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Author's personal copy
Thermochimica Acta 502 (2010) 43–46
Contents lists available at ScienceDirect
Thermochimica Acta
journal homepage: www.elsevier.com/locate/tca
Thermo-analyses of polyaniline and its derivatives
William F. Alvesa,b
, Everaldo C. Venancioc,∗
, Fabio L. Leited
, Darcy H.F. Kandae
,
Luiz F. Malmongee
, José A. Malmongee
, Luiz H.C. Mattosoa,b
a
EMBRAPA Instrumentac¸ ão Agropecuária, C.P. 741, São Carlos (SP), 13560-970, Brazil
b
Dept. Química, Universidade Federal de São Carlos (UFSCar), São Carlos (SP), 13565-905, Brazil
c
Centro de Engenharia, Modelagem e Ciências Sociais Aplicadas (CECS), Universidade Federal do ABC (UFABC), Santo André (SP), 09210-170, Brazil
d
Universidade Federal de São Carlos (UFSCar), C.P. 3031, Sorocaba (SP), 18052-780, Brazil
e
Dept. Física e Química, Universidade Estadual Paulista Julio de Mesquita Filho, Ilha Solteira (SP), 15385-000, Brazil
a r t i c l e i n f o
Article history:
Received 21 August 2009
Received in revised form 6 January 2010
Accepted 2 February 2010
Available online 16 February 2010
Keywords:
Polyaniline
DSC
TGA
Poly(o-methoxyaniline)
Poly(o-ethoxyaniline)
a b s t r a c t
In this work, is presented the thermal behavior of polyaniline (PANI) and its derivatives poly(o-
ethoxyaniline) (POEA) and poly(o-methoxyaniline) (POMA), which were studied by using differential
scanning calorimetry (DSC), modulated DSC (TMDSC), respectively, and thermal gravimetric analysis
(TGA). The results from diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) and thermal
analysis showed the formation of crosslinking isomerization reaction during the heating process. The
results showed that the maximum weight loss and the crystallinity degree depend on the type of the
aromatic ring substituent group, i.e. hydrogen, ethoxy or methoxy.
© 2010 Elsevier B.V. All rights reserved.
1. Introduction
Polyaniline (PANI) and its derivatives, e.g., poly(o-
methoxyaniline) (POMA) and poly(o-ethoxyaniline) (POEA)
[1,2] have been intensively studied due to their electrical and
optical properties associated with low costs, easy processabil-
ity, its environmental stability and relatively simple method of
synthesis [3,4]. The thermal analysis of conducting polymers,
i.e. PANI, POMA and POEA, is crucial to define their performance
on application processes of these materials [5]. Thus, thermal
analysis of conducting polymers provides important information
about the effect of morphological structure and other process,
such as chemical reaction, which are sensitive to thermal effects
(temperature changes), e.g., crosslinking reaction processes among
PANI chains. These processes have been studied by differential
scanning calorimetry (DSC) [6–8] and dynamical mechanical
thermal analysis (TDMTA) [9–12].
In this work, the glass transitions (Tg) for the chemically synthe-
sized non-conducting form of PANI, POMA and POEA, in the powder
∗ Corresponding author at: Centro de Engenharia, Modelagem e Ciências Sociais
Aplicadas (CECS), Universidade Federal do ABC (UFABC), Rua Santa Adélia 166, Bairro
Bangu, Santo André (SP), 09210-170, Brazil. Tel.: +55 11 49963166;
fax: +55 11 49963166.
E-mail address: everaldo.venancio@ufabc.edu.br (E.C. Venancio).
form, were studied using modulated DSC (MDSC). The hypothesis of
that a chemical crosslinking reaction occurs during the heating pro-
cess was further confirmed by supporting experimental methods
such as diffuse reflectance infrared Fourier transform spectroscopy
(DRIFTS), DSC and TGA.
