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C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3
. sc iencedi rec t .com
avai lab le at wwwjournal homepage: www.elsev ier .com/ locate /carbon
Hierarchical porous carbon obtained from animal boneand evaluation in electric double-layer capacitors
Wentao Huang a, Hao Zhang b,c, Yaqin Huang a,*, Weikun Wang b, Shaochen Wei a
a State Key Laboratory of Chemical Resource Engineering, The Key Laboratory of Beijing City on Preparation and Processing of Novel Polymer
Materials, Beijing University of Chemical Technology, 15 BeiSanhuan East Road, Beijing 100029, Chinab Research Institute of Chemical Defense, 35 Huayuan North Road, Beijing 100191, Chinac University of Science & Technology Beijing, 30 Xueyuan Road, Haidian District, Beijing 100083, China
A R T I C L E I N F O A B S T R A C T
Article history:
Received 3 June 2010
Accepted 16 October 2010
Available online 21 October 2010
0008-6223/$ - see front matter Crown Copyrdoi:10.1016/j.carbon.2010.10.025
* Corresponding author: Fax: +86 10 64438266E-mail address: [email protected]
Animal bone, an abundant biomass source and high volume food waste, had been converted
into a hierarchical porous carbon in a simple two-step sustainable manner to yield a highly
textured material. The structures were characterized by nitrogen sorption at 77 K, scanning
electron microscopy and X-ray diffraction. The electrochemical measurement in 7 M KOH
electrolyte showed that the porous carbon had excellent capacitive performances, which
can be attributed to the unique hierarchical porous structure (abundant micropores with
the size of 0.5–0.8 and 1–2 nm, mesopores and macropores with the size of 2–10 and 10–
100 nm), high surface area (SBET = 2157 m2/g) and high total pore volume (Vt = 2.26 cm3/g).
Its specific capacitance was 185 F/g at a current density of 0.05 A/g. Of special interest was
the fact that the porous carbon still maintained 130 F/g even at a high current density of
100 A/g.
Crown Copyright � 2010 Published by Elsevier Ltd. All rights reserved.
1. Introduction
Biological materials always possess elaborate structures and
compositions, which grant them appropriate features to per-
form well in the nature system and can not be achieved
through artificial synthesis absolutely. However, biological
system, a vast material bank, can provide not only raw mate-
rials but also fantastic inspirations for human to develop new
materials with refined mimic structures and outstanding
functions like natural materials. Bioinspired design strategies
are booming in the preparation of materials such as medical
materials and other functional materials [1–4]. The develop-
ment of novel materials exploited from natural preorganised
systems, particularly those from inexpensive, abundant, and
sustainable biomass would go in some way to achieving the
goals of the future society. In this context the preparation of
hierarchical porous carbon (HPC) materials from renewable
natural resources is proposed.
ight � 2010 Published by
.(Y. Huang).
HPC materials, owning interesting structures which
include the combination of micropores, mesopores or mac-
ropores, display excellent potential for applications in gas
storage, biosensor, catalysis, and energy storage [5–9]. Cur-
rently, HPCs are mainly synthesized using template methods
[10–17]. With this approach, a carbon precursor/inorganic
template composite is first formed, followed by carboniza-
tion, then chemical leaching of the template material. Such
methodology is tedious, requiring multiple synthetic steps,
especially the precursor infiltration into the template, caustic
chemical treatments, and long curing times; scale-up has also
proven difficult and is not cost-effective due to the destruc-
tion of expensive templates. The development of an inexpen-
sive synthesis pathway for the generation of HPC materials
through the recycling/utilization of natural biomaterials
would be highly serviceable to overcome the weaknesses of
the traditional template methods. Biominerals are mostly
natural inorganic/organic composites and the inorganic and
Elsevier Ltd. All rights reserved.
