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www.elsevier.com/locate/micromeso
Microporous and Mesoporous Materials 83 (2005) 262–268
Mesoporous silica framed by sphere-shaped silica nanoparticles
Dong-Wook Lee a,b, Son-Ki Ihm b, Kew-Ho Lee a,*
a Membrane and Separation Research Center, Korea Research Institute of Chemical Technology,
P.O. Box 107, Yuseong, Daejeon 305-606, South Koreab Department of Chemical and Biomolecular Engineering, National Research Laboratory for Environmental Catalysis,
Korea Advanced Institute of Science and Technology, 373-1 Guseong-dong, Yuseong-gu, Daejeon 305-701, South Korea
Received 1 July 2004; received in revised form 23 December 2004; accepted 6 May 2005
Available online 16 June 2005
Abstract
Organic template-derived mesoporous silica with narrow pore size distribution was prepared through a colloidal silica–citric acid
system. Colloidal silica sol with 5 nm in particle diameter was firstly prepared under base-catalyzed condition via hydrolysis of tet-
raethyl orthosilicate (TEOS) and condensation reaction. Subsequently, colloidal silica–citric acid nanocomposite solution was syn-
thesized by addition of citric acid to the as-prepared colloidal silica sol. After the elimination of citric acid via thermal treatment at
500 �C, the mesoporous silica was successfully obtained, and its pore size was easily controlled in the range from 2 nm up to 15 nm
maintaining the narrow pore size distribution, the high specific surface area (800–900 m2/g) and the pore volume (0.6–1.4 cm3/g).
Comparing with a polymeric silica–citric acid system, the colloidal silica–citric acid system showed an increase in the controllable
pore size and the structural stability. The sphere-shaped silica nanoparticles as a framework with highly branched structure led to
the rigid structure of the framework and the thicker pore wall, suppressing the shrinkage of the silica structure in spite of the large
vacancy produced by the removal of citric acid.
� 2005 Elsevier Inc. All rights reserved.
Keywords: Mesoporous silica; Silica nanosphere; Citric acid; Nanocomposite
1. Introduction
Mesoporous silicates such as MCM-41 [1,2] with high
surface area and sharp pore size distribution have at-
tracted great technological and scientific interest since
1992 [3–7]. A sharp pore size distribution of MCM-41
in mesoscale, which is induced by a hexagonal array ofionic surfactants, is considered to provide molecular
recognition ability for large organic compounds. The
mesoporous materials are generally prepared with ionic
[7–9] or neutral [10–13] surfactants as a structure-direct-
ing agent, and the pore size of those materials is adjusted
by changing the structure and size of the surfactant
1387-1811/$ - see front matter � 2005 Elsevier Inc. All rights reserved.
doi:10.1016/j.micromeso.2005.05.004
* Corresponding author.
E-mail address: [email protected] (K.-H. Lee).
molecules. Recently, Wei et al. and Takahashi et al. have
reported a novel preparation method of the mesoporous
silica via the non-surfactant templating route using
polymeric silica framework [14–19]. They synthesized
the amorphous silica framework from acid-catalyzed
sol–gel reaction of tetraethyl orthosilicate (TEOS), and
used non-surfactant organic compounds as a templatingagent such as D-glucose, D-maltose, dibenzoyl-L-tartaric
acid, citric acid, malic acid, lactic acid and tartaric acid.
After the elimination of the non-surfactant organic com-
pounds via solvent extraction [16] or thermal treatment
[19], the mesoporous silica was synthesized, and its pore
size was controlled in the range from 2 nm to 6 nm,
combined with high surface area and pore volume. In
addition, Takahashi et al. [19] proved the pore forma-tion mechanism of the mesoporous silica via the poly-
meric silica–citric acid system.
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D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268 263
In this paper, we used colloidal silica nanoparticles
as a framework, synthesized from the base-catalyzed
sol–gel reaction of TEOS, to fabricate the mesoporous
silica with citric acid as a templating agent. Comparing
with the polymeric silica–citric acid system, the pore
properties of the mesoporous silica derived from colloi-dal silica–citric acid system were observed by investigat-
ing pore size distribution, specific surface area and pore
volume, obtained by nitrogen adsorption/desorption
isotherms. It is well-known that the colloidal silica clus-
ters show different shape and structure from the poly-
meric silica. We discussed the effect of such structure
of the colloidal silica nanoparticles on the pore structure
of the mesoporous silica.