2. Experimental
PANI, POMA and POEA were chemically synthesized accord-
ing to the method described in the literature [13,14]. The polymer
obtained was a dark precipitate, with expected average molecular
weight (MW) of ∼41,400 g mol−1 and polydispersivity (MW/Mn) of
2.3. Dedoping was performed by treatment with a 0.1 M ammo-
nium hydroxide aqueous solution for 16 h at room temperature
(∼25 ◦C) to yield the polymer in the emeraldine base form (EB). The
polymer was then transferred to a glass desiccator without desic-
cant agent and then dried under dynamic vacuum for 24 h at room
temperature (∼25 ◦C).
A model Q 600 TA Instruments TGA was used to investigate
the thermal stability of the polymers in the powder form in the
temperature range from 25 to 900 ◦C, under N2 gas atmosphere
(50 ml/min), for the thermal treatment the system was first equi-
librated at 220 ◦C for 1 h under N2 gas atmosphere (50 ml/min).
After the thermal treatment of PANI (EB), POMA (EB) and POEA (EB)
the DRIFTS spectra were performed on a fully computerized Nico-
let NEXUS® 670 using the software OMNIC. All the DRIFTS spectra
0040-6031/$ – see front matter © 2010 Elsevier B.V. All rights reserved.
doi:10.1016/j.tca.2010.02.003
Author's personal copy
44 W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46
were recorded on a Nicolet NEXUS® 670 spectrometer at a resolu-
tion of 1 cm−1 and using 64 scans. The temperature ramp used was
10 ◦C/min. In all experiments, PANI and its derivatives were present
in equal amount, the total weight being at about 8.0 ± 1.0 mg. The
thermal treatment of the EB powder was carried out by using a 2920
DSC Thermal Analysis under nitrogen gas purge (50 ml/min) and a
heating rate of 10 ◦C/min, where the system was first equilibrated
at −50 ◦C and then heated up to 150 ◦C. After the first run with the
equipment on the DSC mode, the DSC Thermal Analysis equipment
was switched to the TMDSC mode and then all subsequent runs
were done with the DSC Thermal Analysis equipment in the mod-
ulated DSC (TMDSC) mode by using a 2920 modulated DSC. The
TMDSC experiments were carried out as follows: the system was
first equilibrated at −50 ◦C for 5 min, and then it was heated up to
150 ◦C using a heating rate of 5 ◦C/min with a period modulation of
60 s, and the temperature amplitude of modulation was ±1.0 ◦C.
The as prepared powder of the EB form of the samples, i.e.
PANI, POMA and POEA, were treated at different temperature
ranges as follows. It was used a 2920 DSC Thermal Analysis under
nitrogen gas purge (50 ml/min) and a heating rate of 10 ◦C/min,
where the system was first equilibrated at −50 ◦C and then heated
up to T2. The samples were then kept at T2 for 2 h under N2
gas atmosphere (50 ml/min). The thermal treatment was carried
out at different temperatures, T2 = 25, 50, 100, 150 and 220 ◦C,
respectively. After the thermal treatment, 1.3 mg of the sample
was dissolved in dimethylacetamide (DMAc) and then the UV–VIS
spectra were recorded using a fully computerized Shimadzu
spectrophotometer, model UV-1601PC, in a wavelength range of
900–250 nm.
3. Results and discussion
Fig. 1 shows the DRIFTS results for emeraldine base (EB) powder
of PANI, POMA and POEA. The samples analyzed, with and without
thermal treatment, showed differences in DRIFTS spectra, such as
an increase in the absorption band at ∼1520 cm−1, which is due
to the axial bending of the benzoid–nitrogen (B–N) chemical bond,
and a decrease in the absorption band at ∼1600 cm, which is due
to the axial bending of the quinoid–nitrogen (Q–N) chemical bond.
This result indicates the conversion of quinoid-like structures to
benzoid-like structures due to the crosslinking isomerization reac-
tion [15].
