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C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7
. sc iencedi rec t . com
ava i lab le a t wwwjournal homepage: www.elsevier .com/ locate /carbon
Graphene-supported platinum and platinum–rutheniumnanoparticles with high electrocatalytic activity for methanoland ethanol oxidation
Lifeng Dong a,*, Raghavendar Reddy Sanganna Gari a, Zhou Li b,Michael M. Craig c, Shifeng Hou d
a Department of Physics, Astronomy, and Materials Science, Missouri State University, Springfield, MO 65897, USAb Greenwood Laboratory School, Missouri State University, Springfield, MO 65897, USAc Department of Biomedical Sciences, Missouri State University, Springfield, MO 65897, USAd Department of Chemistry and Biochemistry, Montclair State University, Montclair, NJ 07043, USA
A R T I C L E I N F O
Article history:
Received 26 August 2009
Accepted 20 October 2009
Available online 23 October 2009
0008-6223/$ - see front matter � 2009 Elsevidoi:10.1016/j.carbon.2009.10.027
* Corresponding author: Fax: +1 417 8366226.E-mail address: LifengDong@MissouriStat
A B S T R A C T
In this study, Pt and Pt–Ru nanoparticles were synthesized on graphene sheets and their
electrocatalytic activity for methanol and ethanol oxidation was investigated. Experimen-
tal results demonstrate that, in comparison to the widely-used Vulcan XC-72R carbon black
catalyst supports, graphene-supported Pt and Pt–Ru nanoparticles demonstrate enhanced
efficiency for both methanol and ethanol electro-oxidations with regard to diffusion effi-
ciency, oxidation potential, forward oxidation peak current density, and the ratio of the for-
ward peak current density to the reverse peak current density. For instance, the forward
peak current density of methanol oxidation for graphene- and carbon black-supported Pt
nanoparticles is 19.1 and 9.76 mA/cm2, respectively; and the ratios are 6.52 and 1.39,
respectively; the forward peak current density of ethanol oxidation for graphene- and car-
bon black-supported Pt nanoparticles is 16.2 and 13.8 mA/cm2, respectively; and the ratios
are 3.66 and 0.90, respectively. These findings favor the use of graphene sheets as catalyst
supports for both direct methanol and ethanol fuel cells.
� 2009 Elsevier Ltd. All rights reserved.
1. Introduction
Fuel cells have been receiving increased attention recently
due to the depletion of fossil fuels and the increase in envi-
ronmental pollution. Among different types of fuel cells, di-
rect methanol and ethanol fuel cells are excellent power
sources due to their high energy density, low pollutant emis-
sion, low operating temperature (60–100 �C), and ease of han-
dling liquid fuel. However, there are still some critical
obstacles inhibiting broad applications of direct methanol
and ethanol fuel cells, including low electrocatalytic activity
of anodes for methanol and ethanol oxidation reactions and
er Ltd. All rights reservede.edu (L. Dong).
the high cost of noble metal platinum (Pt)-based catalysts.
In order to enhance the catalytic activity and reduce the
usage of Pt-based catalysts, one strategy is to explore novel
carbon materials to effectively disperse catalyst particles.
Vulcan XC-72R carbon black has been the most widely-used
carbon support for the preparation of fuel cell catalysts be-
cause of its exceptional electronic conductivity and surface
area [1–3]. During the past several years, a number of research
groups have investigated carbon nanotubes as catalyst sup-
ports and have demonstrated that carbon nanotubes can
more effectively improve electrocatalytic activity of Pt nano-
particles for methanol and ethanol oxidation compared to
.
