Marzieh Shabani and
Masoud Jamshidi*
Constructional Polymers and Composites Research Laboratory, School of Chemical, Petroleum and Gas Engineering, Iran University of Science and Technology (IUST), Tehran, Iran. E-mail: mjamshidi@iust.ac.ir; Fax: +98-21-77240495; Tel: +98-21-77240255
First published on 14th September 2022
In this work, a vulcanized blend of natural rubber (NR) and styrene butadiene rubber (SBR) (i.e. at weight ratio of 50:50) as a model for tire rubber was devulcanized using probe sonication. The effect of processing parameters such as sonication media, power, temperature and time on sol/gel contents and devulcanization percent of rubbery samples was investigated. Moreover, the influence of pre-immersion of vulcanized NR/SBR samples in different liquids (i.e. water, oil and toluene) was assessed for different sonication times (i.e. 10 to 60 min) and powers (i.e. 30 to 60 W). It was found that pre-immersion of rubber particles in oil significantly increased the devulcanization percent. The optimum conditions for devulcanization of the NR/SBR blend via probe sonication were found to be 60 Watts, 20 min, oil and 24 h for sonication power, sonication time, pre-immersion/sonication media and pre-immersion time, respectively. The highest obtained devulcanization percent in this step was about 40%. The effects of two devulcanizing chemical agents (i.e. diphenyl disulfide and VitaX) on devulcanization performances of the samples were also studied. Results showed that higher devulcanization percent (i.e. about 52%) was obtained by using VitaX. It was also observed that VitaX significantly improved re-vulcanization speed (i.e. cure rate index) and decreased scorch time. It was also found that lower content of VitaX (i.e. 0.6 phr) caused better curing properties but lower mechanical properties compared to the higher content (i.e. 1.2 phr).
Nowadays, automotives have become an undeniable human need. On this basis, the need for tire rubber has increased significantly in past decades. Millions of tires are produced annually in the world and they are turned into waste after usage. The tire waste, due to their huge content and negative effects on ecosystems, have become a major environmental problem. On this basis, recycling of waste tire rubber has been essential from environmental and economical points of view7,8
Some methods were used for elimination of waste tire rubbers that include burning as a heat source,9 landfilling,10,11 reclaiming12–14 etc. It has been known that burning and landfilling of tire rubbers impact environment by releasing greenhouse gases (i.e. SOx and COx) in the air and immigration of the toxic low molecular weight organic matters in to the soil, respectively.
Rubber reclaiming attracted attention of researchers in the beginning. However, reclaimed ground tire rubbers (GTRs), due to the very low mechanical properties, disappointed producers. In fact, during reclaiming a rubber, thermal/mechanical stresses are encountered to ground waste rubber particles that cause fracture in the polymer backbone and so significant decrement in the mechanical properties of the recycled product.15–17
On this basis, an effective method is needed for recycling waste rubbers. Literature review among published articles in this field shows that devulcanization (i.e. reverse process of vulcanization) is a promising method for this purpose.18–20 Different methods has been introduced for devulcanization of rubbers especially for ground tire rubbers (GTRs). For instance, mechanical,21 thermal,22 thermo-mechanical,23 chemo-thermomechanical,24 ultrasonic25 and microwave26,27 processes has been used for devulcanization of waste rubbers.
The aim of devulcanization is breaking in C–S and S–S bonds (i.e. cross-links) instead of C–C bonds (i.e. backbone) in the vulcanized rubber network. In theory, fracture in C–C bonds needs to higher energy than C–S and S–S bonds, but in real condition both chain scission and cross-link breakage occur during devulcanization.28 On this basis, the best devulcanization method is a process with higher cross-link breakage to chain scission ratio.
Using ultrasonic waves is one of the most considerate methods for waste rubber recycling. Two sonication based methods have been conventionally used for rubber recycling: extrusion-sonication of waste rubber and sonication of rubber particles in an ultrasonic bath. Liang and Isayev et al.29 used ultrasonic waves for devulcanization of rubbers by combination of sonication and extrusion methods. They assessed the effect of rubber compound and ultrasonic amplitude on devulcanization of unfilled and silica-filled natural rubber. Based on the results, ultrasonic amplitude had a direct relationship with power. However, the die pressure illustrated an inverse trend which is a consequence of rubber thixotropic properties and declining in the chain breakage. Also, sonication caused breaking in the NR chains that caused declining in the rubber–silica connections. The devulcanazation of SBR contained carbon black (CB) was also investigated.30–32 It was performed by an extruder equipped to an ultrasonic die. It was claimed that the revulcanized samples prepared from devulcanized SBRs had close properties to the virgin rubber. The devulcanization of BR and SBR/BR blend via sonication-extrusion process was also investigated by Liang et al.33,34 They evaluated effects of different fillers (i.e. carbon black, silica and silanized silica) by a single screw extruder and various ultrasonic amplitudes. It was found that carbon black promoted the mechanical properties of SBR/BR blend compared to silica filler. It was proposed that CB made some bridges in rubber structure which caused improved properties. Based on the experiments, silica containing BR that contained long side branches, showed strong rubber–filler interactions that caused better distribution of silica in rubber matrix but declined rolling resistance of the rubber.
