# Dielectric Behaviour of Zn/Al-NO3 LDHs Filled with Polyvinyl Chloride Composite at Low Microwave Frequencies

Authors: Ethar Y. Salih; Zulkifly Abbas; Samer Hasan Hussein Al Ali; Mohd Zobir Hussein
Journal: Advances in Materials Science and Engineering
 (2014)

---

## Abstract

Recently, researchers have shown great interest in improving the thermal, mechanical, dielectric, and microwave properties of pure polymers through the use of polymer-based composites. The essential properties of polymer-based composites can be modified by varying the amount of Zn/Al-NO3 layered double hydroxide (LDH) added to polyvinyl chloride (PVC). Therefore, by determining the optimal ratio of LDH in the PVC matrix, the dielectric properties of PVC-LDH composites can be improved. An LDH was prepared using the coprecipitation method, while PVC-LDH composites were prepared using tetrahydrofuran (THF) as the solvent. The composites were characterised using X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR), and scanning electron microscopy (SEM), and room temperature dielectric measurements were investigated using an RF Impedance/Material Analyzer (Agilent 4291). The results confirmed that the prepared composites were pure. Additionally, the presence of LDH in the PVC matrix was verified. The dielectric measurements showed that an increase in the LDH concentration leads to an increase in the dielectric constant and the dielectric loss factor. When used as dielectric filler in the PVC matrix, the LDH improved the dielectric properties of the fabricated composites. The results indicate that these composites show great potential for use as microwave absorbers at low microwave frequencies.


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## Body

## 1. Introduction

PVC is a thermoplastic polymer that is used widely in floor and roof tiles, window and door frames, water pipes, sheets, packing films, and electrical wires and cables because of its good dielectric and mechanical properties, ease of processing, and low cost [1, 2]. Both the microwave and mechanical properties of PVC are controlled by the amorphous phase that forms at 95°C, which is the glass transition temperature [2]. The dielectric properties of PVC have been studied by a number of researchers. The characteristics of PVC have also been examined through radio frequency measurements [3]. Microwave measurements on PVC were reviewed by Amrhein and Mueller [4]. The microwave properties of PVC remain stable up to 90°C, which is near the glass transition temperature [5].LDH (layered double hydroxide) is a layered inorganic compound, that is, composed of an ionic lamellar solid that contains infinite brucite-type layers. LDH is positively charged and contains exchangeable hydrate gallery anions. The ability of LDH to intercalate anions makes it useful as a catalyst, a tailor-made adsorbent, or a precursor material for oxides [6]. The optical properties of LDH have been found useful for solar energy applications [7]. The thermal properties of LDH enable the anions within the structure to be reoriented [8]. Ahmed et al. studied the thermal, optical, and dielectric properties of LDH for different molar ratios [6]. LDH was found to have good dielectric properties at room temperature. LDH is highly recommended for the use in the microwave applications, such as electromagnetic interference (EMI) and electromagnetic compatibility (EMC), because of the enhanced saturated magnetisation [9].In the last decade, much research has shown that PVC properties can be enhanced by the addition of a variety of fillers, such as metal chlorides, metal carboxylates, clays, metals, and metal hydroxides [1, 10–18]. Of the aforementioned fillers, LDH is also known as an anion-exchanging mineral filler. LDH has attracted much interest among researchers as an efficient filler because of its observable effect on the PVC matrix [17, 18]. Hence, PVC properties can be enhanced by many types of LDH materials. Because PVC is used in electrical wires and cables [2] and because LDH has good dielectric properties [6] and can be used for microwave applications [9], it is advantageous to study the effect of LDH on the PVC matrix. This study focuses on the dielectric properties of PVC-LDH composites, where the results will be compared to the dielectric properties of pure PVC.


