Introduction

In materials science, one of the most important phenomena is the reinforcement of rubber by fine, rigid entities, dispersed particulate, or phase-separated domains. To know significant reinforcement, the size of the hard phase should be small, smaller than a micron, reinforcement increases resistance to fracture and stiffness [1]. Filling polymers by a combination of fillers receive continuous interest because of their natural ability to improve heat stability [2], mechanical properties [3], flame retardancy [4], abrasion resistance [5, 6] of the polymer matrix, and gas barrier properties [7]. Carbon black is a conventional reinforcing agent that increases the mechanical and abrasion properties of polymers [8]. Nanoparticles are a unique scientific interest as they are great effectively a bridge between molecular or atomic structure and bulk materials [9]. Metal oxide nanoparticles are the most important materials due to the great widespread applications some metal oxide nanoparticles (CaO, ZnO, TiO2, and CeO2) can use in various aspects including sensors, catalysis, environmental remediation, and optoelectronic materials [10,11,12,13,14,15,16,17]. There are some methods that CaO nanoparticles can be synthesized which include thermal decomposition method [18], solution combustion method [19], microwave processing [20], sonochemical method [15], coprecipitation method [21], and sol–gel method [22]. EPDM (ethylene propylene diene monomer) is a commercially important as unsaturated polyolefin rubber. In general, EPDM compound has excellent chemical resistance to water, ozone, brake fluid, radiation, weather, and glycol. EPDM high resilience is preferred. EPDM is good vulcanizates, providing improved wet electrical properties. EPDM is resistant to oxygenated solvents, salt solutions, and synthetic hydraulic fluids. By a gel-free process when diene vinyl norbornene is mixing on the EPDM backbone, a significantly improved terpolymer is obtained for cable and wire applications. Other applications of EPDM are automotive body seals, mounts, roofing, weather-stripping, hose, ducts, tubing, and tires. EPDM molded rubber is used for fillers and bumpers to get damp vibrations around the vehicle [23,24,25]. Although the possibility use of polymer nanocomposites in the electrical insulating industry is still in its early stages, polymeric materials offer great benefits in outdoor insulation systems due to their great dielectric properties, better pollution performance, low cost, ease of processing, and lightweight [26]. Mohamed et al. [27] investigated the effect of CaO nanoparticles on the properties of Polyamide6 (PA 6) by adding 0.5% calcium oxide nanoparticles to it using melt compounding HAAKE twin screw extruder. Their result revealed that tensile strength and stiffness increase and elongation at break decrease by adding CaO nanoparticles. CaO nanoparticles improved the thermal stability of the composite. Sunil et al. [28] studied thermal properties of CaO nanofluids, by using CaO nanoparticles as a bio-lubricant, an additive is synthesized from chicken eggshells and dispersed rice bran oil as a base fluid ultrasonicated for 20 min; at 20 kHz using probe sonicator as a mixer, the result revealed that thermal stability of rice bran oil increase by 18.2% and 25% due to the addition of 0.25 wt% and 0.50 wt% of CaO nanofluids, respectively, but it does not affect rice bran oil oxidation behavior. Rana et al. [29] studied electrical, mechanical, and thermal properties of EPDM rubber with different amounts of montmorillonite (MMT) nano clay reinforced (2 wt%, 4 wt%, and 6 wt%); the two-roll mill was used for blending it. Mechanical properties increase with an increasing amount of clay, such as tensile strength, and young modulus, with increasing frequency dielectric constant decrease and conductivity increase. By adding nano clay to the EPDM dielectric constant and conductivity increase and the higher value, it was observed 2 wt% nanocomposites. The value of storage modulus increase significantly, the higher value of thermal stability observed in 2 wt%. Wang et al. [30] studied thermal conductivity and mechanical properties of EPDM rubber with different amounts of nano ZnO reinforced (10, 20, 40, 60, 80, 110, 140, 180, and 210 phr, respectively). Nano ZnO particles enhance better dynamic heat build-up mechanical properties by in situ modification.It can be found a few papers in the literature about the CaO-EPDM rubber composite. The effect of the nanocrystalline CaO on the mechanical behavior of CaO-EPDM rubber composite is not detailed. In this work, we prepare the CaO particles from an aqueous solution. We investigate the structure of the CaO. In the second part of the paper, we are using the CaO particles in EPDM rubber as reinforcement.

