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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 554
THERMAL ANALYSIS AND DC CONDUCTIVITY OF
POLYPYRROLE/YTTRIUM OXIDE COMPOSITES
T.K. Vishnuvardhan1
, V.R. Kulkarni2
1
Department of Chemistry, Central college, Bangalore university, Bangalore-560001, Karnataka, India
2
Department of Chemistry, Acharya Institutes of Technology, Soldevanahalli, Bangalore-560107, Karnataka, India
vishnu33vardhan@gmail.com
Abstract
Polypyrrole/Yttrium Oxide (PPy/Y2O2) Composites are synthesized by chemical method. Thermal stability of the above composites is
characterized by TGA and DSC. Dc conductivity measurements of the composites are also carried out. The results are used to
calculate the activation energy. Sensor activities of the composites are also discussed.
----------------------------------------------------------------------***-----------------------------------------------------------------------
1. INTRODUCTION
Organic and metallo-organic polymers gained importance
because of their electrical, electronic, non-linear optical,
electrochemical and photochemical applications (1-5). In order
to make use of these polymer composites for specific
applications, they are modified either by co-polymerization or
by making blends with other polymers (6). Production of
blends using organic and metallo-organic polymers is an
attempt to derive new polymeric materials by combining the
properties of the individual components of the blend (7). The
use of blends/composites in various electric and electronic
devices attracted attention because of their conducting nature,
chemical stability and the economic viability. Among the
many conducting polymers, PPy seems to be one of the best
candidates for preparing conducting polymer composites since
it is stable both thermally and environmentally (8).
Conductivity of the polymer and polymer composites are
explained by many literatures (9-11).
In this article, we present the study of thermal analysis of the
PPy/Y2O2 composites. The Dc conductivity measurements of
the composites are carried out by two probe method. Results
are fitted with linear fit curve and activation energy is also
calculated. Data is further tested by IV plots.
2. SYNTHESIS OF PPY/YTTRIUM OXIDE
COMPOSITES
The synthesis of PPy/Yttrium oxide composites is similar to
that of pure PPy, except that oxide is present during in situ
synthesis. A 0.02 mole of pyrrole was added drop wise to 100
ml suspension containing 0.06 mole of FeCl3 and varied
amounts of Y2O3 (10%, 20%, 30%, 40% and 50%)powders
with continuous stirring for 3 hrs. at 0 0
C. The black
precipitate of the PPy/Yttrium oxide composites formed was
collected by filtration and thoroughly washed with distilled
water, until the filtrate became colorless. Any unreacted
pyrrole in the composite was removed by washing the
precipitate with methanol and the composite was dried under
vacuum at room temperature (24 0
C).
The TGA of PPy, PPy/Yttrium oxide composites we recorded
over a temperature range of 26 0
C to 1200 0
C in nitrogen
atmosphere using a STA 409C thermal analyzer, to analyze
the degradation pattern of polymer composites.
Simultaneously, Differential Thermal Analysis (DTA) data
was also recorded. Reference material used in the TGA/DTA
is Alumina with heating rate of temperature is 5 0
C/min.
Differential scanning calorimetric studies on PPy/Yttrium
oxide composites were carried out using a METTLER thermal
analyzer. DSC was recorded from 50 0
C to 600 0
C. The
heating rate was kept constant at 10 0
C per minute.
2.1 Effect of Temperature on Dc Conductivity:
2.1. Pellet Preparation
The powder of the PPy/Y2O2 composites are crushed and
ground finally in the presence of acetone medium in agate,
mortar. Finally ground powder is pressed to form, pellets of
0.1-0.25 cm. thickness and diameter of 10 mm or by applying
a pressure of 90M Pa in a hydraulic press. The thickness of
these pellets was measured using a micrometer screw-gauge.
2.1.2 Preparation of Electrodes on the Pellets
The pellets of Polypyrrole composites are coated with silver
paste on either side of the surfaces. The copper electrodes are
placed on each of the surface to obtain better electrical
contacts.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 555
2.1.3 Thermal Analysis:
The DTA and TGA traces of pure PPy and PPy/Y2O2 sample
shows small exothermic dip at 69.9 0
C which may be for the
loss of dopant and an endothermic shoulder at 90.8 0
C
corresponding to the loss of water molecules. This is followed
by the broad exothermic peak may be due to the degradation
of the PPy chains.
