# Characterization of MWCNT-PEDOT: PSS Nanocomposite Flexible Thin Film for Piezoresistive Strain Sensing Application

Authors: Roopa Hegde; Koona Ramji; Swapna Peravali; Yallappa Shiralgi; Gurumurthy Hegde; Lavakumar Bathini
Journal: Advances in Polymer Technology
 (2019)

---

## Abstract

Multiwalled carbon nanotubes (MWCNTs) were synthesized by the reduction of ethyl alcohol with sodium borohydride (NaBH4) under a strong basic solvent with the high concentration of sodium hydroxide (NaOH). Nanocomposites of different concentration of MWCNT dispersed in poly(3,4-ethylene dioxythiophene) polymerized with poly(4-styrene sulfonate) (PEDOT:PSS) were prepared and deposited on a flexible polyethylene terephthalate (PET) polymer substrates by the spin coating method. The thin films were characterized for their nanostructure and subsequently evaluated for their piezoresistive response. The films were subjected to an incremental strain from 0 to 6% at speed of 0.2 mm/min. The nanocomposite thin film with 0.1 wt% of MWCNT exhibits the highest gauge factor of 22.8 at 6% strain as well as the highest conductivity of 13.5 S/m. Hence, the fabricated thin film was found to be suitable for piezoresistive flexible strain sensing applications.