Materials and methodology

Materials

Materials used in the present study are ethylene propylene diene monomer (Keltan 778) DSM-LANXESS, with an ethylene content of 67% and ethylidene norbornene (ENB) 4.3%, stearic acid as a lubricant, paraffin oil (Ph.Hg. VIII quality), and triallyl cyanurate (TAC) as a vulcanization accelerator, which were kindly provided by Borsod ChemZrt. CaO nanocrystalline particles were produced by precipitation method using 1 mol/L of CaCl2 and 2 mol/L of NaOH as a reactant at the institute of nanotechnology department in the University of Miskolc. Dicumyl peroxide 98% were purchased from (Alfa Aesar). The composition of the material is represented in Table 1.

Table 1 Composition of the samples
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Sample preparation

Preparation of the calcium oxide particles

In this experiment, CaO nanocrystalline particles have been prepared by precipitation methods. The reactants that were used to prepare CaO is 1 mol/L of CaCl2 and 2 mol/L of NaOH; first of all, 20 cm3 of CaCl2 and 20 cm3 of NaOH were heated up to 80 °C on the hot plate of magnetic. NaOH was added dropwise into CaCl2 at the fixed temperature of 80 °C while stirring continues for 30 min and (1300 rpm) viscously was produced. The precipitate was collected by filtration after rinsed five times with distilled water to remove impurities. In this work, the reactions that occurred are shown at Eqs. (1) and (2).

$${\mathrm{CaCl}}_{2}+2\mathrm{NaOH} \ \frac{80^\circ{\rm C} }{}\ \mathrm{Ca}{(\mathrm{OH})}_{2} + 2\mathrm{NaCl}$$
(1)
$${\mathrm{Ca}\left(\mathrm{OH}\right)}_{2}\ \frac{650^\circ{\rm C} }{}\ \mathrm{CaO}+{\mathrm{H}}_{2}\mathrm{O}$$
(2)

The white calcium hydroxide (Ca(OH)2) precipitate was calcined in the furnace at 650 °C after that holding furnace for 1 h at this fixed temperature, finally collecting the nanocrystalline particles CaO and putting them in an airtight container. This method can be used as a cheap, simple, and convenient way for producing calcium oxide and hydroxide nanocrystalline particles in the industrial large scale.

Preparation of EPDM rubber/CaO nanocomposites

In this section, the procedure for preparing EPDM rubber/CaO nanocomposite is shown and discussed by using two methods of mixing. First using the conventional way on twin roll-mill adding the components on the molten polymer. The second way starts with pre-dispersing the nanocrystalline particles in the plasticizer oil by ultrasonic vibration. The EPDM rubber was rolled on twin-roll mill with 150 mm in diameter (Schwabenthan 150 U, Germany) at 110 °C temperature at 16 rpm without friction for approximately 5 min. Thereafter the oil (stearic acid if any), CaO nanocrystalline particles, dicumyl peroxide (DCP), and triallyl cyanurate (TAC). In case of ultrasonic mixing, the CaO was dispersed in the plasticizer oil, and this milk like material was added first onto the EPDM felt. It was interesting observation that the ultrasonically mixed CaO containing sheets were not rugged. Finally, the blended rubber/CaO nanocrystalline particle mixtures were compression-molded for the sample preparation of tensile and hardness in 120 mm × 120 mm mold and simultaneously cross-linked for 8 min at 165 °C, using oil-hydraulic pressure 30 bar.

Characterization CaO powder

Scanning electron microscopy (SEM)

Surface morphological features were studied by using (Helios G4 PFIB CXe) scanning electron microscope equipped with a high voltage of 10 kV. The samples were coated with gold to improve the electrical conductivity and reduce the charging for getting good image quality for analysis.

X-ray diffraction (XRD)

The crystallite size and weight percentage of calcium oxide powder were examined by using (Bruker D8 Advance diffractometer) X-ray diffraction (XRD).

$$D=\frac{0.9\lambda }{\beta cos\theta }$$
(3)

where D is the mean crystalline size (nm), \(\lambda\) is the wavelength of Cu Kα (0.154 nm), \(\beta\) is the full width at half maximum intensity (FWHM) in radian, and \(\theta\) is the Bragg angle.

