Journal of Composites
Volume 2014 (2014), Article ID 838975, 9 pages
http://dx.doi.org/10.1155/2014/838975

Research Article

Synthesis, Characterization, and Photoconductivity Studies on Poly(2-chloroaniline) and Poly(2-chloroaniline)/CuO Nanocomposites

Porselvi Linganathan,¹ Jency Sundararajan,² and Jhancy Mary Samuel¹

¹Department of Chemistry, Auxilium College, Vellore, Tamil Nadu 632006, India
²Department of Electrical Engineering, University of Washington, Seattle, WA 98195, USA

Received 19 June 2014; Revised 20 August 2014; Accepted 10 September 2014; Published 14 October 2014

Academic Editor: Suying Wei

Copyright © 2014 Porselvi Linganathan et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

The poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages (5%, 10%, 15%, 20%, and 25%) were synthesized by in situ chemical oxidative polymerization method using ammonium per sulphate (oxidant), HCl (dopant), and dodecyl benzene sulphonic acid as a surfactant at 0°C. The formation of polymer and its composites was confirmed by FTIR and UV-Visible spectroscopy. The SEM and X-ray diffraction studies clearly indicate the uniform dispersion of CuO nanoparticles into the polymer matrix. The thermal stability of the polymer and its composites increased with increase in the percentage of CuO nanoparticles. The polymer and composites exhibit fluorescence property and hence can be used in the light emitting diodes. The current voltage (I-V) curves clearly illustrate the enhanced conductivity on light exposure compared to the dark current. The conductivity of the polymer increased with increase in the percentage of CuO nanoparticles. Poly(2-chloroaniline)/CuO nanocomposites with 25% of CuO show a maximum conductivity of  S cm⁻¹. The composites synthesized behave as organic metals due to their semiconducting nature.

1. Introduction

Electrically conducting polymers are a class of synthetic metals that combine the chemical and mechanical properties of polymers with the electronic properties of metals and semiconductors [1]. Typical conducting polymers include polyacetylene, polyaniline, polypyrrole, polythiophene, poly(para phenylene), poly(phenylene vinylene), and polyfuran [2]. Ease of synthesis, environmental stability, ease of transformation in cathodic protection, and special electronic, optical, and magnetic properties attract researchers to extensively study polyaniline in the recent past [3]. In spite of various advantages, polyaniline has certain limitations when it comes to its applications as it is neither soluble nor fusible in organic solvents as well as water [4]. In order to overcome such disadvantages, attempts have been made by the use of molecular design, modification of monomer structure, use of functionalized acid dopant, formation of blends/composites, and copolymerization [5].

Organic-inorganic composites have attracted considerable attention as they can combine the advantages of both components and may offer special properties through reinforcing or modifying each other [6]. To improve and extend the functions of the conducting organic materials, inorganic materials such as metals and metal oxides are often incorporated to form multifunctionalized composites for various applications in the fields of electronics, sensors, catalysis, energy, electromagnetic interference shielding, and biomedicine [7]. The inorganic fillers at nanoscale exhibit high surface to volume ratio and thus are expected to modify the electrical, optical, thermal, and dielectric properties of polymer drastically [8].

Polyaniline and its derivatives have attracted considerable attention to the preparation of its composites with metals and metal oxides, such as conducting polyaniline/WO [9], polyaniline/ZnO-ZrO₂ [10], polyaniline/Fe₃O₄ [11], polyaniline/TiO₂ [12], polyaniline/NiO [6], polyaniline/Fe₂O₃ [13], polyaniline/Se [14], polyaniline/Nb₂O₅ [15], polyaniline/Co₃O₄ [16], polyaniline/ZnO [17], polyaniline/CdS [18], polyaniline/Cu [19], poly(2-chloroaniline)/SiO₂ [1], polyaniline-dodecylbenzenesulfonic acid (DBSA)/organophilic clay [20], polyaniline/SnO₂ [21], polyaniline/CuO [22], and poly(o-chloroaniline)/ZnO [23] nanocomposite systems. However to the best of our knowledge there are no reports on the study of poly(2-chloroaniline)/CuO nanocomposites.