2. Experimental
2.1. Synthesis of mesoporous silica via a polymeric
silica–citric acid system
Polymeric silica sol was synthesized under acid-cata-lyzed condition via hydrolysis of tetraethyl orthosilicate
(TEOS) and condensation reaction. A molar ratio of
TEOS, water and nitric acid was 1:5.8:0.083. A mixture
of TEOS, water and nitric acid was stirred at room tem-
perature for 20 min. The reaction mixture was diluted
with additional water to adjust the volume to 500 ml,
and refluxed for 8 h at 80 �C [20]. Polymeric silica–citric
acid nanocomposite solution was prepared by addition
Fig. 1. Preparation procedures of the mesoporous silica through (a) a polym
of citric acid to the as-prepared polymeric silica sol,
which is similar to the method previously reported by
other research groups [16,19]. The nanocomposite solu-
tion was stirred vigorously at room temperature for
10 min. Drying and calcination were carried out at
70 �C and 500 �C, respectively. Fig. 1a shows the proce-dure for synthesis of the mesoporous silica via the poly-
meric silica–citric acid system.
2.2. Synthesis of mesoporous silica via a colloidal
silica–citric acid system
Transparent colloidal silica sol was synthesized from
base-catalyzed condition at a TEOS:NH3:H2O:EtOHmolar ratio of 1:0.086:53.6:40.7. Prior to the addition
of the NH3/H2O mixture, the TEOS/ethanol mixture
was stirred vigorously at 50 �C. The addition of NH3/
H2O was carried out dropwise, followed by refluxing
the mixture for 3 h, resulting in the stable colloidal silica
sol including sphere-shaped silica nanoparticles with
5 nm in diameter. Subsequently, various concentrations
of citric acid were added to the as-prepared colloidal sil-ica sol, and the mixture was stirred vigorously at room
temperature for 10 min, followed by drying the solution
at 70 �C for 24 h. The citric acid surrounded by the silica
framework was removed by calcination at 500 �C for
2 h. The procedure for synthesis of the mesoporous sil-
ica via the colloidal silica–citric acid system is schemat-
ically shown in Fig. 1b.
eric silica–citric acid system and (b) a colloidal silica–citric acid system.
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264 D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268
2.3. Characterization
Nitrogen adsorption/desorption isotherms of the
mesoporous silica were taken by a micromeritics ASAP
2400 instrument. Pore size distribution curves were
obtained from the desorption branch by using theBarrett–Joyner–Halenda (BJH) method. The XRD
patterns taken by a Rigaku D/MAX-2200V instrument
(operated at 1.6 kW) were utilized to investigate the
crystallization of citric acid in silica–citric acid nano-
composites [19]. For TEM analysis of the mesoporous
silica synthesized via the colloidal silica–citric acid nano-
composite, the samples were prepared by spin-coating
the nanocomposite solution on a Mo grid, followed bycalcination at 500 �C. TEM analysis was carried out
by using a Carl Zeiss EM912X instrument (operated at
120 kV). Cross polarization magic angle spinning (CP/
MAS) 29Si NMR spectra of the dried and calcined nano-
composites were taken by a Bruker DSX300 instrument.
Thermal gravimetry and differential thermal analysis
(TG–DTA) of the dried colloidal silica–citric acid nano-
composite was conducted at a heating rate of 10 �C/minunder a flow of air on a TA instrumental, SDT2960.
Fig. 2. A TEM image of sphere-shaped silica nanoparticles in the
transparent colloidal silica sol. Sphere-shaped silica nanoparticles
below 5 nm were obtained under base-catalyzed condition.