## 2. Materials and Methods

### 2.1. Materials

PVC (Mw
≈
530
g
·
mol
-
1) and THF (99.8
%) were supplied by Sigma-Aldrich and J. T. Baker, respectively. Other materials used, including NaOH (99%), Zn(
NO
3
)
2
·
6
H
2
O
(
98.1
%
), and Al
(
NO
3
)
3
·
9
H
2
O
(
98
%
), were purchased from Sigma (St Louis, MO). Deionised water was used as the solvent in the preparation of the Zn/Al LDH.


### 2.2. Preparation of LDH and PVC-LDH Composites

Zn/Al-NO3 (LDH) preparation was carried out using the coprecipitation method described by Al Ali et al. [19]. A hydrous solution containing 2 mol/L of NaOH was mixed with a 250 mL solution containing Al3+ and Zn2+ with a molar ratio of 1 : 4 of Al3+ to Zn2+. A pH of 7 was obtained via the dropwise addition of NaOH, which resulted in a white solution. Pure LDH was obtained by introducing nitrogen into the atmosphere to eliminate the O2 and prevent the formation of a carbonate. The white solution was aged at 70°C for approximately 18 hours, followed by washing and centrifuging using deionised water, and then drying at 60°C in an oven. Part of the powder was mixed with polyvinyl alcohol (PVA), which acted as a binder, and then pressed at 5 tons for 5 minutes to produce an LDH pellet.A uniform amount of polyvinyl chloride was dissolved in THF with 500 rpm magnetic stirring for 24 hours to obtain a homogenous solution with no precipitation of the PVC. The PVC and LDH solutions ranged from 1 to 9%wt of LDH in a constant amount of PVC. The PVC/LDH solution was then magnetically stirred at 60°C for 6 hours until a homogenous mixture was obtained. The solution was allowed to dry for 24 hours at room temperature and was then hot pressed to 1 mm thickness.


### 2.3. Characterisations

Room-temperature dielectric properties were measured via the capacitance technique (Agilent 4291B, RF-Impedance/Material analyser) in the frequency range of 1 MHz to 1.2 GHz. The compressed pellets of the samples (PVC, LDH, and PVC-LDH composites) were placed between two plates, which served as parallel capacitors. The dielectric properties were acquired from the measured admittance of the MUT. While the presence of LDH in the PVC matrix was identified using X-ray diffraction patterns (XRD; Model X′PERT-PRO PANALYTICAL) using CuKa radiation with λ
=
0.154
nm, a current of 30 mA, and a scanning rate of 0.06/s in the range 4°–70°. The compact char surface (FTIR) was distinguished in the range of 400 to 4000 cm−1 on a Thermo Nicolet Nexus with a resolution of 4 cm−1. Scanning electron microscopy (SEM; Model Hitachi) at 5.00 KV was used to confirm the homogeneous distribution of LDH on the surface of the PVC.


## 2.1. Materials

PVC (Mw
≈
530
g
·
mol
-
1) and THF (99.8
%) were supplied by Sigma-Aldrich and J. T. Baker, respectively. Other materials used, including NaOH (99%), Zn(
NO
3
)
2
·
6
H
2
O
(
98.1
%
), and Al
(
NO
3
)
3
·
9
H
2
O
(
98
%
), were purchased from Sigma (St Louis, MO). Deionised water was used as the solvent in the preparation of the Zn/Al LDH.


## 2.2. Preparation of LDH and PVC-LDH Composites

Zn/Al-NO3 (LDH) preparation was carried out using the coprecipitation method described by Al Ali et al. [19]. A hydrous solution containing 2 mol/L of NaOH was mixed with a 250 mL solution containing Al3+ and Zn2+ with a molar ratio of 1 : 4 of Al3+ to Zn2+. A pH of 7 was obtained via the dropwise addition of NaOH, which resulted in a white solution. Pure LDH was obtained by introducing nitrogen into the atmosphere to eliminate the O2 and prevent the formation of a carbonate. The white solution was aged at 70°C for approximately 18 hours, followed by washing and centrifuging using deionised water, and then drying at 60°C in an oven. Part of the powder was mixed with polyvinyl alcohol (PVA), which acted as a binder, and then pressed at 5 tons for 5 minutes to produce an LDH pellet.A uniform amount of polyvinyl chloride was dissolved in THF with 500 rpm magnetic stirring for 24 hours to obtain a homogenous solution with no precipitation of the PVC. The PVC and LDH solutions ranged from 1 to 9%wt of LDH in a constant amount of PVC. The PVC/LDH solution was then magnetically stirred at 60°C for 6 hours until a homogenous mixture was obtained. The solution was allowed to dry for 24 hours at room temperature and was then hot pressed to 1 mm thickness.


