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Conducting composites of polypyrrole with polytetramethylbisphenol A carbonate

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Polytetramethylbisphenol A Carbonate

EMRE KALAYCIOCLU, URAL AKBULUT, and LEVENT TOPPARE'

Department of Chemistry, Middle East Technical University, 06531 Ankara, Turkey

SYNOPSIS

A new conducting composite of polypyrrole (PPy) has been prepared electrochemically where polytetramethylbisphenol A carbonate is used as the insulating matrix polymer. Characterization of the freestanding films of the composites were based on scanning electron microscopy, differential scanning calorimetry, and Fourier transform infrared studies as well as electrical conductivity measurements and solubility. Electrical conductivities were measured by a four-probe technique. Spectroscopic methods, together with conductivity and solubility studies, indicate that the synthesized composite is a homogeneous blend of the two polymers. No evidence of hydrogen bonding in the composite or grafting of the two polymers has been found, contrary to the PPy-polybisphenol A carbonate case. 0 1996 John Wiley & Sons, Inc.

INTRODUCTION

In recent years, numerous studies on electrical conducting polymers have been published. This intensive interest may be attributed t o possible widespread applications of conducting polymers. Heterocyclic polymers particularly have high con- ductivity, such as polypyrrole (PPy) and poly- thiophene ( P T h ) , and their derivatives are of great interest.'-5 These heterocyclic polymers are pre- pared as freestanding films by the electrochemical oxidation of the monomers on platinum or I T 0 electrodes.6-8 However, these conducting polymers have some disadvantages in practical use due t o their poor mechanical and physical properties. As reported by several groups, the electrochemical polymerization of the monomer can also occur on a n electrode which is already coated with a n or- dinary insulating polymer, leading to conducting

composite^.^-^^ In this case, monomers of con- ducting element diffuse into the insulating poly- mer coated on an electrode and start polymeriza- * T o whom correspondence should be addressed. Present address: Department of Chemistry, Bilkent University, 06533 Ankara, Turkey.

Journal of Applied Polymer Science, Val. 61, 1067-1075 (1996)

0 1996 John Wiley & Sons, Inc. CCC OOZl-8995/96/071067-09

tion in the interface between the electrode surface and the host polymer film. T h e objective here is t o obtain homogeneous polymer composites which carry the properties of both conducting and in- sulating polymers, to a certain extent. This kind of conducting polymer synthesis not only improves the poor mechanical and physical properties of heterocyclic polymers but also retains the con- ductivity to a desirable value.14-17 For some of the composites, several spectroscopic techniques re- vealed t h a t the composites which were electro- chemically synthesized have different behaviors than the simple mechanical mixture of the two polymers. Studies previously reported t h a t unlike PTh/polycarbonate (PC), PTh/polystyrene (PS),

and PPy/PS composites, PPy/PC composites possessed very different properties from those of a simple mixture of the two polymers. Low per- colation thresholds were obtained via chemical interactions between the PC and PPY.''-~~ This can be ascribed to a better homogeneity and also t o the possible hydrogen bonding and formation of grafting. Fourier transform infrared (FTIR) analysis of PPy/PC blends revealed t h a t the car- bony1 band broadened together with the formation of a new band a t 1766 cm-l. This new band was interpreted as the H-bonded carbonyl group in the

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-

100- E 0 \ v) A = v

5

0 9 0 - D

5

m

-

080 - 0 7 0 1 1 I I 2 0 00 40 00 60.00 80 00 Weight % of PPy

Figure 1 Conductivities of P P y / T M P C films.

composite. In the differential scanning calorimetry (DSC) studies, P P y / P C composite gave a specific glass transition temperature (T,) a t 337"C,

whereas the

Tg

of P C was reported a s 145°C.21 This result reinforced the idea of forming a homoge- neous composite of P P y / P C not only by simple blending but also by grafting, t o a certain extent. Thermogravimetric analysis (TGA) showed t h a t t h e weight loss did not correspond t o the loss of host polymer in the PPy/PC composite a s i t did in some other composites. T h i s observation con- sequently suggested t h a t t h e strong chemical bonding formed in the PPy/PC blend was stable enough t o prevent the thermal decomposition of pure PC. Scanning electron micrograph (SEM) studies also supported the formation of a homo- geneous composite; no morphologic change was observed between S E M photographs of the P P y / P C films washed with chloroform, t h e solvent of the host polymer, a n d t h e unwashed P P y / P C film. The earlier report concluded that PPy could ap- proach P C to create a chemical interaction. We now

which is prepared by electrochemical technique, as mentioned above. The choice of T M P C lies in the fact that the methyl groups will obscure the for- mation of H-bonding and grafting due to steric hin- derance. We propose that the presence of methyl groups on the insulating polymer will prevent pyrrole oligomers from coming close to the carbonyl moiety of TMPC, thus drastically decreasing the possibility of a chemical interaction between the two polymers. Consequently, the resulting composites will have quite different properties from PPy/PC systems.