Saputra et al.35 investigated effect of deep eutectic solvents and their content at different heating times on devulcanization of GTR in an ultrasonic bath. They assessed the relationship between devulcanization performances and solvents viscosity. It was found that low viscosity solvent led to success in de-cross-linking process. They realized that increase in the heating time caused decline in the cross-link density and enhancement of devulcanization percentage. The Horikx theory was also used to determine chain scission to cross-links breakage ratio. It was found that the most broken bonds belonged to cross-links which exposed to a selective devulcanization.
Kim et al.36 investigated devulcanization of waste tire rubber through probe sonication. They studied devulcanization of rubber through determination of prepared free sulfur content that formed by cross-links breakage. The rubber fragments were prepared by cryogenic processing of tire scrap (i.e. both the tread wear and sidewall). The fragmented samples were immersed in acetone for 24 h to extract plasticizers, paraffin's and antioxidants. The samples showed increased volume that confirmed suitable swelling. Thereafter, the samples were sonicated by a probe ultrasonic device and then refluxed and filtered to remove carbon black. The samples then dried and analyzed for sulfur content. It was found that sonication in presence of H2O2 effectively increased fracture in the sulfur bonding and cross-links.
Based on the literature review, it was found that sonication-based devulcanization of waste rubbers have been studied in few researches. Besides, in most cases ultrasonic devulcanization performed by altering mechanical stresses (i.e. in an extruder) along with sonication by a horn or ultrasonic bath.37 In one investigation, probe sonication was used for devulcanization of waste tire rubber but the devulcanization properties (gel/sol fractions and devulcanization percentage) and process parameters (sonication power, time and etc.) were not assessed. Due to the fact that probe sonication is a simple method and involve higher energies to the rubber particles (e.g. GTRs) compared to sonication bath, investigating the method and the influencing parameters would be a challenging subject.
In this study, probe sonication was used for devulcanization of a cured NR/SBR blend as a model tire rubber. For this purpose, NR/SBR blend (i.e. at NR:SBR ratio of 50:50) was prepared and vulcanized. The sample were ground to particles with mesh size of 16. The crumbed particles were devulcanized by probe sonication and also sonication in presence of chemical agent (DPDS and VitaX). Effect of sonication media, swelling media, sonication power-time and chemical agent content on devulcanization percent, cross-link density, sol/gel fractions, curing and mechanical properties of the devulcanized samples was evaluated. The samples characterized with oscillating disc rheometer (ODR), Fourier-transform infrared spectroscopy (FTIR), differential scanning calorimetry (DSC) and thermogravimetric (TGA) analysis. Finally the mechanical properties of the recycled rubbers in blend with pristine rubber was evaluated.
