OPTIMIZATION OF MIXING CONDITIONS FOR SILICA-REINFORCED NATURAL RUBBER TIRE TREAD COMPOUNDS
Abstract
The dump temperature and mixing interval between rubber, silica, and silane coupling agent for silica-filled natural rubber (NR) tire tread compounds using bis-triethoxysilylpropyl tetrasulfide (TESPT) as silane were optimized. The dump temperature turns out to be the key parameter governing the properties of the silica-filled NR compounds. The increase in viscosity of the compounds by changing the dump temperature from 100 to 150 °C indicates that inevitably some cross-linking of NR occurs by sulfur contained in TESPT, simultaneous with the silanization reaction between silica and silane. However, the viscosity decreases again when dump temperatures above 150 °C are applied, indicating a dominant occurrence of degradation of the NR molecules. The results are in good agreement with bound rubber contents. The overall properties indicate that a dump temperature in the range of 135–150 °C and a silica–silane–rubber mixing interval of 10 min are the most appropriate mixing conditions for silica-filled NR compounds with TESPT as coupling agent.
INTRODUCTION
Natural rubber (NR) is a renewable material that combines excellent mechanical and dynamic properties, and its use covers a wide variety of applications, mostly in the form of filler-reinforced vulcanizates. The commonly used reinforcing fillers in rubber compounds are carbon black and silica. Replacement of carbon black by silica is growing, especially in the tire industry, since the introduction of the “Green Tire Technology” by Michelin in 1992.1 Silica significantly reduces rolling resistance and improves wet traction of tire tread compounds compared with carbon black.2 However, a major drawback of using silica is difficulties in processing that come from the polarity difference between silica and rubber.
The polar nature of silica negatively affects its compatibility with nonpolar elastomers. The silica surface is acidic with a number of silanol groups. Hence, it forms strong hydrogen bonds or reacts with either basic or polar materials, such as accelerators, resulting in the adsorption of curatives by silica. In addition, strong hydrogen bonds between the silica particles themselves result in tight silica aggregates and agglomerates causing poor dispersion of silica in rubber compounds.3 A good dispersion of filler in a rubber compound is very important for the mechanical and dynamic properties.3,4 The dispersion of silica-filled rubber compounds is generally worse than that of carbon black–filled ones. Moreover, when a large amount of silica is added, the viscosity substantially increases, making the rubber compounds more difficult to process and causing wear of the processing equipment. These difficulties can be overcome by use of silane coupling agents, which are able to combine chemically with silica and rubber during the mixing and vulcanization stages, respectively.5–7 As a consequence, mixing of silica-filled compounds is basically different from that of carbon black.
Mixing of rubber and silica with a silane coupling agent involves the reaction between silanol groups on the silica and ethoxy or hydroxyl groups of the silane, that is, the silanization reaction. However, the efficient use of silane as a coupling agent in the silica-filled rubber compounds is rather limited, caused by side reactions. Various mixing-processing conditions need to be optimized for silanized silica-filled compounds.8 The temperature window for mixing silica compounds is rather limited by the low silanization rate needed to avoid scorch. High temperatures improve the silanization rate due to the temperature dependence of the reaction5 and reduction of sterical hindrance of the silylpropyl groups of the coupling agent by increased thermal mobility.9 Based on a study with SBR/BR compounds,10 the dump temperature should be in the range of 145 °C to 155 °C to achieve good silanization and to avoid pre-cross-linking. Furthermore, a mixing time of at least 10 min is needed for the silanization reaction during the first mixing step.
Most of the work in this area was focused on synthetic rubbers, in particular SBR/BR-based compounds for passenger tires. There are only a few studies dealing with silica-filled NR. The optimization of mixing conditions for silanized conventional silica-filled NR compounds was studied by Wolff.11 The author concluded that an increase of mixing temperature and time for silica modification with silane enhances the compatibility between silica and NR through a chemical coupling bond of bis-triethoxysilylpropyl tetrasulfide (TESPT) with the rubber. The overall properties are dependent on the extent of this interaction. However, it was stated that the in situ modification reaction of silica with TESPT should not be considered an optimum reaction, since the recipe was composed of only 20 phr of silica in combination with 40 phr of carbon black.