In the present investigation, poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages of CuO (5%, 10%, 15%, 20%, and 25%) were prepared by in situ chemical oxidative polymerization technique using hydrochloric acid as dopant, ammonium per sulphate as an oxidant, and dodecyl benzene sulphonic acid as a surfactant (it can act as another dopant as well) at 0–5°C. This pathway was selected because one expects that the presence of dodecyl benzene sulphonic acid in the polymer composites enhances the solubility, stability, and conductivity in organic solvents and hence the processability. The resulting polymer and polymer composites were characterized by FT-IR, UV, SEM, XRD, and fluorescence studies. The thermal properties were studied by TGA and DTA analysis and the electrical conductivities were measured from the I-V graph using two-point probe method.

2. Experimental

2.1. Synthesis of Poly(2-chloroaniline) and Poly(2-chloroaniline)/CuO Nanocomposites

2-Chloroaniline, ammonium per sulphate, and dodecyl benzene sulphonic acid were purchased from LOBA Chemic, Qualigens, and Avra Synthesis Pvt. Ltd, respectively. CuO nanoparticles were purchased from Sigma Aldrich.

The poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages (5%, 10%, 15%, 20%, and 25%) were synthesized by chemical in situ oxidative polymerization method [24]. The equimolar volumes of 0.6 M solution of 2-chloroaniline and hydrochloric acid were prepared in double distilled water, mixed and kept in the freezing mixture. CuO was added in various weight percentages (5%, 10%, 15%, 20%, and 25%) to the above solution and kept for vigorous stirring (30 min) to keep the CuO suspended in the solution. The black coloured CuO nanoparticles were consistently dispersed in the monomer solution. 0.6 M ammonium per sulphate (12.78 g in 100 mL water) and 0.03 M dodecyl benzene sulphonic acid (1 mL in 100 mL of water) were taken in separate beakers. The oxidant and the surfactant were added slowly to the mixture containing 2-chloroaniline and CuO nanoparticles for more than 30 minutes and the stirring was continued for six hours. The product was placed in the refrigerator overnight. The green coloured product was filtered, washed, and dried. The same procedure was adopted for the synthesis of poly(2-chloroaniline)/CuO nanocomposites of various weight percentages of CuO (5%, 10%, 15%, 20%, and 25%).

Adopting the same procedure, poly(2-chloroaniline) was prepared in the absence of CuO. The polymer composites were obtained in higher yields than the polymer. The weight of the poly(2-chloroaniline) obtained is 3.37 g. The weights of the poly(2-chloroaniline)/CuO nanocomposites with various weight percentages (5%, 10%, 15%, 20%, and 25%) are 3.49 g, 3.75 g, 4.02 g, 4.29 g, and 4.51 g, respectively. The percentage yields of poly(2-chloroaniline)/CuO nanocomposites (5%, 10%, 15%, 20%, and 25%) when compared to the pure polymer are 3.5%, 11.2%, 19.3%, 27.2%, and 33.8%. When the CuO weight percentage increases gradually the incorporation of CuO nanoparticles into the polymer matrix also increases as evident from the results. The polymer and polymer composites were soluble in DMSO and partially soluble in most of the organic solvents.

2.2. Characterization

The FT-IR spectra of poly(2-chloroaniline) and poly(2-chloroaniline/CuO) nanocomposites in KBr were recorded by Thermo Nicolet, Avatar 370 spectrophotometer from 500 cm⁻¹ to 4000 cm⁻¹. The UV-Visible spectra were recorded from 200–800 nm using Systronics double beam spectrophotometer 2201. XRD analyses of polymer and polymer composites were performed on a Bruker AXS D8 advance X-ray diffractometer using Cu-K, wavelength 1.5406 Å. The surface morphology of the polymer and polymer composites was studied using a JEOL model JSM-6390LV Scanning Electron Microscope at an accelerating voltage of 15 KV. Thermogravimetric analyses were carried out with a Perkin Elmer STA 6000 at the heating rate of 10°C/min from 40°C to 750°C under an inert gas atmosphere.