Fig. 2 shows the weight loss (TGA) of PANI, POMA, and POEA
during heating treatment from room temperature (25 ◦C) up to
900 ◦C carried out under inert atmosphere (N2). It can be observed a
weight loss between 25 and 120 ◦C due to the removal of adsorbed
water molecules [16–19], i.e., 6 wt.% for PANI, 4 wt.% for POMA, and
1 wt.% for POEA, respectively. The weight loss observed between
382 and 640 ◦C (PANI), 300 and 600 ◦C (POMA), and 268 and 600 ◦C
(POEA), respectively, are due to the polymer degradation. The dif-
ferences observed for PANI (Ti = 382 ◦C), POMA (Ti = 300 ◦C) and
POEA (Ti = 382 ◦C) for the thermal degradation temperature (Ti)
are related to the crosslinking isomerization process that is taking
place prior beginning of the degradation process. The crosslink-
ing process might be affected by the size of the alkoxy substituent
and subsequently the degradation process upon the thermal treat-
ment. However, from these results it is not possible to state that
the crosslinking process occurs through a different mechanism for
the different types of polymer, i.e. PANI, POMA, and POEA. The pres-
ence of the alkoxy groups, i.e. methoxy (POMA) and ethoxy (POEA),
results in a steric effect, which blocks the crosslinking chemical
reaction. In the PANI system, where the monomer aromatic ring
does not contain any alkoxy group, the crosslinking isomeriza-
tion reaction proceeds as expected, i.e. the degree of crooslinking
in polyaniline system is much higher than on POMA and POEA
systems. These results suggest that the crosslinking isomerization
Fig. 1. DRIFTS spectra of (a) PANI, (b) POMA and (c) POEA, recorded without
(room temperature, 25 ◦
C) previous thermal treatment and after thermal treat-
ment at 220 ◦
C during 1 h under nitrogen (N2) gas atmosphere. Temperature ramp:
10 ◦
C/min.
process enhances the thermal stability of the polymer as it could
be observed from the results presented in Fig. 2a. Fig. 2b shows
a higher weight loss rate (maximum derivative value as shown in
the dot line curve) for POEA, which indicates that there is also an
effect of the size of the alkoxy group on the thermal stability of the
polymer, i.e. larger alkoxy groups results in a polymer with lower
thermal stability.
Fig. 3 shows the DSC results (first scan) for PANI, POMA, and
POEA, it can be observed two peaks in Fig. 3. The first peak,
endothermic, with a maximum at ∼120 ◦C for PANI and POMA,
and ∼110 ◦C for POEA, is due to removal of adsorbed water [20].
The second peak, exothermic, observed between 175 and 350 ◦C,
Author's personal copy
W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46 45
Fig. 2. Weight loss (TGA) (a) and derivative thermal gravimetric analysis (DTG) (b)
results for PANI (solid line), POMA (dot line), and POEA (dash line), respectively. TGA
temperature ramp: 10 ◦
C/min under nitrogen gas (N2) atmosphere.
might be due to re-crystallization followed by crosslinking isomer-
ization reaction (see schema of Fig. 4) [21,22]. Fig. 5 shows the
UV–VIS spectra for samples of the EB form of PANI, POMA and POEA,
treated at different temperature ranges, which were then dissolved
in DMAc. These results (Fig. 5) show that the solubility of the treated
samples in DMAc decreased after the thermal treatment done at
T2 = 150 ◦C and T2 = 220 ◦C, which agree with the results presented
in Fig. 3, which indicates that, even at T2 = 150 ◦C, the crosslink-
ing isomerization reaction might occur. The samples treated at
T2 = 100 ◦C showed no differences compared to the samples treated
at T2 = 25 ◦C. The sample treated at T2 = 220 ◦C is insoluble in DMAc,
which indicates that the extent of the crosslinking isomerization
reaction is significant at T2 = 220 ◦C.
The glass transition temperature (Tg) of PANI, POMA and POEA
was determined by combining DSC and TMDSC. The adsorbed water
Fig. 3. DSC results for PANI, POMA, and POEA. DSC temperature ramp: 10 ◦
C/min
under nitrogen gas (N2) atmosphere.
was first removed from the sample by heating the sample from
room temperature (25 ◦C) up to 150 ◦C (heating rate of 10 ◦C/min)
under nitrogen gas atmosphere, which was done by using the DSC
technique in order to verify the water content removal (Fig. 6a).