Initially the steep trace TGA consists of two stages of weight
loss, one from room temperature to 150 0
C and another from
200 to 400 0
C. Further as the degradation continues and
complete at about 11000
C. Steep trace of PPy indicates
amorphous nature. The first stage weight loss may be due to
water and the weight loss found to be 7.02%., the second stage
weight loss may be due to the degradation of PPy-Cl chain,
and the weight loss at this stage is-21.73%. The total weight
loss at 1100 0
C is about -95%.
This ensures the complete degradation of the polymer. The
onset temperature (Tonset) and Tmax for second step degradation
is 310 0
C and 400 0
C, respectively. These are also confirmed
from the DTG trace. Similarly on set temperature for the
composites are shown in the table
Table 1: Indicate the onset temperature and weight loss from TGA for PPy and PPy/Y2O3 composites
Composites Onset
Temperature 0
C
(from TGA)
Completed
degradation
Temperature 0
C
Total loss
Occurred
(from TGA)
Temperature
At which
Maximum
Weight loss 0
C
(From DTA)
PPy 69.9 1100 95% 704
PPY/20%Y2O3 70.2 1000 80% 846
PPy/50%Y2O3 74.9 920 53% 897
The DSC curve of PPy and PPy/Y2O3sample have a broad
characteristic endothermic dip indicates the glass transition
temperature of Polypyrrole at 97.32 0
C. The nature of the
curve indicates that the loss of water is overlapping with Tg of
polymer (which is well matching with the reported value).
Lack of any shoulder or melting peak beyond this region
indicates amorphous nature with less orderness of the polymer
molecules.
The DSC curve of PPy/50%Y2O3composite trace has a sharp
dip at higher temperature, namely at 125.16 0
C. This
sharpness indicates the better crystalline. It also contains few
more inflection points; one at 295.74 0
C may be due to the
melting of PPy chain, the other at 489.87 0
C may be due to
phase change of Y2O3.
2.2 Effect of Temperature on Conductivity Ppy/Y2o3
Composites
Figure 1 shows the temperature dependence of σ DC for the
PPy and PPy/Y2O3Samples. In this figure symbols indicate
log values of experimental conductivities (for temperature
range from 100-200 0
C) for various composites. Solid lines
indicate their fitting by linear fit equation by using the origin
6.0. The conductivity of all the composites shows that, as the
temperature is increased conductivity increases. This figure
also indicates that, conductivity increases as the percentage of
oxide is increased and then for further increase in oxide
content the conductivity decreases. Conductivity of polymer
depends on the conjugation length. In the synthesis process,
pyrrole monomer was first adsorbed on the surface of
Y2O3Concentration, and as a result, the amount of pyrrole
associated with each CeO2 concentration, and as a result, the
amount of pyrrole associated with each Y2O3 particle is
diminished.
Figure 1: Arrhenius plot of conductivity of PPy/Y2O3samples
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 556
The temperature variation of conductivity of PPy composites
is well described by Mott’s variable range hopping formalism.
This is applicable only in amorphous semiconductors. This is
applicable only in amorphous semiconductors. Larger
activation energy Implies higher potential barrier in the
conduction process originating from the reduction of polymer
chain length. Lower conductivity and higher activation energy
are due to the poor contact between the polymer and oxide
particles. Dispersion of oxide in the conducting polypyrrole
due to percolation introduces more conducting paths resulting
in higher conductivity. Loading in the polymer increases the
conductivity is explained in literature (12)
Table 2: Indicates the activation energy of the conduction
process for PPy/Y2O3 samples. It indicates that as the oxide
content Increases the activation energy goes on decreasing.
But in case of PPy/40% Y2O3shows highest activation energy
Table 2: Activation energy for PPy/Y2O3composites
composites Activation
Energy me V
Pure PPy 302.85
PPy/10%CeO2 203.98
PPy/20%CeO2 194.98
PPy/30%CeO2 149.51
PPy/40%CeO2 94.08
PPy/50%CeO2 393.23
Current Voltage plot of PPy CeO2 composites:
Figure 2: Representative Current -Voltage plots of PPY/Y2O3
samples
Figure 2 show the current voltage plots of the representative
PPy/Y2O2 composites respectively. They show very good
linearity in the range studied. Beyond this range thermal
fluctuations due to significant joule heating take place and non
linearity sets in.