Brunauer–Emmett–Teller (BET)

The specific surface area and the distribution of pore sizes of the CaO nanocrystalline particles calcined at 650 °C were examined by using (TriStar 3000) Brunauer–Emmett–Teller (BET).

Mechanical characterization

Tensile test

Tensile testing is one of the most basic engineering tests and supplies useful information about a material and its related properties. For engineering structures, these properties can be used for analysis and design and for improving new materials that better suit a specified use [31]. EPDM rubber and different wt% of CaO particles samples were to characterize the material under the tensile loading by using Instron 5566 universal testing machine. In each set, three samples were tested according to ISO 527 standard. The crosshead speed was 100 mm/min. The thickness and width of the tensile samples used were about 1 mm (individually measured) and 4.6 mm, respectively. The gauge length of the specimen used was 25 mm.

Hardness test

Hardness test is defined as hardness resistance of materials against indenter by harder materials. Shore A is used for softer rubbers and soft plastic like plasticized PVC. One advantage of the Shore procedure is its mobile application capability since hand-held devices are often used [32]. In the present study, hardness measurements were made according to ISO 868 standard at 23 ± 1 °C using Shore A hardness tester (Zwick/Roell) machine. Each sample was 3 mm in thickness, and five different positions were tested from each rubber. Arithmetic mean value was calculated.

Thermal characterization

In this study, there were two different thermal characterization tests performed for investigating the thermal properties with the help of dynamic mechanical analysis (DMA) and thermogravimetric analysis (TGA).

Dynamic mechanical analysis (DMA)

DMA is a nondestructive test technique in the area of polymer matrix analysis [33]. The thermomechanical behavior of the EPDM samples was characterized by the use of (Metravib 1DB DMA25 instrument) DMA solicitation type: tension–compression over a temperature range of − 80 to 80 °C with a heating rate of 2 °C per minute at a frequency of 10 Hz. The thickness and width of the tensile specimens used were 1 mm and 10 mm, respectively (measured by accuracy of 0.05 mm); also the gauge length of the specimen used was 15 mm. It is important to use a low heating rate so that the sample can have enough time to achieve the thermal balance within the chamber. As a function of temperature, the storage modulus and the loss factor tan (δ) were measured. Glass transition temperatures (Tg) were evaluated as the maximum point temperature of tan (δ).

Thermogravimetric analysis (TGA)

TGA is the most commonly used thermal characterization technique to identify information about changes in percent weight of the analyzed specimens as a constant heating rate with respect to temperature or a constant temperature with respect to time [34]. In the present research, thermal stability and mass change of neat EPDM and its nanocomposite as a function of temperature from 40 to 655 °C and constant heating rate 10 °C/min was investigated. The measurement carried out by (MOM Derivatograph-C) instrument.

Volume resistivity

In the present study, the measurements of volume resistivity were observed of neat EPDM rubber and the nanocomposites, by a high-insulation resistance meter device (Danbridge DB621 Megohmmeter). Volumetric resistivities were evaluated by applying 1 kV to the surfaces of the samples for 60 s; the plate was about 1 to 1.4 mm thick, individually measured. The resistance of the specimens were so high that the measurement was not possible. Therefore, new and specific electrode was made for the present study as shown in Fig. 1 to measure the volume resistivity. The accuracy of this arrangement is less than the standard electrode system, but for comparative study, it is suitable. All of the electrical property measurements were carried out at room temperature.

Fig. 1
figure 1

(a, b) New electrode system for volume resistivity measurement

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Results and discussions

Mechanical, thermal, crystallographic, and electrical properties of neat EPDM and its nanocomposites are discussed in this section.

CaO powder characterization

Scanning electron microscopy (SEM)

SEM micrographs of CaO nanocrystalline particles were taken for two different nominal magnifications, namely 10 k × , and 50 k × which are shown in Fig. 2a, b, respectively. SEM micrographs of CaO nanocrystalline particles showed that mainly the spherical shape and average size of nanocrystalline particles was 280 nm.