After the sample has reached the room temperature, it was then
heated up from room temperature to 150 ◦C (heating rate of
5 ◦C/min) by using TMDSC technique (Fig. 6b). As it can be seen from
Fig. 5b there is a baseline change in the TMDSC curve at ∼67 ◦C. The
changes in the baseline might be due to structural changes in the
polymer morphology due to the thermal treatment, i.e. the sample
presented a glass transition after the thermal treatment, where the
values for the glass transition temperature (Tg) are Tg(PANI) = 67 ◦C,
Tg(POMA) = 68 ◦C, and Tg(POEA) = 70 ◦C, respectively. Similar results
were observed by Ding et al. [15], where they reported a glass
transition for PANI emeraldine base from TMDSC technique mea-
surements.
Fig. 4. Scheme of PANI crosslinking isomerization reaction [15].
Author's personal copy
46 W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46
Fig. 5. UV–VIS spectra for samples of EB form of (a) PANI, (b) POMA and (c) POEA
dissolved in dimethylacetamide (DMAc). The samples were treated at different tem-
peratures, as indicated in the figure, prior dissolving in the solvent (DMAc). The
UV–VIS spectra were recorded at room temperature (25 ◦
C).
Fig. 6. Thermal analysis results for PANI, POMA, and POEA, under nitrogen gas atmo-
sphere. (a) DSC measurements results from room temperature (25 ◦
C) up to 150 ◦
C;
the samples were then cooled down to room temperature under nitrogen gas atmo-
sphere before doing the TMDSC measurements. (b) TMDSC measurement results
from room temperature (25 ◦
C) up to 150 ◦
C.
4. Conclusions
The thermal behavior of polyanilines, i.e. PANI, POMA, and
POEA, in the form of emeraldine base, measured by using DSC and
TMDSC techniques, might indicate that the crystallization and re-
crystallization temperatures of POMA and POEA are lower than for
PANI. This behavior is due to the presence of the alkoxy groups
in the monomer aromatic ring. No change in the Tg values was
observed in amorphous phase of the polymers, i.e. PANI, POMA,
and POEA. The crosslinking isomerization reaction plays an impor-
tant role on the polymer thermal stability. The combined results
from DRIFTS and thermal analysis (TGA, DTG, DSC, and TMDSC)
showed that PANI has higher thermal stability compared to POMA
and POEA, which indicates the effect of the presence of alkoxy
groups in the POMA and POEA systems on the crosslinking iso-
merization process. We believe that the extent of the crosslinking
isomerization process is responsible for the higher thermal stability
presented by PANI.
Acknowledgements
The financial support given by LABEX-Embrapa, CNPq, CAPES,
FINEP and FAPESP are gratefully acknowledged.
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Thermo analyses of polyaniline and its derivatives

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  • 2. Author's personal copy Thermochimica Acta 502 (2010) 43–46 Contents lists available at ScienceDirect Thermochimica Acta journal homepage: www.elsevier.com/locate/tca Thermo-analyses of polyaniline and its derivatives William F. Alvesa,b , Everaldo C. Venancioc,∗ , Fabio L. Leited , Darcy H.F. Kandae , Luiz F. Malmongee , José A. Malmongee , Luiz H.C. Mattosoa,b a EMBRAPA Instrumentac¸ ão Agropecuária, C.P. 741, São Carlos (SP), 13560-970, Brazil b Dept. Química, Universidade Federal de São Carlos (UFSCar), São Carlos (SP), 13565-905, Brazil c Centro de Engenharia, Modelagem e Ciências Sociais Aplicadas (CECS), Universidade Federal do ABC (UFABC), Santo André (SP), 09210-170, Brazil d Universidade Federal de São Carlos (UFSCar), C.P. 3031, Sorocaba (SP), 18052-780, Brazil e Dept. Física e Química, Universidade Estadual Paulista Julio de Mesquita Filho, Ilha Solteira (SP), 15385-000, Brazil a r t i c l e i n f o Article