EXPERIMENTAL

PPy-TMPC composites were synthesized by electro- chemical polymerization of pyrrole onto a TMPC- coated electrode a t a constant potential of +1.5 V versus Ag"/Ag+ ( M ) . A Wenking POS 73 Po- tentiostat was used for the supply of a constant po- tential in the electrochemical polymerization.

T M P C (Bayer) was dissolved in chloroform ( 10

mg L-') and coated on the platinum electrode by dipping the electrode into the solution. The amounts

of insulating and conducting polymer coatings were estimated gravimetrically.

A three-compartment cell equipped with plati- num foils ( 1.5 cm2) as the working and counter elec- trodes and a capillary reference electrode ( Ag

"

/

Ag+) was utilized in potentiostatic polymerization. The solvent was acetonitrile (Merck) and the sup- porting electrolyte was tetrabutylammonium tetra- fluoroborate ( Aldrich ). As a control, the above ex- periment was also run under the absence of pyrrole. This assured that there were no changes either chemically or by weight in the host polymer. Further details on the potentiostatic electrolyses have been given elsewhere.22

Table I Conductivities of Unwashed and Washed Electrolytic Films Composition of Electrolytic Films (in PPy) Unwashed Electrolytic Film Washed Electrolytic Films 35% 7.8 S/cm 8.8 S/cm 40 ?6 8.5 S/cm 39.0 S/cm 45% 11.1 S/cm 14.7 S/cm

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45 40 aJ 0 g 35 c

-

[

F

s?

3 0 25 20 100 9 5 al 0 2

=

9 0 6 F

'

85

i

80 75 I I )OO 3500 3000 2500 2000 1500 1000 500 ( A ) Wovenumber (cm-1) I 4000 3500 3000 2500 2000 I500 1000 500 Wovenumber (cm-l)

(B)

Figure 2

wt); (D) unwashed electrolytic film (50% PPy wt/wt).

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1

1 I

4000 3500 3000 2500 2000 1500 1000 500

Wovenumber (cm-1)

(D)

(5)

-0.3 0 . I L 45 95 145 195 245 295 345 39 139 98 "C 146.58 "C (I) -0.08608 W/9 -0 I 100 150 200 0 5 0 3

-

-

2

8 0.1

-

LL 0 I c -0 I Temperature ("C) 193 91 "C (I) -0 03049 W/9 188 62 "c I / I

/

I

\;J

83.56 O C Figure 3

mixture of t h e two polymers (40% P P y wt/wt).

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01 - 40 140 240 340 440 I - 0 2 -0 3 Ternpemture ("C )

Figure 3 (Continued from the previous page) 89 26°C

-

Conductivities of the samples were measured via a four-probe technique. The composites were char- acterized by FTIR (Nicolet 510 FT-Spectrometer) ,

S E M ( J E O L JSM-6400 Scanning Microscope), DSC (910 S; Dupont Instrument), and TGA (951

Thermogravimetric Analyzer; Dupont Instrument).

RESULTS AND DISCUSSION

A black film was produced by electrochemical po- lymerization of pyrrole onto a TMPC-coated anode electrode. This film could readily be peeled off the electrode surface as a freestanding film.

Conductivities of several freestanding films in dif- ferent P P y percentages were measured. As seen in Figure 1, which gives the relation between the com- position and the conductivity of freestanding films, there is no percolation threshold; that is, conduc- tivity increases correspondingly as the amount of conducting polymer increases in the composite.

T h e freestanding films were left in the chloro- form, which is the solvent of the host polymer, for at least 1 wk. Weight loss revealed t h a t TMPC, the host polymer, can be removed from the produced composite by simple washing. It was observed that after washing the freestanding films, the conductiv- ity increased compared with unwashed films (Table

I ) . This may be attributed to the removing of the host polymer from the electrolytic film upon simple washing.

FTIR analysis of washed and unwashed free- standing films and pure conducting and insulating polymers was performed. Comparing the FTIR spectroscopies of washed and unwashed films indi- cated that the peak carbonyl moiety disappeared upon washing the film [Fig. 2 (c-d)

1.

Moreover, no significant difference was observed between the FTIR spectra of the pure conducting polymer and the washed freestanding film [Fig. 2 ( a-c )

1.

These are evidence that the two polymers used in the syn- thesis of the composite forms only physical adhesion rather than chemical bonding.

DSC studies also revealed that thermal behavior of the P P y / T M P C electrolytic composite is not much different than that of a simple mechanical mixture of the two polymers (Fig. 3 ) .

Interpretation of TGA scans is further evidence that PPy does not chemically interact with T M P C in the electrochemical preparation. T h e TGA scan

of washed freestanding film is the same as the pure P P y film [Fig. 4 ( a-c)

1.