Sample | NR Masterbatch (phr) | SBR Masterbatch (phr) |
---|---|---|
Raw elastomeric gum | 100 | 100 |
Carbon black (N550) | 60 | 60 |
Process oil | 20 | 20 |
ZnO | 5 | 5 |
Stearic acid | 1 | 1 |
Sample code | Condition | ||||||||
---|---|---|---|---|---|---|---|---|---|
Pre-immersion media | Sonication media | Sonication power (W) | Sonication time (min) | Pre-immersion time (hr) | |||||
Water | Oil | Toluene | Water | Oil | Toluene | ||||
DGR-Ctrl | — | — | — | — | — | — | 0 | 0 | 0 |
DGR-W(45-20) | — | — | — | √ | — | — | 45 | 20 | 0 |
DGR-O(45-20) | — | — | — | — | √ | — | 45 | 20 | 0 |
DGR-T(45-20) | — | — | — | — | — | √ | 45 | 20 | 0 |
DGR-W24(45-20) | √ | — | — | √ | — | — | 45 | 20 | 24 |
DGR-O24(45-20) | — | √ | — | — | √ | — | 45 | 20 | 24 |
DGR-T24(45-20) | — | — | √ | — | — | √ | 45 | 20 | 24 |
DGR-T24W(45-20) | — | — | √ | √ | — | — | 45 | 20 | 24 |
DGR-O24W(45-20) | — | √ | — | √ | — | — | 45 | 20 | 24 |
DGR-O24T(45-20) | — | √ | — | — | — | √ | 45 | 20 | 24 |
DGR-O24(30-10) | — | — | — | — | √ | — | 30 | 10 | 24 |
DGR-O24(30-20) | — | √ | — | — | √ | — | 30 | 20 | 24 |
DGR-O24(30-30) | — | √ | — | — | √ | — | 30 | 30 | 24 |
DGR-O24(60-20) | — | √ | — | — | √ | — | 60 | 20 | 24 |
DGR-O24(60-25) | — | √ | — | — | √ | — | 60 | 25 | 24 |
DGR-O24(60-30) | — | √ | — | — | √ | — | 60 | 30 | 24 |
To evaluate cross-link density (CLD) of the samples, they were immersed in toluene at room temperature for 72 h. The solvent was refreshed three times with pure solvent over the swelling time (each 24 h). Thereafter, the samples were removed from solvent and quickly dried by filter paper and weighted. Finally, the samples were dried in an oven at 70 °C for 12 h to evaporate the rest of solvent and then weighted again. The cross-link density (eqn (1)) was calculated using Flory–Rehner equation41 as following:
(1) |
The volume fraction of polymer in swollen specimen (Vr) was measured as following:
(2) |
The density of dry samples was measured according to ASTM D6814 (ref. 42) using the eqn (3) as following:
(3) |
In which, A and B are weight of the specimen in air (g) and methanol (g), respectively. On this basis, the density of pristine NR/SBR sample was obtained 1.129 g cm−3.
The devulcanization percentages of the samples was also calculated using eqn (4):41
(4) |
The tensile tests were carried out on dumbbell-shaped specimens (type C) using a SANTAM STM150 Universal Machine at room temperature (25 ± 2 °C) to evaluate tensile strength and elongation at break of the pristine and re-vulcanized samples based on the ASTM D 412.44 The uniform crosshead speed of 500 mm min−1 was applied in tension and the test was repeated 10 times for each sample.
Fig (1a) shows the effect of sonication media on devulcanization percentage. It is clearly seen that type of sonication media affects the devulcanization percent (i.e. in the samples processes without pre-immersion). It is well known that breakage of these bubbles induce sonication energy to the ground rubber particles. However, due to the hydrophobic nature of rubber particles, they had not intimate contact to water (in contrary to toluene) that this decreased induced sonication energy to the particles. The low DP of the sample in oil media was attributed to its higher viscosity that dissipated induced sonication energy to the GTRs. The highest devulcanization percentage was obtained (i.e. about 28%) in the case of using toluene as sonication media. The devulcanization performances of the samples are illustrated in Table 3.
Samples | CLD (×104) (±st. dev.) (%) | Sol fraction (±st. dev.) (%) | Gel fraction(±st. dev.) (%) |
---|---|---|---|
a UB:Ultrasonic bath. | |||
DGR-Ctrl | 1.95 (±0.08) | 10.5((±0.03) | 89.5 (±0.03) |
DGR-T(45-20) | 1.4 (±0.095) | 18.95 (±0.019) | 81.05 (±0.019) |
DGR-O(45-20) | 1.44 (±0.034) | 15 (±0.02) | 85 (±0.02) |
DGR-W(45-20) | 1.54 (±0.035) | 13.5 (±0.015) | 86.5 (±0.015) |
DGR-T24(45-20) | 1.46 (±0.039) | 13 (±0.01) | 87 (±0.01) |
DGR-O24(45-20) | 1.32 (±0.031) | 20 (±0.02) | 80 (±0.02) |
DGR-W24(45-20) | 1.54 (±0.028) | 15.4 (±0.025) | 84.6 (±0.025) |
DGR-T24W(45-20) | 1.43 (±0.018) | 16 (±0.02) | 84 (±0.02) |
DGR-O24W(45-20) | 1.35 (±0.015) | 18 (±0.03) | 82 (±0.03) |
DGR-O24T(45-20) | 1.30 (±0.031) | 20 (±0.01) | 80 (±0.01) |