The present work aims at optimizing the mixing conditions, that is, mixing temperature and silica–silane–rubber mixing interval, which may have an influence on mixing quality and silanization efficiency of silica-filled natural rubber compounds. Mooney viscosity, cure characteristics, filler–filler and rubber–filler interactions, as well as mechanical and dynamic properties of the rubber compounds and vulcanizates, are evaluated.
EXPERIMENT
MATERIALS
The natural rubber used was Ribbed Smoked Sheet 3 (RSS3), locally produced in Pattani, Thailand. The solution SBR (Buna VSL 5025-0 HM, Lanxess GmbH, Leverkusen, Germany) contains 25% styrene and 75% butadiene, 50% of which is in the vinyl configuration. The compounding ingredients were highly dispersible silica with cetyl trimethylammonium bromide (CTAB) specific surface area12 171 m2/g (Ultrasil 7005, Evonik GmbH, Essen, Germany), TESPT with sulfur content of approximately 22 wt% (Zhenjiang Wholemark Fine Chemicals, Taohuawu, China), treated distillate aromatic extract (TDAE) oil (Vivatec 500, Hansen & Rosenthal, Hamburg, Germany), zinc oxide (Global Chemical, Bangpoo, Thailand), stearic acid (Imperial Chemical, Bangkok, Thailand), polymerized 2,2,4-trimethyl-1,2-dihydroquinoline (TMQ), diphenylguanidine (DPG), and N-cyclohexyl-2-benzothiazolesulfenamide (CBS; all from Flexsys, Brussels, Belgium), and sulfur (Siam Chemical, Bangkok, Thailand).
COMPOUND PREPARATION
The compound recipe used for this study is shown in Table I. The amounts of TESPT and DPG applied in this recipe were based on the CTAB specific surface area of the silica according to Eqs. 1 and 2 as suggested by Guy et al.13:
where Q is the silica content (phr) and CTAB is specific surface area of the silica used (m2/g).
The mixing was performed using an internal mixer with a mixing chamber of 500 cm3 (Chareon Tut Co., Ltd., Bang Sao Thong, Thailand). The mixer was operated at a fill factor of 70% and a rotor speed of 60 rpm. Initial temperature settings of the mixer were adjusted in the range of 50 to 140 °C (Table II). NR was initially masticated for 2 min. Then, half of the silica and silane were added and mixed for half the duration of the silica–silane–rubber mixing interval, that is, 2.5, 5, 7.5, and 10 min, prior to adding the second half of silica and silane together with TDAE oil. The mixing was then continued to the full intervals, that is, 5, 10, 15, and 20 min. Subsequently, the other ingredients: ZnO, stearic acid, TMQ, and DPG, except CBS and sulfur, were added and mixed for 3 min. The compounds were then dumped, sheeted out on a two-roll mill, and kept overnight prior to incorporation of CBS and sulfur on a two-roll mill.
Mixer temperature settings and silica–silane–rubber mixing intervals prior to adding other chemicals were varied following the experimental design as shown in Table II. Gum or unfilled compounds were included in this study in order to determine the reinforcement parameter (αF) from the cure characteristics; see below.
MOONEY VISCOSITY AND CURE CHARACTERISTICS
The compounds were tested for their Mooney viscosities by using a Mooney viscometer (ViscTech+, TechPro, Cuyahoga Falls, OH) at 100 °C with large rotor according to ASTM D1646. The value is represented as ML1+4 @ 100 °C.
The cure characteristics were determined using a moving die processability tester (MDPt; TechPro). The increase in torque (S′) at a temperature of 150 °C, a frequency of 0.833 Hz, and 2.79% strain was measured for 30 min. The optimum vulcanization time (t90) was determined and used for press-curing of the samples.
CHARACTERIZATION OF FILLER–FILLER AND FILLER–RUBBER INTERACTIONS
Reinforcement Parameter
The reinforcement parameter (αF) was calculated by using the data from the cure characteristics according to Eq. 314:
where
−
= torque difference of the silica-filled rubber;
−
= torque difference of the corresponding gum or unfilled compound; mF/mP = filler loading, where mF and mP correspond to the mass fractions of filler and polymer, respectively. The reinforcement parameter, αF turns out to be a filler specific feature, independent of the cure system, and closely related to the morphology of the filler in the compound.14
Flocculation Rate Constant
Silica flocculation can be observed by following the changes of the storage modulus of uncured compounds without curatives at low strain amplitude during thermal annealing.15 In order to calculate the flocculation kinetics of the silica, the storage modulus at 0.56% strain amplitude can be monitored during heating at 100 °C for 12 min by using the MDPt, according to Mihara et al.16 The degree of flocculation (x) can be expressed by the ratio of the Payne effect at time t and at infinite time:
where G′(t) is the storage modulus at 0.56% strain amplitude after heating time t; G′(i) is the storage modulus after preheating for 1 min; G′(f) is the storage modulus at infinite time, taken as 12 min in order to reduce measuring time.
As mentioned by Bohm and Nguyen,15 silica flocculation can be experimentally described as a first-order reaction for which the kinetics can be described by a simple model equation. Mihara et al.16 take this information and apply the following equation to calculate the flocculation rate constant (ka).
where ka is the rate constant; t is the heating time; x is the degree of flocculation; and 1 and 2 refer to different heating times t.
Payne Effect
Storage shear moduli (G′) of compounds cured to their t95 at 150 °C were measured under shear deformation using a rubber process analyzer (RPA; Alpha Technologies, Akron, OH). A strain sweep test was done in the range of 0.56–100% strain at 0.50 Hz and 100 °C.
Bound Rubber Content
Bound rubber measurements were carried out both with and without ammonia treatment. The ammonia treatment was done in order to cleave the physical linkages between rubber and silica, so that the true chemically bound rubber could be determined.17 The procedure adopted for the bound rubber measurement was as follows:
-
0.2 g of sample, that is, uncured master batch (without curatives), was put into a metal cage and immersed in 20 mL of toluene for 72 h at room temperature. Toluene was renewed every 24 h.
-
The sample was removed from the toluene, dried at 105 °C for 24 h.
-
The sample was immersed again in 20 mL of toluene for 72 h at room temperature in either a normal or an ammonia atmosphere in order to cleave the physical linkages. Toluene was renewed every 24 h.
-
The sample was dried at 105 °C for 24 h and weighed.
The bound rubber content was calculated according to Eq. 617:
where Wfg is the weight of silica with the bound rubber attached; Wf is the weight of silica in the specimen; and Wp is the weight of polymer in the specimen. Wf and Wp are calculated with reference to the compound formulation and initial sample weight.
VULCANIZATION AND MEASUREMENT OF TENSILE AND TEAR PROPERTIES
The compounds were press vulcanized at 150 °C to t90. The vulcanized sheets having a thickness of about 2 mm were die-cut to dumbbell-shaped specimens for tensile tests and to angle-shape specimens (die type C) for tear tests. The tests were performed at a crosshead speed of 500 mm/min according to ASTM D412 and ASTM D624, using a Hounsfield tensile tester. The mean values of tensile and tear properties taken from five specimens are reported.
DETERMINATION OF DYNAMIC MECHANICAL PROPERTIES
The vulcanizates cured to their t95 at 150 °C in the RPA were tested for dynamic mechanical properties using a frequency sweep test. The frequencies were varied in a range of 0.05–33 Hz at a fixed strain and temperature of 3.49% and 60 °C, respectively.
CURE CHARACTERISTICS OF NR AND SBR COMPOUNDS IN THE PRESENCE OF TESPT AND DPG (WITHOUT CBS AND SULFUR)
In order to explain the difference in change of Mooney viscosities with dump temperature of silica-filled NR compounds in comparison with previous experience with SBR compounds,10 two additional compounds were prepared. These compounds were composed of rubber with only TESPT and DPG at amounts of 5.0 and 1.5 phr, respectively. The compounds were prepared using a two-roll mill; rubber was milled for 6 min, then DPG was added and mixed for 2 min, and TESPT was subsequently incorporated and mixed for 2 min. The compounds were sheeted out to a thickness of about 0.5 cm and kept overnight prior to testing.
The cure characteristics of these compounds were analyzed by using the RPA with a frequency of 0.833 Hz and strain 2.79% for 12 min. The testing temperature was varied from 120 to 180 °C with an increment of 10 °C for each separate test.
RESULTS AND DISCUSSION
PROCESSING PROPERTIES
Mixing Temperatures and Torques
The initial mixer temperatures settings and silica–silane–rubber mixing intervals prior to the addition of other chemicals were varied so that the influence of different dump (end) temperatures on the silica-filled NR compounds could be evaluated. The dump temperatures as a function of initial temperature settings and silica–silane–rubber mixing intervals of the silica-filled NR compounds, in comparison with those of gum compounds, are shown in Figures 1 and 2, respectively. By increasing the initial mixer temperature setting (Figure 1), the dump temperatures of both filled and gum compounds increase linearly. The filled compound shows a significantly higher dump temperature than that of the gum compound, attributed to the influence of hydrodynamic effects leading to higher shear forces generated during mixing. By choosing the initial mixer temperature settings in the range of 50–140 °C, dump temperatures in the range of 90–170 °C could be obtained. Considering the different silica–silane–rubber mixing intervals of filled and gum compounds (Figure 2), longer periods clearly give higher dump temperatures for both compounds, and the filled compounds have again higher dump temperatures than the gum compounds.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