Examining the TGA of un- washed freestanding film revealed a weight loss cor- responding to the loss of host polymer [Fig. 4 ( d )

1.

SEM studies revealed that the solution and elec- trode sides of the PPy/TMPC electrolytic composite

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120 - 494 95 "C - 80 - - I 673 59°C

-

60

-

$

P

-

- S P 4 0 - c_v

-

20 - 0 5714 % 0 30 230 430 630 830 Temperature ("C) 2 0 15 V \ 10

g

z

-

S P 2 b 0 - 0 5 - - 0 0 + - 0 5 125 0 20

-

9

..

3 15

g

i P 3 10 ' ?

P

d 0 05 0.00 ( A )

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Ternperoture ("C)

(C)

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(b)

SEM micrographs of the electrolytic film: (A) Figure 5

electrode side; (B) solution side.

do not have the same morphology. The differing morphology of the two sides indicates that blending these two polymers electrochemically does form a composite rather than a graft c ~ p o l y m e r ' ~ (Fig. 5 ) .

CONCLUSION

Evidence has indicated that PPy cannot be linked to TMPC in the PPy/TMPC composite as it can to polybisphenol-A carbonate. It may be strongly due to the steric hinderance of methyl groups at- tached to the phenyl groups, which prevents pyrrole oligomers from interacting with the carbonyl moiety

of TMPC.

This study indirectly confirms the existence of H-bonding between PPy and PC, and the formation of grafting in P P y / P C composite. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. REFERENCES

1. K. Kaneto, S. Ura, K. Yoshino, and Y. Inuishi, Jpn. J . Appl. Phys., 2 3 , L189 ( 1984).

2. R. L. Elsenbaumer, K. Y. Jen, G. G. Miller, and L. W. Shacklette, Synth. Met., 1 1 8 , 277 (1987).

3. G. Tourillon, in Handbook of Conducting Polymers, T. A. Skotheim., Ed., Marcel Dekker, New York, 1986. 4. D. Braun, D. Moses, C. Zhang, and A. J. Heeger,

Synth. Met., 5 5 , 4 1 4 5 ( 1993).

5. S. Dogan, U. Akbulut, T. Yalcin, S. Suzer, and L. Toppare, Synth. Met., 6 0 , 27 ( 1993).

6. A. F. Diaz, K. K. Kanazawa, and G. P. Gardini, J . Chem. Soc., Chem. Commun., 635 ( 1 9 7 9 ) .

G. Tourillon and F. Gamier, J . Electroanal. Chem., 135, 173 ( 1 9 8 2 ) .

A. F. Diaz and K. K. Kanazawa, Chem. SOC., 1 7 , 45 (1981 ) .

0. Niwa and T. Tamamura, J . Chem. SOC., Chem. Commun., 817 ( 1984).

M. De Paoli, R. J. Waltman, A. F. Diaz, and J. Bargon, J . Chem. SOC., Chem. Commun., 1015 ( 1 9 8 4 ) . M.-A. De Paoli, R. J. Waltman, A. F. Diaz, and J. Bargon, J . Polym. Sci., Polym. Chem. Ed., 23, 1687 ( 1985).

0. Niwa, T. Tamamura, and M. Kakuchi, Macromol- ecules, 20, 749 ( 1987).

G. Nagasubramanian and S. DiStefano, J . Electro- chem. SOC. Extended Abstr., 8 5 , 659 ( 1 9 8 5 ) .

S . Dogan, U. Akbulut, and L. Toppare, Synth. Met., 5 3 , 29 ( 1 9 9 2 ) .

F. Selampinar, U. Akbulut, T. YalCin, $. Suzer, and L. Toppare, Synth. Met., 6 2 , 201 ( 1 9 9 4 ) .

U. Geissler, M. L. Hallensleben, and L. Toppare, Adu. Mat., 104, 3 ( 1 9 9 1 ) .

U. Geissler, M. L. Hallensleben, and L. Toppare, Synth. Met., 40, 239 ( 1 9 9 1 ) .

R. Zallen, The Physics of Amorphous Solids, Wiley: New York, 1983, Chap. 4.

M. Aldiss and A. R. Bishop, Polymer, 2 6 , 6 2 2 (1985).

S . Hotta, S. D. D. V. Rughooputh, and A. J. Heeger, Synth. Met., 2 2 1 , 7 9 ( 1 9 8 7 ) .

H. L. Wang, L. Toppare, and J. E. Fernandez, Mac- romolecules, 2 3 , 1053 ( 1 9 9 0 ) .

L. Toppare, S. Eren, 0. Ozel, and U. Akbulut, J . Ma- cromol. Sci., Chem., 2 1 , 1281 ( 1984).

Received May 15, I995

Şekil

Figure  1  Conductivities of  P P y / T M P C   films.

Referanslar

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