history: Received 21 August 2009 Received in revised form 6 January 2010 Accepted 2 February 2010 Available online 16 February 2010 Keywords: Polyaniline DSC TGA Poly(o-methoxyaniline) Poly(o-ethoxyaniline) a b s t r a c t In this work, is presented the thermal behavior of polyaniline (PANI) and its derivatives poly(o- ethoxyaniline) (POEA) and poly(o-methoxyaniline) (POMA), which were studied by using differential scanning calorimetry (DSC), modulated DSC (TMDSC), respectively, and thermal gravimetric analysis (TGA). The results from diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) and thermal analysis showed the formation of crosslinking isomerization reaction during the heating process. The results showed that the maximum weight loss and the crystallinity degree depend on the type of the aromatic ring substituent group, i.e. hydrogen, ethoxy or methoxy. © 2010 Elsevier B.V. All rights reserved. 1. Introduction Polyaniline (PANI) and its derivatives, e.g., poly(o- methoxyaniline) (POMA) and poly(o-ethoxyaniline) (POEA) [1,2] have been intensively studied due to their electrical and optical properties associated with low costs, easy processabil- ity, its environmental stability and relatively simple method of synthesis [3,4]. The thermal analysis of conducting polymers, i.e. PANI, POMA and POEA, is crucial to define their performance on application processes of these materials [5]. Thus, thermal analysis of conducting polymers provides important information about the effect of morphological structure and other process, such as chemical reaction, which are sensitive to thermal effects (temperature changes), e.g., crosslinking reaction processes among PANI chains. These processes have been studied by differential scanning calorimetry (DSC) [6–8] and dynamical mechanical thermal analysis (TDMTA) [9–12]. In this work, the glass transitions (Tg) for the chemically synthe- sized non-conducting form of PANI, POMA and POEA, in the powder ∗ Corresponding author at: Centro de Engenharia, Modelagem e Ciências Sociais Aplicadas (CECS), Universidade Federal do ABC (UFABC), Rua Santa Adélia 166, Bairro Bangu, Santo André (SP), 09210-170, Brazil. Tel.: +55 11 49963166; fax: +55 11 49963166. E-mail address: everaldo.venancio@ufabc.edu.br (E.C. Venancio). form, were studied using modulated DSC (MDSC). The hypothesis of that a chemical crosslinking reaction occurs during the heating pro- cess was further confirmed by supporting experimental methods such as diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS), DSC and TGA. 2. Experimental PANI, POMA and POEA were chemically synthesized accord- ing to the method described in the literature [13,14]. The polymer obtained was a dark precipitate, with expected average molecular weight (MW) of ∼41,400 g mol−1 and polydispersivity (MW/Mn) of 2.3. Dedoping was performed by treatment with a 0.1 M ammo- nium hydroxide aqueous solution for 16 h at room temperature (∼25 ◦C) to yield the polymer in the emeraldine base form (EB). The polymer was then transferred to a glass desiccator without desic- cant agent and then dried under dynamic vacuum for 24 h at room temperature (∼25 ◦C). A model Q 600 TA Instruments TGA was used to investigate the thermal stability of the polymers in the powder form in the temperature range from 25 to 900 ◦C, under N2 gas atmosphere (50 ml/min), for the thermal treatment the system was first equi- librated at 220 ◦C for 1 h under N2 gas atmosphere (50 ml/min). After the thermal treatment of PANI (EB), POMA (EB) and POEA (EB) the DRIFTS spectra were performed on a fully computerized Nico- let NEXUS® 670 using the software OMNIC. All the DRIFTS spectra 0040-6031/$ – see front matter © 2010 Elsevier B.V. All rights reserved. doi:10.1016/j.tca.2010.02.003