3. Results and discussion
3.1. Pore properties of mesoporous silica derived
from the colloidal silica–citric acid system
We report the synthesis method for the organic tem-
plate-derived mesoporous silica with narrow pore size
distribution and freely controlled pore size by using
sphere-shaped colloidal silica nanoparticles as a frame-
work. When we use the colloidal silica–citric acid sys-
tem, the pore size can be easily tailored from 2 to
15 nm maintaining narrow pore size distribution, high
surface area and pore volume. The easy control of poresize up to 15 nm is attributed to the highly branched
structure of the colloidal silica nanoparticles, which
gives rise to rigid structure and good thermal stability
of the silica framework, suppressing the shrinkage of sil-
ica framework in spite of the large vacancy produced by
the removal of citric acid as a template. The addition of
citric acid, which acts as a template and not an acid cat-
alyst for the sol–gel reaction of TEOS, to the silica solsleads to the formation of silica–citric acid nanocompos-
ites, and the space among the silica frameworks is filled
with the amorphous citric acid. However, at excess con-
centration of citric acid more than the saturated concen-
tration, the change in pore properties of the silica, such
as an increase in pore size with the concentration of cit-
ric acid, is not observed, because the citric acid not occu-
pying the volume among the silica frameworks iscrystallized [16,19]. In addition, when the organic tem-
plate is eliminated by thermal treatment, unexpected
shrinkage of the silica framework could partially or to-
tally occurs, which results in broad pore size distribution
or the restriction of the pore size control.
In this study, the limitation of pore size control in the
silica–citric acid system has been overcome by using col-
loidal silica nanoparticles as a framework due to thedenser structure of the primary particle of the colloidal
silica than that of the polymeric silica. Transparent col-
loidal silica sol with sphere-shaped silica nanoparticles
was synthesized under base-catalyzed condition via
hydrolysis of tetraethyl orthosilicate (TEOS) and con-
densation reaction. Fig. 2 shows a TEM image of the
transparent colloidal silica sol. Sphere-shaped silica par-
ticles with uniform particle size below 5 nm were ob-tained under base-catalyzed condition with low
concentration of NH3 as a catalyst. For comparison
with the colloidal silica system, polymeric silica sol
was also prepared under acid-catalyzed condition. Var-
ious concentrations of citric acid as a template were sim-
ply added to the as-prepared silica sols, and the mixture
was stirred vigorously at room temperature for 10 min.
The solution was dried at 70 �C, followed by the elimi-nation of citric acid via thermal treatment at 500 �C.In the case of the polymeric silica–citric acid system,
the pore size of the mesoporous silica was increased
up to 6 nm with an increase of the molar ratio of citric
acid to polymeric silica in the solution of the polymeric
silica–citric acid nanocomposite, designated as CA/PS
(see Fig. 3a). The specific surface area and total pore
volume (obtained by the nitrogen adsorption isothermfollowing the BJH method) was nearly constant over
the range of 1000–1200 m2/g and was increased from
0.6 cm3/g to 1.4 cm3/g, respectively. However, the in-
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Fig. 3. Pore size distributions of the mesoporous silica prepared by
using (a) the polymeric silica–citric acid system and (b) the colloidal
silica–citric acid system. (c) N2 adsorption/desorption isotherms of the
mesoporous silica synthesized via the colloidal silica–citric acid system.
Fig. 4. The XRD patterns for (a) the dried polymeric silica–citric acid
nanocomposite at CA/PS = 0.97 and (b) the dried colloidal silica–citric
acid nanocomposite at CA/CS = 0.97.
D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268 265
crease in pore size and total pore volume was restricted
at CA/PS = 0.97. Maximum controllable pore size is
about 6 nm, and further increase of pore size is consid-
ered to be impossible due to the saturation of citric acid
(at CA/PS = 0.97) in the space surrounded by the silica
frameworks (see Figs. 3a and 4a). As shown in Fig.
