Abstract. Nanocomposites based on polyaniline (PANI) and montmorillonite (MMT) were prepared by in-situ polymerization of aniline monomers
using FeCl3 as oxidant in the presence of MMT. X-ray diffraction patterns
(XRD) showed that the obtained materials were in the nanostructures. The
chemical structure of PANI in nanocomposites were characterized by FTIR and Raman spectra. The thermal analysis (TGA) showed that PANI in
the nanocomposites was stable until 6000C. Adsorption properties of the
nanocomposites were investigated.
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JOURNAL OF SCIENCE OF HNUE
Natural Sci., 2008, Vol. 53, N
◦
. 5, pp. 104-109
POLYANILINE/MONTMORILLONITE NANOCOMPOSITES
FOR ADSORPTION PURPOSES
Vu Quoc Trung, Nguyen Van Thang
Pham Van Hoan and Nguyen Duc Chuy
Hanoi National University of Education
Abstract. Nanocomposites based on polyaniline (PANI) and montmoril-
lonite (MMT) were prepared by in-situ polymerization of aniline monomers
using FeCl3 as oxidant in the presence of MMT. X-ray diffraction patterns
(XRD) showed that the obtained materials were in the nanostructures. The
chemical structure of PANI in nanocomposites were characterized by FT-
IR and Raman spectra. The thermal analysis (TGA) showed that PANI in
the nanocomposites was stable until 6000C. Adsorption properties of the
nanocomposites were investigated.
1. Introduction
Conducting polymers are novel organic semiconducting materials with great
promise because of their wide range of potential technological applications [1]. This
includes their applications in electrochemical batteries, electrochromic devices, light
emitting diodes, non-linear optics, photovoltaic devices, FET circuits and LEDs [1],
as a corrosion inhibitor [2] and as a material for the electromagnetic interference
shielding [3]. The understanding of the nature of these polymers is of utmost impor-
tance for developing electrochemical devices. Among the conducting polymers, PANI
has been studied extensively due to the commercial availability of the monomer, its
easy synthesis, well-behaved electrochemistry, good environmental stability, high
conductivity and multiple redox and protonation states [1,4].
Normally intractable PANI can be made processable either by making it sol-
uble by doping it with organic sulfonic acids [4] or by the preparation of polyaniline
in colloidal form [5]. Polymeric as well as non-polymeric surfactants have been used
to make colloidal polyaniline. The presence of a surfactant or polyelectrolyte sig-
nificantly modifies both the microscopic and macroscopic properties of the final
polymer. Recently, the electrical and electrochemical properties of conducting poly-
mer/clay nanocomposites in which clay as organic surfactants have been studied and
nanocomposite materials have mainly been performed as corrosion inhibitors [6].
In this paper, the doped PANI/MMT nanocomposites were prepared by in-
situ polymerization using iron trichloride as an oxidant. Properties of the obtained
104
Polyaniline/montmorillonite nanocomposites for adsorption purpose
material were characterized by XRD, TGA, FT-IR and Raman spectra. The elec-
tromagnetic interference shielding of this nanocomposite was investigated.
2. Content
2.1. Experiments
2.1.1. Preparation of PANI/MMT nanocomposites
PANI/MMT nanocomposites were chemically prepared as the procedure de-
scribed in [5,7]. Firstly, a dispersion was prepared by mixing (for 30 min.) of 10.0 g
Na
+
-MMT (prepared from bentonite Dilinh-Vietnam as described in [7]) and 2.0 ml
aniline monomers in a mixture of 80.0 ml distilled water and 20.0 ml isopropanol.
Chloride acid was added into the suspension to obtain a medium of pH = 3. Then
7.5 g FeCl3 (water-free, Fluka Chemie) was added to the oxide particle dispersion
during stirring. The colour of the mixture was changed from grey to green black.
After 2 hours of stirring, the particles were cleaned by distilled water, filtered and
dried at 40 - 50
0
C for several days under low pressure.