---

## Body

## 1. Introduction

Multiwalled carbon nanotubes (MWCNTs) have unique electrical [1] and mechanical properties [2]. The piezoresistive properties of arbitrarily dispersed MWCNT networks in polymer matrix were studied [3].Carbon nanotubes(CNTs) are effective because of their high aspect ratios that form conductive paths at a very low concentration of CNTs [4]. CNT networks can be visualized as a box of the three-dimensional statistical resistors network model with a tunneling effect between adjacent nanotubes. A percolation behavior between CNT and polymer forms conductive paths because of interconnecting CNTs within the network [5]. The piezoresistivity of the CNT network is a function of the conductive paths formed by CNTs, tunneling between neighboring CNTs and CNT piezoresistivity.Currently, there are many techniques to produce high-quality MWCNT, namely, electric arc discharge [6], chemical vapour deposition (CVD) [7], and laser vaporization [8]. Production of MWCNT by laser ablation and arc discharge methods cannot be scaled up to industrial capacities. However, the CVD method is useful for the large-scale production of MWCNT. In this paper, the synthesis of MWCNT was performed using modified Wolff-Kishner reduction process.Various investigations were carried out on CNT films [9, 10] and CNT/polymer composites [11, 12] for application as strain sensors. CNT film shows weak stress transfer due to bonding by weak van der Waals forces [10]. To overcome this drawback, CNTs are integrated into a polymer matrix to decrease the slippage between the adjoining CNTs and improve the stress transfer properties. Hence, CNT/polymer-based nanocomposites are one of the best suitable materials for strain sensing application [13].Nanocomposite material has at least one of the dimensions of one of its constituents in nanometer scale [14]. Silicon or metals such as NiCr or Cu-Ni on flexible substrates suffer from the ease of fracture under a large applied load [15] and hence polymer-based composites filled with nanoparticles are preferable for their similar application. The conductive polymers with MWCNT as filler combine the electrical, electronic properties of a metal and mechanical properties of a conventional polymer and hence can be used in flexible electronics and strain sensors [16, 17].The polymer, PEDOT (polythiophene derivative, poly(3,4-ethylene dioxythiophene)), shows high conductivity in comparison with other polymers [18]. However, PEDOT has poor solubility in water and organic solvents. The solubility can be improved by using water-soluble polyelectrolyte, such as PSS (poly-(styrene sulfonic acid)) which is dissolved into PEDOT to form a PEDOT: PSS aqueous composite [19].The piezoresistive study was conducted on pure MWCNT films as well as MWCNT dispersed in various polymer matrixes resulting in MWCNT-polymer nanocomposite films. Fabrication of pure MWCNT films was undertaken by solution/filtration method and the changes in resistance of pure MWCNT were proportional to the applied strain and the temperature effect on the resistance of the film was observed [9]. Polyimide (PI)-MWCNT composites were prepared by in situ polymerization and the nanocomposites showed increasing variation in electrical resistivity with the increasing applied pressure which makes them ideal for fabrication of a polymer pressure sensor [20]. Another piezoresistive response study of MWCNT-PI nanocomposite was demonstrated with different MWCNT concentrations. Here, the surface conductivity of the nanocomposite was determined by atomic force microscopy in current mode. This nanocomposite was proved to be useful for strain sensing element in a microelectromechanical system (MEMS)/nanoelectromechanical system (NEMS) based piezoresistive pressure sensor applications [21]. The typical percolation phenomenon was observed in a nanocomposite with MWCNT as conductive filler and Styrene-Butadiene-Styrene (SBS) as a polymer matrix while testing for electrical and mechanical properties. Unlike in the above discussed studies, the resistance of the MWCNT-SBS nanocomposite film decreased rapidly with increasing stress for a low range of stress [22]. The piezoresistive properties of MWCNT-polypropylene nanocomposites for different MWCNT concentrations were characterized above electrical percolation under quasistatic tension. It was observed that, with the increase in MWCNT concentration, the electrical conductivity of the nanocomposites increased monotonically. The sensitivity of nanocomposites was found to be higher for composites with lower MWCNT concentration [23]. The piezoresistive sensors array was developed by screen printing of MWCNT in poly(dimethylsiloxane) (PDMS) matrix on flexible polyethylene terephthalate (PET) substrate. The increase in resistance was recorded in structures under the influence of increasing compressive forces [24]. MWCNT-PDMS piezoresistive nanocomposite was studied for an extremely small range of pressure required for finger sensing. MWCNTs were modified by poly(3-hexylthiophene) (P3HT) [25] to attain a homogeneous dispersion and for lowering the percolation threshold of MWCNT in PDMS. MWCNT-epoxy nanocomposite was investigated under uniaxial cyclic tensile and compressive loading in low strain range applications. It was observed that the nanocomposite showed stable response and durable behavior after uniaxial tensile and compressive cycles with increasing change in resistance [26]. Another study on piezoresistive properties of MWCNT-epoxy composites was conducted by the electrochemical impedance spectroscopy (EIS) where the bend over the sensor area was tested by digital image correlation (DIC) under quasistatic uniaxial tension. A highly deformable nanocomposite consisting of MWCNT in elastic polyurethane was studied under compression, bending, and extending and also exposed to chemical vapors showing corresponding resistance change [27]. Flexible and deformable sensors were developed with MWCNT-latex thin films by spray-coating and integrating it with fabric. Spatial pressure sensing was achieved and validated using an electrical impedance tomography algorithm. The resistivity distribution of the fabric and its changes on application of pressure at different locations were evaluated by the algorithm [28].The electrical properties of MWCNT-PEDOT: PSS thin films under temperature and humidity effects were studied and it was concluded that this nanocomposite is insensitive to humidity and hence can be used as strain sensors [29]. As brought out above, the PEDOT: PSS is a good material to be used as the polymer matrix since it shows high conductivity and the MWCNT as nanofiller has shown excellent piezoresistive response when dispersed in the polymer matrix for an applied strain. We have investigated the effects of using different wt% of synthesized MWCNT in PEDOT: PSS on the conductivity, electrical resistance, and a gauge factor of MWCNT-PEDOT: PSS.