782 C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7
Vulcan XC-72R carbon black [4–12]. In 2005, graphene, a
mono-atomic sheet of hexagonally arranged carbon atoms,
was successfully synthesized [13–15]. Graphene has exhibited
excellent electrical conductivity and extremely high specific
surface area (2600 m2/g), and therefore, graphene should be
explored as a support material to improve electrocatalytic
activity of catalyst particles for methanol and ethanol oxida-
tions [16,17]. In this study, for the first time to our knowledge,
we have systematically investigated the effects of graphene
as a catalyst support on the electrocatalytic activity of Pt
and Pt–Ru nanoparticles for both methanol and ethanol oxi-
dation used in fuel cell applications.
2. Experimental
2.1. Synthesis of graphene-supported Pt and Pt–Runanoparticles
Because graphene has a structure similar to that of carbon
nanotubes, we adapted a method used to prepare carbon
nanotube-supported Pt and platinum–ruthenium (Pt–Ru) cat-
alysts to generate graphene-supported Pt and Pt–Ru catalysts
[18]. For the synthesis of graphene-supported Pt catalysts,
100 mg of graphene oxide powder was dispersed in 10 ml of
ethylene glycol (EG) solution and sonicated for 30 min. Graph-
ene oxide was prepared from graphite powder according to a
method reported by Hummers and Offeman [19]. An aliquot
(1.5 ml) of hexachloroplatinic acid (H2PtCl6, Sigma–Aldrich)
EG solution (7.4 mg H2PtCl6/ml EG) was added into the graph-
ene oxide solution and mechanically stirred for 2 h. Sodium
hydroxide (2.5 M in EG solution) was added to adjust the pH
of the solution to 13.0 (Accumet Model 15 pH meter), and then
the solution was fluxed under flowing argon at 130 �C for 3 h.
The solid was filtered, washed with DI water, and dried in an
oven at 80 �C for 12 h. For the synthesis of graphene-sup-
ported Pt–Ru catalysts, the only difference was to add 1.5 ml
of EG solution, including both H2PtCl6 and ruthenium chloride
(RuCl3, Sigma–Aldrich) (7.4 mg H2PtCl6 and 7.4 mg RuCl3 per
ml of EG), into the graphene oxide solution. Similar proce-
dures were used to prepare graphite (99%, 300 mesh, Fisher
Scientific) and carbon black (Vulcan XC-72R, Fuel Cell Store)
supported Pt and Pt–Ru catalysts.
2.2. Electron microscopy characterization
The morphology of catalyst supports, Pt and Pt–Ru nanoparti-
cles, and the distribution of the nanoparticles on different
supports were explored using a JEOL JSM-840A scanning elec-
tron microscope (SEM) and an FEI Quanta 200 field emission
scanning electron microscope (FESEM) equipped with an Ox-
ford INCA 250 silicon drift X-ray energy dispersive spectrom-
eter (EDS).
