4 research outputs found
Phase- and Crystal Structure-Controlled Synthesis of Bi<sub>2</sub>O<sub>3</sub>, Fe<sub>2</sub>O<sub>3</sub>, and BiFeO<sub>3</sub> Nanomaterials for Energy Storage Devices
Controlling the phase and crystal structure of nanomaterials
is
a challenging mission in a wet chemical method and has remarkable
importance to the materials properties. Herein, we demonstrate a facile
sol–gel method to synthesize Bi2O3, Fe2O3, BiFeO3, Bi36Fe2O57, secondary phase, and mixed phase of BiFeO3 (Bi25FeO40 and Bi2Fe4O9) by tailoring the parameters such as molar concentration,
calcination temperature, and duration. Further, all the electrode
materials were demonstrated for supercapacitor (SC) application. The
pure-phase BiFeO3 nanoparticles show a highest specific
capacitance of 253 F/g at a current density of 1 A/g compared to all
other electrodes under a 3 M KOH electrolyte. The higher specific
capacitance of BiFeO3 nanoparticles is ascribed to their
higher surface area, pure ABO3 structure, and lower charge-transfer
resistance. Moreover, the BiFeO3 nanoparticles were also
tested under a neutral electrolyte (1 M Na2SO4) and found to have 3.7 times lower specific capacitance compared
to the alkaline electrolyte (3 M KOH). The electrokinetic study of
the as-synthesized active electrodes illustrates the maximum capacitive
involvement to store the overall charge. The BiFeO3 nanoparticles
display outstanding stability with a retention rate of 99.02% after
1100 consecutive galvanostatic charge–discharge cycles at various
current densities. Moreover, a solid-state symmetric SC device (SSD)
was fabricated using BiFeO3 nanoparticles. The device delivered
a maximum energy density of 17.01 W h/kg at a current density of 1
A/g and a power density of 7.2 kW/kg at a current density of 10 A/g.
The BiFeO3 SSD showed an excellent capacitive retention
rate of 88% after 5000 cycles, suggesting that it could be a promising
electrode material for practical application in energy storage devices
Microwave-Assisted Solvothermal Synthesis of Cupric Oxide Nanostructures for High-Performance Supercapacitor
Enhancing
the performance and stability of the low-cost materials
for electrochemical energy storage device is an important aspect.
Herein, we report microwave-assisted solvothermal synthesis of three-dimensional
(3D) spherical CuO structures composed of either one-dimensional (rod-like)
or two-dimensional (2D) flake-like building blocks by varying the
reaction medium, i.e., water and ethylene glycol (EG). A higher EG
in the reaction medium facilitates formation of the flake-like structures.
A specific surface area of 168.47 m<sup>2</sup> g<sup>–1</sup> is achieved with the 3D flower-like CuO, synthesized using copper
acetate precursor in 1:3 water/EG solvent ratio. The same sample delivers
a specific capacitance of 612 F g<sup>–1</sup> at an applied
current density of 1 A g<sup>–1</sup> and shows high stability
with capacity retention of 98% after 4000 galvanostatic charge–discharge
cycles. The high specific capacitance of flower-shaped CuO architecture
is attributed to large surface area and availability of sufficient
pores for ions diffusion. Furthermore, two-electrode asymmetric supercapacitor
device is fabricated using the 3D flower-shaped CuO as positive electrode
and activated carbon as negative electrode, which shows an energy
density of 27.27 Wh kg<sup>–1</sup> at a power density of 800
W kg<sup>–1</sup>. This underlines the potential of inexpensive
CuO architecture as an active material for energy storage devices
Bond-Energy-Driven, Low- or High-Angle-Grain-Boundary-Movement-Mediated Synthesis of Porous Se–Te for Use in Water-Splitting Reactions
Herein, for the first
time, we applied the metal–metal-bond-energy factor to the
evolution of a porous Se–Te alloy. The porous Se–Te
material has been prepared from the constituents’ elemental
states, through only a heating–cooling process in silicone
oil without the use of any reagent, surfactant, or capping agent.
Surprisingly, the reaction occurred at a much lower temperature (240
°C) than the mp (450 °C) of Te<sup>0</sup>. The reaction’s
nucleation and growth by means of varied bond energy have been clarified
for the first time. A difference in the bond energies of a hetero
metal–metal bond (Se–Te) and a homo metal–metal
bond (Se–Se) directs nucleation and growth toward the fabrication
of a porous structure, even from the constituents’ elemental
states, in which low-angle-grain-boundary (LAGB) and high-angle-grain-boundary
(HAGB) movements play governing roles. Proper band-gap alignment of
Se and Te makes the alloy composite applicable to water-splitting
reactions under Xe-arc-lamp illumination. PEC efficiency of Se–Te
was found to be higher than those reported for Se and other composite
materials
Nitrogen-Enriched Nanoporous Polytriazine for High-Performance Supercapacitor Application
Polytriazine
with high nitrogen content (c.a. 50.5 wt %) has been
synthesized by an ultrafast microwave-assisted method using melamine
and cyanuric chloride. The nitrogen-enriched nanoporous polytriazine
(NENP-1) has exhibited high specific surface area (maximum SA<sub>BET</sub> of 838 m<sup>2</sup> g<sup>–1</sup>) and narrow
pore size distribution. The NENP-1 has been employed as electrode
material for supercapacitor application. A maximum specific capacitance
(C<sub>sp</sub>) of 1256 F g<sup>–1</sup> @1 mV s<sup>–1</sup> and 656 F g<sup>–1</sup> @1 A g<sup>–1</sup> are estimated
from the cyclic voltammetry (CV) and galvanostatic charge/discharge
(GCD) measurements, respectively, in a three-electrodes configuration.
This C<sub>sp</sub> value is considered as very high for a nonmetallic
system (organic polymer). Superior capacitance retention of 87.4%
of its initial C<sub>sp</sub> was observed after 5000 cycles at a
current density of 5 A g<sup>–1</sup> and demonstrates its
potential as an efficient electrode material for practical applications.
To test this claim, an asymmetric supercapacitor device (ASCD) was
fabricated. The C<sub>sp</sub> values of the device in the two-electrode
configuration are 567 F g<sup>–1</sup> @5 mV s<sup>–1</sup> and 287 F g<sup>–1</sup> @4 A g<sup>–1</sup> in the
CV and GCD measurements, respectively. The ASCD has shown superior
energy density and power density of 102 Wh kg<sup>−1</sup> and
1.6 kW kg<sup>–1</sup>, respectively, at the current density
of 4 A g<sup>–1</sup>. The energy density is much higher than
the best reported supercapacitors and also close to the commercial
batteries. This indicates the material could bridge the gap between
the commercial batteries and supercapacitors