4a, there are diffraction peaks corresponding to citric
acid crystals in the dried polymeric silica–citric acid
nanocomposite at CA/PS = 0.97. In the case of the col-
loidal silica–citric acid system, the pore size of the meso-
porous silica was surprisingly increased from 2 to
15 nm with an increase in the molar ratio of citric acid
to colloidal silica, designated as CA/CS. Although the
pore size of the mesoporous silica became larger up to15 nm, sharp pore size distribution was successfully
maintained (Fig. 3b). The specific surface area was
nearly constant over the range of 800–900 m2/g, and
total pore volume was increased from 0.6 cm3/g to
1.4 cm3/g with the increase in the CA/CS ratio. Due to
a little increase in wall thickness of the mesoporous silica
induced by larger diameter of the primary particles of the
colloidal silica, the specific surface area was somewhatsmaller than that of the mesoporous silica derived from
the polymeric silica–citric acid system, however the spe-
cific surface area is still high. Fig. 3c shows N2 adsorp-
tion/desorption isotherms of the mesoporous silica
synthesized from the colloidal silica–citric acid nanocom-
posites. All of the samples give typical type IV isotherms
with a H2 hysteresis loop as defined by IUPAC [21]. A
type H2 hysteresis loop is commonly associated withink-bottle pores or voids between close-packed spherical
particles. When the CA/CS ratio increased, an increase
in total pore volume was observed, and the sharp inflec-
tion of the hysteresis loop shifted toward higher P/Po
values, indicating that pore diameter of the mesoporous
silica increased. Fig. 4b shows that the saturation of cit-
ric acid in the colloidal silica–citric acid nanocomposite
occurred at CA/CS = 0.97. Comparing with the poly-meric silica, a ratio of Si interacting with CA to Si not
interacting with CA is smaller in the case of sphere-
shaped colloidal silica, because Si in the core of the silica
sphere substantially exists without interaction with CA.
Although the citric acid saturation for both polymeric
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Fig. 6. The XRD patterns of the dried colloidal silica–citric acid
nanocomposites: (a) at CA/CS = 0.46 and (b) at CA/CS = 0.74. A
broad halo of amorphous silica indicates that the amorphous silica–
citric acid nanocomposite was formed.
266 D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268
silica and colloidal silica system occurred at CA/
Si = 0.97, considering a ratio of citric acid to the surface
silanol groups interacting with citric acid, the saturated
concentration of citric acid for the colloidal silica–citric
acid system is actually higher than that for the polymeric
silica–citric acid system. Therefore it is concluded thatthe increase in the saturated concentration of citric acid
contributed to the pore size tuning up to 15 nm via the
colloidal silica–citric acid system. Fig. 5 shows TEM
images of the mesoporous silica synthesized at different
CA/CS ratio. There are a number of regular mesopores
surrounded by the sphere-shaped silica nanoparticles
with highly branched structure.
3.2. Pore formation via the colloidal silica–citric acid
system
Under acid-catalyzed condition, the rate of hydroly-
sis is large compared to the rate of condensation. After
monomers are depleted, condensation between com-
pletely hydrolyzed species occurs by cluster–cluster
aggregation leading to weakly branched structures ofprimary silica particles with low fractal dimension. On
the contrary, under base-catalyzed condition, dissolu-
tion and redistribution reactions provide a continual
source of monomers which condense preferentially with
clusters rather than each other. Therefore growth occurs
primarily by monomer–cluster aggregation resulting in
highly branched primary particles with high fractal
dimension [22]. The highly branched structure of the col-loidal silica leads to rigidity of the silica framework,
making it possible to maintain the sharp pore size distri-
bution, high surface area and pore volume during calci-
nation of the colloidal silica–citric acid nanocomposite.
That is, even though the diameter of the space occupied
with citric acid was 15 nm large, sphere-shaped silica
nanoparticles with highly branched structure led to the
Fig. 5. TEM images of the calcined colloidal silica–citric acid nanocompos
prepared by spin-coating the nanocomposite solution on a Mo grid, followe
protection of the silica frameworks against the shrink-
age during calcination.
Below the saturated concentration of citric acid, the
addition of citric acid to the as-prepared colloidal silica
sol leads to the formation of an amorphous silica–citric
acid nanocomposite without crystallization of citric acid(Fig. 6). In the nanocomposite, a little attractive interac-
tion between citric acid and silica is induced by weak
hydrogen bonding of surface silanol groups with hydro-
xyl groups in citric acid. Because the strength of the
hydrogen bonding is not so strong to prevent additional
condensation of the silanol during calcination, the silica
gel can obtain high rigidity leading to the maintenance
of the bulky mesoporous structure without shrinkageof the framework [19]. In order to confirm the absence
ites: (a) at CA/CS = 0.16 and (b) at CA/CS = 0.46. The samples were
d by calcination at 500 �C.