2.1.2. Characterization of PANI nanocomposites
Thermal gravimetric analysis (TGA) was done by Ghimashu-50 H with scan
rate of 10
0
C/min in atmospheric condition. The X-ray diffraction patterns of MMT,
monomer-absorbed MMT and PANI/MMT nanocomposites were done by SIMENS
D-5005. The chemical structure of the nanocomposites was characterized by Fourier
transform infrared spectroscopy (FT-IR) and Raman spectroscopy. FT-IR spectra
were performed by GBC Cintra 40-Nicolet Nexus 670 FT-IR. Raman spectra were
measured by a Laser Raman Spectrophotometer (Ramalog 9I, USA). The electro-
magnetic shielding features of the nanocomposites were performed by HP8720D Net-
work Analyzer (USA).
2.2. Results and discussion
2.2.1. FT-IR and Raman scattering spectra
Table 1. Wavenumbers and assignments
of the Raman bands of PANI/MMT nanocomposites
Wavenumber (cm
−1
)
Soluble
PANI [8]
Oxidized
PANI/MMT
State Assignment
1626 - 1630 1620 (shoulder) I C-C ring stretching
1585 - 1600 1582 (strong) II C-C ring stretching
1506 - 1516 absence II C=N stretching
1480 - 1486 1490 (shoulder) II C=N stretching
1339 - 1349 1336 III and IV C-N
+
stretching
105
Vu Quoc Trung, Nguyen Van Thang, Pham Van Hoan and Nguyen Duc Chuy
1257 - 1266 1263 (weak) I C-N stretching
1190 - 1197 absence I C-H in-plane bending
1171 - 1174 1168 II C-H in-plane bending
885
890 (weak) I in-plane bending deformation
830 - 836 absence II in-plane bending deformation
800 - 815
819 II C-H out-of-plane bending
712 - 724 absence I C-H out-of-plane deformation
685 - 698 685 (weak) II C-H out-of-plane deformation
636 610 I in-plane ring deformation
511 - 526 510 out-of-plane C-N-C torsion
412 - 420 414 II out-of-plane C-H wag
PANI is usually produced by the anodic oxidation of aniline in acidic aqueous
solution (electrochemical polymerization), but can also be prepared by chemical
oxidation (chemical polymerization) [4]. Hence, it is not surprising that the oxidation
of PANI is pH-dependent. It is generally accepted that there are different, possibly
coexisting forms of PANI, including (I) benzoid form with free amine groups, (II)
quinoid form with imine groups, (III) protonic amines (bipolarons) and (IV) radical
cationic state (polarons) (Figure 1).
Figure 1. Structures of PANI [4]
Figure 2. Raman spectra of PANI/MMT
(nanocomposites measured at 514 nm
with power of 1 mW)
The typical Raman spectra of
PANI presents in a range of 1000-1700
cm
−1
[8]. Peaks corresponded to pure
leucoemeraldine base (I) are at 1620,
1263, 890 and 610 cm
−1
(Figure 2).
While all peaks related to the oxidized
emeraldine and pernigraniline base (II)
are very clear and strong such as a
peak at 1582 cm
−1
(C-C ring stretch-
ing) and 1168 cm
−1
(C-H in-plane bend-
ing). In addition, a peak at 1336 cm
−1
corresponds to emeraldine salt (III and
IV). These evidences show that PANI in
106
Polyaniline/montmorillonite nanocomposites for adsorption purpose
nanocomposites presents in both an oxidized state and a neutral one (Figure 2). Ta-
ble 1 gives the assignments of some typical Raman bands and it is in comparison
with the frequencies collected on soluble oxidized PANI [8].
Figure 3. FT-IR spectra
of PANI/MMT nanocomposites
The principal absorption bands
observed in the FT-IR spectra of
PANI/MMT powder (in KBr) is
given in Figure 3. In the region 1650
- 1400 cm
−1
to the aromatic ring
breathing, stretching N-H deforma-
tion and C-N are observed. Bands at
1563 and 1479 cm
−1
are the charac-
teristic bands of nitrogen benzenoid
and quinoid form and are present due
to the conducting state of PANI [4].