Fig. 2
figure 2

SEM micrographs of CaO nanocrystalline particles for different nominal magnifications. (a) M = 10 k × , (b) M = 50 k × 

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X-ray diffraction (XRD)

Powder X-ray diffraction (XRD) was used to analyze the crystallographic structure of the synthesized specimens, the crystallite size, and the weight percentage of calcium oxide powder. The analysis was observed with the help of (Bruker D8 Advance diffractometer) X-ray diffraction (XRD). It’s revealed that from Fig. 3a, b, that Ca(OH)2 after calcination at 650 °C for 1 h remain CaCO3 because the reaction of carbonation happen fast for Ca(OH)2 and CaO by atmospheric CO2 and increasing specific surface area those are reported in the literature [18, 35]. The predominant peaks happen around 2θ = 37.5°, and the average crystallite sizes were estimated from line broadening using Scherrer formula from Eq. (3) [18]. The average crystallite size of CaO and CaCO3 was 100 ± 20 nm and Ca(OH)2 was 5 nm. Also, the weight percentage of CaO nanocrystalline particles decrease from 73.71 to 66.62% after 1 month in characterization.

Fig. 3
figure 3

Powder X-ray diffraction patterns of CaO particles (a) after 1 day and (b) after 1 month

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Brunauer–Emmett–Teller (BET)

The specific surface area and the distribution of pore sizes of the CaO-NPs calcined at 650 °C were examined from N2 gas adsorption–desorption measurements. Figure 4a describes the N2 adsorption isotherm of type III hysteresis, which is characteristic of microporous materials [36]. From the Barrett–Joyner–Halenda (BJH) pore-size distribution plot (Fig. 4b), the estimated average pore diameter was found to be 21.5062 nm. The BET surface area, micropore area, and micropore volume were 4.3439 m2/g, 0.8627 m2/g, and 0.000371 cm3/g, respectively. It can be classified that most of the pores are mesopores (pore sizes between 2 and 50 nm), which is matched with the literature of N. Tangboriboon et al. [37] and Zahra Mirghiasi et al. [18].

Fig. 4
figure 4

(a) N2 adsorption–desorption isotherm and (b) pore size distribution of synthesized CaO nanocrystalline particles

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Mechanical characterization

Tensile strength

The tensile stress–strain response of ultrasonic and without ultrasonic has been shown in Fig. 5a. In each set, three samples were tested for both cases, the average of the tensile test are presented in Fig. 5a for both mixing. A great improvement has been seen in the % modulus, and decrement in the tensile strength and % failure strain are observed, as the CaO content increases from 0 to 8 wt%. Also, the tensile modulus of neat EPDM and its nanocomposites were measured which is presented in Fig. 5b for both cases. It revealed that the maximum % modulus that has been shown by using ultrasonic mixing was 24% and without ultrasonic mixing was 18% higher than neat EPDM for 8 wt% of CaO, due to stiffening of EPDM structure by adding CaO particles. The behavior of the ultrasonic treated sample is better due to the more homogeneous distribution of the CaO, and the formation of agglomerates is avoided, as one can observe on Fig. 11. The CaO particles were agglomerated without ultrasonic treatment (Fig. 11a, c), but using ultrasonic mixing, the formation of agglomeration of CaO could be avoided, and the particles were well dispersed (Fig. 11b, d); therefore, tensile strength is higher compared with the samples without ultrasonic treatment [42].

Fig. 5
figure 5

(a)Tensile stress values of neat EPDM rubber and its nanocomposites with and without ultrasonic mixing. (b) Tensile modulus values of neat EPDM rubber and its nanocomposites with and without ultrasonic mixing

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Fig. 6
figure 6

Shore hardness of neat EPDM rubber and its nanocomposites. Using ultrasonic mixing and without ultrasonic mixing