DGR-O24(30-10) | 1.71 (±0.024) | 17.5 (±0.02) | 82.5 (±0.02) |
DGR-O24(30-20) | 1.64 (±0.035) | 17 (±0.033) | 83 (±0.033) |
DGR-O24(30-30) | 1.62 (±0.027) | 16.65 (±0.01) | 83.35 (±0.01) |
DGR-O24(60-20) | 1.19 (±0.046) | 22 (±0.05) | 78 (±0.05) |
DGR-O24(60-25) | 1.35 (±0.015) | 18.5 (±0.01) | 81.5 (±0.01) |
DGR-O24(60-30) | 1.37 (±0.066) | 16.25 (±0.022) | 83.75 (±0.022) |
DGR-O24 (60-20)-VitaX0.6 | 1.13 (±0.04) | 19.15 (±0.03) | 80.85 (±0.03) |
DGR-O24 (60-20)-VitaX1.2 | 0.93 (±0.068) | 20 (±0.03) | 80 (±0.03) |
DGR-O24 (60-20)-DPDS1.2 | 1.45 (±0.096) | 15.4 (±0.025) | 84.6 (±0.025) |
DGR-O24 (30-10)-VitaX0.6 | 1.22 (±0.067) | 13.37 (±0.035) | 86.62 (±0.035) |
DGR-O24 (30-10)-VitaX1.2 | 1.24 (±0.083) | 16.1 (±0.01) | 83.9 (±0.01) |
DGR-O24 (30-10)-DPDS1.2 | 1.45 (±0.097) | 15 (±0.05) | 87 (±0.05) |
DGR-O24 (60-20)-UBa | 1.35 (±0.099) | 15.83 (±0.084) | 84.17 (±0.084) |
DGR-O24 (60-20)-VitaX1.2-UB | 1.32 (±0.019) | 17 (±0.02) | 83 (±0.02) |
It is clearly seen that cross-link density (CLD) decreased significantly in the devulcanized samples compared to the control sample (i.e. the mechanically devulcanized sample). It proves that probe sonication caused fracture in the cross-links properly as it was desired. The sol content shows that low molecular weight and soluble chains increased considerably in the sonicated samples. This was attributed to the chain scissions that occurred during devulcanization in the rubber matrix.
The figure also shows the effect of pre-immersion of the samples in the individual liquids for 24 h. Results showed that DP just increased in the case of using oil as pre-immersion media. It is also obviously seen that just using oil as pre-immersion media could influence CLD and sol/gel fractions of the sonicated samples (see Table 3). This was attributed to diffusion of the oil into the rubber bulk during pre-immersion step that swelled and expanded its network and helped effective devulcanization during sonication. In contrary, the CLD of samples was not affected after 24 h of immersing in water and toluene, however, their sol content changed significantly.
The pre-immersion of the samples in water caused increment in the sol content that means it increased the chain scission. In contrary, pre-immersion in toluene caused decrement in the chain scission. In fact, the chain scission represents unsuitable devulcanization of GTRs that decreases the mechanical properties.33,34
Based on the results, toluene and oil were selected as effective liquids for pre-immersion step. The effect of water, toluene and oil as sonication media was also evaluated. Results are shown in Fig. (1b) and Table 3. It is obviously seen that using different liquids for pre-immersion and sonication has negligible effect on devulcanization percent. On this basis, the DGR-O24 sample and oil were selected as the best devulcanized sample (32%) and the best media for pre-immersion/sonication, respectively.
Fig. 2 Devulcanization percent of the DGR-O24 samples sonicated at different powers and times in oil (after 24 h pre-immersion in oil). |
Negligible changes was observed in devulcanization percent of the samples at sonication power of 30 W (at all times). The highest DP was obtained at sonication power and time of 60 W and 20 min (38%), respectively. Similar to the CLD and sol fraction results, herein the DP increased with increment in the induced energy. The reverse results was obtained at sonication times of 25 and 30 min at amplitude of 60 W. It was postulated that due to the very high energies encountered to the particles, their surface scorched and formed an insulated layer which decreased wave intrusion toward the particles core. Fig. 3 shows a schematic for partial devulcanization of the rubber particles that happened under probe sonication.
In these schematic, the mechanism of partial devulcanization of ground rubber particle due to sonication was illustrated. The degree of cross-links breakage incredibly depends on ultrasonic amplitude, time and kind of liquid. The more sonication amplitude causes decrement in the area of intact cross-linked core and improvement in the DP and crosslinks breakage. In contrast, at low sonication powers, devulcanization just occurs at a thin surface layer of the particles.