  • 3. Author's personal copy 44 W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46 were recorded on a Nicolet NEXUS® 670 spectrometer at a resolu- tion of 1 cm−1 and using 64 scans. The temperature ramp used was 10 ◦C/min. In all experiments, PANI and its derivatives were present in equal amount, the total weight being at about 8.0 ± 1.0 mg. The thermal treatment of the EB powder was carried out by using a 2920 DSC Thermal Analysis under nitrogen gas purge (50 ml/min) and a heating rate of 10 ◦C/min, where the system was first equilibrated at −50 ◦C and then heated up to 150 ◦C. After the first run with the equipment on the DSC mode, the DSC Thermal Analysis equipment was switched to the TMDSC mode and then all subsequent runs were done with the DSC Thermal Analysis equipment in the mod- ulated DSC (TMDSC) mode by using a 2920 modulated DSC. The TMDSC experiments were carried out as follows: the system was first equilibrated at −50 ◦C for 5 min, and then it was heated up to 150 ◦C using a heating rate of 5 ◦C/min with a period modulation of 60 s, and the temperature amplitude of modulation was ±1.0 ◦C. The as prepared powder of the EB form of the samples, i.e. PANI, POMA and POEA, were treated at different temperature ranges as follows. It was used a 2920 DSC Thermal Analysis under nitrogen gas purge (50 ml/min) and a heating rate of 10 ◦C/min, where the system was first equilibrated at −50 ◦C and then heated up to T2. The samples were then kept at T2 for 2 h under N2 gas atmosphere (50 ml/min). The thermal treatment was carried out at different temperatures, T2 = 25, 50, 100, 150 and 220 ◦C, respectively. After the thermal treatment, 1.3 mg of the sample was dissolved in dimethylacetamide (DMAc) and then the UV–VIS spectra were recorded using a fully computerized Shimadzu spectrophotometer, model UV-1601PC, in a wavelength range of 900–250 nm. 3. Results and discussion Fig. 1 shows the DRIFTS results for emeraldine base (EB) powder of PANI, POMA and POEA. The samples analyzed, with and without thermal treatment, showed differences in DRIFTS spectra, such as an increase in the absorption band at ∼1520 cm−1, which is due to the axial bending of the benzoid–nitrogen (B–N) chemical bond, and a decrease in the absorption band at ∼1600 cm, which is due to the axial bending of the quinoid–nitrogen (Q–N) chemical bond. This result indicates the conversion of quinoid-like structures to benzoid-like structures due to the crosslinking isomerization reac- tion [15]. Fig. 2 shows the weight loss (TGA) of PANI, POMA, and POEA during heating treatment from room temperature (25 ◦C) up to 900 ◦C carried out under inert atmosphere (N2). It can be observed a weight loss between 25 and 120 ◦C due to the removal of adsorbed water molecules [16–19], i.e., 6 wt.% for PANI, 4 wt.% for POMA, and 1 wt.% for POEA, respectively. The weight loss observed between 382 and 640 ◦C (PANI), 300 and 600 ◦C (POMA), and 268 and 600 ◦C (POEA), respectively, are due to the polymer degradation. The dif- ferences observed for PANI (Ti = 382 ◦C), POMA (Ti = 300 ◦C) and POEA (Ti = 382 ◦C) for the thermal degradation temperature (Ti) are related to the crosslinking isomerization process that is taking place prior beginning of the degradation process. The crosslink- ing process might be affected by the size of the alkoxy substituent and subsequently the degradation process upon the thermal treat- ment. However, from these results it is not possible to state that the crosslinking process occurs through a different mechanism for the different types of polymer, i.e. PANI, POMA, and POEA. The pres- ence of the alkoxy groups, i.e. methoxy (POMA) and ethoxy (POEA), results in a steric effect, which blocks the crosslinking