## 2. Experimental Details

There are various methods for the synthesis of MWCNT as arc discharge, laser vaporization, pyrolysis, and CVD. In this paper, synthesis of MWCNT was performed using modified Wolff-Kishner reduction process. This is a base-catalyzed process that produces alkane from the corresponding aldehydes or ketones. Aldehydes or ketones are converted to the corresponding hydrazone and thereafter decomposed in the presence of strong basic conditions to yield the reduced alkyl derivative and nitrogen. MWCNTs were synthesized using modified Wolff-Kishner reduction process where it has advantages over other conventional processes such as it is performed under mild conditions, high purity CNTs are produced because no catalysts are added, and the yield is about 50% relative which is higher than those obtained with other low-temperature methods. MWCNTs were synthesized by the reduction of ethyl alcohol with sodium borohydride (NaBH4) under a strong basic solvent with the high concentration of sodium hydroxide (NaOH). Ethyl alcohol (90%) of 80 mL volume, sodium borohydride (99.99%) of 4.2 g, and 15 mL of 10 M sodium hydroxide (97%) solution were added to a 250 mL flask. The mixtures were stirred with a magnetic stirrer for 30 min and then transferred to a 125 mL Parr reactor (model 4750, Parr Company, Moline, IL). The Parr reactor was sealed and then kept at 180°C for 20 h in a furnace and cooled down to room temperature. The end products were washed with alcohol and distilled water several times and then dried in a vacuum oven at 60°C for 10 h.Different MWCNT concentrations (0.025, 0.05, 0.075, and 0.1 wt%) were dispersed in 0.2 wt% sodium dodecyl benzene sulfonate (SDBS) by sonication. The prepared dispersion was mixed with PEDOT: PSS at a volume ratio of 1:1 and was magnetically stirred for 15 min at 1600 rpm. MWCNT-PEDOT:PSS (62μL) was deposited on a polymer substrate PET (0.125 mm thickness) with predefined shape (1.5 cm × 1 cm) by spin coating at a spin speed of 200 rpm. The thin films were dried and baked in an oven at 70°C for 1 hour. Figure 1(a) shows the schematic of MWCNT-PEDOT: PSS thin film and Figure 1(b) shows the prepared films with the film thickness of 5 μm measured by Filmetrics F-20 are used for the current investigations.Figure 1
(a) Schematic drawing of the thin film side view. (b) Samples of the prepared MWCNT-PEDOT: PSS thin film.
(a) (b)


## 3. Results and Discussion

### 3.1. X-Ray Diffraction

Phase analysis was studied by using X-Ray Diffractometer (XRD) with Cu-Kα X-radiation of wavelength 1.54056 Å at 45 kV and 40 mA. The diffraction was conducted in the Bragg angles between 10° and 80° as shown in Figure 2. The XRD patterns of MWCNT, PEDOT:PSS, and MWCNT-PEDOT:PSS nanocomposite thin film are shown in Figure 2. There are two characteristic peaks at 26.2° and 43.5°, with an interlayer d-spacing of 3.38818 Å and 2.07503 Å, respectively, corresponding to the MWCNT. The XRD patterns of MWCNT-PEDOT:PSS nanocomposite thin film show peak at 25.9°, which is almost identical to the pristine PEDOT:PSS. It is interesting to see that the diffraction peaks of MWCNT at 43.5° disappeared after the MWCNT-PEDOT:PSS nanocomposite was formed.Figure 2
X-ray Diffraction of MWCNT, PEDOT:PSS and MWCNT-PEDOT:PSS nanocomposite thin film.


### 3.2. TEM Characterization

The MWCNTs were observed under Transmission Electron Microscopy (TEM) using an accelerating voltage of 15 kV. The image in Figure3 reveals a straight morphology of nanotubes. The nanotubes are visible as a bamboo-like structure with closed ends and have many walls aligned parallel to the tube axis.Figure 3
TEM images of MWCNT at 50 nm.