C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3 839
organic components are often organised into nanometer
sized domains. It is our hope that the biocomposites can act
as useful precursor biomass for the preparation of HPCs,
whereby the organic component can be carbonised in the
presence of the (structure donating) inorganic component,
which finally can be removed easily.
Animal bone, a unique natural composite material, at-
tracts our attention for the development of HPC as raw mate-
rials. First, bone is such a mineral and organic matrix [18,19],
on a volumetric basis it consists of about 33–43% apatite min-
erals and 32–44% organics. Nano plate-like apatite crystals
disperse within the discrete spaces within the collagen fibrils.
The organic materials can act as carbon precursor, mean-
while the apatite crystals can act as natural template for
the forming of abundant mesopores and macropores (30–
200 nm) [20]. Second, bone is a hierarchically structured
material with concentric lamellae or plywood-like lamellae
sub-microstructure, which is useful for forming hierarchical
structure of the carbon materials. In addition, bone, one kind
of food industry byproducts, is very cheap and environment
friendly with abundant production, especially its application
for preparation of porous carbon materials will be quite
advantageous.
Therefore we prepared HPC using animal bone natural
template, in which the template preparation and tedious infil-
tration are unnecessary now. Furthermore, we tailored the
pore structure and improved the surface area through chem-
ical activation, and evaluated it in electric double-layer capac-
itor (EDLC). The results demonstrate that the tailored HPC
exhibits attractive properties and is a promising electrode
material for EDLC. The tailored HPC has the specific capaci-
tance of 185 F/g at a current density of 0.05 A/g in 7 M KOH.
Of special interest is the fact that it still maintains 130 F/g
even at a high current density of 100 A/g.
2. Experimental
2.1. Preparation of HPC
The dried pig bone (purchased from market in Beijing) parti-
cles were pre-carbonized in a tuber furnace under N2 circum-
stance at 450 �C. Then the pre-carbonized bone particles were
ground and carbonized again using the following heating pro-
gram: (1) ramp at 2.5 �C/min to 850 �C, and hold for 1 h; (2)
cool naturally to room temperature. The obtained product
was washed in diluted HNO3, rinsed with distilled water,
and dried at 110 �C for 12 h. The final product was named as
HPC–0, some other ground pre-carbonized bone was mixed
with KOH agent with a weight ratio of 1:1 and treated by using
a similar procedure above, and the obtained product was la-
belled HPC-1.
2.2. Structure and texture characterization
Micromeritics ASAP 2010 instrument was used to characterize
the surface area and pore-structure of the carbon samples
using N2 sorption at 77 K. The scanning electron microscopy
(SEM) image was obtained on a HITACHI S-4700 electron
microscope. Powder X-ray diffraction (XRD) pattern was
recorded on a Rigaku D/max- 2500VB2+/pC diffractometer
using Cu Ka radiation.
2.3. Electrode preparation and electrochemical measure-ments
In order to evaluate the electrochemical performances of the
as-prepared HPC-1 in EDLC, a mixture of 87 wt% of HPC-1,
10 wt% of acetylene black and 3 wt% of polytetrafluoroethyl-
ene (PTFE, as a binder, FR301B, 3F Corp., Shanghai, China)
binder was pressed into pellets as electrodes. Then the
electrodes were dried under vacuum at 120 �C for 12 h. A but-
ton-type capacitor was assembled with two carbon electrodes
separated by polypropylene membrane using 7 M KOH aque-
ous solution as electrolyte. For comparison, a commercial
activated carbon, YP17 from Kuraray Chemical Corporation,
was used as a reference.
A two-electrode system was used in cyclic voltammetry
(CV), galvanostatic charge–discharge measurements and elec-
trochemical impedance spectroscopy. The galvanostatic
charge/discharge test was carried out on a Land cell tester
between 0 and 1.0 V. The cyclic voltammetry and impedance
spectra were recorded on an electrochemistry workstation
Solartron 1280B. The specific capacitance (Csp) of a single
HPC-1 electrode was calculated from the discharge part of gal-
vanostatic charge/discharge curves, by the formula Csp = 2It/
Vm, where I was the discharge current, t was the discharge
time, V was the potential change in discharge between 0
and 1.0 V and m was the mass of the active electrode material
in one electrode. The IR drop at the beginning of the discharge
was omitted.