chemical reaction. In the PANI system, where the monomer aromatic ring does not contain any alkoxy group, the crosslinking isomeriza- tion reaction proceeds as expected, i.e. the degree of crooslinking in polyaniline system is much higher than on POMA and POEA systems. These results suggest that the crosslinking isomerization Fig. 1. DRIFTS spectra of (a) PANI, (b) POMA and (c) POEA, recorded without (room temperature, 25 ◦ C) previous thermal treatment and after thermal treat- ment at 220 ◦ C during 1 h under nitrogen (N2) gas atmosphere. Temperature ramp: 10 ◦ C/min. process enhances the thermal stability of the polymer as it could be observed from the results presented in Fig. 2a. Fig. 2b shows a higher weight loss rate (maximum derivative value as shown in the dot line curve) for POEA, which indicates that there is also an effect of the size of the alkoxy group on the thermal stability of the polymer, i.e. larger alkoxy groups results in a polymer with lower thermal stability. Fig. 3 shows the DSC results (first scan) for PANI, POMA, and POEA, it can be observed two peaks in Fig. 3. The first peak, endothermic, with a maximum at ∼120 ◦C for PANI and POMA, and ∼110 ◦C for POEA, is due to removal of adsorbed water [20]. The second peak, exothermic, observed between 175 and 350 ◦C,
  • 4. Author's personal copy W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46 45 Fig. 2. Weight loss (TGA) (a) and derivative thermal gravimetric analysis (DTG) (b) results for PANI (solid line), POMA (dot line), and POEA (dash line), respectively. TGA temperature ramp: 10 ◦ C/min under nitrogen gas (N2) atmosphere. might be due to re-crystallization followed by crosslinking isomer- ization reaction (see schema of Fig. 4) [21,22]. Fig. 5 shows the UV–VIS spectra for samples of the EB form of PANI, POMA and POEA, treated at different temperature ranges, which were then dissolved in DMAc. These results (Fig. 5) show that the solubility of the treated samples in DMAc decreased after the thermal treatment done at T2 = 150 ◦C and T2 = 220 ◦C, which agree with the results presented in Fig. 3, which indicates that, even at T2 = 150 ◦C, the crosslink- ing isomerization reaction might occur. The samples treated at T2 = 100 ◦C showed no differences compared to the samples treated at T2 = 25 ◦C. The sample treated at T2 = 220 ◦C is insoluble in DMAc, which indicates that the extent of the crosslinking isomerization reaction is significant at T2 = 220 ◦C. The glass transition temperature (Tg) of PANI, POMA and POEA was determined by combining DSC and TMDSC. The adsorbed water Fig. 3. DSC results for PANI, POMA, and POEA. DSC temperature ramp: 10 ◦ C/min under nitrogen gas (N2) atmosphere. was first removed from the sample by heating the sample from room temperature (25 ◦C) up to 150 ◦C (heating rate of 10 ◦C/min) under nitrogen gas atmosphere, which was done by using the DSC technique in order to verify the water content removal (Fig. 6a). After the sample has reached the room temperature, it was then heated up from room temperature to 150 ◦C (heating rate of 5 ◦C/min) by using TMDSC technique (Fig. 6b). As it can be seen from Fig. 5b there is a baseline change in the TMDSC curve at ∼67 ◦C. The changes in the baseline might be due to structural changes in the polymer morphology due to the thermal treatment, i.e. the sample presented a glass transition after the thermal treatment, where the values for the glass transition temperature (Tg) are Tg(PANI) = 67 ◦C, Tg(POMA) = 68 ◦C, and Tg(POEA) = 70 ◦C, respectively. Similar results were observed by Ding et al. [15], where they reported a glass transition for PANI emeraldine base from TMDSC technique mea- surements. Fig. 4. Scheme of PANI crosslinking isomerization reaction [15].