A custom built two-probe optoelectrical measurement unit was used to study the photoconductivity properties of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages. Schematic representation of the measurement system is displayed in Figure 1. The setup consisted of an optical microscope (bright LED illuminator with 6-watt power), probe station (with tungsten probes from Micromanipulator Company), a Keithley source meter, a nanoammeter, and a computer. The probes from the sample are connected to the Keithley source meter, which was controlled by computer using the lab software. Current voltage (I-V) characteristics in dark and light environments were carried out for poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites at atmospheric pressure and room temperature. A sweep voltage of ±10 V was used to perform the measurements.

Figure 1: Schematic representation of the custom built experimental setup used to carry out electrical measurement.

3. Results and Discussion

3.1. FT-IR Spectroscopy

The FTIR spectrum of pure poly(2-chloroaniline) is shown in Figure 2(a). The N–H stretching frequency of poly(2-chloroaniline) is observed at 3074 cm⁻¹. The asymmetric and symmetric stretching frequencies of –CH present in dodecyl benzene sulphonic acid (DBSA) are observed at 2924 cm⁻¹ and 2856 cm⁻¹. The characteristic peaks due to quinonoid and benzenoid rings of poly(o-chloroaniline) occur at 1581 cm⁻¹ and 1510 cm⁻¹ [25, 26]. The peak at 1303 cm⁻¹ is due to aromatic C–N stretching vibration. The bands at 918 cm⁻¹ and 833 cm⁻¹ are due to –CH out of plane bending vibration of 1, 2, 4 tri substituted aromatic rings. The peak at 748 cm⁻¹ corresponds to the chloro group attached to the phenyl ring. All the above peaks confirm the polymerization of 2-chloroaniline.

(a)

(b)

Figure 2: (a) IR spectrum of poly(2-chloroaniline). (b) IR spectrum of poly(2-chloroaniline)/CuO nanocomposite with 5% CuO nanoparticles.

The FTIR spectra of poly(2-chloroaniline)/CuO with 5% of CuO are shown in Figure 2(b). The N–H stretching frequency of poly(2-chloroaniline)/CuO is observed at 3066 cm⁻¹. The asymmetric and symmetric stretching frequencies of –CH present in dodecyl benzene sulphonic acid (DBSA) are observed at 2922 cm⁻¹ and 2854 cm⁻¹. The characteristic peaks due to quinonoid and benzenoid rings of poly(2-chloroaniline) occur at 1579 cm⁻¹ and 1504 cm⁻¹. The peak at 1300 cm⁻¹ is due to aromatic C–N stretching vibration. The bands at 898 cm⁻¹ and 827 cm⁻¹ are due to –CH out of plane bending vibration of 1, 2, 4 tri substituted aromatic rings. The peak at 750 cm⁻¹ corresponds to the chloro group attached to the phenyl ring. The characteristic stretching frequencies are shifted towards the lower frequency side in the composite when compared to poly(2-chloroaniline). The above peaks confirm the formation of composite and also suggest a van der Waals kind of interaction between the polymeric chain and CuO nanoparticles. The same results were found in the polymer composites with 10%, 15%, 20%, and 25% of CuO which confirm the formation of poly(2-chloroaniline)/CuO composites.