## 2.3. Characterisations

Room-temperature dielectric properties were measured via the capacitance technique (Agilent 4291B, RF-Impedance/Material analyser) in the frequency range of 1 MHz to 1.2 GHz. The compressed pellets of the samples (PVC, LDH, and PVC-LDH composites) were placed between two plates, which served as parallel capacitors. The dielectric properties were acquired from the measured admittance of the MUT. While the presence of LDH in the PVC matrix was identified using X-ray diffraction patterns (XRD; Model X′PERT-PRO PANALYTICAL) using CuKa radiation with λ
=
0.154
nm, a current of 30 mA, and a scanning rate of 0.06/s in the range 4°–70°. The compact char surface (FTIR) was distinguished in the range of 400 to 4000 cm−1 on a Thermo Nicolet Nexus with a resolution of 4 cm−1. Scanning electron microscopy (SEM; Model Hitachi) at 5.00 KV was used to confirm the homogeneous distribution of LDH on the surface of the PVC.


## 3. Results and Discussion

### 3.1. X-Ray Diffraction

Figure1 shows the XRD patterns of the LDH particles. The LDH structure was identified by XRD diffraction patterns. The (003), (006), (009), and (110) diffraction peaks of LDH, corresponding to the basal and higher-order reflections, were at 9.8°, 19.8°, 29.8°, and 60.25°, respectively. The basal spacing values for (d
003), (d
006), (d
009), and (d
110) were found to be 8.95, 4.47, 2.65, and 1.53 Å, respectively. These values were obtained using the XRD software and are in good agreement with the literature [20]. According to the well-known Debye-Scherer’s formula (equation (1)), the crystallite size of LDH was calculated to be 83.898 nm at 003 planes. Figure 2 shows the XRD patterns for the PVC-LDH composites at varying concentrations of LDH. There are no undesirable peaks, which confirms the purity of the prepared composites. Lack of peaks in the PVC-1%wt LDH could be because of the low LDH concentration, which makes the region of the sample that was tested insensitive to the X-rays. All samples were highly crystallised, as indicated by the highly intense and sharp peaks (Figure 2)
(1)
D
=
k
λ
β
cos
⁡
⁡
θ
,
where the unit for D is in nm, K is the shape factor (normally 0.9), λ is the X-ray wavelength, and θ is the Bragg diffraction angle where the peak is observed. β is the full width of the diffraction line at half of the maximum intensity in radians (FWHM data converted to radians).Figure 1
XRD patterns of Zn/Al-NO3.Figure 2
XRD patterns of polyvinyl chloride-Zn/Al-NO3 at varying concentrations of LDH.Table1 and Figure 2 show the XRD patterns for PVC-LDH composites at varying concentrations of LDH.Table 1
XRD data of polyvinyl chloride-Zn/Al-NO3 composites.
Sample
2
θ
d-Spacing
1%wt
—
—
3%wt
10.01
8.83
5%wt
9.95
8.85
7%wt
9.94
8.89
9%wt
9.94
8.89