### 3.3. FESEM Characterization

Samples of the nanocomposite thin films were investigated by Field Emission Scanning Electron Microscope (FESEM), which is used to perform qualitative analyses on their surface morphology and microstructure. The FESEM, JEOL/JSM-7100F was equipped with detectors of secondary electrons (SE) and an energy dispersive X-ray spectrometer (EDAX). The FESEM was operated using an accelerating voltage of 15 kV at room temperature. FESEM images of MWCNT-PEDOT: PSS film in Figure4(a) showing MWCNT with different diameters (22.5nm, 30 nm, and 35.6nm) are observed. FESEM images in Figures 4(d), 4(e), and 4(f) show MWCNT at different magnifications while the images at Figures 4(b) and 4(c) show MWCNT distribution at low and high MWCNT concentration.Figure 4
FESEM images of (a) MWCNT-PEDOT:PSS film from the side view showing MWCNT with different diameter, (b) MWCNT at 0.025 wt%, (c) MWCNT at 0.075 wt%, (d) MWCNT at 43,000 magnification, (e) MWCNT at 35,000 magnification, (f) MWCNT at 14,000 magnification.
(a) (b) (c) (d) (e) (f)


### 3.4. EDAX Analysis

The elemental composition of the MWCNT-PEDOT: PSS film was confirmed by the Energy Dispersive Spectroscopy (EDAX) at room temperature as shown in Figure5. The EDAX spectrum indicates the presence of carbon, sodium, sulfur, and oxygen at concentrations specified in Table 1.Table 1
Different elements like carbon, sodium, sulfur, and oxygen present in MWCNT-PEDOT:PSS film.
Element Weight% Atomic% C K 6.83 26.16 Na K 0.9 1.8 S K 3.22 4.62 O 23.41 67.29Figure 5
EDAX Analysis of MWCNT-PEDOT:PSS film showing different elements mainly carbon, sodium, sulphur, oxygen as shown in Table1.


### 3.5. Fourier Transform Infrared Spectrometer Studies

Figure6 shows FTIR (Fourier Transform Infrared Spectrometer) spectra of MWCNT, PEDOT:PSS and MWCNT-PEDOT:PSS, respectively. The absorption bands for MWCNT-PEDOT:PSS appeared at 997, 1060, 1192, and 1429 cm−1. The vibrations at 1203, 1145, and 1090 cm−1 for PEDOT:PSS may originate from the stretching of C–O–C bond in the ethylene dioxy group. The addition of MWCNT results in a shift of the absorption peak toward the lower wavenumber (from 1203 cm−1 to 1192 cm−1). There is a distinct absorption valley around 1000 nm.Figure 6
FTIR of MWCNT, PEDOT:PSS and MWCNT-PEDOT: PSS films; MWCNT-PEDOT:PSS1-0.025wt% MWCNT, MWCNT-PEDOT:PSS2-0.05wt% MWCNT, MWCNT-PEDOT:PSS3-0.075wt% MWCNT, MWCNT-PEDOT:PSS4-0.1wt% MWCNT.


### 3.6. Electrical Properties of MWCNT-PEDOT:PSS

The conductivity of the MWCNT-PEDOT: PSS films containing 0.025 wt%, 0.05 wt%, 0.075 wt%, and 0.1 wt% of MWCNT was measured using a four-point probe resistance measurement technique. The electrical conductivity of the films increases with the increase in the wt% of MWCNT in the PEDOT: PSS matrix. The maximum conductivity of the MWCNT-PEDOT: PSS thin film for 0.1 wt% is 13.5 S/m and the minimum conductivity is observed at 0.025 wt% which is 8.5 S/m as shown in Figure7(a). Accordingly, the resistance of the MWCNT-PEDOT: PSS thin films decreases with increase in MWCNT concentration in the PEDOT: PSS as shown in Figure 7(b). Further, it is observed in Figure 7(a) that there is a notable increase in the conductivity in films with more than 0.075 wt% of MWCNT. The corresponding critical concentration when there is a sudden increase in conductivity is called the percolation threshold.Figure 7
(a) Conductivity of MWCNT-PEDOT: PSS film increases with increasing wt% of MWCNT. (b) Resistance of MWCNT-PEDOT: PSS film decreases with increasing wt% of MWCNT.
(a) (b)Higher conductivity of films with higher MWCNT is due to the phenomena of percolation (conductive paths) created by the MWCNT in the PEDOT:PSS matrix and also due to the strong interfacial connection between the MWCNT and the thiophene rings of PEDOT. This enables electronic density transfer between them, so the mobile charge carriers are then shifted more in the PEDOT chains.