2.3. Electrocatalytic activity measurements
Electrocatalytic activities of Pt and Pt–Ru nanoparticles on dif-
ferent supports were measured in a conventional three elec-
trode cell using a CHI 600C electrochemical work station. Pt
wire served as a counter electrode, Ag/AgCl as a reference
electrode, and glassy carbon (3 mm diameter), coated with
nanoparticles, as a working electrode. To fabricate a working
electrode, 7.6 mg of catalyst powder was dispersed in 2 ml of
ethanol solution and sonicated for 30 min; 30 ll of the sus-
pension was placed onto the surface of a glassy carbon elec-
trode and dried for 15 min; and 10 ll of 5% Nafion 117 solution
(Sigma–Aldrich) was sequentially applied and dried for
15 min. The Nafion acted as an adhesive to affix the catalyst
membrane to the electrode surface. Prior to electrochemical
characterizations, all electrolyte solutions were de-aerated
under flowing nitrogen gas for 20 min. Electrocatalytic oxida-
tion of methanol on graphene-, graphite-, and carbon black-
supported Pt and Pt–Ru nanoparticles was measured in 1 M
CH3OH + 0.5 M H2SO4 electrolyte by cyclic voltammetry be-
tween �0.3 and 1.0 V. The potentials were measured and re-
ported with respect to the Ag/AgCl electrode. After
methanol oxidation measurements, the electrodes were
stored in distilled water for 30 min prior to ethanol oxidation
measurements. Electrocatalytic oxidation of ethanol on
graphene-, graphite-, and carbon black-supported Pt and Pt–
Ru nanoparticles was measured in 1 M CH3CH2OH + 0.5 M
H2SO4 electrolyte by cyclic voltammetry between �0.3 and
1.0 V.
Electrical current density was calculated by normalizing
electrical current on the area of 3 mm diameter glassy carbon
electrodes. In order to ensure the reproducibility of experi-
mental results, all electrocatalyst powders, including graph-
ene-, graphite-, and carbon black-supported Pt and Pt–Ru
nanoparticles, were synthesized for three times; the same
amount of catalytic powder was cautiously loaded onto the
electrodes.
3. Results and discussion
3.1. Structural characterization
Graphene, graphite, and Vulcan XC-72R carbon black have dif-
ferent morphologies and dimensions (Fig. 1). Graphene sheets
(Fig. 1a) are rippled and crumpled, with a dimension of sev-
eral hundred nm to several lm; graphite supports (Fig. 1b)
are platelets with a dimension ranging from 5 to 60 lm; and
carbon black (Fig. 1c) has a much smaller dimension that var-
ies from 30 to 100 nm. The morphological variety of graphene
and graphite supports will assist in the correlations between
support morphology and its effects on electrocatalytic activity
of methanol and ethanol oxidations in comparison to the
widely-used Vulcan XC-72R carbon black.
Several groups have reported that metallic nanoparticles
not only play an essential role in catalytic reduction of graph-
ene oxide with ethylene glycol, but also prevent the aggrega-
tion and restacking of the reduced graphene oxide by the
formation of graphene particle composites [20,21]. Since Pt
has a much higher atomic number (Z = 78) than C (Z = 6), we
employed a backscattered electron (BSE) detector to investi-
gate the configuration of Pt nanoparticles formed on graph-
ene sheets. Backscattered electron imaging is a Z-contrast
technique that yields compositional contrast information in
the acquired images. The signal from the BSE detector is
proportional to the backscatter coefficient, which nearly
Fig. 1 – SEM images of three types of catalyst supports
demonstrating different morphologies and dimensions: (a)
graphene, (b) graphite, and (c) Vulcan XC-72R carbon black.
Images are presented at magnifications appropriate for
demonstration of support features.
C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7 783
monotonically increases with increasing Z. A typical second-
ary electron (SE) image of graphene-supported Pt nanoparti-
cles is demonstrated in Fig. 2a, and a corresponding BSE
image of the same region is shown in Fig. 2b. In Fig. 2b, the
higher Z particles appear brighter than the lower Z back-
ground structures. The bright particles are Pt nanoparticles,
with a size of less than 10 nm, that are difficult to detect in
the SE image (Fig. 2a). EDS spectra in Fig. 2c and d further con-
firm that Pt and Pt–Ru nanoparticles, respectively, were
formed on graphene sheets. The oxygen signal indicates that
the conversion of graphene oxide into graphene with ethyl-
ene glycol is incomplete, and the sodium signal results from
sodium nitrate and sodium hydroxide, which were used dur-
ing the preparation of graphene oxide and the synthesis of
nanoparticles, respectively. Similar results were observed for
graphite- and carbon black-supported Pt and Pt–Ru
nanoparticles.
3.2. Electrocatalytic activity for methanol oxidationreaction
The electrocatalytic activity of methanol oxidation on graph-
ene-supported Pt and Pt–Ru nanoparticles was characterized
by cyclic voltammetry in an electrolyte of 1 M CH3OH and
0.5 M H2SO4 at 50 mV/s. The voltammograms of each sample
became similar and stable after the fifth cycle. The resulting
voltammograms from the fifth cycle are shown in Fig. 3.