### 3.2. Fourier Transform Infrared (FTIR) Spectra Study

Figure3 shows the FTIR spectrum of the PVC, LDH, and PVC-LDH composite samples. The unexpected broad band is attributed to the O–H stretching of hydroxyl groups by approximately 3389 cm−1. The nitrate that is intercalated between the interlayers of LDH appeared at 1334 cm−1. The peaks obtained under 800 cm−1 are caused by the metal-oxygen vibrations, ν(M–O) stretching, and ν(M–O–H) bending [20]. The PVC curve is also shown in Figure 3. Bands in the range of 610–840 cm−1 and 1240–1540 cm−1 are attributed to C–Cl stretching and bending of C–H bonds, respectively [21]. Another band at 1090 cm−1 is attributed to bending of the C–C bond. Figure 3 also shows the FTIR spectrum of the as-synthesised PVC-LDH composites. In general, the spectrums are composed of combined spectral band features of the LDH and PVC. This indicates that PVC coated the surface of the LDH.Figure 3
FTIR study of polyvinyl chloride-Zn/Al-NO3 at varying compositions of LDH.


### 3.3. Scanning Electron Microscopy (SEM)

Scanning electron microscopy (SEM) images and energy dispersive X-ray spectroscopy (EDX) patterns of the PVC-LDH composites are shown in Figure4. The SEM images reveal the incorporation of LDH particles in the PVC matrix. Figures 4(a), 4(b), 4(c), 4(d), and 4(e) show PVC as the polymeric matrix with varying concentrations of LDH as the filler at 300x. Figure 4 also shows that there were no aggregates or agglomerates in the composite samples, and the samples were in the shape of a single plate. The elemental analysis of the composites was conducted using the energy dispersive X-ray pattern of the 9%wt LDH sample (Figure 4(f)). It can be clearly observed that the LDH was not affected by the presence of the PVC components in the composites, where the peaks of different components indicate the presence of filler (LDH) in the PVC matrix.SEM images of (a) 1%wt, (b) 3%wt, (c) 5%wt, (d) 7%wt, and (e) 9%wt PVC-LDH, (f) EDX of 9%wt.
(a)
(b)
(c)
(d)
(e)
(f)


### 3.4. Room-Temperature Dielectric Properties

The electromagnetic wave behaviour depends essentially on the dielectric properties (the dielectric constant and the dielectric loss factor). The dielectric constant,ε
′, is represented by the storage of electromagnetic waves in the material, while the dielectric loss factor, ε′′, is the dissipation of energy.Figure5 shows the variation of the room-temperature dielectric constant and dielectric loss factor of pure LDH in the frequency range of 1 MHz to 1.2 GHz. It is clear that the LDH possesses high dielectric properties, as indicated by the values of the dielectric constant and dielectric loss factor. However, the dielectric constant demonstrated higher values than the dielectric loss factor. The dielectric response of this material structure is believed to be caused by two charge carriers [6, 22], the proton and the gallery ions. The proton originates from the polarisation of water clusters in the LDH interlayer and the creation of OH− and OH
3
+ at each end of the path along which the proton is transferred. The second carrier is the NO
3
-, and it serves as a supplemental carrier, moving from its equilibrium position under the influence of the electric field. It should be noted that the dielectric properties of the pure LDH decreased with the frequency increment because of anomalous low frequency dispersion (ALFD), where the current carrier is dominated in the dielectric system [23].Figure 5
Dielectric properties versus frequency of Zn/Al-NO3.The effect of varying concentrations of LDH as filler (1%wt, 3%wt, 5%wt, 7%wt, and 9%wt) on both the dielectric constant and the dielectric loss factor of a PVC matrix is shown in Figures6(a) and 6(b), respectively.Dielectric properties of polyvinyl chloride-Zn/Al-NO3 composites; (a) dielectric constant, (b) dielectric loss factor.
(a)
(b)In Figure6, insignificant changes in the dielectric properties of the pure PVC were observed with good agreement with previous findings [24]. For the PVC-LDH composites, the dielectric properties were enhanced by the varying concentrations of LDH. In the effective medium theory [25], the dielectric properties of polymer-based composites can be increased by the addition of fillers with high dielectric properties. In this study, both a higher dielectric constant and a higher dielectric loss factor were obtained for the composites with higher concentrations of pure LDH. With the addition of only 1%wt LDH into the PVC matrix, an increase was observed in both the dielectric constant and the dielectric loss factor. An even higher concentration of LDH resulted in higher dielectric properties. The results suggest that the addition of LDH to PVC can alter the properties of PVC, transforming it from a nearly stable dielectric material to a dispersive material. Medium-loss materials have a dielectric loss factor in the range of 0.05 to 0.1, while high-loss materials have a dielectric loss factor above 0.1 [26]. Therefore, by increasing the concentration of pure LDH to 5%wt or more, the PVC can be easily transformed from a medium-loss to a high-loss material.


