7 research outputs found
Fabrication of High-Surface-Area Graphene/Polyaniline Nanocomposites and Their Application in Supercapacitors
Graphene/polyaniline (PANI) nanocomposites
were prepared by reducing graphene oxide with hydrazine in the presence
of different amounts of polyaniline nanoparticles. In situ cryo-transmission
electron microscope (TEM) images of a graphene oxide (GO)/PANI solution
revealed that the PANI nanoparticles were anchored on the surface
of the GO sheets. During the reduction, the as-adsorbed PANI nanoparticles
were sandwiched between layers of graphene sheets. These PANI nanoparticles
acted as spacers to create gaps between neighboring graphene sheets,
resulting in a higher surface area compared to pure graphene. Graphene/PANI
nanocomposites exhibited the high specific surface area of 891 m<sup>2</sup>/g. Utilizing this composite material, a supercapacitor with
a specific capacitance of 257 F/g at a current density of 0.1 A/g
has been achieved
Novel Pyrolyzed Polyaniline-Grafted Silicon Nanoparticles Encapsulated in Graphene Sheets As Li-Ion Battery Anodes
A simple method to fabricate graphene-encapsulated
pyrolyzed polyaniline-grafted Si nanoparticles has been developed.
Instead of using Si nanoparticles with a native oxide layer, HF-treated
Si nanoparticles were employed in this work. The uniqueness of this
method is that, first, a PANI layer over the Si nanoparticles was
formed via the surface-initiated polymerization of aniline on the
surface of aniline-functionalized Si nanoparticles; then, the PANI-grafted
Si nanoparticles were wrapped by the GO sheets via π–π
interaction and electrostatic attraction between the GO and the PANI.
Finally, the GO and PANI were pyrolyzed, and this pyrolyzed PANI layer
tightly binds the graphene sheets and the Si nanoparticles together
in the composite. The composite materials exhibit better cycling stability
and Coulombic efficiency as anodes in lithium ion batteries, as compared
to pure Si nanoparticles and physically mixed graphene/Si composites.
After 300 cycles at a current density of 2 A/g, the composite electrodes
can still deliver a specific capacity of about 900 mAh/g, which corresponds
to ∼76% capacity retention. The enhanced performance can be
attributed to the absence of surface oxides, the better electronic
conductivity, faster ion diffusion rate, and the strong interaction
between the graphene sheets and the tightly bound carbon-coated Si
nanoparticles
Hierarchical Nanocomposites of Vanadium Oxide Thin Film Anchored on Graphene as High-Performance Cathodes in Li-Ion Batteries
Hierarchical nanocomposites of V<sub>2</sub>O<sub>5</sub> thin
film anchored on graphene sheets were prepared by slow hydrolysis
of vanadyl triisobutoxide on graphene oxide followed by thermal treatment.
The nanocomposite possessed a hierarchical structure of thin V<sub>2</sub>O<sub>5</sub> film uniformly grown on graphene, leading to
a high specific surface area and a good electronic/ionic conducting
path. When used as the cathode material, the graphene/V<sub>2</sub>O<sub>5</sub> nanosheet nanocomposites exhibit higher specific capacity,
better rate performance, and longer cycle life, as compared to the
pure V<sub>2</sub>O<sub>5</sub>. The nanocomposite cathode was able
to deliver a specific capacity of 243 mAh/g, 191 mAh/g, and 86 mAh/g
at a current density of 50 mA/g, 500 mA/g, and 15 A/g, respectively.
Even after 300 cycles at 500 mA/g, the composite electrode still exhibited
a specific capacity of ∼122 mAh/g, which corresponds to ∼64%
of its initial capacity. This enhanced electrochemical performance
can be attributed to facile electron transport between graphene and
V<sub>2</sub>O<sub>5</sub>, fast Li-ion diffusion within the electrode,
the high surface area of the composites, and a pore structure that
can accommodate the volume change during lithiation/delithiation,
which results from the unique hierarchical nanostructure of the V<sub>2</sub>O<sub>5</sub> anchored on graphene
Structural Modification of Graphene Sheets to Create a Dense Network of Defect Sites
Pt/graphene
composites were synthesized by loading platinum nanoparticles
onto graphene and etched at 1000 °C in a hydrogen atmosphere.
