4, 5, 8, 10 A g-1.
Figure 5 (b) shows the cyclic voltammogram (CV) of and Fe-MOF@PANI (0.1 M)
displays a potential range of 0.0-1.0 V at a scan rate of 200 V s-1.
Notably, the CV curve indicates that 0.1 M Fe-MOF@PANI exhibits a significantly
wide rectangular shape compared to Fe-MOF suggesting superior charge storage
capacitance in 0.1 M Fe-MOF@PANI. Figure 5 (c) represents the GCD graph of
Fe-MOF and Fe-MOF@PANI at a current density of 1 A g-1. 0.1 M
Fe-MOF@PANI demonstrates as high as capacitance of 234.6 F g-1 at a
current density of 1 A g-1. The enhanced performance of 0.1 M
Fe-MOF@PANI is attributed to its high conductivity and the pseudocapacitive
behaviour of PANI incorporated on the surface of Fe-MOF. Similarly, the CV of
Fe-MOF and Fe-MOF@PANI at a scan rate of 200 V s-1 have been
depicted in the figure 5 (d). Figures 5 (e) represent the GCD curve of Fe-MOF
at different current densities of 0.3, 0.5, 0.8, 1, and 2 A g-1 with
capacitance of 7.5 F g-1, 5.5 F g-1, 4.8 F g-1,
4 F g-1 and 4 F g-1, respectively. Figure 5 (f) shows the
CV curve of Fe-MOF at various scan rates (10, 20, 50, 100, 150, and 200 V s-1).
Therefore, the results underscore that 0.1 M Fe-MOF@PANI exhibits superior
capacitance compared to Fe-MOF. Moreover, Figure 6 depicts the electrochemical
stability of 0.1 M Fe-MOF@PANI at a current density of 10 A g-1 for
400 cycles. In summary, the comprehensive data confirms that 0.1 M Fe-MOF@PANI
exhibits a promising capacitance of 234.6 F g-1 at a current density
of 1 A g-1 compared to Fe-MOF and Fe-MOF@PANI samples (Dixit et al.,
2023; Saleem et al., Zaka et al., 2023; Vinodh et al., 2022; Karbhal et al.,
2021; Lu et al., 2021; Zhou et al., 2019; Karbhal et al., 2016).

Figure 5.
Electrochemical performance of Fe-MOF and Fe-MOF@PANI composite in 1 M H2SO4
(a) GCD curves of 0.1 M Fe-MOF@PANI at a current density of 1, 2, 3, 4, 5, 8,10
A g-1 (b) CV curve of Fe-MOF@PANI at a scan rate of 10 to 200 V s-1
(c) GCD curves of Fe-MOF and Fe-MOF@PANI composite at a current density of 1 A
(d) CV curve of Fe-MOF and Fe-MOF@PANI at a scan rate of 200 V s-1
(e) GCD curves of Fe-MOF at different current density (f) CV curve of Fe-MOF at
a scan rate of 10 to 200 V s-1.
Table
1 illustrates the comparative properties of different MOF-based materials for
supercapacitors (Liu et al., 2024; Jeong et al., 2023; Brindha et al., 2022;
Chu et al., 2020; Peng et al., 2020; Qu et al., 2020; Shi et al., 2020; Zhou et
al., 2019; Zhu et al., 2018).
Figure 6. Cycle
stability plot of FE-MOF@PANI up to 400 cycles at 10 A g-1
Table
1. Comparative properties of different MOF-based materials
for supercapacitors
S. No.
|
Material
|
Method
|
Specific
capacitance
|
Specific
energy
density
|
Specific
power
density
|
Specific
capacitance retention
|
Ref.
|
1.
|
CoN-MOFa
|
Solvothermal
|
2033 F g-1
at 1 A g-1
|
16.8 Wh kg−1
|
23200 W kg−1
|
96% capacitance retention after 5000 cycles
|
Chu et al., 2020
|
2.
|
CuO-MOF@CF/
NiCo2S4@CFb
|
Hydrothermal
|
2426.6 F g-1
|
164.85 Wh kg−1
|
3780 W kg−1
|
96.43 % after 10,000 cycles
|
Liu et al., 2024
|
3.
|
NiCoMOF@NiCo CNFc
|
-
|
295.4 mA h g-1 (1063.4 C g-1)
at 1 A g-1
|
45.4 Wh kg−1
|
800 W kg−1
|
Capacitance retention of 70% after 4000
cycles
|
Jeong et al., 2023
|
4.
|
Fe-MOF@ACd
|
-
|
628.5 F g−1
|
16.24 Wh kg−1
|
897.5 W kg−1
|
∼82% of its initial capacity (628.5 F g−1)
after 10,000 cycles
|
Brindha et al., 2022
|
5.
|
(Ni-MOF)/Ti3C2TXe
|
Ultrasonic method
|
867.3 F g-1at
1 A g-1
|
-
|
-
|
87.1% retention after 5000 cycles at 5 A g-1
|
Peng et al., 2020
|
6.
|
AZA-MOFs@COFsf
|
-
|
20.3 µF cm-2
|
1.16 F cm-3
|
-
|
Capacitance retention 89.3 % after 2000
cycles
|
Qu et al., 2020
|
7.
|
Co-MOF/NFg
|
Solvothermal
|
13.6 F cm-2 at 2 mA cm-2
|
1.7 m h cm-2
|
4.0 mW cm-2
|
Capacitance retention of 69.7% after 2000
cycles
|
Zhu et al., 2019
|
8.
|
Graphene-MOF Complex
|
Ultrasonication
|
397 F g-1 at 1 A g-1
|
21.1 Wh kg−1
|
304 W kg−1
|
98% of the initial capacitance maintained
after 60000 times charge/discharge
|
Shi et al., 2020
|
9.
|
NiCo-PTCDAh-MOFs
|
Hydrothermal
|
234 F g-1at
1 A g-1
|
51.98 Wh kg−1
|
0.8 KW kg−1
|
Retains 84.8% of the initial capacity after
2000 cycles
|
Zhou et al., 2019
|
10.
|
Fe-MOF@PANI
|
Hydrothermal
|
234.6
F g-1 at 1 A g-1
|
-
|
-
|
Capacitance
retention of 87% after 400 cycles
|
This
Work
|
Table Footnote: aCoNi: Cobalt/Nickel; bCuO-MOF@CF/NiCo2S4@CF:
Copper oxide MOF@ Nickel-Copper Sulfide Carbon Fiber; cNiCoMOF@NiCo
CNF: Nickel copper MOF@ nickel copper carbon nanofiber; dFe-MOF@AC:
Iron MOF@ activated carbon; eNi-MOF/Ti3C2TX: Titanium Carbide; fCOFs:
Covalent Organic Frameworks; gNF: Nickel Foam; hPTCDA: Perylene-Tetracarboxylic-Dianhydride
Conclusion
Fe-MOF@PANI
was synthesized using hydrothermal process. FESEM characterization confirmed
the successful incorporation of granular PANI over the surface of the Fe-MOF.
The key role of PANI in enhancing the performance of the Fe-MOF was
investigated using electrochemical characterizations. The synthesized Fe-MOF@PANI
achieved a capacitance of 234.6 F g-1 at a current density of 1 A g-1
and exhibited excellent cyclic stability of 87% after 400 cycles at a current
density of 10 A g-1. The performance of Fe-MOF@PANI shows promising
electrochemical behaviour as an electrode material for supercapacitors.
Acknowledgements
The
authors are thankful to DST-PURSE (SR/PURSE/2022/145), SERB (EEQ/2022/000967)
and SERB (CRG/2022/003926) projects for supporting the work with financial
assistance.
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