3. Results and discussion
3.1. Structure and texture characterization
The nitrogen adsorption–desorption isotherm and the corre-
sponding DFT (density functional theory) pore size distribu-
tion curve of the HPC–0 are shown in Fig. 1. It can be seen
from Fig. 1a that the isotherm of the HPC–0 taken up a shape
of type IV (according to IUPAC classification). The steep in-
crease of nitrogen uptake at low relative pressure close to
0.01 suggested the formation of micropores in large quanti-
ties, which could be produced by the dissociated leaving
groups (e.g., CO2, H2O, H2S, NH3) caused by the pyrolysis of
the organics. Obvious capillary condensation step (hysteresis
loop) and the continuous accretion of nitrogen adsorption at
the relative pressure from 0.4 to 1.0 indicated developed mes-
oporous structure and the appearance of macroporosity.
Fig. 1b shows its pore size distribution, which was calculated
from nitrogen desorption isotherms using DFT. The pores
were mainly distributed in three regions: 0.6–0.9, 1.1–2.0 and
2–100 nm, while there were few macropores of pore size
above 200 nm, representing two level micropores, mesopores
and macropores respectively. This result indicated that the
porous carbon prepared using bone possessed the hierarchi-
cal pore structure. The mesopores and macropores might be
formed by the natural minerals, and the fact that the pore
sizes were agreed with the sizes of apatite crystals in bone
Fig. 1 – (a) Nitrogen adsorption–desorption isotherm and (b) the corresponding DFT pore size distribution curve of the HPC–0.
The insert is a SEM image of the HPC–0.
840 C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3
demonstrates the role of apatite crystals as natural templates
[18–20].
HPC-1 was developed by chemical activation using KOH.
Fig. 2a and b displays the Nitrogen adsorption–desorption iso-
therm and the corresponding DFT pore size distribution
curve. In Fig. 2a, the Nitrogen adsorption–desorption iso-
therm also showed a type IV shape with obvious hysteresis
loop and the final increased tail at the relative pressure from
0.9 to 1.0. Compared with the HPC–0, the HPC-1 displayed
more increment in nitrogen adsorption capacity at the entire
relative pressure region, which suggested that additional
pores were created and some small pores were widen by
chemical activation [21,22]. The result can demonstrate that
micropores, mesopores and macropores of the carbon were
enhanced by KOH activation. It can be seen in Fig. 2b that
the HPC-1 also has a hierarchical pore size distribution
(mainly in four regions: 0.5–0.8, 1.0–2.0, 2–10 and 10–
Fig. 2 – (a) Nitrogen adsorption–desorption isotherm and (b) the
The insert is a SEM image of the HPC-1.
100 nm), representing two level micropores, small mesopores,
broad mesopores and macropores, respectively. Compared
the DFT pore size distribution curves of the two samples, it
can be seen that the volumes of two level micropores and
small mesopores improved by KOH activation, meanwhile,
the volume of broad mesopores and macropores decreased.
The formation mechanisms of the hierarchical pore stuctrure
need further investigation in detail.
SEM image of the HPC-1 (inserted in Fig. 2b) also displays
the microstructure of the porous carbon with interconnected
pores.
The textural characteristics of the HPC samples calculated
from nitrogen adsorption–desorption isotherms are listed in
Table 1. After KOH treatment, the specific surface area (SBET),
total pore volume (Vt) and micropore volume (Vmi) of the
hierarchical porous carbon increased remarkably from 861
to 2157 m2/g, 1.17 to 2.26 cm3/g, and 0.33 to 0.77 cm3/g,
corresponding DFT pore size distribution curve of the HPC-1.