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The tensile strength decreases by adding CaO nanocrystalline particles, which is agreed with the literature [38, 39] [44, 45]. In the literature of Wang et al. [30], they studied thermal mechanical properties of EPDM rubber with different amounts of nano ZnO reinforced. Nano ZnO particles enhance better dynamic heat build-up mechanical properties by in situ modification. Also, from the literature of Su et al. [40], they investigated mechanical, electrical, and cure properties of EPDM mixed with Sm2O3. Furthermore, rubber filled with KH845-4-treated Sm2O3 had higher tensile and tear strength than rubber filled with SG-Si602-treated Sm2O3. This is due to the possibility of sulfuric atoms participating in the peroxide-cured system. But SG-Si602-treated Sm2O3 has maximum hardness. Mishra [41] studied mechanical and thermal properties of EPDM rubber filled with nano CaCO3, commercial CaCO3, and fly ash. Mechanical properties such as tensile strength and elongation at break increase with increasing amount of filler especially calcium carbonate nanocrystalline particles have better result comparing with commercial CaCO3 and fly ash. Nanocrystalline particles showed appreciable result.

Hardness test

Figure 6 revealed that the hardness of the materials increases with adding CaO nanocrystalline particles, and the graph showed hardness of matrix gradually increases by adding the particles for both cases, with ultrasonic and without ultrasonic mixing. The maximum hardness observed in 8 wt% of CaO particles for both cases with ultrasonic and without ultrasonic mixing was 64.2 and 64.1, respectively; almost both cases have the same hardness about 26% higher than neat EPDM. From the literature of Su et al. [40], they investigated mechanical, electrical, and cure properties of EPDM mixed with Sm2O3. SG-Si602-treated Sm2O3 has maximum hardness. Aguilera-Camacho et al. [43] investigated the effect of CaO nanocrystalline particles on microhardness and tribological properties of poly(methyl methacrylate) coating; it prepared via in situ polymerization adding 0.05 wt% CaO nanocrystalline particles to the PMMA matrix, the result showed by using CaO nanocrystalline particles to PMMA hardness increase. Hamza [44] studied mechanical properties and thermal aging of EPDM with different amounts of high abrasion furnace (HAF) carbon black. It was observed that hardness increases with an increasing amount of carbon black.

Fig. 7
figure 7

(a) TGA curve and (b) DTG curve for neat EPDM rubber and its nanocomposites using ultrasonic mixing

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Thermal analysis

Thermogravimetric analysis (TGA)

The temperature correlated with the derivative curve’s peak value estimates the thermal stability of nanocomposites and neat EPDM rubber. The higher the peak temperature, the better the thermal stability. Figures 7a, 8a represent the TGA curves for neat EPDM, and different weight contents of CaO particles included EPDM samples for both cases. It is revealed from Figs. 7a, 8a that the %wt loss is higher for neat EPDM rubber, while wt% is lower for CaO/EPDM nanocomposite as increasing the temperature from 40 to 655 °C for both cases using or without using ultrasonic mixing. It is observed from derivative thermogravimetry (DTG) peak curve especially for ultrasonic mixing which represents from Table 2 and Fig. 7b derivative peak temperature increase with adding of CaO to EPDM rubber, the maximum peak temperature revealed by adding 8 wt% of CaO. In conclusion, the thermal stability increases with the dispersion of CaO particles. It is observed from Table 2 using ultrasonic mixing that the overall %wt loss at 655 °C is 98.52%, 93.78%, 93.84% 91.54%, and 86.4% for neat EPDM rubber, 1 wt%, 2 wt%, 4 wt%, and 8 wt% nanocomposites, respectively. Derivative thermogravimetry (DTG) peak curve without using ultrasonic mixing represents in Table 3 and Fig. 8b; the maximum peak temperature revealed by adding 2 wt% of CaO. Also, it is observed from Table 3 without using ultrasonic mixing that the overall %wt loss at 655 °C is 98.52%, 94.31%, 991.9% 90.07%, and 87.34% for neat EPDM rubber, 1 wt%, 2 wt%, 4 wt%, and 8 wt% nanocomposites, respectively. This confirms that CaO addition to EPDM led to protecting EPDM structure against thermal degradation. It is supposed that the reason of thermal degradation of EPDM is the presence of acidic decomposition products of peroxide crosslinking agent. Radical decomposition of peroxide takes place only in a basic environment. The better is the dispersion of CaO, the less is the probability of areas of the thermal degradation.