This results in the formation of a dense array of nanostructured defect
sites in the graphene, including trenches, nanoribbons, islands, and
holes. These defect sites result in an increase in the number of unsaturated
carbon atoms and, consequently, enhance the interaction of the CO<sub>2</sub> molecules with the etched graphene. This leads to a high
capacity for storing CO<sub>2</sub>; 1 g of the etched samples can
store up to 76.3 cm<sup>3</sup> of CO<sub>2</sub> at 273 K under ambient
pressure
Facile Preparation of Graphene/SnO<sub>2</sub> Xerogel Hybrids as the Anode Material in Li-Ion Batteries
SnO<sub>2</sub> has been considered
as one of the most promising anode materials for Li-ion batteries
due to its theoretical ability to store up to 8.4 Li<sup>+</sup>.
However, it suffers from poor rate performance and short cycle life
due to the low intrinsic electrical conductivity and particle pulverization
caused by the large volume change upon lithiation/delithiation. Here,
we report a facile synthesis of graphene/SnO<sub>2</sub> xerogel hybrids
as anode materials using epoxide-initiated gelation method. The synthesized
hybrid materials (19% graphene/SnO<sub>2</sub> xerogel) exhibit excellent
electrochemical performance: high specific capacity, stable cyclability,
and good rate capability. Even cycled at a high current density of
1 A/g for 300 cycles, the hybrid electrode can still deliver a specific
capacity of about 380 mAh/g, corresponding to more than 60% capacity
retention. The incorporation of graphene sheets provides fast electron
transfer between the interfaces of the graphene nanosheets and the
SnO<sub>2</sub> and a short lithium ion diffusion path. The porous
structure of graphene/xerogel and the strong interaction between SnO<sub>2</sub> and graphene can effectively accommodate the volume change
and tightly confine the formed Li<sub>2</sub>O and Sn nanoparticles,
thus preventing the irreversible capacity degradation
Rate-Dependent, Li-Ion Insertion/Deinsertion Behavior of LiFePO<sub>4</sub> Cathodes in Commercial 18650 LiFePO<sub>4</sub> Cells
We have performed operando synchrotron
high-energy X-ray diffraction (XRD) to obtain nonintrusive, real-time
monitoring of the dynamic chemical and structural changes in commercial
18650 LiFePO<sub>4</sub>/C cells under realistic cycling conditions.
The results indicate a nonequilibrium lithium insertion and extraction
in the LiFePO<sub>4</sub> cathode, with neither the LiFePO<sub>4</sub> phase nor the FePO<sub>4</sub> phase maintaining a static composition
during lithium insertion/extraction. On the basis of our observations,
we propose that the LiFePO<sub>4</sub> cathode simultaneously experiences
both a two-phase reaction mechanism and a dual-phase solid-solution
reaction mechanism over the entire range of the flat voltage plateau,
with this dual-phase solid-solution behavior being strongly dependent
on charge/discharge rates. The proposed dual-phase solid-solution
mechanism may explain the remarkable rate capability of LiFePO<sub>4</sub> in commercial cells
<i>In Situ</i> X‑ray Near-Edge Absorption Spectroscopy Investigation of the State of Charge of All-Vanadium Redox Flow Batteries
Synchrotron-based <i>in situ</i> X-ray near-edge absorption
spectroscopy (XANES) has been used to study the valence state evolution
of the vanadium ion for both the catholyte and anolyte in all-vanadium
redox flow batteries (VRB) under realistic cycling conditions. The
results indicate that, when using the widely used charge–discharge
profile during the first charge process (charging the VRB cell to
1.65 V under a constant current mode), the vanadium ion valence did
not reach VÂ(V) in the catholyte and did not reach VÂ(II) in the anolyte.
Consequently, the state of charge (SOC) for the VRB cell was only
82%, far below the desired 100% SOC. Thus, such incompletely charged
mix electrolytes results in not only wasting the electrolytes but
also decreasing the cell performance in the following cycles. On the
basis of our study, we proposed a new charge–discharge profile
(first charged at a constant current mode up to 1.65 V and then continuously
charged at a constant voltage mode until the capacity was close to
the theoretical value) for the first charge process that achieved
100% SOC after the initial charge process. Utilizing this new charge–discharge
profile, the theoretical charge capacity and the full utilization
of electrolytes has been achieved, thus having a significant impact
on the cost reduction of the electrolytes in VRB