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ISSN: 0973-4945; CODEN ECJHAO E-Journal of Chemistry
http://www.ejchem.net 2012, 9(4), 2332-2337
Synthesis and Characterization of Boron
Trifluoride Doped High Performance Polyaniline
K. BASAVAIAH1*
, D. SAMSONU2, AND A. V. PRASADA RAO
1
1Department of Inorganic and Analytical Chemistry, Andhra University, Visakhapatnam-
530003, India 2Departments of Organic, Foods, Drugs and Water, Andhra University, Visakhapatnam-
530003, India
Received 28 July 2011; Accepted 4 October 2011
Abstract: We report simple synthesis of boron trifluoride (BF3) doped defect
free high performance polyaniline (HPPANI) in two step method. Firstly,
HPPANI was prepared via self-stabilization dispersion polymerization method
in a heterogeneous reaction medium. Second step involves doping of
emeraldine base form of HPPANI with boron trifluoride under reduced vacuum.
The resultants BF3 doped HPPANI have been well characterized by using UV-
Visible spectroscopy, Fourier transform infrared spectroscopy (FTIR), scanning
electron microscopy (SEM) and thermogravimetry. The spectroscopic data
indicated that the interaction between HPPANI and BF3.Thermogravimetry
studies revealed that the BF3 doping improved the thermal stability of defects
free PANI.
Keywords: Conducting polymers; High performance PANI; Doping; Boron trifluoride; Thermal stability.
Introduction
Conducting polymers have attracted increasing attention because they offers the possibility
of generation of novel materials with diverse applications for electromagnetic interference
(EMI) shielding, rechargeable battery, chemical sensor, organic light emitting devices,
corrosion devices, and microwave absorption1–5
. Among conducting polymers, polyaniline
(PANI) is the promising electrical conducting polymer due to its a broad range of tunable
properties derived from its structural flexibility, good environmental stability, easy
preparation in aqueous solution, and organic solvents, optical, electrical properties and
unique redox chemistry6-7
. Moreover, PANI exhibits a large spin density so interesting
electrical and magnetic properties arise that are highly dependent on the doping level and the
structure of the polymer. However, PANI suffers from poor processability because it is
infusible and insoluble in common solvents.
mailto:[email protected]
Synthesis and Characterization of Boron Trifluoride Doped 2333
PANI synthesized in standard Mac Diarmid method8, the macroscopic precipitation
polymerization of aniline occurs at the interface of growing particles and the aqueous
reaction medium and also inside the swollen particles. The resulting PANI has defects due to
a randomly branched backbone, some cross linking, ortho-coupling, and Michael reductive
addition of aniline9. To prevent the undesired side reaction and macroscopic precipitation,
several methods have been developed and the most effective method is self-stabilized
dispersion polymerization in a heterogeneous medium. A defect free PANI was prepared by
self-stabilized dispersion polymerization method in heterogeneous medium10
. The rationale
behind this method is that the organic phase acts to separate the insoluble aniline oligomers
and grow PANIchains from the reactive ends of the chains in the aqueous phase. Thus
prevent the macroscopic precipitation and undesired side reactions.
In this study, we reoprt synthesized defect free PANI via self-stabilized dispersion
polymerization method in heterogeneous reaction medium. The emeraldine base form of
defect free PANI was doped with boron trifluoride (BF3) by using BF3-etharate complex
under control atmosphere.
Experimental
Aniline, Boron trifluoride- Etherate (BF3-Etherate), Ammonium persulphate [APS,
(NH4)2S2O8], Chloroform, Methanol, Sodium hydroxide (NaOH) were obtained from Merck
Chemicals, India and used as received. Aniline was double distilled under reduced vacuum
and stored at 0-5 oC before use. Double distilled water was used throughout all the synthetic
processes. All other reagents were analytical grade and used without further purification.
Synthesis of High performance Polyaniline (HPPANI)
In typical synthesis, aniline solution in 1M HCl was added to a chloroform / water mixer
(1:2 vol./vol.) and stirred at -16 0C until the solution became colloidal dispersion. A pre-
cooled acidic solution of oxidant, ammonium persulfate, (APS) was added drop wise to the
colloidal dispersion, with rigorous stirring. The polymerization reaction was preceded for
another 12 hours at -16 0C. The colloidal dispersion slowly tuned to the dark green colour
characteristic of PANI. The reaction mixture was filtered, washed with water and methanol
periodically to remove unreacted reagents. Finally, dedoped with 0.5 M NaOH solution and
dried under dynamic vacuum at room temperature.
Preparation of Boron Trifluoride (BF3) Doped High Performance Polyaniline
EB form of HPPANI powder was doped with boron trifluoride (BF3) using boron trifluoride-
etharate complex under anhydrous condition because high susceptibility of BF3 towards
hydrolysis, doping was carried out strictly anhydrous conditions. BF3-Etherate, 1:1 complex
of BF3 and diethyl ether was used for doping. In order to reduce the exposure to atmosphere,
BF3-etherate was distilled in vacuum and distillate was collected directly over the
emeraldine base HPPANI powder. The reactivity of BF3 in BF3 –etherate complex is
remarkably reduced, makes it a lot easier to handle. In order to achieve maximum doping,
excess dopant was added and reaction mixture was left to equilibrate for 24 hours and after
which un-reacted BF3 -etherate was removed under dynamic vacuum at room temperature.