Figure 3 shows typical torque curves during mixing of silica-filled NR compounds prepared by adjusting the initial temperature setting in order to reach different dump temperatures, as they are indicated in the figure. The relation between dump temperatures and initial mixer temperature settings are given in Figure 4. The torque curves show quite different behaviors at different mixing times. Higher mixer temperature settings correspond to lower mixing torques in the range of 0–600 s mixing time, as depicted also in Figure 4: the torque average at 300 s in the first nonproductive stage substantially decreases with increasing mixer temperature setting. This is commonly the result of lower mixture viscosity due to the higher temperature. However, in the second nonproductive stage, the compounds with low initial mixer temperature settings (i.e., 50 and 70 °C) again show the decrease of mixing torque, while the compounds with high initial mixer temperature settings (i.e., 110 and 140 °C) display rather constant mixing torque with a slight increase at the end of this mixing stage. In this latter case, the lower mixture viscosity due to the higher temperature is balanced by the higher mixture viscosity due to a better silanization reaction and some premature cross-linking caused by sulfur in TESPT. For mixing times larger than 600 s, a crossover of the curves can be observed in Figure 3. Figure 4 shows that the mixing torque at 720 s increases with increasing mixer temperature setting to reach a maximum for a temperature setting of 110 °C. At the end of mixing, that is, 890 s, the torque also displays such a maximum. There are three possible reactions occurring during mixing: (1) silanization, (2) premature cross-linking due to sulfur in TESPT, and (3) rubber degradation. At dump temperatures lower than 150 °C, silanization and some premature cross-linking are dominant so that the mixing torque increases at the later stage of mixing. However, at very high initial mixer temperature settings and consequent high compound dump temperatures, degradation of the natural rubber becomes dominant resulting in a decrease of torque. Some chemical ingredients (i.e., ZnO, stearic acid, TMQ, and DPG) were added at the last stage of mixing. These chemicals, especially stearic acid, can provide an additional peptizing effect causing the mixing torque at 890s to be lower than at 720s, as shown in Figure 4. However, since every compound was mixed using the same quantities of ingredients and mixing procedure, this additional peptizing effect is presumed to be more or less the same. The change of torque as function of initial mixer temperature setting can therefore be explained using the three possible reactions as mentioned here before.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
Mooney Viscosity of the Compounds
The Mooney viscosities of the silica-filled NR compounds prepared with the different mixer temperatures and silica–silane–rubber mixing intervals in comparison with those of the gum compounds are shown in Figures 5a,b, respectively. The filled compounds show much higher viscosities than the gum compounds, attributed to the hydrodynamic effect, filler–filler, and filler–rubber interactions, and possibly some premature cross-linking of the rubber caused by sulfur in the TESPT in the presence of DPG accelerator. For the silica-filled compounds, the Mooney viscosities initially increase with higher dump temperature, upon which the values gradually drop off when the dump temperature is over 150 °C. This result corresponds with the change in mixing torque average (Figure 4). Furthermore, the silica-filled compounds mixed with longer silica–silane–rubber mixing intervals, that is, longer overall mixing times, give higher Mooney viscosities, given an initial mixer temperature setting, as shown in Figure 5b. On the other hand, the Mooney viscosities of the gum compounds show composite trends to decrease with higher mixer temperature settings and with prolonged silica–silane–rubber mixing intervals. This is while a longer mixing time between silica, silane, and NR results in a higher dump temperature, as displayed in Figure 2, giving an increase in degree of silanization of the silica and possibly some premature cross-linking of the rubber. Whereas the gum compound does not involve silica–silane–rubber reactions, the higher mixing temperatures can only lead to softening and destruction of the NR molecules. For these reasons, it is important to reconfirm that the mixer temperature setting has more of an effect than the time allocated for silanization of the silica-filled NR system, as already reported by Wolff.11