The efficiencies of the Pt and Pt–Ru nanoparticles on metha-
nol oxidation were compared with regard to oxidation poten-
tial, forward oxidation peak current density, and the ratio of
the forward peak current density to the reverse peak current
density; these data are summarized in Table 1.
Graphene-supported Pt nanoparticles have a higher activ-
ity for methanol oxidation and a better tolerance to CO in
comparison to carbon black- and graphite-supported Pt nano-
particles (Fig. 3a). On the forward potential sweep, the current
increases slowly at lower potentials and then quickly in-
creases at potentials higher than 0.5 V, with oxidation occur-
ring at approximately 0.65 V. The magnitude of the peak
current density is directly proportional to the amount of
methanol oxidized at the electrode. The peak current density
observed with graphene is approximately 19 mA/cm2, nearly
two times to three times the peak current density for carbon
black and graphite, respectively; this result suggests that
graphene plays a critical role in promoting the methanol oxi-
dation of Pt nanoparticles. In the reverse potential sweep, an
oxidation peak is observed around 0.46 V, putatively associ-
ated with the removal of CO and other residual carbon species
formed on the electrode in the forward sweep. The reverse
anodic peak current density (2.93 mA/cm2) is much lower
than those measurements for carbon back (7.01 mA/cm2)
and graphite (6.17 mA/cm2). The ratio of the forward anodic
peak current density (IF) to the reverse anodic peak current
density (IR) can be used to describe the catalyst tolerance to
CO and other carbonaceous species. Graphene-supported Pt
nanoparticles have a ratio of 6.52, much higher than carbon
black (1.39) and graphite (1.03) supported Pt nanoparticles, a
result which suggests that graphene-supported Pt nanoparti-
cles generate a more complete oxidation of methanol to car-
bon dioxide.
As shown in Fig. 3b, the addition of Ru results in a negative
shift of oxidation potential of methanol at all three electrodes
with the decreasing of IR and the increasing of the IF to IR ratio.
The oxidation peak potential of methanol was 0.50 V com-
pared with an oxidation potential of 0.65 V for graphene-Pt
nanoparticles. This observation suggests that the presence
of Ru can significantly decrease the barrier to methanol oxi-
dation, and that Pt–Ru nanoparticles perform in a better fash-
ion than Pt nanoparticles. Conversely, the oxidation potential
000
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CCC
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NaNaNa
PtPtPt
PtPtPt000
300300300
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900900900
120012001200
150015001500
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Cou
nts
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nts
EEEnergy (keV)EEEnergy (keV)
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((c) (d)
Fig. 2 – (a) SE image of graphene-supported Pt nanoparticles and its corresponding Z-contrast BSE image (b) shows that Pt
nanoparticles with a dimension less than 10 nm were synthesized on graphene sheets. EDS spectra (c and d) were obtained
from graphene-supported Pt and Pt–Ru nanoparticles, respectively.
784 C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7
of methanol at both carbon black- and graphite-supported Pt–
Ru nanoparticles minimally shifts 0.02 V (0.58–0.56 V) and
0.01 V (0.59–0.58 V), respectively. These data indicate that
graphene-supported Pt–Ru nanoparticles may be an ideal
candidate for direct methanol fuel cell electrodes. The above
data also clearly support the proposition that Ru–Pt nanopar-
ticles can effectively advance the oxidation of methanol to
CO2 and inhibit the accumulation of CO and other carbona-
ceous species formed on the graphene, carbon black, and
graphite electrodes. For graphene electrodes especially, there
is no obvious reverse peak in Fig. 3b. Similar effects of Ru on
other catalysts for methanol oxidation have been reported by
a number of research groups [22,23].