CONCLUSIONS
PPy/Y2O3 composite shows the high thermal stability due to
metal oxides. Activation energy of these compostes shows
highest for ppy/50% Y2O3 due to more metal oxide particles
increases the higher activation energy. It will be maximum
upto critical percentages latter activation energy decreases.
Current voltage characteristics of these polymer composites
are also accounted. These electrical properties of polymer
PPy/Y2O3 composites have strong applications in battery and
sensor applications.
REFERENCES:
[1]. J. L. Bredas, R. RChance(Eds.), Conjugated Polymeric
Materials-Opportunities in optoelectronics and Molecular
Electronics, NATO Advanced study Series,(Kluwer,
Dordrecht, 1990) p-112.
[2]. S. Bhattacharyya and S. K. Saha, Applied Physics Letters
80, ( 24) 2002, 4612
[3]. J.G. Park, B. Kim, S.H. Lee, Y.W. Park Thin Solid Films
438 –439 (2003) 118–122.
[4]. T K Vishnuvardhan, V R Kulkarni, C Basavaraja and S C
Raghavendra Bull. Mater. Sci., 29, (1) 2006, 77–83
[5]. Jung-Chul Lee , Wonjoo Lee , Sung-Hwan Han, Tae Geun
Kim, Yun-Mo Sung Electrochemistry Communications 11
(2009) 231–234
[6]. W.A.Gazotti Jr., GGasalbore-Miceli, S.Mitzakoff,
A.Geri,M.C.Gallazzi, M.A.DePaoli, Electrochem.Acta
44(1999)1965.
[7]. S.Venkatachalam,P.V.Prabhakaran, Eur.Poly.J. 5(1993)29
[8]. Bernd Tiek and walter Gabriel, Polymer, 31 (1990) 20.
[9]. Raghu M, Subramanyam S.V, Chatterjee S, Phys.Rev.B.
1991,43, (5) 4236.
[10]. Epistein A.J, Rommelman H, Abkowitz M, and Gibson
H.W, Phys.Rev.Lett. 1981,47,1549.
[11]. Pople J.A, and Walnsely S.H, Mol. Phys. 5,15(1962).
[12].Geon-Woong Lee, Min Park, Junkyung Kim, Jae Ik Lee
and Ho Gyu Yoon Composites Part A: Applied Science and
Manufacturing 37,( 5), 2006, 727–734

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Thermal analysis and dc conductivity of

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 554 THERMAL ANALYSIS AND DC CONDUCTIVITY OF POLYPYRROLE/YTTRIUM OXIDE COMPOSITES T.K. Vishnuvardhan1 , V.R. Kulkarni2 1 Department of Chemistry, Central college, Bangalore university, Bangalore-560001, Karnataka, India 2 Department of Chemistry, Acharya Institutes of Technology, Soldevanahalli, Bangalore-560107, Karnataka, India vishnu33vardhan@gmail.com Abstract Polypyrrole/Yttrium Oxide (PPy/Y2O2) Composites are synthesized by chemical method. Thermal stability of the above composites is characterized by TGA and DSC. Dc conductivity measurements of the composites are also carried out. The results are used to calculate the activation energy. Sensor activities of the composites are also discussed. ----------------------------------------------------------------------***----------------------------------------------------------------------- 1. INTRODUCTION Organic and metallo-organic polymers gained importance because of their electrical, electronic, non-linear optical, electrochemical and photochemical applications (1-5). In order to make use of these polymer composites for specific applications, they are modified either by co-polymerization or by making blends with other polymers (6). Production of blends using organic and metallo-organic polymers is an attempt to derive new polymeric materials by combining the properties of the individual components of the blend (7). The use of blends/composites in various electric and electronic devices attracted attention because of their conducting nature, chemical stability and the economic viability. Among the many conducting polymers, PPy seems to be one of the best candidates for preparing conducting polymer composites since it is stable both thermally and environmentally (8). Conductivity of the polymer and polymer composites are explained by many literatures (9-11). In this article, we present the study of thermal analysis of the PPy/Y2O2 composites. The Dc conductivity measurements of the composites are carried out by two probe method. Results are fitted with linear fit curve and activation energy is also calculated. Data is further tested by IV plots. 