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
Cure Characteristic of the Compounds
The cure characteristics of the silica-filled NR compounds, scorch time (tc10), cure time (t90), cure rate index, as well as rheometer minimum torque (
), are shown in Figure 6. With higher dump temperature the scorch time and cure rate index of the silica-filled compounds slightly increase, while the optimum cure time shows no significant change. The longer scorch time enhances processing safety, while the higher cure rate leads to a similar optimum cure time, that is, better scorch safety with the same curing cycle. Moreover, the rheometer minimum torques of the compounds reach a maximum value at a dump temperature in the range of 135–150 °C, which corresponds with a similar maximum in the mixing torque average at the end of compounding, that is, 890 s of mixing time (Figure 4), and in the Mooney viscosity (Figure 5).



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
SILICA DISPERSION
Reinforcement Parameter of the Compounds
Basically, a lower reinforcement parameter indicates a better dispersion of a filler in a polymer.14 In Figure 7, the reinforcement parameters of the silica-filled NR compounds are shown as a function of dump temperature. The compounds prepared with higher dump temperature show a lower reinforcement parameter, indicating a better dispersion. However, a minimum αF is observed in the dump temperature range of 135–170 °C, which agrees with the highest mixing torque average, Mooney viscosity, and minimum cure torque as displayed in Figures 4, 5, and 6b, respectively.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
Filler Flocculation of the Compounds
Dispersion stability of the filler particles or filler aggregates in the rubber matrix influences the morphology of the filled rubber compounds. Reinforcing fillers, that is, carbon black and silica, are able to flocculate because of the poor compatibility with the rubbers and their self-association, leading to a change in morphology and consequently deterioration in the physical properties of the vulcanizates.15 It has been documented before that silica causes a greater degree of flocculation than carbon black, while silica is more polar and has a stronger self-association tendency through hydrogen bonding when compared with carbon black.18 It is worth mentioning that the flocculation process can occur during compound storage as well as directly prior to the onset of vulcanization in the absence of shear.15 The kinetics of the flocculation process can be monitored by determination of the storage modulus during thermal annealing of a compound under a condition that represents vulcanization. The flocculation rate constant (ka) of the silica-filled NR compounds as a function of dump temperature is shown in Figure 8. This value indicates how fast the silica flocculation process develops just before cross-linking, so that the parameter can be considered to represent silica dispersion stability as well as the degree of dispersion in silica-filled rubber compounds. Generally, a lower ka value means a smaller tendency toward agglomeration in the rubber matrix. In other words, a smaller amount of silica flocculation corresponds to better dispersion stability and finer morphology, presuming that silica is well dispersed during mixing. As expected, mixing until elevated dump temperature and at longer mixing times enhances the dispersion stability of silica in the NR compounds, indicated by a decrease of the flocculation rate constant. This is in agreement with the degree of dispersion indicated by the reinforcement parameter (Figure 7). By increasing dump temperature, a better silica dispersion and distribution as well as a better homogenization of the distance between the silica aggregates is achieved. The plateau for the reinforcement parameter and the flocculation rate constant observed after the dump temperature of 135 °C indicates the best possible level of the silica dispersion that we can obtain under the mixing conditions employed in this study.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
BOUND RUBBER CONTENT OF THE COMPOUNDS
The bound rubber contents of the silica-filled compounds were evaluated under two conditions, that is, with and without ammonia treatments. The ammonia treatment was used to cleave the physical linkages formed by physical adsorption, so that only the amount of chemically bound rubber, that is, strong filler–rubber interactions and covalent bonds, were determined. Figure 9 shows the bound rubber contents as a function of dump temperature of the compounds measured without and with ammonia treatment. It is evident that the bound rubber content measured with ammonia treatment is lower than that measured without ammonia treatment. With increasing dump temperature and larger silica–silane–rubber mixing intervals, both total and chemically bound rubber contents in the compounds significantly increase, but they level off when the dump temperature exceeds 135 °C. If one considers the physical linkages obtained by subtracting the chemically bound rubber from the total bound rubber content (Figure 9b), the physically bound rubber of the compounds prepared at dump temperatures over 150 °C starts to decrease, whereas the chemically bound rubber content remains unchanged. The decrease of physically bound rubber content might be attributed to the lower molecular weight of the NR molecules after mixing. Basically, natural rubber molecules can easily be broken down by excessively high temperatures and shearing action because it has reactive double bonds in every repeating unit along the rubber chain. Hence, under excessive mixing conditions, the NR chains are broken down, leading to lower physical linkages in the compound. This phenomenon corresponds well with the decrease of Mooney viscosities at very high dump temperatures, as previously shown in Figure 5. Interestingly, the chemically bound rubber does not show any such dependence.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
DYNAMIC PROPERTIES OF THE COMPOUNDS AND VULCANIZATES
The Payne effect, that is, the storage modulus difference between small (0.56%) and large (100%) strains, analyzed with a first and second sweep, and tan δ at 60 °C of the silica-filled NR vulcanizates are shown as a function of dump temperature in Figure 10. By increasing the dump temperature and mixing time, the Payne effect as a measure of filler–filler interaction decreases, even in the second sweep test (Figure 10a). However, for dump temperatures above 135 °C, there is no further change of the Payne effect. Regarding the tan δ at 60 °C of the vulcanizates (Figure 10b), which is commonly used as an indication of rolling resistance of tires for which a lower value indicates a lower rolling resistance or less fuel consumption,2 the compounds prepared with higher dump temperature and longer silica–silane–rubber mixing interval have lower tan δ at 60 °C. The reduction of tan δ at 60 °C levels off for dump temperatures above 135 °C.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