Fig. 4 shows that both chemical agents significantly increased devulcanization percent of the sonicated samples (DGR-O24), however, higher DPs were obtained using VitaX. Devulcanization percent was improved considerably at higher VitaX loading content (i.e. 1.2 phr). The VitaX content had negligible effect on devulcanization percent at lower sonication energies. Furthermore, DPDS had lower impact on devulcanization percent compared to VitaX at low and high sonication energies. The better results obtained by VitaX were related to its complex chemistry and its different application process.27 In fact, using processing oil along with VitaX caused more intrusion of the VitaX into the particles core. On the other hand, using VitaX increased the thickness of the devulcanized layer in the partially devulcanized particles. In the case of using DPDS, it just acted on the surface of the rubber particles this limited its devulcanizing performance. The results were in good correlation with CLD and sol fraction results.
Fig. 4 Devulcanization percent of the samples devulcanized in presence of different chemical agents. |
Fig. 6 Pyrolysis-FTIR spectra of different samples; (a) from 400 to 600 cm−1, (b) from 600 to 1200 cm−1, (c) from 1200 to 1550 cm−1 and (d) from 1550 to 1800 cm−1. |
Characterized peak | Wavenumber (cm−1) | Components | Ref. |
---|---|---|---|
S–S stretching | 540 | Crosslinks | 7,12,15 |
C–S stretching | 603 | Crosslinks | 7,26 |
CC bending | 870 | NR | 15 |
C–C bending | 900–1000 | NR &SBR | 15 |
C–C stretching | 1018 | Carbon black | 5,7,15 |
CC stretching | 1645 | NR/SBR | 12,15,26 |
CO | 1720 | CBS-stearic acid | 5,9,12 |
CC–H | 3070 | — | 15,21,26 |
Comparing the spectrums of the virgin NR/SBR and DGR-Ctrl samples showed that rubber grinding and then mechanical devulcanization affected the rubber network structure according to the peaks appeared at wavelength of 2800 to 3200 cm−1. It is apparent that the intensity of the peaks related to CH and CH2 groups are reduced and CH3 has been added after grinding. This change simply confirmed chain scission and creation of new CH3 groups at the end of the broken chains. The peak at 3500 cm−1 is related to tension vibration of hydroxyl groups of carbon black. Moreover, the presence of a sharp peak at 1650 cm−1 (bending vibration of OH groups) could also confirm the presence of moisture in the sample. The observed peak at 1690 cm−1 was related to –CHCH– groups in the virgin and control rubbers. The twin peaks at 1450 and 1550 cm−1 should be attributed to the benzene rings in the SBR. Peaks in the range of 750 to 1200 cm−1 was corresponded to the flexural vibration of alkane compounds (–CH2–CH2–) which increased by grinding of vulcanized rubber. This confirmed occurrence of chain scission and formation of smaller chains in the mechanically devulcanized sample (DGR-Ctrl). The increase in the intensity of the peaks in DGR-O24(60-20)-VitaX1.2 sample confirmed more failure of the rubber network after sono-chemical devulcanization.
The peak appeared at 720 cm−1 was related to the –C–SH bonds which increased in devulcanized samples. This confirmed that more breakage happened in the cross-links (i.e. –S–S– bonds) in presence of sonication.
As it is seen, the Tg values for both NR (i.e. Tg1) and SBR (i.e. Tg2) parts were increased in the mechanically and sono-chemically devulcanized samples compared to the uncured virgin rubber. This was attributed to the networked structure that created due to the primary and secondary vulcanization steps that was performed on the devulcanized samples. The exothermic peak observed at about 160 °C in all samples was corresponded to the curing temperature of the rubbers. It is obviously seen that this peak weakened in the mechanically and sono-mechanically samples due to lower cross-links occurred in these samples compared to the virgin rubber.
According to the results, the glass transition temperature increased in the DGR-O24(60-20)-Vitax1.2 compared to the DGR-Ctrl sample. This was attributed to presence of higher amounts of low molecular weight chains (i.e. broken chains) in the mechanically devulcanized sample. This confirms more crosslinks breakage instead of chain scission in the sono-chemically devulcanized sample.