### 3.7. Electromechanical Testing

The electromechanical properties of the MWCNT-PEDOT: PSS thin films for different wt% of MWCNT were also analyzed using a microtensile test machine as shown in Figure8 and four-point probe resistance measurement technique. The applied strain was changed from 0 to 6% at speed of 0.2 mm/min using microtensile test machine. The change in the film resistance for corresponding increase in the strain was measured by a four-point probe resistance measurement.Figure 8
Microtensile test machine.The sheet resistance and relative change in sheet resistance as a function of strain of the MWCNT-PEDOT:PSS thin films for different wt% of MWCNT were plotted as shown in Figures9(a) and 9(b). In Figure 9(a), it is observed that the sheet resistance of MWCNT-PEDOT:PSS film increases with the increase in the strain for all wt% of MWCNT due to the breakdown of existing conductive paths and increase in intertube distances between MWCNT. A high tensile strain on the nanocomposite thin film leads to the tunneling effect between adjacent MWCNT which in turn leads to a sharp increase in the resistance of the nanocomposite. In Figure 9(b), the MWCNT-PEDOT: PSS films show a nonlinear behavior with an exponential increase in relative change in sheet resistance under tension load which is due to the arbitrary distribution of the MWCNT in the film as observed in FESEM images in Figures 4(b) and 4(c).Figure 9
(a) Sheet resistance of MWCNT-PEDOT: PSS film increases with increasing Strain % for different wt% of MWCNT. (b) Relative change in resistance of MWCNT-PEDOT: PSS film increases with increasing Strain% for different wt% of MWCNT.
(a) (b)In order to find how the change in resistance depends upon the material physical quantities, the expression is(1)R=ρlAwhere R is the resistance of a material, ρ is the resistivity of a material, l is the length, and A is the area.R is differentiated w.r.t. stress s:(2)dRds=ρAδlδs+lAδρδs-ρlA2δAδsDividing R=ρl/A on both sides,(3)dRds=1lδlδs+1ρδρδs-1AδAδsIt can be observed that per-unit change in resistance is due to per-unit change in length, per-unit change in area, and per-unit change in resistivity.Gauge factor is defined as the ratio of relative change in resistance with respect to the applied strain. The gauge factor (GF) is given by(4)GF=ΔR/Riℇ=Rf-Ri/RiℇRf is the final resistance after deformation, Ri is the initial resistance without deformation, and Ɛ is the applied strain.The slope of the graph of relative changes in resistance with the strain from Figure9(b) is the gauge factor which is defined by (4). As mentioned in Table 2, the highest gauge factor is obtained for 0.1 wt% of MWCNT in PEDOT: PSS matrix for 6% strain which is 22.8 evaluated from (4). Highest gauge factor is obtained for 0.1 wt% of MWCNT in PEDOT: PSS matrix which is the wt% of MWCNT close to the percolation threshold. The gauge factor in the linear-elastic region of the thin film prepared with 0.3 wt% MWCNT-epoxy by screen printing method was reported as 14.19 [30], which is around 7 times higher than the conventional strain sensors. Hence, the fabricated MWCNT-PEDOT: PSS thin film with 0.075wt% MWCNT-PEDOT:PSS by spin coating method from our work represents a good gauge factor value of 15.156 in the linear-elastic region observed below 1.5% strain. From our previous work [31], the highest gauge factor is achieved for 0.05 wt% of carbon nanospheres (CNS) in PEDOT: PSS matrix for 6% strain which is 34.57. Highest gauge factor is obtained for 0.05 wt% of CNS in PEDOT: PSS matrix which is the wt% of CNS close to the percolation threshold.Table 2
Gauge factor of nanocomposite thin film.
Sample Name Gauge factor (6% strain) 0.025 wt% MWCNT-PEDOT:PSS 16.8347 0.050 wt% MWCNT-PEDOT:PSS 15.6217 0.075 wt% MWCNT-PEDOT:PSS 14.2421 0.100 wt% MWCNT-PEDOT:PSS 22.8782