Table 1 – Textural characteristics of the HPCs.
Sample ID SBETa (m2/g) Vt
b(cm3/g) Vmc (cm3/g) Vmi/Vt Wave
d (nm)
HPC–0 861 1.17 0.33 0.28 5.45HPC-1 2157 2.26 0.77 0.34 4.18
a BET (Brunauer–Emmett–Teller) surface area, measured in relative pressure range of 0.04–0.20.b Total pore volume, measured at P/P0 = 0.99.c Micropore volume, calculated by HK (Horvath–Kawazoe) method from adsorption curve.d Average pore width, estimated from the equation of 4 Vt/SBET.
C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3 841
respectively. The microporosity (Vmi/Vt) also rised from 0.28 to
0.34, but its amplification is lower than that of micropore vol-
ume, suggesting that additional mesopores were formed after
activation. However, the average pore width (Wave) decreased
from 5.45 to 4.18 nm. All the changes are probably due to the
activation opening the closed pores, drilling new narrow
micropores and widening the pre-existent pores. Further-
more, the weight ratio of KOH/pre-carbonized bone was only
one, which is lower than that used in literatures [23,24], indi-
cating that the porous and loose bone is in favor of improving
the efficiency of activating agent and then cutting the cost.
To examine the graphitic character of the HPC-1, wide an-
gle powder XRD analysis was also performed (Fig. 3). The
HPC-1 exhibited a broad reflection at a 2h value of about 24�,which may be attributed to the (002) reflection of a gra-
phitic-type lattice. A weak reflection centered around 43� cor-
responds to a superposition of the (100) and (101) reflections
of a graphitic-type carbon structure, indicating a limited de-
gree of graphitization in this material.
3.2. Electrochemical characterizations
Cyclic voltammetry measurements were conducted to test
the EDLC performances of the HPC-1. Fig. 4a shows the cyclic
voltammogram of HPC-1 based capacitor between 0 and 1.0 V
scanned at 100, 200, and 500 mV/s. And the CV curves exhibit
excellent rate performance without any redox peak in the
chosen voltage range. It can be observed that the HPC-1 car-
bon presented a rectangular voltammogram shape at the
100 mV/s, indicative of excellent candidate as electrode mate-
rial for electrochemical double-layer capacitor. Generally
Fig. 3 – XRD pattern of the HPC-1.
speaking, at higher scan rates, the CV profiles will usually
deviate from the ideal rectangular shape due to polarization.
But in this work, until the scan rate increased to 200 mV/s, the
CV curve still remained its symmetrical rectangular shape, al-
most perfect for EDLCs. Even if the scan rate increased to as
high as 500 mV/s, the CV curves almost kept rectangular,
which reflected the capability of the HPC-1 based capacitor
to cycle at high current densities. The rectangular shapes of
all CV curves from HPC-1 are much better than those from
the KOH-activated carbon nanotubes tested by the same
way in [25]. According to the work of Wang et al. [11], ion-buf-
fering reservoirs can be formed in the macropores to mini-
mize the diffusion distances to the interior surfaces, the
mesoporous walls provide low-resistant pathways for the
ions through the porous particles, and the micropores
strengthen the electric double layer capacitance. So this fur-
ther confirms that the hierarchical porous structure helps to
maintain good capacitive behavior of the HPC-1 at high sweep
rates, which is due to fast ionic transportation within the
mesopores and short diffusion distance from mesopores to
micropores.
A more detail investigation of the electrochemical proper-
ties of the sample HPC-1 was carried out by analysis of the
electrochemical impedance spectrum (EIS). The Nyquist plots
of HPC-1 electrode are shown in Fig. 4b. The curve presented a
depressed semicircle in middle and high frequency region,
and a nearly perpendicular line in low frequency region.