MECHANICAL PROPERTIES OF THE VULCANIZATES
Figure 11 shows the tensile strength, elongation at break, reinforcement index (i.e., the ratio of the moduli at 300% and 100% elongations or M300/M100), and tear resistance of the silica-filled NR vulcanizates prepared with varying dump temperatures and silica–silane–rubber mixing intervals. With varying dump temperatures and mixing times the elongation at break of the NR vulcanizates remains more or less the same, while the tensile strength slightly decreases with increasing dump temperature but shows no dependence on mixing times. The decrease of tensile strength, reinforcement index, and tear resistance when the dump temperature exceeds 150 °C is caused by the inevitable NR degradation under high temperature and shearing force. The degradation of NR with and without antioxidant after mixing in an internal mixer at 160 °C and 180 °C for 10 min was clearly demonstrated by Narathichat et al.19 Considering the reinforcement index, an increasing dump temperature and silica–silane–rubber mixing interval leads to an optimum at 135 °C; thereafter the values gradually decrease when the dump temperature exceeds 150 °C. A change of tear resistance of the vulcanizates with varying dump temperatures and mixing times displays the same sort of dependence as that of the reinforcement index.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
COMPETITIVE REACTIONS BETWEEN SILANIZATION, PREMATURE CROSS-LINKING, AND DEGRADATION IN TESPT-SILICA-FILLED NR COMPOUNDS
With respect to the change of the NR compound viscosities with dump temperature, as reflected in the final mixing torques, Mooney viscosities, and rheometer minimum torques in Figures 4, 5, and 6b, respectively, each separate property reveals the same trend. With increasing mixing temperatures, the compound viscosities initially increase then reach a maximum for a dump temperature range of 135–150 °C. For dump temperatures above 150 °C, the compound viscosity drops. This phenomenon is different from the work reported by Wolff,11 in which a steady decrease of viscosity with increasing dump temperature from 110 to 170 °C for silica-filled NR compounds was observed. However, it should be noted that only 20 phr of silica was used in combination with 40 phr of carbon black in that work. In the case of silica-TESPT-filled SBR/BR compounds, Reuvekamp et al.10 reported a rather constant viscosity with increasing dump temperatures from 120 to 150 °C, but an increased Mooney viscosity when dump temperatures above 150 °C were obtained, caused by premature scorch of the rubber by sulfur contained in the TESPT. It is clear that the NR and SBR/BR compounds display remarkably opposite trends of compound viscosities with varying mixing conditions.
The mixing torque can be used as an indication for what is happening. During mixing times of 120–720 s in Figure 3, which represent the first and second incorporations of silica, silane, and processing oil, the decrease in the mixing torques with increasing temperature, especially after the first incorporation, is due to several factors. These include softening of the rubber at high temperature and the breakdown of NR chains and silica structures by the mixing temperature due to mechanical energy input, in combination with the hydrophobation effect of the TESPT-silica surface modification. However, interestingly, a crossover of mixing torques is noticed at the final stage of mixing. It demonstrates that, besides the silanization reaction between silica and silane, a cross-linking or scorch reaction of NR with sulfur released from TESPT is simultaneously taking place, that is, a bond between silica–silane–rubber and rubber–rubber is created in the compound and consequently causes a rise in the compound viscosity. In order to prove this, the cure characteristic of NR and TESPT was investigated in comparison with that of SBR as shown in Figure 12. The test was performed with compounds without CBS and elemental sulfur. It is clearly seen that NR readily reacts with TESPT at a temperature as low as 120 °C, and the reaction rate increases rapidly at higher temperatures, as seen from a change of the cure curves. SBR shows a different behavior, since it starts to react with TESPT at a higher temperature, that is, 150 °C. The rheometer torque differences, commonly used to indicate the extent of cross-linking of both compounds, are shown in Figure 13. The value for the NR+TESPT compound substantially increases from a test temperature of 120 °C up to 150 °C and then gradually decreases at higher temperatures: a sort of reversion. On the other hand, the torque difference for the SBR+TESPT compound remains constant up to a temperature of 140 °C, and then increases rapidly when the cure temperature exceeds 150 °C. These results indicate that the viscosity of silica-TESPT-filled rubber compounds significantly depends on a premature cross-linking reaction that takes place during the mixing process as a result of available sulfur in TESPT, in addition to the silanization reaction and the thermomechanical shearing action. The large difference between the torque scale variation for SBR and NR in Figures 12 and 13 arises from the difference in molecular structures of NR and SBR. The torque increases observed in these rheometer curves are due to the light cross-links caused by sulfur in TESPT only. A combination of partial cross-links and bulky phenyl groups in the styrene part of SBR causes a larger restriction to movement of molecular chains under shear and hence larger torque increase for SBR compared with NR. In this context it is worth mentioning that TESPT was first developed as a sulfur-cure accelerator with sulfur-donor properties before it became commonly accepted as a coupling agent.20,21 Therefore, the increase of the silica-filled NR compound viscosities for dump temperatures in the range of 100–145 °C (Figure 5) is to a large extent due to the silica–silane–NR coupling reaction that occurs during the mixing process, and this reaction reaches its maximum at a dump temperature around 135–150 °C. This premature cross-linking reaction dominates over the breakdown of rubber chains and silica structures.