## 3.1. X-Ray Diffraction

Phase analysis was studied by using X-Ray Diffractometer (XRD) with Cu-Kα X-radiation of wavelength 1.54056 Å at 45 kV and 40 mA. The diffraction was conducted in the Bragg angles between 10° and 80° as shown in Figure 2. The XRD patterns of MWCNT, PEDOT:PSS, and MWCNT-PEDOT:PSS nanocomposite thin film are shown in Figure 2. There are two characteristic peaks at 26.2° and 43.5°, with an interlayer d-spacing of 3.38818 Å and 2.07503 Å, respectively, corresponding to the MWCNT. The XRD patterns of MWCNT-PEDOT:PSS nanocomposite thin film show peak at 25.9°, which is almost identical to the pristine PEDOT:PSS. It is interesting to see that the diffraction peaks of MWCNT at 43.5° disappeared after the MWCNT-PEDOT:PSS nanocomposite was formed.Figure 2
X-ray Diffraction of MWCNT, PEDOT:PSS and MWCNT-PEDOT:PSS nanocomposite thin film.


## 3.2. TEM Characterization

The MWCNTs were observed under Transmission Electron Microscopy (TEM) using an accelerating voltage of 15 kV. The image in Figure3 reveals a straight morphology of nanotubes. The nanotubes are visible as a bamboo-like structure with closed ends and have many walls aligned parallel to the tube axis.Figure 3
TEM images of MWCNT at 50 nm.


## 3.3. FESEM Characterization

Samples of the nanocomposite thin films were investigated by Field Emission Scanning Electron Microscope (FESEM), which is used to perform qualitative analyses on their surface morphology and microstructure. The FESEM, JEOL/JSM-7100F was equipped with detectors of secondary electrons (SE) and an energy dispersive X-ray spectrometer (EDAX). The FESEM was operated using an accelerating voltage of 15 kV at room temperature. FESEM images of MWCNT-PEDOT: PSS film in Figure4(a) showing MWCNT with different diameters (22.5nm, 30 nm, and 35.6nm) are observed. FESEM images in Figures 4(d), 4(e), and 4(f) show MWCNT at different magnifications while the images at Figures 4(b) and 4(c) show MWCNT distribution at low and high MWCNT concentration.Figure 4
FESEM images of (a) MWCNT-PEDOT:PSS film from the side view showing MWCNT with different diameter, (b) MWCNT at 0.025 wt%, (c) MWCNT at 0.075 wt%, (d) MWCNT at 43,000 magnification, (e) MWCNT at 35,000 magnification, (f) MWCNT at 14,000 magnification.
(a) (b) (c) (d) (e) (f)


## 3.4. EDAX Analysis

The elemental composition of the MWCNT-PEDOT: PSS film was confirmed by the Energy Dispersive Spectroscopy (EDAX) at room temperature as shown in Figure5. The EDAX spectrum indicates the presence of carbon, sodium, sulfur, and oxygen at concentrations specified in Table 1.Table 1
Different elements like carbon, sodium, sulfur, and oxygen present in MWCNT-PEDOT:PSS film.
Element Weight% Atomic% C K 6.83 26.16 Na K 0.9 1.8 S K 3.22 4.62 O 23.41 67.29Figure 5
EDAX Analysis of MWCNT-PEDOT:PSS film showing different elements mainly carbon, sodium, sulphur, oxygen as shown in Table1.