3.2. UV-Visible Spectroscopy

The UV-Visible spectra of pure poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various percentages of CuO (5%, 10%, 15%, 20%, and 25%) are shown in Figure 3 ((A)–(F)). The spectra of the poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with various weight percentages in DMSO (solvent) show three absorption bands at ~250 nm, ~360 nm, and ~550 nm. The absorption bands ~250 nm are due to transition of the benzenoid rings and ~360 nm are due to transition of quinonoid rings. The bands around 550 nm are due to the electron transition between the highest occupied molecular orbital of the benzenoid ring to the lowest unoccupied molecular orbital of the quinonoid ring [27, 28]. The intensities of the three absorption bands increase with increase in the percentage of CuO. When compared to poly(2-chloroaniline), the poly(2-chloroaniline)/CuO nanocomposites are absorbed at higher wavelength. The red shift which is observed in the polymer composites of varying composition is attributed to the presence of CuO embedded into the polymer chain. This also results in the broadening of the absorption. This type of interaction may be due to the hydrogen bonding between N–H···O of the polymer and CuO, respectively.

Figure 3: UV-Visible spectra of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages of CuO nanoparticles.

3.3. X-Ray Diffraction Studies

The XRD patterns of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages (5%, 10%, 15%, 20%, and 25%) are compared in Figure 4 ((A)–(G)).The XRD pattern of CuO nanoparticles is shown in Figure 4(G). Figure 4(A) shows the diffraction peaks (broad) around 2θ = 7° and 26° due to the characteristic peaks of emeraldine salt structure [29]. This also substantiates the absorption in the IR spectrum at 1124 cm⁻¹ which is the electrical conductivity peak due to the emeraldine salt structure. In Figure 4(G), the CuO nanoparticles show two sharp peaks between 2θ = 30° and 40° due to highly crystalline nature of CuO nanoparticles.In the composites, the high intensity peaks of CuO were masked by the presence of poly(2-chloroaniline). The peak at 2θ = 26° seems to shift to higher wavelength with decreasing intensity as the percentage of CuO increases. This observation from the XRD data endorses the uniform molecular level dispersion of CuO nanoparticles into the poly(2-chloroaniline) chain.

Figure 4: XRD patterns of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with 5%, 10%, 15%, 20%, and 25% of CuO nanoparticles and pure CuO, respectively.

3.4. Thermogravimetric Analysis

Thermal degradation patterns of the pristine poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites are displayed in Figure 5(a) ((A)–(F)). The derivative curves of poly(2-chloroaniline) and composites are shown in Figure 5(b). The TGA of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites undergo four weight loss steps. The first step weight loss around 100°C is due to removal of water; the second weight loss around 300°C is due to removal of HCl; the third weight loss around 450°C is due to removal of dodecyl benzene sulphonic acid dopant; and the exothermic decomposition of poly(2-chloroaniline) starts around 500°C. The decomposition of poly(2-chloroaniline) is continuous up to 700°C and even after 700°C the complete decomposition has not taken place. The decomposition of the poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites leaves some char content. This shows that the presence of chlorine has prevented the complete decomposition. When compared to the poly(2-chloroaniline), the poly(2-chloroaniline)/CuO nanocomposites with various weight percentages show lower weight losses. The poly(2-chloroaniline) has 29.98% residue and the poly(2-chloroaniline)/CuO nanocomposites with 5%, 10%, 15%, 20%, and 25% have 35.30%, 36.98%, 37.00%, 38.38%, and 40.52% residues, respectively. Though several reports demonstrate that the lowered thermal stability of polymer composites with the incorporation of inorganic materials is due to the weakened interfacial interaction between the two components [30, 31], in the present work, the thermal stability of the polymer composites improved because of the presence of CuO nanoparticles. When the temperature is increased the polymer (organic polymer) decomposed continuously but the CuO present in the polymer matrix does not decompose as the thermal stability of CuO is high. As the percentage of CuO increases, the amount of CuO in the polymer matrix also increases and hence the percentage of residue increases gradually.

(a)

(b)

Figure 5: (a) TGA of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with 5%, 10%, 15%, 20%, and 25% of CuO and pure CuO nanoparticles, respectively. (b) TGA derivative curve of poly(2-chloroaniline).