Fig. 8
figure 8

(a) TGA curve and (b) DTG curve for neat EPDM rubber and its nanocomposites without using ultrasonic mixing

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Fig. 9
figure 9

(a) Storage modulus; (b) loss factor (tan δ) for neat EPDM and its nanocomposites using ultrasonic mixing

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Table 2 TGA properties for neat EPDM rubber and its nanocomposites using ultrasonic mixing
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Table 3 TGA properties for neat EPDM rubber and its nanocomposites without ultrasonic mixing
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Dynamic mechanical analysis (DMA)

The thermomechanical behavior of the samples was characterized by the use of DMA over a temperature range of − 80 to 80 °C with a heating rate of 2 °C per minute at a frequency of 10 Hz. The thickness and width of the tensile samples used were ≈ 1 mm and ≈ 10 mm, respectively; also the gauge length of the specimen used was 15 mm. Calculations were performed with the measured dimensions. It is important to use a low heating rate so that the sample can have enough time to achieve the thermal balance within the chamber. As a function of temperature, the storage modulus and the tan (δ)/loss factor were measured. Glass transition temperature (Tg) were determined at the maximum point of tan/loss tangent as shown in Figs. 9b, 10b which is denoted in Table 4 using ultrasonic mixing and without ultrasonic mixing. Figures 9a, 10a illustrate the effect of temperature on the storage modulus for both cases. The viscoelastic behavior of the matrix or composites is classified into three regions: glassy, transitional, and rubbery. The result revealed that storage modulus decreases as a function of temperature because of material further goes into a rubber state by increasing temperature. The decrease in storage modulus as temperature increases is visible in Figs. 9a, 10a, for both cases; also a dramatic drop was observed in the glass transition region due to segmental mobility of the EPDM rubber, around – 39 °C to – 28 °C. Some researchers corresponding loss tangent (Tan δ) peak as glass transition temperature [29, 45]. The glass transition temperature in the present study is denoted in Table 4 for both cases. The result indicated that glass transition temperature increases with adding CaO nanocrystalline particles to the matrix for both cases, and the maximum (Tg) showed in 1 wt% CaO for the ultrasonic mixing. The thermal stability increases with adding CaO particles to the EPDM rubber. In the literature of Mohamed et al. [27] who investigated the effect of CaO particles on the properties of polyamide 6 (PA 6) by adding 0.5% calcium oxide, CaO nanocrystalline particles improved the thermal stability of the composite. Rana et al. [29] studied electrical, mechanical, and thermal properties of EPDM rubber with different amounts of MMT nano clay reinforced (2 wt%, 4wt%, and 6 wt%); the higher value of thermal stability is observed in 2 wt%. Mishra [41] studied mechanical and thermal properties of EPDM rubber filled with nano CaCO3, commercial CaCO3, and fly ash. Synthesizing nanoparticles done by solution spray, thermal properties improved, and nano CaCO3 is more stable than the other; flame retardancy increase with the amount of filler, and nanoparticles showed appreciable result.

Fig. 10
figure 10

(a) Storage modulus; (b) loss factor (tan δ) for neat EPDM and its nanocomposites without ultrasonic mixing

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Fig. 11
figure 11

SEM micrographs for EPDM rubber mixed with CaO particles (a,c) without ultrasonic mixing (b,d) using ultrasonic mixing. (Nominal magnification is 5 k ×)

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Table 4 Glass transition temperature for Neat EPDM and its nanocomposites, with or without ultrasonic mixing
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Scanning electron microscopy (SEM) analysis for composite

SEM micrographs of EPDM/CaO composite were taken at a constant scale of 10 μm to see the CaO dispersion in EPDM rubber. The composites are presented in Fig. 11a, c without using ultrasonic mixing and Fig. 11b, d with using ultrasonic mixing. The SEM result revealed that using ultrasonic mixing has a great influence on the dispersion of CaO particle compared to non-using of the ultrasonic mixing; without ultrasonic mixing, it’s obvious in Fig. 11a, c that CaO particles were agglomerated. Also, the best mixing by ultrasonic improved the dispersity and decreased the agglomeration which was showed in 4 wt% and 8 wt% of CaO particles from Fig. 11b, d. As a consequence, higher tensile via using ultrasonic mixing is revealed compared to non-using of ultrasonic mixing as shown in Fig. 5.