As given in Fig. 3c and d, for all graphene-, carbon black-,
and graphite-supported Pt and Pt–Ru nanoparticles, the for-
ward oxidation current density (IF) is proportional to the
square root of the scan rate, suggesting that the oxidation
behavior of methanol at all electrodes is controlled by diffu-
sion processes. The slopes for graphene supports are larger
than those for carbon black and graphite, indicative of a faster
diffusion process of methanol on the surfaces of graphene
sheets than that for methanol on the carbon black and graph-
ite substrata.
3.3. Electrocatalytic activity for ethanol oxidation reaction
In comparison to direct methanol fuel cells, fuel cells based
on direct ethanol oxidation possess several advantages, such
as demonstrating enhanced safety, having a higher energy
density (8.01 vs. 6.09 kW/kg), and being more easily produced
in large quantities from agricultural products and from the
fermentation of biomass [24]. A complete ethanol electro-oxi-
dation involves the release of 12 electrons per molecule and
the cleavage of the C–C bond. Experimental studies have re-
vealed that ethanol is largely and partially oxidized to acetal-
dehyde and acetic acid (two- and four-electron oxidation,
respectively) instead of being fully oxidized (12-electron oxi-
dation) [25]. The ethanol electro-oxidation was considered
more complicated than that of methanol, and consequently,
needs more active and selective catalysts. In this study, we
investigated effects of graphene as a catalyst support for eth-
anol electro-oxidation of Pt and Pt–Ru nanoparticles in com-
parison to the extensively-used Vulcan XC-72R carbon black.
Compared with carbon black and graphite, graphene en-
hances considerably the electrocatalytic activity of Pt nano-
particles for ethanol oxidation by increasing the forward
oxidation current density and decreasing the reverse peak
(a) (b)
(c) (d)
Fig. 3 – Electrocatalytic activity of graphene-, Vulcan XC-72R carbon black-, and graphite-supported Pt and Pt–Ru
nanoparticles for methanol oxidation: cyclic voltammograms of (a) Pt nanoparticles and (b) Pt–Ru nanoparticles in 1 M
CH3OH/0.5 M H2SO4 at 50 mV/s between �0.3 and +1.0 V vs. Ag/AgCl; and the relationship of peak current density vs. scan
rate for (c) Pt nanoparticles and (d) Pt–Ru nanoparticles.
Table 1 – Comparison of electrocatalytic activity of methanol oxidation on graphene-, carbon black-, and graphite-supportedPt and Pt–Ru nanoparticles.
Electrode Forward sweep Reverse sweep IF/IR Ratio
IF (mA/cm2) E (V) IR (mA/cm2) E (V)
Pt–graphene 19.1 0.65 2.93 0.46 6.52Pt–CB 9.76 0.59 7.01 0.43 1.39Pt–graphite 6.33 0.58 6.17 0.41 1.03Pt–Ru–graphene 16.5 0.50 – – –Pt–Ru–CB 5.23 0.58 1.51 0.36 3.46Pt–Ru–graphite 2.32 0.56 1.53 0.37 1.52
C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7 785
current density (Fig. 4a and Table 2). Both IF to IR ratios for car-
bon black and graphite were less than 1.0. As discussed above,
the ratio describes the catalyst tolerance to CO-like interme-
diates formed on electrodes during the forward potential
sweep. The high forward peak current density and the high
IF to IR ratio for graphene-supported Pt nanoparticles indicate
that graphene effectively enhances the complete oxidation of
ethanol to CO2, and fewer CO-like carbonaceous species accu-
mulate on the electrode surface.
