Introduction

EVA, as a typical copolymer, is widely used in numerous applications, such as electronic devices, buildings, packaging, biomedical materials or children toys, due to its good mechanical and physical properties [1]. However, EVA has a high flammability, which makes it burn at a high speed and generate a large amount of heat, and it seriously restricts the applications of EVA in many fields with high demand on flame retardancy [2, 3]. In order to overcome this drawback, one of the most effective ways is to add various flame retardants [4]. It is widely known that halogen-containing flame retardants have high flame-retardant efficiency, but they produce large quantities of smoke, corrosive and toxic gases while burning [5,6,7]. Therefore, the exploration of nontoxic and environmental-friendly flame retardants for EVA has been an urgent task.

In recent years, people are paying advanced attention to develop halogen-free flame retardants for polymers. As a metal hydroxide filler, magnesium hydroxide (MH) was widely used to prepare flame-retardant composites [8, 9]. There were many reports about its application in polymers, such as EVA [10, 11], poly(vinyl chloride) [12], polypropylene [13, 14], polyethylene [15], polyethylene terephthalate [16] or epoxy resin [17], due to its abundant resources, low cost, high thermal stability and good smoke suppression. However, to achieve a desired flame retardancy effect, generally a great amount of fillers are required in the polymer composites (more than 50%), which results in the deterioration of the mechanical properties of polymers [17,18,19,20]. To reduce the negative effects of MH in polymer systems, an effective way is to incorporate other nanofillers to achieve synergetic enhancement in the principle of making best use of advantages and bypassing the disadvantages. In recent years, many researchers have published the synergism of flame retardancy, such as silica [10, 21], zinc borate [11], multiwall carbon nanotube [19], nanoclay [22], hollow glass [23]and expandable graphite [24], combined with MH.

Nanosized carbon materials have attracted a great deal of attention in the past few decades because of their advantageous characteristics [25,26,27], such as low density, high thermal stability and good conductivity. [28, 29]. The previous reports have revealed that nanocarbon black could increase thermal stability and flame retardancy of polyolefin due to its trapping radical effect during the burning of composites [30,31,32]. In comparison with micron-sized additives, nanomaterials showed several advantages, especially with respect to significantly reducing the heat release rate at quite low loading (less than 5%) [29, 31, 33, 34]. To the best of our knowledge, there are no reports about synergistic flame-retardant effects of CB in EVA/brucite system.

In this work, EVA/brucite/CB (EMC) were prepared to investigate the positive effects of CB in an EM flame-retardant system. Their flame retardancy and thermal stability were investigated by LOI, UL-94 test, CCT and TG. Furthermore, their mechanical properties were evaluated by tensile test.

Experimental

Materials

Ethylene-vinyl acetate (EVA) copolymer (Elvax-265, containing 28% vinyl acetates with a melt flow rate of 3 g 10−1 min−1) was supplied by DuPont Company (USA). Brucite (mineral form of MH, with the content of magnesium oxide more than 69%) was kindly supplied by Liaoning Kuandian (Liaoning, China). Carbon black (CB, purity: > 99%) was purchased from Linzi Qishun Chemical Co., Shandong, with the original particle diameter of 17 nm. All the samples were dried in a vacuum oven at 80 °C for 12 h before processing.

Preparation of the flame-retardant EVA composites

All the samples were prepared with the same procedure by melt intercalation method using a microcompounder (MC-15, Xplore Instruments BV, Newsland). The processing of the composites was carried out at a temperature of 180 °C with a screw speed of 50 rpm and residence time of 15 min. For the properties tests, different standard testing bars, according to the standards mentioned in the following part, were obtained by using a hot press machine. All the samples were dried in a vacuum oven at 80 °C for 2 h before processing. The formulations are given in Table 1.

Table 1 Formulations of the EVA composites

Characterization

Thermogravimetric analysis (TG) was determined from room temperature to 600 °C, with a heating rate of 10 °C min−1 in nitrogen atmosphere with a flow speed of 90 mL min−1, using a TA thermogravimetric analyzer (Q50, USA). All the samples were dried in a vacuum oven at 80 °C for 2 h before test.