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935



Citation: Rubber Chemistry and Technology 85, 2; 10.5254/rct.12.88935
As seen from Figure 5, the viscosities of the silanized silica-filled NR compounds tend to decrease again at dump temperatures above 150 °C. This may be attributed to an optimum degree of silica–rubber and rubber–rubber interactions/reactions induced by the TESPT. Furthermore, degradation of rubber chains and/or polysulfide linkages becomes prominent. This observation also can be confirmed by the change of bound rubber content in the compounds (Figure 9). The chemically bound rubber reaches a plateau at a dump temperature of approximately 135 °C, indicating that the silica–silane–rubber and rubber–rubber interactions/reactions remain intact at higher temperature and shear force. Meanwhile, the physically bound rubber content in the compounds prepared at dump temperatures over 150 °C decreases somewhat, suggesting a reduction of chain entanglements or the physical network of rubber molecules due to a chain shortening by the degradation reaction.
The mixing of silica–silane and NR cannot avoid this premature cross-linking when TESPT is used as coupling agent, since the NR starts to react with sulfur present in TESPT at a temperature as low as 120 °C (Figure 13). The increased Mooney viscosity is normally an undesired processing property since it leads to processing difficulties in extrusion and calendering. Surprisingly, this phenomenon does not have an adverse effect on other properties of the compounds and vulcanizates. As illustrated in Figure 6, even better cure characteristics were obtained for compounds prepared with higher dump temperature, as indicated by the faster cure rate and longer scorch time. The improvement in cure behavior could be the result of better silanization so that all silica surfaces are well covered with silane resulting in less acidity and polarity, which in turn prevents a reduction of cure retardation and accelerator adsorption. Furthermore, when DPG is used in the recipe to enhance the silanization reaction22 as well as to act as a secondary accelerator, the higher level of silanization could also mean that a smaller portion of CBS is adsorbed on the still uncovered silica surface, so that this accelerator is more efficiently used for the curing. The improvement of the mechanical properties with increasing dump temperature to the optimum point, that is, in the range of 135–150 °C, especially in terms of reinforcement index (M300/M100) and tear resistance (Figure 11), is accounted for by a better silica dispersion in the NR as indicated by reinforcement parameter (αF), flocculation rate constant (ka), and Payne effect of the compounds in Figures 7, 8, and 10, respectively. This also corresponds with the higher bound rubber content, which indicates a better filler–rubber interaction. The lightly cross-linked network formed at the later stage of mixing restricts the movement of dispersed silica particles. As a consequence, the reagglomeration of silica is reduced, as depicted by a decrease of the flocculation rate constant (Figure 8). The results of this present work show a good agreement with the work reported by Lin et al.,23 in which the compounds comprising of TESPT showed a reduction of silica flocculation when they were mixed at higher dump temperature. Based on the present results, reagglomeration of silica/TESPT-filled NR compounds can be effectively suppressed when sufficiently high mixing temperature is used. This is due not only to better silica dispersion, higher degree of hydrophobation, and greater extent of polymer-filler interaction, but also to the lightly cross-linked network as a result of a small amount of cross-linking during mixing.
The tan δ at 60 °C, a measure of rolling resistance of tires based on silica-filled NR, is shown to improve when the compound dump temperatures are increased, and the optimum temperature is also in a range of 135–150 °C, in agreement with all other properties.
Based on our investigations on the reinforcement parameter, flocculation rate constant, bound rubber content, Payne effect, loss tangent at 60 °C (indication for rolling resistance), and mechanical properties, the optimal mixing conditions for silica-filled NR with TESPT as a coupling agent are a dump temperature in the range of 135–150 °C and 10 min mixing interval of silica–silane–rubber after mastication and before the addition of the other ingredients: ZnO, stearic acid, TMQ, and DPG. The decrease of reinforcement parameter, flocculation rate constant, and Payne effect combined with the increase of bound rubber content can be taken as a proof for proper silanization. However, it is worth emphasizing that the change of Mooney viscosity with dump temperature is different for the NR and SBR cases when TESPT is used. The Mooney viscosity of silica-filled NR compound increases as a result of sulfur in the TESPT to the maximum and thereafter decreases at higher temperatures as NR degradation starts to take place.
CONCLUSIONS
Varying initial mixer temperature settings from 50 to 140 °C and mixing intervals from 5 to 20 min for the silica-filled NR compounds leads to dump (end) temperatures in a range of 90 to 170 °C. The properties of both compounds and vulcanizates show a strong dependence on dump temperature, since the silanization reaction and silica dispersion are key parameters in this system. The optimal mixing conditions for the silica-filled NR compound with TESPT as a coupling agent are a dump temperature in the range of 135–150 °C and 10 min mixing interval of silica–silane–rubber prior to addition of the other ingredients: ZnO, stearic acid, TMQ, and DPG. Mixing performed up to dump temperatures above 150 °C leads to a decrease in vulcanizate properties as a result of NR degradation. During mixing of silica-filled NR compounds with TESPT as a coupling agent, it is evident that in addition to the silanization reaction, premature cross-linking reactions take place since NR can start to react with sulfur coming from TESPT molecules at a temperature as low as 120 °C. However, this phenomenon does not have an adverse effect on the vulcanizate properties.