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Fig. 8. Thermal gravimetry and differential thermal analysis (TG–
DTA) profile of the dried colloidal silica–citric acid nanocomposite at
CA/CS = 0.46.
D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268 267
of any strong interaction between colloidal silica and cit-
ric acid which can inhibit condensation of the silanol
during calcination, cross polarization magic angle spin-
ning (CP/MAS) 29Si NMR was used (Fig. 7). The signals
around �90, �100 and �110 ppm are assigned to Si in
Q2 (Si(OSi)2(OH)2), Q3 (Si(OSi)3OH) and Q4 (Si(OSi)4),respectively [23]. There is relatively small difference be-
tween CP/MAS 29Si NMR spectra of the dried colloidal
silica (Fig. 7a) and those of the dried colloidal silica–cit-
ric acid nanocomposite (Fig. 7c), because any strong
interaction except for weak intermolecular hydrogen
bonding does not arise. After calcination at 500 �C for
2 h, both the colloidal silica and the colloidal silica–citric
acid nanocomposite show a decrease in Q2 and Q3 signaland an increase in Q4 signal due to additional condensa-
tion of the silanol groups during calcination. However,
comparing with CP/MAS 29Si NMR spectra of the cal-
cined colloidal silica (Fig. 7b), the smaller Q4 signal was
observed for the calcined colloidal silica–citric acid
nanocomposite (Fig. 7d). It means that part of the sila-
nol groups forming hydrogen bonding with the hydroxyl
group in citric acid does not participate in condensationduring calcination [19]. Thermal gravimetry and differ-
ential thermal analysis (TG–DTA) of the dried nano-
composite shows the endothermic peak at 190 �C and
Fig. 7. Cross polarization magic angle spinning (CP/MAS) 29Si NMR
spectra: (a) The dried colloidal silica. (b) The colloidal silica calcined at
500 �C for 2 h. (c) The dried colloidal silica–citric acid nanocomposite
at CA/CS = 0.59. (d) The colloidal silica–citric acid nanocomposite
(CA/CS = 0.59) calcined at 500 �C for 2 h.
the exothermic peak at 390 �C (Fig. 8). The endothermic
peak represents the elimination of the citric acid without
interaction with the colloidal silica, and the exothermic
peak corresponds to the decomposition of the citric acid
interacting with the colloidal silica. As a result, pore for-
mation mechanism of the mesoporous silica through the
colloidal silica–citric acid system is nearly consistentwith that via the polymeric silica–citric acid nanocom-
posites, which has been proved by Takahashi et al.
[19]. Consequently, although it is considered that pore
formation procedure of the colloidal silica–citric acid
system is nearly identical to that of the polymeric sil-
ica–citric acid system, extension of the range of control-
lable pore size via the silica–citric acid system was
successfully achieved through substitution of the colloi-dal silica nanoparticles as a framework for the polymeric
silica.
4. Conclusions
The pore size of the mesoporous silica was easily con-
trolled up to 15 nm maintaining narrow pore size distri-bution, high specific surface area and pore volume by
using the colloidal silica–citric acid system. For the poly-
meric silica–citric acid system, controllable pore size was
restricted to 6 nm, and further increase in pore size was
not observed due to the saturation of citric acid. The
range of controllable pore size for the citric acid tem-
plate-derived mesoporous silica was successfully ex-
tended through substitution of the sphere-shaped silicananoparticles as a framework for the polymeric silica,
because the saturated concentration of citric acid for
the colloidal silica–citric acid system is relatively higher
than that for the polymeric silica–citric acid system. In
addition, the highly branched structure of the colloidal
silica nanoparticles gave rise to rigidity of the silica
framework, resulting in maintaining the sharp pore size
distribution, high surface area and pore volume during
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268 D.-W. Lee et al. / Microporous and Mesoporous Materials 83 (2005) 262–268
the pore size tuning up to 15 nm. This material is
potentially expected to be applied to selective catalysis,
chemical sensing, molecular engineering, biochemical
separation and membrane technology.
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