## 3.5. Fourier Transform Infrared Spectrometer Studies

Figure6 shows FTIR (Fourier Transform Infrared Spectrometer) spectra of MWCNT, PEDOT:PSS and MWCNT-PEDOT:PSS, respectively. The absorption bands for MWCNT-PEDOT:PSS appeared at 997, 1060, 1192, and 1429 cm−1. The vibrations at 1203, 1145, and 1090 cm−1 for PEDOT:PSS may originate from the stretching of C–O–C bond in the ethylene dioxy group. The addition of MWCNT results in a shift of the absorption peak toward the lower wavenumber (from 1203 cm−1 to 1192 cm−1). There is a distinct absorption valley around 1000 nm.Figure 6
FTIR of MWCNT, PEDOT:PSS and MWCNT-PEDOT: PSS films; MWCNT-PEDOT:PSS1-0.025wt% MWCNT, MWCNT-PEDOT:PSS2-0.05wt% MWCNT, MWCNT-PEDOT:PSS3-0.075wt% MWCNT, MWCNT-PEDOT:PSS4-0.1wt% MWCNT.


## 3.6. Electrical Properties of MWCNT-PEDOT:PSS

The conductivity of the MWCNT-PEDOT: PSS films containing 0.025 wt%, 0.05 wt%, 0.075 wt%, and 0.1 wt% of MWCNT was measured using a four-point probe resistance measurement technique. The electrical conductivity of the films increases with the increase in the wt% of MWCNT in the PEDOT: PSS matrix. The maximum conductivity of the MWCNT-PEDOT: PSS thin film for 0.1 wt% is 13.5 S/m and the minimum conductivity is observed at 0.025 wt% which is 8.5 S/m as shown in Figure7(a). Accordingly, the resistance of the MWCNT-PEDOT: PSS thin films decreases with increase in MWCNT concentration in the PEDOT: PSS as shown in Figure 7(b). Further, it is observed in Figure 7(a) that there is a notable increase in the conductivity in films with more than 0.075 wt% of MWCNT. The corresponding critical concentration when there is a sudden increase in conductivity is called the percolation threshold.Figure 7
(a) Conductivity of MWCNT-PEDOT: PSS film increases with increasing wt% of MWCNT. (b) Resistance of MWCNT-PEDOT: PSS film decreases with increasing wt% of MWCNT.
(a) (b)Higher conductivity of films with higher MWCNT is due to the phenomena of percolation (conductive paths) created by the MWCNT in the PEDOT:PSS matrix and also due to the strong interfacial connection between the MWCNT and the thiophene rings of PEDOT. This enables electronic density transfer between them, so the mobile charge carriers are then shifted more in the PEDOT chains.