Dump temperature as a function of initial mixer temperature setting for gum- and silica-filled NR compounds, with 10 min mixing interval for silica + silane and rubber.

Dump temperature as a function of silica–silane–rubber mixing interval for gum- and silica-filled NR compounds. The initial mixer temperature settings varied from 50 to 70 °C, as indicated.

Mixing torques for silica-filled NR compounds prepared with various mixer temperature settings, as indicated for each line. The silica–silane–rubber total mixing interval was 10 min.

Correlation between the mixer temperature setting, mixer torque, and dump temperature of silica-filled NR compounds at 300, 720, and 890 s when a 10 min silica–silane–rubber mixing interval was used.

Effect of (a) dump temperature and (b) silica–silane–rubber mixing interval on Mooney viscosity of gum- and silica-filled NR compounds; parameter: initial temperature settings of mixer.

Effect of dump temperature on (a) scorch time, optimum cure time, cure rate index and (b) rheometer minimum torque of silica-filled NR compounds.

Effect of dump temperature on reinforcement parameter of silica-filled NR compounds prepared with various silica–silane–rubber mixing intervals.

Effect of dump temperature on flocculation rate constant of silica-filled NR compounds prepared with various silica–silane–rubber mixing intervals.

Influence of dump temperature on bound rubber contents of silica-filled NR compounds: (a) total (untreated with NH3) and chemically bound rubber (treated with NH3) and (b) physically bound rubber content.

Influence of dump temperature on dynamic properties: (a) Payne effect; and (b) tan δ at 60 °C (frequency 10 Hz) of silica-filled NR vulcanizates prepared with various silica–silane–rubber mixing intervals.

Effect of dump temperature and silica–silane–rubber mixing interval on mechanical properties of silica-filled NR vulcanizates: (a) tensile strength; (b) elongation at break; (c) reinforcement index; and (d) tear resistance.

Cure characteristics of (a) NR and (b) SBR compounds, in the presence of TESPT (5.0 phr) and DPG (1.5 phr) at different cure temperatures.

Rheometer torque difference of NR and SBR compounds as a function of cure temperature in the presence of TESPT (5.0 phr) and DPG (1.5 phr).
Contributor Notes