Limiting oxygen index (LOI) was measured by oxygen index meter (FTT, UK) with sheet dimension of 130 × 6.5 × 3.2 mm3, according to ASTM D 2863-77 standard.

Vertical burning test was carried out on UL-94 vertical flame chamber (FTT, UK) with dimensions of 130 × 13 × 3.2 mm3, according to ASTM D3801 standard.

The fire behavior of the samples was performed on cone calorimeter (FTT, UK), according to the ISO 5660 standard, under a heat flux of 50 kW m−2 with a sample size of 100 × 100 × 3 mm3.

Tensile testing was performed on a universal electromechanical testing machine (INSTRON 3384, USA) according to ASTM D 638 standard at a test speed of 50 mm min−1.

A Zeiss, EVO MA15 (Germany) scanning electron microscope equipped with energy dispersive spectra (EDS) was utilized to characterize the microstructure of the char layer after cone calorimeter test.

Results and discussion

Thermal stability of EVA composites

The thermal stability of EVA and its composites with a different content of CB was investigated by TG in nitrogen atmosphere. Figure 1 shows the TG and the derivative thermogravimetric (DTG) curves, and the corresponding data are listed in Table 2. The temperatures at which 10% (T−10%), 50% (T−50%) and maximum (Tmax) mass loss occurs were used as the measure of the initial degradation temperature, half degradation temperature and maximum degradation temperature, respectively. It was observed that the thermal degradation of pure EVA and its composites was a two-step degradation—elimination of the side group with acetic acid release and then breaking of the main chain [5, 23]. The T−10%, T−50%, Tmax1 and Tmax2 for pure EVA were 320 °C, 426 °C, 325 °C and 439 °C, respectively. Compared with pure EVA, the T−10%, T−50%, Tmax1 and Tmax2 values of EM increased to 334 °C, 461 °C, 338 °C and 459 °C, respectively. However, the T−10%, T50 %, Tmax1 and Tmax2 values of EVA composites with brucite and CB were highest and increased to 352 °C, 485 °C, 356°C and 480 °C, respectively. The results showed that the use of brucite and CB upgraded the thermal stability of the composites, and CB had an obvious synergistic effect on the system. However, the amount of residues of EMC did not show distinct change, indicating that the presence of CB in EMC did not induce catalytic carbonization effect.

Fig. 1
figure 1

TG (a) and DTG (b) curves of pure EVA and its composites at a heating rate of 10 °C min−1 in nitrogen

Table 2 TG and DTG data of pure EVA and its composites in nitrogen

LOI and UL-94

In this segment, the effect of brucite and different contents of CB on the flammability of EVA was investigated by limiting oxygen index (LOI) and vertical burning test (UL-94). Table 3 shows the results for pure EVA and its composites. It could be seen from Table 3 that the LOI value of pure EVA was only 18.5%. When brucite was added, the LOI value of EM increased to 34.0%. As for EMC, with the increase in CB content from 0.5 to 1.0%, the LOI value gradually increased. However, with further increase of CB content more than 1.0%, the LOI exhibited a small decrease, which suggested that 1% was a proper content of CB with best flame retardancy in our EVA system. The UL-94 results showed that the pure EVA had no-rating, while the EM could reach V-1; especially, the dripping of pure EVA also was serious. After the combination of CB and brucite, all composites passed the V-0 rating and demonstrated higher flame retardancy. Obviously, all the additions of brucite and CB reduced the flammability of EVA. For the EMC2 sample with 54% brucite and 1% CB, the LOI reached the maximum value of 35.3%, which means that EMC2 has the best flame retardancy in EVA matrix. Table 4 also shows that all the flame-retardant EMC samples reached V-0 level. On the basis of the above results, CB was an effective synergist in EM system.

Table 3 Results obtained from LOI and UL-94 tests
Table 4 Combustion parameters obtained from cone calorimeter test

Combustion behavior

To further investigate the effect of CB in EM composites, the combustion behavior of EVA and its composites was investigated by cone calorimetry test, and the related data are summarized in Table 5. The heat release rate (HRR), total heat release (THR), smoke release rate (SRR) and total smoke release (TSR) curves versus the burning time for EVA and its composites are presented in Figs. 2, 3, 4 and 5, respectively.