Pumping for longer period of time, leads to partial dedoping.
Characterization
The UV-Visible absorption spectra of the samples were recorded on a Perkin-Elmer double
beam LS-50 spectrophotometer. The samples were dissolved in dry dimethylsulphoxide
(DMSO) and centrifuged to remove any undissolved polymer. The clear solutions were
taken in quartz cuvettes. The infrared spectra were recorded over the range 4000 - 400 cm-1
K. BASAVAIAH et al. 2334
in a Perkin-Elmer Model SPECTRUM 1000 FTIR spectrometer. The powdered samples
were mixed thoroughly with KBr and pressed into thin pellets. Morphology of BF3 doped
HPPANI was examined by scanning electron microscopy (SEM).
Results and Discussion
PANI can be considered as Lewis base due to a lone electron pair on Nitrogen atoms of
PANI. Recently, it was evidenced that the PANI can be doped with Lewis acids and forms
acid- base complexes11
. Like other Lewis acids, BF3 can also form a complex with PANI.
The general structure of PANI doped with Lewis acid (LA) is presented in figure1. Similarly
to the case of protanation, one molecule of dopant is coordinated to nitrogen atom of PANI,
but contrary to the protation, both types of nitrogen atoms of PANI( amine as well as imine
ones) are coordinated by LA. In this case of the formation of a covalent or mixed ionic
covalent bond was proposed. The structures of Lewis acid doped PANI is differ significantly
from those of protanated PANI. Lewis acid-doped PANI systems are expected to be
different from the conventional protonated PANI owing to a qualitatively different chemical
interaction between the dopant and the polymer; for instance, the absence of any counter ion
in these systems may have different influence on the properties. Thus spectroscopic
properties of BF3 doped PANI systems differ from those of protonated PANI.
HN
N
N
HN
N
N
N
LA
LA
LA
NH
LA Figure 1. Chemical structure of Lewis acid (BF3) doped emaraldine base PANI.
Molecular structure of BF3 doped HPPANI was investigated by UV-Visible
spectroscopy and Fourier-transform infrared (FTIR) spectroscopy. UV-Visible absorption
spectra for both undoped HPPANI and BF3 doped HPANI shown in Figure 2. Undoped
HPANI gives two electronic absorption bands at 330 nm and 630 nm approximately. The
broad absorption feature at 630 nm has been assigned to quinoid formation in the backbone
of the PANI, while the band at 330 nm is assigned to the π →π* electronics transition of
benzenoid rings in the HPPANI. In case of BF3 doped HPANI, new absorption bands
appears at 450 nm and 830 nm. These features confirmed the BF3 doping to HPPANI. It is
important to note that the same changes have also been observed in the case of proton doped
PANI12-13
.
LA
Synthesis and Characterization of Boron Trifluoride Doped 2335
Abso
rpti
on
Figure 2. UV-Visible spectra of (a) undoped HPPANI (b) BF3 doped HPPANI.
Figure 3 shows FTIR spectrum for BF3 doped high performance polyaniline, which well
agreed with the previous literature14-18
.
Figure 3. FTIR spctrum for BF3 doped HPPANI.
The FTIR spectrum gives main characteristic peaks at 3180, 1595, 1496, 1408, 1313,
and 827 cm-1
. Peaks at 3180, 1595, and 1496 cm-1
due to N-H stretching vibration, C=C
stretching of quinoid phenyl and benzenoid phenyl rings, respectively. The peak at 1408 cm-1
is due to stretching frequency of B-N=Q moiety (B refers to benzenoid and Q refers to
quinoid ring). The presence of this peak confirms that the HPPANI is doped with BF3. The
peak at 1313 cm-1
is assigned to C-N stretching vibrations of the 1, 4- disubstituted benzene
ring of HPPANI. The peak at 827 cm-1
corresponds to C-H out of plane bending of
1, 4-disubstituted benzene rings of HPPANI.
Figure 4. Scanning electron microscopy (SEM) images of for BF3 doped HPPANI.
Wavelength/nm
Wavenumber
K. BASAVAIAH et al. 2336
Morphology of BF3 doped high performance PANI was investigated by scanning electron
microscopy. SEM images of BF3 doped HPPANI is shown in Figure 4. SEM images
illustrate the synthesized HPPANI particles morphologies at a variety of dimensional levels.
Figure 5 shows a TG –DTG curve of BF3 doped HPANI prepared via self-Stabilized
dispersion polymerization of aniline under N2 flow at a heating rate of 200C per minute
from 50-8500C. The first region at lower temperatures (
Synthesis and Characterization of Boron Trifluoride Doped 2337
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