Fig. 8 The effect of VitaX on thermogravimetric properties of the samples; (a) TGA curve and (b) DTG curve. |
Compounds | Data | Low molecular weight organic mater | NR part | SBR part | Inorganic residues |
---|---|---|---|---|---|
ΔT [°C] | 35 to 320 | 320 to 425 | 425 to 540 | 540 to 750 | |
Cured NR/SBR | Δm [%] | 5.90 | 34.21 | 27.24 | 35.8 |
Tmax [°C] | — | 386 | 457 | — | |
R-DGR-O24(60-20) | Δm [%] | 5.75 | 29.64 | 14.85 | 49.69 |
Tmax [°C] | — | 383.03 | 437.27 | — | |
R-DGR-O24(60-20)-Vitax0.6 | Δm [%] | 7.56 | 19.64 | 18.95 | 54.7 |
Tmax [°C] | — | 389.96 | 433.92 | — | |
R-DGR-O24(60-20)-Vitax 1.2 | Δm [%] | 7.9 | 18.62 | 20.26 | 54.53 |
Tmax [°C] | — | 384.46 | 439.98 | — |
The temperature regions of 320–425 °C and 425–540 °C was attributed to degradation of NR and SBR parts of samples, respectively. It is obvious that both NR and SBR parts of sonicated samples showed lower weight losses compared to the cured NR/SBR sample due to the fractures occurred in polymers chains. It is also seen that the weight loss related to NR part was lower in the devulcanized samples in presence of VitaX compared to DGR-O24(60-20) sample. This shows that in presence of VitaX, fractures occurred mostly in the SBR network instead of NR structure.
Higher thermal stabilities were observed in revulcanized samples due to the presence of intact-crosslinked core of particles that acted as reinforcing filler in devulcanized matrices.
Fig. (9b) shows DTG curves for the samples. The results confirmed the higher thermal stabilities of the devulcanized samples compared to the cured NR/SBR sample due to the increment in the degradation temperatures of the NR and SBR parts.
Compounds | ML [dN m] | MH [dN m] | MH − ML [dN m] | t90 [Minute] | CRI (%) |
---|---|---|---|---|---|
DGR-Ctrl | 0.49 | 10.26 | 9.8 | 8.09 | 29.54 |
DGR-O24(60-20) | 2.2 | 14.28 | 12.1 | 5.5 | 27.72 |
DGR-O24(60-20)-Vitax0.6 | 2.32 | 15.02 | 12.7 | 2.53 | 62.13 |
DGR-O24(60-20)-Vitax1.2 | 2.2 | 11.84 | 9.7 | 5.3 | 36.03 |
Fig. 10 The tensile properties of the re-vulcanized samples; (a) tensile strength/elongation at break and (b) modulus. |
Based on the results, modulus of the samples were obtained. For the effectively devulcanized sample, the modulus content confirmed the TS results. In comparison to the virgin sample, the modulus of VitaX containing samples was considerably increased because of their higher CLD and toughness. Therefore the cross-links breakage were less selective in DGR-O24 (60-20) sample compared to the VitaX containing samples. With regards to elongation at breaks (EBs), it was vivid that DGR-O24 (60-20)-VitaX0.6 with non-selective devulcanization and high toughness resulted in lower EB (63%) than DGR-O24(60-20)-VitaX1.2. All in all, devulcanaized samples show acceptable mechanical properties and confirmed other tests results.
• It was claimed that probe sonication is a promising method for recycling of tire rubber due to its facility and effectiveness compared to other methods (e.g. microwave assisted devulcanization).
• It was found that devulcanization percent (DP) enhanced from 15 to 32% by pre-immersion of ground rubber particles in oil. However, sonication in all the liquids improved DP.
• There is a direct relationship between DP and sonication power, while no specific relation was found between DP and sonication time. Sonication at 60 W/20 min caused 6.34% increment in the DP compared to the sample sonicated for 45 W/20 min.
• Devulcanization percent was improved 100% by using 1.2 phr of VitaX instead of DPDS. It was also about 20% more than DP of the sample contained 0.6 phr of VitaX.
• It was found that probe sonication caused about 27% increment in the DP of the samples in absence of VitaX while it increased up to 65% in presence of VitaX.
• The highest cure rate index (more than 60%) and the lowest scorch time (about 1 min) was obtained in the case of using 0.6 phr of VitaX.
• It was found that devulcanization by sonication caused decrement in the tensile strength (more than 40%) of virgin rubber/devulcanized rubber blend (at 50:50 weight ratio), except for the sample contained 1.2 phr of VitaX that showed the same tensile strength as cured NR/SBR sample.
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