## 3.1. X-Ray Diffraction

Figure1 shows the XRD patterns of the LDH particles. The LDH structure was identified by XRD diffraction patterns. The (003), (006), (009), and (110) diffraction peaks of LDH, corresponding to the basal and higher-order reflections, were at 9.8°, 19.8°, 29.8°, and 60.25°, respectively. The basal spacing values for (d
003), (d
006), (d
009), and (d
110) were found to be 8.95, 4.47, 2.65, and 1.53 Å, respectively. These values were obtained using the XRD software and are in good agreement with the literature [20]. According to the well-known Debye-Scherer’s formula (equation (1)), the crystallite size of LDH was calculated to be 83.898 nm at 003 planes. Figure 2 shows the XRD patterns for the PVC-LDH composites at varying concentrations of LDH. There are no undesirable peaks, which confirms the purity of the prepared composites. Lack of peaks in the PVC-1%wt LDH could be because of the low LDH concentration, which makes the region of the sample that was tested insensitive to the X-rays. All samples were highly crystallised, as indicated by the highly intense and sharp peaks (Figure 2)
(1)
D
=
k
λ
β
cos
⁡
⁡
θ
,
where the unit for D is in nm, K is the shape factor (normally 0.9), λ is the X-ray wavelength, and θ is the Bragg diffraction angle where the peak is observed. β is the full width of the diffraction line at half of the maximum intensity in radians (FWHM data converted to radians).Figure 1
XRD patterns of Zn/Al-NO3.Figure 2
XRD patterns of polyvinyl chloride-Zn/Al-NO3 at varying concentrations of LDH.Table1 and Figure 2 show the XRD patterns for PVC-LDH composites at varying concentrations of LDH.Table 1
XRD data of polyvinyl chloride-Zn/Al-NO3 composites.
Sample
2
θ
d-Spacing
1%wt
—
—
3%wt
10.01
8.83
5%wt
9.95
8.85
7%wt
9.94
8.89
9%wt
9.94
8.89


## 3.2. Fourier Transform Infrared (FTIR) Spectra Study

Figure3 shows the FTIR spectrum of the PVC, LDH, and PVC-LDH composite samples. The unexpected broad band is attributed to the O–H stretching of hydroxyl groups by approximately 3389 cm−1. The nitrate that is intercalated between the interlayers of LDH appeared at 1334 cm−1. The peaks obtained under 800 cm−1 are caused by the metal-oxygen vibrations, ν(M–O) stretching, and ν(M–O–H) bending [20]. The PVC curve is also shown in Figure 3. Bands in the range of 610–840 cm−1 and 1240–1540 cm−1 are attributed to C–Cl stretching and bending of C–H bonds, respectively [21]. Another band at 1090 cm−1 is attributed to bending of the C–C bond. Figure 3 also shows the FTIR spectrum of the as-synthesised PVC-LDH composites. In general, the spectrums are composed of combined spectral band features of the LDH and PVC. This indicates that PVC coated the surface of the LDH.Figure 3
FTIR study of polyvinyl chloride-Zn/Al-NO3 at varying compositions of LDH.