  • 5. Author's personal copy 46 W.F. Alves et al. / Thermochimica Acta 502 (2010) 43–46 Fig. 5. UV–VIS spectra for samples of EB form of (a) PANI, (b) POMA and (c) POEA dissolved in dimethylacetamide (DMAc). The samples were treated at different tem- peratures, as indicated in the figure, prior dissolving in the solvent (DMAc). The UV–VIS spectra were recorded at room temperature (25 ◦ C). Fig. 6. Thermal analysis results for PANI, POMA, and POEA, under nitrogen gas atmo- sphere. (a) DSC measurements results from room temperature (25 ◦ C) up to 150 ◦ C; the samples were then cooled down to room temperature under nitrogen gas atmo- sphere before doing the TMDSC measurements. (b) TMDSC measurement results from room temperature (25 ◦ C) up to 150 ◦ C. 4. Conclusions The thermal behavior of polyanilines, i.e. PANI, POMA, and POEA, in the form of emeraldine base, measured by using DSC and TMDSC techniques, might indicate that the crystallization and re- crystallization temperatures of POMA and POEA are lower than for PANI. This behavior is due to the presence of the alkoxy groups in the monomer aromatic ring. No change in the Tg values was observed in amorphous phase of the polymers, i.e. PANI, POMA, and POEA. The crosslinking isomerization reaction plays an impor- tant role on the polymer thermal stability. The combined results from DRIFTS and thermal analysis (TGA, DTG, DSC, and TMDSC) showed that PANI has higher thermal stability compared to POMA and POEA, which indicates the effect of the presence of alkoxy groups in the POMA and POEA systems on the crosslinking iso- merization process. We believe that the extent of the crosslinking isomerization process is responsible for the higher thermal stability presented by PANI. Acknowledgements The financial support given by LABEX-Embrapa, CNPq, CAPES, FINEP and FAPESP are gratefully acknowledged. References [1] F.L. Leite, L.G. Paterno, C.E. Borato, P.S.P. Herrmann, O.N. Oliveira, L.H.C. Mattoso, Polymer 46 (2005) 12503. [2] W.F. Alves, D.H.F. Kanda, L.F. Malmonge, J.A. Malmonge, L.H.C. Mattoso, J. Appl. Polym. Sci. 105 (2007) 706. [3] J.P.H. Lima, A.M. De Andrade, J. Mater. Sci.: Mater. Electron. 17 (2006) 593. [4] E. Erdem, M. Karakisla, M. Sac¸ ak, Eur. Polym. J. 40 (2004) 785. [5] W. Pan, S.L. Yang, G. Li, J.M. Jiang, Eur. Polym. J. 41 (2005) 2127. [6] E.S. Matveeva, R.D. Calleja, V.P. Parkhutic, Synth. Met. 72 (1995) 105. [7] X.-H. Wang, Y.-H. Geng, L.-X. Wang, X.-B. Jing, F.-S. Wang, Synth. Met. 69 (1995) 263. [8] G. Aysegül, S. Bekirb, T. Muzaffer, Synth. Met. 142 (2004) 41. [9] S. Chen, H. Lee, Macromolecules 26 (1993) 3254. [10] A.J. Milton, A.P. Monkman, Synth. Met. 57 (1993) 3571. [11] Y. Wei, G. Jang, K.F. Hsueh, Polymer 33 (1992) 314. [12] Y. Wei, G. Jang, K.F. Hsueh, E.M. Scherr, A.G. Macdiarmid, A.J. Epstein, Polym. Mater. Sci. 61 (1989) 916. [13] D. Gonc¸ alves Jr., D.S. Dos Santos, L.H.C. Mattoso, F.E. Karasz, L. Akcelrud And, R.M. Faria, Synth. Met. 90 (1997) 5. [14] L.H.C. Mattoso, S.K. Manohar, A.G. Macdiarmid, A.J. Epstein, J. Polym. Sci. Part A: Polym. Chem. 33 (1995) 1227. [15] E.M. Scherr, A.G. Macdiarmid, S.K. Manohar, J.G. Masters, Y. Sun, X. Tang, M.A. Druy, P.J. Glatkowski, V.B. Cajipe, J.E. Fischer, K.R. Cromack, M.E. Jozefowicz, J.M. Ginder, R.P. McCall, A.J. Epstein, Synth. Met. 41 (1991) 735. [16] L. Ding, X. Wang, R.V. Gregory, Synth. Met. 104 (1999) 73. [17] V.G. Kulkarni, L.D. Campbell, W.R. Mathew, Synth. Met. 30 (1989) 321. [18] D. Tsocheva, T. Zlatkov, L. Telemezyan, J. Therm. Anal. 53 (1998) 895. [19] M.C. Gupta, S.S. Umare, Macromolecules 25 (1992) 138. [20] W.A. Gazotti, M.A. De Paoli, Synth. Met. 80 (1996) 263. [21] N.C. de Souza, J.R. Silva, J.A. Giacometti, O.N. Oliveira Jr., Thermochim. Acta 441 (2006) 124. [22] H.S.O. Chan, L.M. Gan, T.S.A. Hor, S.H. Seow, L.H. Zhang, Thermochim. Acta 1 (225) (1993) 75.