3.5. Surface Morphology

SEM micrographs of the pristine poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites containing different amounts of CuO are displayed in Figures 6(a)–6(f). Pristine poly(2-chloroaniline) (Figure 5(a)(A)) shows an aggregated structure, while poly(2-chloroaniline)/CuO nanocomposites exhibit an aggregated grainy morphology. Surface morphology of the poly(2-chloroaniline)/CuO nanocomposites with weight percentages (5% and 10%) are shown in Figures 6(b) and 6(c). Here the morphology is almost analogous to the pristine poly(2-chloroaniline) (Figure 6(a)) because of the lower amount of CuO nanoparticles, whereas in poly(2-chloroaniline) with weight percentages 20% and 25% (Figures 6(e) and 6(f)), the visibility of the CuO particles is very high due to the increase in the amount of CuO nanoparticles in the polymer. But in case of poly(2-chloroaniline)/CuO (15%) nanocomposites (Figure 6(d)), the perceptibility of the embedded CuO nanoparticles into the polymer chain is phenomenal. The SEM pictures obviously reveal that the CuO nanoparticles are embedded in the polymer matrix. The compactness of the polymer nanocomposites is also increased with increase in the CuO weight percentage. Surface morphology is also an evidence for the uniform dispersion of CuO nanoparticles into the poly(2-chloroaniline) chain.

(a)

(b)

(c)

(d)

(e)

(f)

Figure 6: Surface morphology of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with 5%, 10%, 15%, 20%, and 25% of CuO nanoparticles, respectively.

3.6. Fluorescence Studies

The fluorescence spectra of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with various weight percentages in dimethyl sulfoxide are shown in Figure 7. The fluorescence of a conjugated polymer can be described in terms of semiconductor band theory. Upon photoexcitation of a conjugated polymer, the electrons from the valence band are excited to the conduction band and then migrated along the polymer backbone. The excited electron and the oppositely charged hole attract one another. When the excited electron combines with the hole a photon is emitted and it is known as fluorescence. The excitation wavelength of polymer and composites is around 350 nm. The poly(2-chloroaniline)/CuO nanocomposites with various weight percentages show emissions around 360 nm, 450 nm, and 730 nm but the poly(2-chloroaniline) shows emission around 400 nm, 450 nm, and 730 nm. The fluorescence spectra clearly illustrate that the poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages have fluorescence properties and can find applications in the manufacture of light emitting diodes.

Figure 7: Fluorescence spectra of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages of CuO nanoparticles.

3.7. Conductivity Studies

The poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages were finely powdered and pressed into pellets using IR Sample Press using Model AVAPAR-330 Thermonicolate applying a maximum pressure of 15 tons/cm² to form circular pellets of 1 cm diameter each. The thicknesses of the pellets were measured using screw gauge. The pellets were used to perform conductivity studies by applying a bias voltage and monitoring the variations in current. Typical I-V characteristic graph of poly(2-chloroaniline) under dark and light (microscopic light) conditions is displayed in Figure 8. The conductivity studies on the sample revealed an enhanced electrical conductivity upon light exposure compared to the dark current. Precisely, an order of magnitude variation in electrical conductivity was observed. The observed enhancement in the current when exposed to the light is mainly due to the photogeneration of charge carriers present in the poly(2-chloroaniline) chain. The curves show that in both cases the current increases continuously with the applied voltage. The fluctuations in the current are due to the coarse surface of the poly(2-chloroaniline). The same observations were found in the poly(2-chloroaniline)/CuO nanocomposites with various weight percentages.

Figure 8: Current voltage (I-V) curves of poly(2-chloroaniline) in the light and dark conditions.

The resistance of the poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages was determined from the I-V characteristics at a constant voltage (5 V). Resistances were converted into conductivity using the thickness of the pellet. The resistance and conductivity of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages at constant voltage (5 V) in the presence and absence of light were tabulated in Tables 1 and 2, respectively.

Table 1: The conductivity of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites in the presence of light.