The band at 1154 cm
−1
is assigned
to be present due to the charge delo-
calisation on the polymer backbone.
The band at 3434 cm
−1
belongs to the N-H bonds and O-H groups adsorbed in the
material. The presence of the strong band at 1092 cm
−1
is attributed to MMT.
2.2.2. Thermal analyses
Figure 4. TGA curve
of PANI/MMT nanocomposites
Thermal analyses of PANI/MMT
nanocomposites are shown in Figure
4. Under 120
0
C, the weight reduction
originates from water inside samples.
The reduction (5%) in this tempera-
ture range can be explained by the
hydrophilic property of MMT and
the oxidized state of PANI. It is also
the source of the wide band between
3700 and 3000 cm
−1
in the FT-IR
spectra. In the range of 120 - 250
0
C,
the weight reduction is very small,
corresponding to the decomposition
of redundant monomers, oligomers.
At higher temperatures (350 - 700
0
C), the change of weight (20%) is attributed to the decomposition of PANI.
2.2.3. X-ray diffraction patterns
The XRD patterns of the materials before and after polymerization are shown
in Figure 5. At first, Na
+
-MMT was mechanically stirred for 30 min as reference.
107
Vu Quoc Trung, Nguyen Van Thang, Pham Van Hoan and Nguyen Duc Chuy
Figure 5. X-ray diffraction patterns
of MMT (A), monomer-absorbed MMT
(C) and PANI/MMT nanocomposites (B)
However, there are no changes in the
XRD patterns of MMT before and
after stirring. Therefore, the stirring
does not affect the crystalline of the
MMT itself. The diffraction peak of
Na
+
-MMT was observed at 2θ = 8.70,
thus, the basal spacing of Na
+
-MMT
was 1.10 nm (Figure 5A).
The intercalation of aniline
monomers into MMT is shown in Fig-
ure 5B. The basal spacing increased
from 1.10 nm to 1.54 nm , indicating
the expansion of the interlayer space
(d-expansion) by 0.44 nm; and the
successful intercalation by the mechanical intercalation method. The diffraction
peaks of the products after polymerization were shifted to a higher angle than those
before polymerization as shown in Figure 5C, indicating the synthesis of PANI in
the clay layers. As a result, the basal spacing of monomer-absorbed MMT changed
from 1.54 nm to 1.42 nm . They are in agreement with other publications [8].
2.2.4. Shielding effectiveness measurements
Shielding effectiveness is measured as the ratio of the field strength before and
after attenuation and is expressed in decibels (dB) calculated according to formula
as [6]:
SE = 10 log
Pt
Pi
(1)
where SE is the shielding effectiveness; p is the power in watt (i stands for
incident wave, t for transmitted wave).
Figure 6. SE data obtained with the samples of PANI/MMT coated fabrics
108
Polyaniline/montmorillonite nanocomposites for adsorption purpose
The shielding effectiveness as measured by coaxial transmission line method
from 8 to 12 GHz was studied. The result reveals that on using PANI/MMT nanocom-
posite - coated fabric, a shielding effectiveness of around 10 dB (99.9%) is obtained
(Figure 6). It can be explained by the shielding of the layered MMT in the com-
posites. However, for industrial applications, it was of modest value. Therefore, the
shielding effectiveness of these nanocomposites must be improved for a best perfor-
mance of possible applications
3. Conclusion
In this paper, the PANI/MMT nanocomposites were prepared by chemical
polymerization. X-ray diffraction patterns show that the composites are obtained
with nanostructure. The chemical structure of PANI in nanocomposites were charac-
terized by FT-IR and Raman spectra. They showed the same signals in comparison
with that of the soluble PANI prepared by chemical polymerization. The thermal
analysis showed that PANI in the nanocomposites was stable at around 600
0
C. The
shielding effectiveness of the PANI/MMT nanocomposite - coated fabric measured
in the range of 8 - 12 GHz, was in the order of -10 dB. However, for industrial
applications, it was of modest value. Therefore the shielding effectiveness of these
nanocomposites must be improved for possible applications. New results of these
materials will be updated in the next publication.
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