As given in Fig. 4b, the addition of Ru effectively lowers the
potentials for ethanol oxidations and increases the IF to IR ra-
tios. The oxidation peak potential of ethanol was 0.66 V for
graphene-supported Pt–Ru nanoparticles in comparison to
an oxidation potential of 0.72 V for graphene-supported Pt
nanoparticles. The potential shift of ethanol oxidation is
0.06 V, a value that is less than the potential shift of methanol
oxidation (0.15 V, from 0.65 to 0.50 V), thus suggesting that the
graphene-supported Pt–Ru nanoparticles are more suitable
(a) (b)
(c) (d)
Fig. 4 – Electrocatalytic activity of graphene-, Vulcan XC-72R carbon black-, and graphite-supported Pt and Pt–Ru
nanoparticles for ethanol oxidation: cyclic voltammograms of (a) Pt nanoparticles and (b) Pt–Ru nanoparticles in 1 M
CH3CH2OH/0.5 M H2SO4 at 50 mV/s between �0.3 and + 1.0 V vs. Ag/AgCl; and the relationship of peak current density vs.
scan rate for (c) Pt nanoparticles and (d) Pt–Ru nanoparticles.
Table 2 – Comparison of electrocatalytic activity of ethanol oxidation on graphene-, carbon black-, and graphite-supported Ptand Pt–Ru nanoparticles.
Electrode Forward sweep Reverse sweep IF/IR Ratio
IF (mA/cm2) E (V) IR (mA/cm2) E (V)
Pt–graphene 16.2 0.72 4.43 0.48 3.66Pt–CB 13.8 0.65 15.3 0.46 0.90Pt–graphite 7.42 0.63 8.97 0.46 0.83Pt–Ru–graphene 18.1 0.66 5.23 0.46 3.46Pt–Ru–CB 7.50 0.64 4.93 0.36 1.52Pt–Ru–graphite 2.43 0.61 1.22 0.31 1.99
786 C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7
for methanol oxidation than for ethanol oxidation. In addi-
tion, no significant shifts of oxidation potential for ethanol
were observed for carbon black (from 0.65 to 0.64 V) and
graphite (0.63 to 0.61 V) supported Pt nanoparticles.
For all graphene-, carbon black-, and graphite-supported Pt
and Pt–Ru nanoparticles, the forward oxidation peak current
density (IF) is proportional to the square root of the scan rate,
suggesting that the oxidation of ethanol at all electrodes is a
diffusion-controlled phenomenon (Fig. 4c and d). Graphene
has a larger slope than the carbon black and graphite, suggest-
ing that the diffusion efficiency of ethanol inside graphene
sheets is higher than that inside carbon black and graphite
and therefore, can enhance the efficiency and capacity of fuel
cells.
Experimental results on electrocatalytic activity of both
methanol and ethanol oxidations clearly demonstrate that
graphene-supported Pt and Pt–Ru nanoparticles possess
superior electrocatalytic activity compared to Vulcan XC-72R
C A R B O N 4 8 ( 2 0 1 0 ) 7 8 1 – 7 8 7 787
carbon black and graphite supports. Exceptional electrical
conductivity and large surface area are two critical parame-
ters for the development of novel catalyst supports for direct
methanol and ethanol fuel cells. Graphene sheets possess
both advantages when compared to Vulcan XC-72R carbon
black and graphite.
4. Conclusions
Pt and Pt–Ru nanoparticles were successfully synthesized on
graphene sheets. In comparison to Vulcan XC-72R carbon
black as a catalyst support, graphene can more effectively en-
hance electrocatalytic activity of Pt and Pt–Ru nanoparticles
for the oxidation of methanol and ethanol into CO2. With
the introduction of Ru, the reverse peak current density for
graphene is difficult to observe, a result which indicates that
the addition of Ru can efficiently release CO-like carbona-
ceous species adsorbed on the Pt surface. Similar enhance-
ment effects occur regarding the electrocatalytic activity of
Pt and Pt–Ru nanoparticles for ethanol oxidation. These find-
ings suggest promising applications for graphene as catalyst
supports, contingent upon the development of large scale
graphene sheet production.
Acknowledgements
This research was financially supported by a Faculty Research
Grant from Missouri State University and the National Sci-
ence Foundation under Award No. DMR-0821159. Acknowl-
edgment is also made to the Donors of the American
Chemical Society Petroleum Research Fund (47532-GB10) for
partial support of this research.
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