2. SYNTHESIS OF PPY/YTTRIUM OXIDE COMPOSITES The synthesis of PPy/Yttrium oxide composites is similar to that of pure PPy, except that oxide is present during in situ synthesis. A 0.02 mole of pyrrole was added drop wise to 100 ml suspension containing 0.06 mole of FeCl3 and varied amounts of Y2O3 (10%, 20%, 30%, 40% and 50%)powders with continuous stirring for 3 hrs. at 0 0 C. The black precipitate of the PPy/Yttrium oxide composites formed was collected by filtration and thoroughly washed with distilled water, until the filtrate became colorless. Any unreacted pyrrole in the composite was removed by washing the precipitate with methanol and the composite was dried under vacuum at room temperature (24 0 C). The TGA of PPy, PPy/Yttrium oxide composites we recorded over a temperature range of 26 0 C to 1200 0 C in nitrogen atmosphere using a STA 409C thermal analyzer, to analyze the degradation pattern of polymer composites. Simultaneously, Differential Thermal Analysis (DTA) data was also recorded. Reference material used in the TGA/DTA is Alumina with heating rate of temperature is 5 0 C/min. Differential scanning calorimetric studies on PPy/Yttrium oxide composites were carried out using a METTLER thermal analyzer. DSC was recorded from 50 0 C to 600 0 C. The heating rate was kept constant at 10 0 C per minute. 2.1 Effect of Temperature on Dc Conductivity: 2.1. Pellet Preparation The powder of the PPy/Y2O2 composites are crushed and ground finally in the presence of acetone medium in agate, mortar. Finally ground powder is pressed to form, pellets of 0.1-0.25 cm. thickness and diameter of 10 mm or by applying a pressure of 90M Pa in a hydraulic press. The thickness of these pellets was measured using a micrometer screw-gauge. 2.1.2 Preparation of Electrodes on the Pellets The pellets of Polypyrrole composites are coated with silver paste on either side of the surfaces. The copper electrodes are placed on each of the surface to obtain better electrical contacts.
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 555 2.1.3 Thermal Analysis: The DTA and TGA traces of pure PPy and PPy/Y2O2 sample shows small exothermic dip at 69.9 0 C which may be for the loss of dopant and an endothermic shoulder at 90.8 0 C corresponding to the loss of water molecules. This is followed by the broad exothermic peak may be due to the degradation of the PPy chains. Initially the steep trace TGA consists of two stages of weight loss, one from room temperature to 150 0 C and another from 200 to 400 0 C. Further as the degradation continues and complete at about 11000 C. Steep trace of PPy indicates amorphous nature. The first stage weight loss may be due to water and the weight loss found to be 7.02%., the second stage weight loss may be due to the degradation of PPy-Cl chain, and the weight loss at this stage is-21.73%. The total weight loss at 1100 0 C is about -95%. This ensures the complete degradation of the polymer. The onset temperature (Tonset) and Tmax for second step degradation is 310 0 C and 400 0 C, respectively. These are also confirmed from the DTG trace. Similarly on set temperature for the composites are shown in the table Table 1: Indicate the onset temperature and weight loss from TGA for PPy and PPy/Y2O3 composites Composites Onset Temperature 0 C (from TGA) Completed degradation Temperature 0 C Total loss Occurred (from TGA) Temperature At which Maximum Weight loss 0 C (From DTA) PPy 69.9 1100 95% 704 PPY/20%Y2O3 70.2 1000 80% 846 PPy/50%Y2O3 74.9 920 53% 897 The DSC curve of PPy and PPy/Y2O3sample have a broad characteristic endothermic dip indicates the glass transition temperature of Polypyrrole at 97.32 0 C. The nature of the curve indicates that the loss of water is overlapping with Tg of polymer (which is well matching with the reported value). Lack of any shoulder or melting peak beyond this region indicates amorphous nature with less orderness of the polymer molecules. The DSC curve of PPy/50%Y2O3composite trace has a sharp dip at higher temperature, namely at 125.16 0 C. This sharpness indicates the better crystalline. It also contains few more inflection points; one at 295.74 0 C may be due to the melting of PPy chain, the other at 489.87 0 C may be due to phase change of Y2O3. 