## 3.3. Scanning Electron Microscopy (SEM)

Scanning electron microscopy (SEM) images and energy dispersive X-ray spectroscopy (EDX) patterns of the PVC-LDH composites are shown in Figure4. The SEM images reveal the incorporation of LDH particles in the PVC matrix. Figures 4(a), 4(b), 4(c), 4(d), and 4(e) show PVC as the polymeric matrix with varying concentrations of LDH as the filler at 300x. Figure 4 also shows that there were no aggregates or agglomerates in the composite samples, and the samples were in the shape of a single plate. The elemental analysis of the composites was conducted using the energy dispersive X-ray pattern of the 9%wt LDH sample (Figure 4(f)). It can be clearly observed that the LDH was not affected by the presence of the PVC components in the composites, where the peaks of different components indicate the presence of filler (LDH) in the PVC matrix.SEM images of (a) 1%wt, (b) 3%wt, (c) 5%wt, (d) 7%wt, and (e) 9%wt PVC-LDH, (f) EDX of 9%wt.
(a)
(b)
(c)
(d)
(e)
(f)


## 3.4. Room-Temperature Dielectric Properties

The electromagnetic wave behaviour depends essentially on the dielectric properties (the dielectric constant and the dielectric loss factor). The dielectric constant,ε
′, is represented by the storage of electromagnetic waves in the material, while the dielectric loss factor, ε′′, is the dissipation of energy.Figure5 shows the variation of the room-temperature dielectric constant and dielectric loss factor of pure LDH in the frequency range of 1 MHz to 1.2 GHz. It is clear that the LDH possesses high dielectric properties, as indicated by the values of the dielectric constant and dielectric loss factor. However, the dielectric constant demonstrated higher values than the dielectric loss factor. The dielectric response of this material structure is believed to be caused by two charge carriers [6, 22], the proton and the gallery ions. The proton originates from the polarisation of water clusters in the LDH interlayer and the creation of OH− and OH
3
+ at each end of the path along which the proton is transferred. The second carrier is the NO
3
-, and it serves as a supplemental carrier, moving from its equilibrium position under the influence of the electric field. It should be noted that the dielectric properties of the pure LDH decreased with the frequency increment because of anomalous low frequency dispersion (ALFD), where the current carrier is dominated in the dielectric system [23].Figure 5
Dielectric properties versus frequency of Zn/Al-NO3.The effect of varying concentrations of LDH as filler (1%wt, 3%wt, 5%wt, 7%wt, and 9%wt) on both the dielectric constant and the dielectric loss factor of a PVC matrix is shown in Figures6(a) and 6(b), respectively.Dielectric properties of polyvinyl chloride-Zn/Al-NO3 composites; (a) dielectric constant, (b) dielectric loss factor.
(a)
(b)In Figure6, insignificant changes in the dielectric properties of the pure PVC were observed with good agreement with previous findings [24]. For the PVC-LDH composites, the dielectric properties were enhanced by the varying concentrations of LDH. In the effective medium theory [25], the dielectric properties of polymer-based composites can be increased by the addition of fillers with high dielectric properties. In this study, both a higher dielectric constant and a higher dielectric loss factor were obtained for the composites with higher concentrations of pure LDH. With the addition of only 1%wt LDH into the PVC matrix, an increase was observed in both the dielectric constant and the dielectric loss factor. An even higher concentration of LDH resulted in higher dielectric properties. The results suggest that the addition of LDH to PVC can alter the properties of PVC, transforming it from a nearly stable dielectric material to a dispersive material. Medium-loss materials have a dielectric loss factor in the range of 0.05 to 0.1, while high-loss materials have a dielectric loss factor above 0.1 [26]. Therefore, by increasing the concentration of pure LDH to 5%wt or more, the PVC can be easily transformed from a medium-loss to a high-loss material.


## 4. Conclusion

LDH was successfully prepared and different compositions of PVC-LDH composites were obtained using a THF solution. The purity of the prepared materials was investigated using XRD and FTIR, while the surface morphology was studied using SEM. The present investigation revealed that the addition of 5%wt LDH can transform PVC from a medium-loss to a high-loss material. The presence of the LDH filler increases the dielectric loss of these composites, which leads to an increase in the probability that the composites will absorb electromagnetic waves at low microwave frequencies. Hence, these composites are recommended highly for use in electromagnetic interference applications.



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*Source: 647120-2014-12-03.xml*