## 3.7. Electromechanical Testing

The electromechanical properties of the MWCNT-PEDOT: PSS thin films for different wt% of MWCNT were also analyzed using a microtensile test machine as shown in Figure8 and four-point probe resistance measurement technique. The applied strain was changed from 0 to 6% at speed of 0.2 mm/min using microtensile test machine. The change in the film resistance for corresponding increase in the strain was measured by a four-point probe resistance measurement.Figure 8
Microtensile test machine.The sheet resistance and relative change in sheet resistance as a function of strain of the MWCNT-PEDOT:PSS thin films for different wt% of MWCNT were plotted as shown in Figures9(a) and 9(b). In Figure 9(a), it is observed that the sheet resistance of MWCNT-PEDOT:PSS film increases with the increase in the strain for all wt% of MWCNT due to the breakdown of existing conductive paths and increase in intertube distances between MWCNT. A high tensile strain on the nanocomposite thin film leads to the tunneling effect between adjacent MWCNT which in turn leads to a sharp increase in the resistance of the nanocomposite. In Figure 9(b), the MWCNT-PEDOT: PSS films show a nonlinear behavior with an exponential increase in relative change in sheet resistance under tension load which is due to the arbitrary distribution of the MWCNT in the film as observed in FESEM images in Figures 4(b) and 4(c).Figure 9
(a) Sheet resistance of MWCNT-PEDOT: PSS film increases with increasing Strain % for different wt% of MWCNT. (b) Relative change in resistance of MWCNT-PEDOT: PSS film increases with increasing Strain% for different wt% of MWCNT.
(a) (b)In order to find how the change in resistance depends upon the material physical quantities, the expression is(1)R=ρlAwhere R is the resistance of a material, ρ is the resistivity of a material, l is the length, and A is the area.R is differentiated w.r.t. stress s:(2)dRds=ρAδlδs+lAδρδs-ρlA2δAδsDividing R=ρl/A on both sides,(3)dRds=1lδlδs+1ρδρδs-1AδAδsIt can be observed that per-unit change in resistance is due to per-unit change in length, per-unit change in area, and per-unit change in resistivity.Gauge factor is defined as the ratio of relative change in resistance with respect to the applied strain. The gauge factor (GF) is given by(4)GF=ΔR/Riℇ=Rf-Ri/RiℇRf is the final resistance after deformation, Ri is the initial resistance without deformation, and Ɛ is the applied strain.The slope of the graph of relative changes in resistance with the strain from Figure9(b) is the gauge factor which is defined by (4). As mentioned in Table 2, the highest gauge factor is obtained for 0.1 wt% of MWCNT in PEDOT: PSS matrix for 6% strain which is 22.8 evaluated from (4). Highest gauge factor is obtained for 0.1 wt% of MWCNT in PEDOT: PSS matrix which is the wt% of MWCNT close to the percolation threshold. The gauge factor in the linear-elastic region of the thin film prepared with 0.3 wt% MWCNT-epoxy by screen printing method was reported as 14.19 [30], which is around 7 times higher than the conventional strain sensors. Hence, the fabricated MWCNT-PEDOT: PSS thin film with 0.075wt% MWCNT-PEDOT:PSS by spin coating method from our work represents a good gauge factor value of 15.156 in the linear-elastic region observed below 1.5% strain. From our previous work [31], the highest gauge factor is achieved for 0.05 wt% of carbon nanospheres (CNS) in PEDOT: PSS matrix for 6% strain which is 34.57. Highest gauge factor is obtained for 0.05 wt% of CNS in PEDOT: PSS matrix which is the wt% of CNS close to the percolation threshold.Table 2
Gauge factor of nanocomposite thin film.
Sample Name Gauge factor (6% strain) 0.025 wt% MWCNT-PEDOT:PSS 16.8347 0.050 wt% MWCNT-PEDOT:PSS 15.6217 0.075 wt% MWCNT-PEDOT:PSS 14.2421 0.100 wt% MWCNT-PEDOT:PSS 22.8782


## 4. Conclusion

Synthesis of MWCNT is performed by the reduction of ethyl alcohol with sodium borohydride (NaBH4) under a strong basic solvent with the high concentration of sodium hydroxide (NaOH). The MWCNT-PEDOT: PSS nanocomposites for different wt% of MWCNT have been prepared and this nanocomposite was deposited on the PET thin films by the spin coating technique. Characterization using FESEM revealed the lower concentration of MWCNT for 0.025 wt% and higher concentration of MWCNT for 0.075 wt% MWCNT concentration in PEDOT:PSS polymer matrix. Predominantly, MWCNTs with diameters (22.5nm, 30 nm, and 35.6nm) are observable in the FESEM images. The maximum conductivity of the MWCNT-PEDOT: PSS thin film for 0.1 wt% observed was 13.5 S/m. The piezoresistive behavior of MWCNT-PEDOT: PSS thin films on a flexible substrate was tested on the microtensile tester and four-point probe resistance measurement. The conductivity of the thin films decreases as the applied strain increased. The highest gauge factor for 0.1 wt% of MWCNT in PEDOT: PSS matrix for 6% strain obtained is 22.8 and it is concluded that the MWCNT-PEDOT: PSS thin film can be used for piezoresistive flexible strain sensing applications.



---

*Source: 9320976-2019-06-10.xml*