Table 5 Mechanical properties of pure EVA and its composites
Fig. 2
figure 2

Heat release rate curves of EVA and its composites from cone calorimeter test

From Fig. 2, it could be found that the pure EVA was easily flammable after ignition and exhibited a sharp HRR curve at 125 s, and the peak value of HRR was as high as 1139 kWm−2. When 55% of brucite was added to EVA, the EM sample burned slowly compared with pure EVA and the PHRR decreased to 357 kWm−2. Furthermore, after the CB was added into the EM systems, the EMC samples burned more slowly than pure EVA and EM. The HRR curve of EMC2 with the content of 1% CB is shown to be smoothest and lowest of the curves. At the end of burning, as shown in Fig. 3, pure EVA released a total heat of 110 kJ m−2. The THR values for EMC2 were decreased to 75 kJ m−2, and the reduction in THR was around 32%. The reduction in HRR and THR of EMC composites indicated that the CB participated in the carbonization process and was kept in the condensed phase, which was in accordance with the TG and residual char results. Lower HRR and THR values were crucial for saving lives and assets during a fire.

Fig. 3
figure 3

Total heat release curves of EVA and its composites by cone calorimeter test

Smoke production during combustion is another very important factor in fire safety fields [35, 36]. It is reported that the acute toxicity of fire gases is mainly responsible for over 70% of people killed by fires. From Fig. 4, the SPR curve of pure EVA was the highest and sharpest one among the samples, and its peak value was 0.084 m2 s−1. The peak in the SPR curve of EM was 0.040 m2 s−1. The SPR curve of EMC2 was lowest and smoothest among all the samples, with a peak value of 0.021 m2 s−1. Compared with pure EVA, the reduction of the peak values in the SPR curve was 52.38% and 65.48%. Figure 5 presents the total smoke production of pure EVA and flame-retardant EVA composites. The TSR of pure EVA was 10.03 m2 m−2, and the TSR of EM was 5.97 m2 m−2. Additionally, meanwhile, it was observed that the TSR values decreased greatly with the addition of CB in the EVA and brucite system, being the EMC2, with the 1% of CB, the lowest among all the samples. It demonstrated that an appropriate amount of CB and brucite could produce an obvious smoke suppression in flame-retardant EVA composites.

Fig. 4
figure 4

Smoke production rate curves of EVA and its composites from cone calorimeter test

Fig. 5
figure 5

Total smoke release curves of EVA and its composites from cone calorimeter test

The structure and morphology of the residual char after cone calorimeter testing were analyzed, which was helpful to clarify the effect of nanofillers during combustion. Therefore, investigating the residual char would provide an insight into the synergistic flame-retardant effects and mechanism of CB in condensed phase. Photographs of the burning residue after cone calorimeter testing are presented in Fig. 6. As shown in Fig. 6a, pure EVA was completely decomposed without any residual char. In Fig. 6b, the EM sample with EVA matrix filled with 55% of brucite presented a thick and hard layer, but it contained large cracks. As it has been demonstrated, magnesium oxide generated and covered the surface of the flame-retardant material, which improved the flame resistance of polymer materials [23]. However, after the CB was added into the EM systems, the sample of EMC illustrated less and thinner residual surface cracks, with compact charred layers on the sample surface. The results indicated that the incorporation of CB and MH could reinforce the thermal stability of the charred layers, which acted as an excellent barrier for mass and thermal transport.

Fig. 6
figure 6

Digital photographs of the char residues after the cone colorimeter test from a pure EVA, b EM, c EMC1, d EMC2, e EMC3, f EMC4

Flame-retardant mechanism

It has been demonstrated that MH can achieve a better flame retardancy due to the endothermic decomposition reaction of MH, which can reduce the EVA surface temperature and free water molecules to dilute the concentrated combustible gas during the combustion. Furthermore, the magnesium oxide builds a protective layer on the composite surface, which cuts off the sources of heat at the point of the combustion and also inhibits the release of flammable gas, thus reducing the flame and smoke effects [22, 23]. Besides, the previous research also demonstrated that carbon black can promote the polymer carbonization to generate a solid-phase flame-retardant mechanism during polymer combustion [16, 37, 38].