Percentage of CuO (%)
Current
(at = 5 V)
Sheet resistance ()
Thickness () (cm)
Resistivity () =
Conductivity = () (S cm⁻¹)

0
3.10E − 06
1.61E + 06
0.038
6.13E + 04
1.63E − 05

5
8.58E − 06
5.83E + 05
0.066
3.84E + 04
2.60E − 05

10
1.12E − 05
4.46E + 05
0.053
2.36E + 04
4.23E − 05

15
2.10E − 05
2.38E + 05
0.06
1.43E + 04
6.99E − 05

20
2.84E − 05
1.76E + 05
0.075
1.32E + 04
7.57E − 05

25
3.16E − 05
1.58E + 05
0.047
7.44E + 03
1.34E − 04

Table 2: The conductivity of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites in the absence of light.

Percentage of CuO (%)
Current
(at = 5 V)
Sheet resistance ()
Thickness () (cm)
Resistivity () =
Conductivity = () (S cm⁻¹)

0
4.05E − 06
1.23E + 06
0.038
4.69E + 04
2.13E − 05

5
1.19E − 05
4.19E + 05
0.066
2.77E + 04
3.61E − 05

10
1.90E − 05
2.64E + 05
0.053
1.40E + 04
7.15E − 05

15
2.29E − 05
2.18E + 05
0.06
1.31E + 04
7.63E − 05

20
3.01E − 05
1.66E + 05
0.075
1.25E + 04
8.03E − 05

25
4.82E − 05
1.04E + 05
0.047
4.88E + 03
2.05E − 04

Figure 9 shows the conductivity data for poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages (5%, 10%, 15%, 20%, and 25%) in the presence and absence of light. The conductivity of the poly(2-chloroaniline)/CuO nanocomposites with various weight percentages shows higher conductivity than the poly(2-chloroaniline). When the percentage of CuO is increased the conductivity of the polymer is also increased. An order of magnitude increase in conductivity was observed in the poly(2-chloroaniline)/CuO nanocomposite (with 25% of CuO) compared to the poly(2-chloroaniline).

Figure 9: Conductivity of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO with 5%, 10%, 15%, 20%, and 25% of CuO nanoparticles.

When compared to the conductivity of poly(2-chloroaniline) in the presence and absence of light, high conductivity was detected in the presence of light. The observed enhancement in the current when exposed to the light is mainly due to the photogeneration of charge carriers present in the poly(2-chloroaniline) chain. The enhancement of conductivity was also observed in poly(2-chloroaniline)/CuO nanocomposites with various weight percentages inthe presence of light.

4. Conclusion

Poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages of CuO (5%, 10%, 15%, 20%, and 25%) were successfully synthesized by in situ chemical oxidative polymerization method using ammonium per sulphate (oxidant), HCl (dopant), and dodecyl benzene sulphonic acid as the surfactant at 0°C. FTIR spectra of poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites with various weight percentages of CuO nanoparticles show the characteristics peaks with shifts in the wavelength in the case of composites confirming that there is interaction between the poly(2-chloroaniline) and the CuO nanoparticles. With increasing the percentage of the CuO the broadening of the peak was also observed in the UV spectrum, indicating that the absorption bands of poly(2-chloroaniline) were influenced by CuO nanoparticles present in the polymer chain. Poly(2-chloroaniline)/CuO nanocomposites show higher thermal stability than poly(2-chloroaniline) and the thermal stability increased with increase in the CuO percentage. The decreased crystallinity of CuO nanoparticles in the polymer composites indicates the uniform dispersion of CuO into the poly(2-chloroaniline) chain. The SEM pictures clearly reveal that CuO nanoparticles are embedded in the polymer matrix. The compactness of the composites increased with increase of the CuO percentage. The fluorescence intensity increased with increase in the CuO nanocomposites. From I-V curves the conductivity of the poly(2-chloroaniline) and poly(2-chloroaniline)/CuO nanocomposites was found in the light and dark condition. The enhanced conductivity was observed in the presence of light due to the excitation of charge carriers in the presence of light. Poly(2-chloroaniline)/CuO nanocomposites with 25% of CuO show a maximum conductivity of 2.05 × 10⁻⁴ S cm⁻¹.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

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