Fig. 12
figure 12

Measured resistance of neat EPDM and its nanocomposites

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Volume resistivity

The measurements of volume resistivity were observed of neat EPDM rubber and the nanocomposites. The dielectric strength, dielectric constant, and surface and volumetric resistance are the key electrical properties that identify the properties of an insulating material. The resistance of the specimen was so high that the measurement was not possible. Therefore, new and specific electrode was made as shown in Fig. 1 to measure the volume resistivity. In the present study, volumetric resistivities were evaluated by applying 1 kV to the surfaces of the samples for 60 s; the plate was 1 mm thick. The calculated and comparative measurement is explained in Table 5. The resistance of blade electrode system (R1) is 201GΩ which is parallel to the resistance to be measured (R2). For parallel resistance

Table 5 Measured resistance for EPDM and its nanocomposite
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$$\frac{1}{R}=\frac{1}{R1}+\frac{1}{R2}\ \mathrm{is}\ \mathrm{valid}\ \mathrm{or}\ R=R1\times R2 \ \mathrm{by} \ \mathrm{other}\ \mathrm{notaion}$$
(4)

Because R was measured, the resistance of the sample can be calculated as:

$$R2=\frac{1}{\frac{1}{R} - \frac{1}{R1}}$$
(5)

Comparative measurement was carried out with a plasticized PVC plate. Its specific volume resistance was ρ = 1.92·1012 [Ω.cm]. The measured resistance was 173.2GΩ. From this data, the equivalent A/l is 700 cm. However, its accuracy is not better than ± 20%. The values in the last column were calculated by this A/l value.

Remark: Calculating with the smallest specific volume resistivity (EPDM/8 wt% CaO) the resistance with the standard arrangement (10 cm2 electrode and about 1.4 mm thickness) the resistance would be about 4TΩ; well over the top limit of the instrument.

The result observed from Table 5 and Fig. 12 that by adding CaO nanocrystalline particles to EPDM rubber, the volume resistivity and measured resistivity of EPDM gradually decreases in both cases. Because of the low resistivity, EPDM with 8 wt% of CaO is suitable for use in insulating applications. In the literature of Zonghuan Li, et al. [46], the effect of different carbon black structures on the electrical properties of filled EPDM rubber revealed that adding carbon black is useful for insulating purpose. Also cure, mechanical, and electrical properties of EPDM filled with Sm2O3 and treated with various coupling agents were compared in the literature of Su et al. [40]. The result revealed that by adding Sm2O3 to EPDM rubber, volume resistivity decreases. The EPDM composites are extremely good insulators.

Conclusion

The calcium oxide nanocrystalline particles were successfully synthesized by the precipitation method. SEM revealed that the nanocrystalline particles mostly spherical and the average particle size is about 280 nm. From BET analysis, surface area, micropore area, and micropore volume were 4.3439 m2/g, 0.8627 m2/g, and 0.000371 cm3/g, respectively. It can be classified that most of the pores are mesopores (pore sizes between 2 and 50 nm). Also, XRD analysis indicates that the average crystallite size of CaO and CaCO3 was 100 ± 20 nm, and Ca (OH)2 was 5 nm. Also, the weight percentage of CaO nanocrystalline particles decrease from 73.71 to 66.62% after 1 month in characterization. The experimental results obtained from the thermal, electrical, and mechanical characterization of composites using ultrasonic are:

  1. 1-

    Using ultrasonic mixing as a pre-mixing has a great influence on the dispersion of CaO nanocrystalline particles in the EPDM rubber matrix.

  2. 2-

    Using ultrasonic mixing revealed a great improvement in the mechanical and thermal properties of EPDM rubber by adding CaO nanocrystalline particles. The tensile modulus and hardness gradually increased by adding CaO nanocrystalline particles. From DMA and TGA measurement, the thermal stability of the rubber matrix was increased by adding CaO nanocrystalline particles.

  3. 3-

    Interesting observation that the ultrasonically mixed CaO containing sheets were not rugged.

  4. 4-

    Volume resistivity gradually decrease with increasing CaO nanocrystalline particles.