To further investigate the flame-retardant mechanism, SEM and EDS were used to investigate the microstructure and elements of char residues and obtain more detailed information about post-thermal degradations. Figure 7 shows the SEM images and EDS of EM and EMC2 from cone calorimeter test. It illustrates (Fig. 7a) that there were lots of holes on the surface of EM charred residue. Therefore, the heat and flammable volatiles could penetrate the char layer into the flame zone during burning. However, Fig. 7b shows the continuous and compact char layer structure on the surface of EMC residue, and there was also almost no flaw or holes on the EMC2 residue. The EDS results showed that the content of carbon on the EMC2 charred residue surface is more than on EM residue. Apparently, from the above observations, the SEM and EDS results indicated the addition of CB obviously increased the char residue of EVA composites and played synergistic effect on flame-retardant EVA composites with brucite [39].

Fig. 7
figure 7

Microscopic residues of a EM and b EMC2 at flameout after burning under 50 kW m−2

From the above discussion, we could conclude that the synergistically enhanced flame resistance of EMC composites, due to the carbonization and physical process in the condensed phase. Scheme 1 shows the thermo-decomposition process of flame-retardant EMC composites during burning. The detailed flame-retardant mechanism was proposed as follows. Firstly, when the flame spread onto the surface of the EMC composites, the polymer under the fire passed to a molten state with the decomposition of EVA and brucite, and because of the lower density of CB, it was accumulated on the liquid-phase surface and further promotes the carbonization. Meanwhile, the brucite decomposed into magnesium oxide and water, the water vapor diluted the flammable gases, and the magnesium oxide covered the surface of the composite to isolate the flame. With the burning, the carbon black and magnesium oxide aggregated and formed a barrier layer. Moreover, the cross-linked carbonation between the fillers further improved the stiffness of the condensed phase and restrained the combustion of the composites.

Scheme 1
scheme 1

Schematic illustration of the proceeding combustion of EMC composites

Mechanical properties

According to the research performed, it is demonstrated that CB displayed some positive effects on improving the thermal stability and flame retardancy of EVA composites. The effect of CB on the mechanical properties of EVA was investigated by tensile testing. The detailed data of tensile strength and elongation at break are summarized in Table 5. The tensile stress and elongation at break of pure EVA were 22.7 MPa and 1297%. It had been observed that the incorporation of brucite and carbon black obviously decreased the mechanical properties of the EM and EMC composites. The tensile strength of EM and EMC composites was between 11 MPa and 12 MPa which had the slight changes; there were also no significant differences in the elongation at break among the composites. It was mainly due to the CB, with nanoparticle size, which can distribute among the bigger particles of brucite [37]. This indicated that small amount of CB particles did not reduce the mechanical properties of EMC composites.

Conclusions

In this paper, the flammability characteristics and thermal degradation behavior of EVA composites with brucite and CB have been compared by melt blending method. TG and DTG results indicated that the addition of CB to the EMC system could improve the thermal stability of the EVA composites. Compared with EVA and EM composites, when 0.5% CB was added into the EM system, the LOI of EMC1 reached a value of 34.8% and passed the V-0 rating in the UL-94 test. With the addition of 1% CB in the EMC system, the LOI of EMC2 further increased, up to 35.3%, and also passed the V-0 rating in the UL-94 test. Combustion behavior obtained from cone calorimeter testing showed that HRR, THR, SPR and TSR for EMC2 were lowest among all the samples. The photographs of residual char showed that adding a moderate quantity of CB would promote the formation of a compact and smooth char structure. The incorporation of CB did not have negative effect on the tensile performance of EVA composites. In summary, a moderate amount of CB imparted EVA/brucite composites an improvement in thermal stability and flame retardancy.