2.2 Effect of Temperature on Conductivity Ppy/Y2o3 Composites Figure 1 shows the temperature dependence of σ DC for the PPy and PPy/Y2O3Samples. In this figure symbols indicate log values of experimental conductivities (for temperature range from 100-200 0 C) for various composites. Solid lines indicate their fitting by linear fit equation by using the origin 6.0. The conductivity of all the composites shows that, as the temperature is increased conductivity increases. This figure also indicates that, conductivity increases as the percentage of oxide is increased and then for further increase in oxide content the conductivity decreases. Conductivity of polymer depends on the conjugation length. In the synthesis process, pyrrole monomer was first adsorbed on the surface of Y2O3Concentration, and as a result, the amount of pyrrole associated with each CeO2 concentration, and as a result, the amount of pyrrole associated with each Y2O3 particle is diminished. Figure 1: Arrhenius plot of conductivity of PPy/Y2O3samples
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 02 Issue: 09 | Sep-2013, Available @ http://www.ijret.org 556 The temperature variation of conductivity of PPy composites is well described by Mott’s variable range hopping formalism. This is applicable only in amorphous semiconductors. This is applicable only in amorphous semiconductors. Larger activation energy Implies higher potential barrier in the conduction process originating from the reduction of polymer chain length. Lower conductivity and higher activation energy are due to the poor contact between the polymer and oxide particles. Dispersion of oxide in the conducting polypyrrole due to percolation introduces more conducting paths resulting in higher conductivity. Loading in the polymer increases the conductivity is explained in literature (12) Table 2: Indicates the activation energy of the conduction process for PPy/Y2O3 samples. It indicates that as the oxide content Increases the activation energy goes on decreasing. But in case of PPy/40% Y2O3shows highest activation energy Table 2: Activation energy for PPy/Y2O3composites composites Activation Energy me V Pure PPy 302.85 PPy/10%CeO2 203.98 PPy/20%CeO2 194.98 PPy/30%CeO2 149.51 PPy/40%CeO2 94.08 PPy/50%CeO2 393.23 Current Voltage plot of PPy CeO2 composites: Figure 2: Representative Current -Voltage plots of PPY/Y2O3 samples Figure 2 show the current voltage plots of the representative PPy/Y2O2 composites respectively. They show very good linearity in the range studied. Beyond this range thermal fluctuations due to significant joule heating take place and non linearity sets in. CONCLUSIONS PPy/Y2O3 composite shows the high thermal stability due to metal oxides. Activation energy of these compostes shows highest for ppy/50% Y2O3 due to more metal oxide particles increases the higher activation energy. It will be maximum upto critical percentages latter activation energy decreases. Current voltage characteristics of these polymer composites are also accounted. These electrical properties of polymer PPy/Y2O3 composites have strong applications in battery and sensor applications. REFERENCES: [1]. J. L. Bredas, R. RChance(Eds.), Conjugated Polymeric Materials-Opportunities in optoelectronics and Molecular Electronics, NATO Advanced study Series,(Kluwer, Dordrecht, 1990) p-112. [2]. S. Bhattacharyya and S. K. Saha, Applied Physics Letters 80, ( 24) 2002, 4612 [3]. J.G. Park, B. Kim, S.H. Lee, Y.W. Park Thin Solid Films 438 –439 (2003) 118–122. [4]. T K Vishnuvardhan, V R Kulkarni, C Basavaraja and S C Raghavendra Bull. Mater. Sci., 29, (1) 2006, 77–83 [5]. Jung-Chul Lee , Wonjoo Lee , Sung-Hwan Han, Tae Geun Kim, Yun-Mo Sung Electrochemistry Communications 11 (2009) 231–234 [6]. W.A.Gazotti Jr., GGasalbore-Miceli, S.Mitzakoff, A.Geri,M.C.Gallazzi, M.A.DePaoli, Electrochem.Acta 44(1999)1965. [7]. S.Venkatachalam,P.V.Prabhakaran, Eur.Poly.J. 5(1993)29 [8]. Bernd Tiek and walter Gabriel, Polymer, 31 (1990) 20. [9]. Raghu M, Subramanyam S.V, Chatterjee S, Phys.Rev.B. 1991,43, (5) 4236. [10]. Epistein A.J, Rommelman H, Abkowitz M, and Gibson H.W, Phys.Rev.Lett. 1981,47,1549. [11]. Pople J.A, and Walnsely S.H, Mol. Phys. 5,15(1962). [12].Geon-Woong Lee, Min Park, Junkyung Kim, Jae Ik Lee and Ho Gyu Yoon Composites Part A: Applied Science and Manufacturing 37,( 5), 2006, 727–734