The equivalent series resistance (ESR) of the HPC-1 was only
0.65 X, estimated from the value of the real axis at 1000 Hz,
indicating the outstanding ionic conductivity which relates
to the mobility of ions inside the pores and the electric con-
ductivity of carbon materials. The previous XRD pattern in
Fig. 3 also showed that the localized graphitic structure re-
sulted in some ordered microcrystalline structure leading to
high conductivity, which agreed with the quite low ESR of
HPC-1. The nearly perpendicular line reflected the excellent
properties of double layer capacitor of the HPC-1 electrode.
Fig. 5 shows specific capacitance obtained at various dis-
charge rates for the HPC-1. It is clear that with increasing dis-
charge rate the specific capacitances decreased for the HPC-1,
which was attributable to the decreased surface sites for elec-
trochemical double layer formation. The specific capacitance
of the HPC-1 reached 185 F/g at a current density of 0.05 A/g,
which has a relatively high specific capacity [25,26]. Despite
relatively high capacitance, the HPC-1 has slightly lower
capacitance compared to some of the activated carbon with
super high surface area. In future, it is maybe we can increase
the surface area of HPC-1 by some methods which can be fur-
ther improved the capacitance.
Fig. 4 – (a) Cyclic voltammograms for the HPC-1 in 7 M KOH electrolyte corresponding EDLC systems at potential scan rates of
100, 200 and 500 mV/s and (b) Nyquist plots of HPC-1 electrode.
Fig. 5 – Specific capacitance at various discharging rates for
the capacitors using HPC-1 and YP17 as electrode materials.
Fig. 6 – Charge–discharge curves of the HPC-1, current: (a)
100 A/g, (b) 50 A/g, (c) 40 A/g.
842 C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3
Moreover, the specific capacitance of the sample was
dropped slowly as the current increases. When at 10 A/g, its
specific capacitance only decreased to 143 F/g. However, its
specific capacitance could be kept at 130 F/g even at a high
current density of 100 A/g, which was 70.3% of the specific
capacitance at 0.05 A/g, while the specific capacitance of com-
mercial activated carbon YP17 were 158 F/g at 0.05 A/g and
only 109 F/g at 10 A/g. Obviously, the HPC-1 carbon owned
good capacitive performance at high currents and the effi-
ciency of the ion reach micropores was really high because
of the hierarchically porous structure.
The galvanostatic charge/discharge curves of HPC-1 at dif-
ferent current densities are shown in Fig. 6. It showed that
HPC-1 possessed typical triangular shapes with a little galva-
nostatic discharge decrease caused by the inner resistance
throughout the current range of 40–100 A g�1, indicating good
capacitive properties. The specific capacitances determined
by Csp = 2It/Vm are 139, 139 and 130 F g�1 with the current
of 40, 50, 100 A g�1 for HPC-1, respectively. The main reason
for the good performance at different charge/discharge rate
may be that the mesopores/macropores in HPC-1 sample
can improve the ion transfer and reduce the inner resistance
of the electrodes.
4. Conclusions
We report the fabrication and properties of novel hierarchical
porous carbon materials using animal bone natural template
and KOH activation, and its potential application as electrode
materials for EDLC. Structure and texture analysis reveal that
the porous carbon has high surface area (2157 m2/g), large pore
volume (2.26 cm3/g), hierarchical pore structure of abundant
interconnected micropores, mesopores and macropores and
graphitic structure. Electrochemical studies revealed superior
electrochemical performances of the porous carbon in KOH
electrolyte. Its specific capacitance is 185 F/g at a current den-
sity of 0.05 A/g and maintains 130 F/g at 100 A/g, demonstrat-
ing superior capacitive properties. The investigation provides
C A R B O N 4 9 ( 2 0 1 1 ) 8 3 8 – 8 4 3 843
a simple, powerful, sustainable and cost-effective method to
produce an advanced functional carbon materials with hierar-
chical porous structure, which could be an interesting candi-
date for not only energy storage but also other applications
such as biosensor and catalysis.
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