The Reinforcement of Rubber by Resins

1962 ◽  
Vol 35 (5) ◽  
pp. 1308-1341 ◽  
Author(s):  
Jean LeBras

Abstract According to the partial conclusions drawn from the results given in each of the three chapters of this review, one can say that the question of reinforcement by resins, if it has not yet attained the aims sought for, has accumulated a great deal of useful information and now seems in a position to make rapid progress. The most significant point that seems to emerge is the necessity for the establishment of strong chemical bonds between the resin particle and the elastomer. This is undoubtedly not sufficient, and other characteristics of the particle must also intervene; but we have said above that one could now imagine a systematic study of the influence of these characteristics, and we need not return to it here. Many questions are still posed and the investigator will have the task of answering them. We consider it important to insist, however, in this conclusion, on some very recent results which it seemed preferable to us to mention here rather than to incorporate them in the text. In fact, they will either bring a confirmation on the influence of chemical bonds or show the possibility of preparing rubbers which should lend themselves remarkably well to this kind of reinforcement. In studying the crosslinking phenomena that involve the well known hardening of dry natural rubber on storage, Sekhar has shown that reactive groups are present as in integral part of the polyisoprene chain when it leaves the tree. These reactive groups have the characteristic property of carbonyl groups or, more specifically, aldehyde groups. They are responsible for crosslinking of the rubber molecules, and reactive monofunctional amines or other carbonyl reagents are capable of inhibiting this crosslinking effectively. From the critical concentration of reagent required to inhibit hardening, one has to postulate the presence of 9 to 29 aldehyde groups per polyisoprene molecule, assuming a molecular weight of 1,000,000). Because of the presence of these aldehyde groups on the chain of the rubber hydrocarbon, one was led logically to suppose that molecules of aminoplast resins formed in the latex might be fixed chemically on the rubber through the aid of these groups. This is what Sekhar and Angove realized with hydrazine-formalde-hyde resins. At a concentration of 5% and less of resin based on rubber, the latex remained fluid with no tendency to gel. Films and foam rubbers prepared from such resin latex showed considerable reinforcement: thus for a 3% resin content, for example, the tensile strength of a latex film passes from 285 kg/cm2 for the control to 362 kg/cm2 (the elongation in both cases being 925%), the 600% modulus from 32 to 75 kg/cm2, the tear resistance from 64 to 100 kg/cm. It is therefore with the greatest interest that one should consider such reinforcement results obtained with such a small proportion of resin; they emphasize the very important part that must be played by a strong chemical bond between the filler particle and the elastomer. It is evident, however, that the small proportion of aldehyde groups present on the rubber molecule limits the possibilities of such a fixation and must not permit to obtain the maximal reinforcing effects. That is why it seems necessary to pay a great attention to the reaction of glyoxal on rubber, which is endowing this latter with aldehyde-α alcohol side groups and gives it the reactivity toward the resins that seems to be desirable. We may therefore think that the years to come will bring into this field new and useful results, with a view toward the improvement of the characteristics of vulcanized rubber and ever-widening development of its application.

1953 ◽  
Vol 26 (4) ◽  
pp. 759-763 ◽  
Author(s):  
B. Dogadkin ◽  
Z. Tarasova

Abstract According to the hypotheses developed by the authors, vulcanized rubber is a system in which the molecular chains are united by local molecular and chemical bonds of varying intensity. The concentration, distribution, and strength of these bonds determine the principal physical and mechanical properties of the vulcanizates. Consequently the study of the structure of the vulcanizate is of primary practical value. The explanation of the nature of the bonds in a vulcanizate by chemical methods is very difficult, mainly because of the impossibility of distinguishing the specific chemical groups which enter into the composition of the different molecular chains from those bonds between the chains which are responsible for the development of spatial structures. From this view point, the thermo-mechanical method described below, which is based on the study of stress relaxation at different temperatures, is of great significance. As was shown by Dogadkin and Reznikovskii˘, the delayed stress relaxation in a vulcanizate at temperatures up to 70° C is caused by rupture of the local intermolecular bonds and the regrouping of the structural elements of the polymeric chains without destruction of the chemical bonds between them. Accordingly, after some time at these temperatures, a practically balanced stress is established, which depends on the number of the stronger bonds remaining. At temperatures above 70° C, rupture of the chemical bonds between the chains takes place; its speed increases with decrease of the energy activating the rupture of the given type of bond. Particularly in the case of sulfur vulcanizates, we can assume that the following types of bonds exist between the chains of the rubber: (1) —C—C—, which develop as a result of the polymerizationprocesses; (2) —C—S—C— monosulfide; (3) —C—S—S—C— disulfide, and (4) —C—Sn—C— polysulfide, formed as a result of the direct participation of the vulcanizing agent, sulfur, in the process of joining of the molecular chains. The energy of these chains can be estimated as 62.7 kcal, per mole for C—C, 54.5 kcal. per mole for C—S, and 27.5 kcal. per mole for the —S—S bond. Naturally, the heat stability of a vulcanizate will depend on which of the indicated types of bonds predominates.


Holzforschung ◽  
2010 ◽  
Vol 64 (5) ◽  
Author(s):  
Tuula Lehtimaa ◽  
Susanna Kuitunen ◽  
Ville Tarvo ◽  
Tapani Vuorinen

Abstract The role of chlorine (III) compounds, i.e. chlorous acid (HClO2) and chlorite (ClO2 -), in chlorine dioxide bleaching were investigated by treating different pulps with Cl(III). It was discovered that in addition to its fully inorganic reactions, chlorous acid is consumed by organic structures present in the pulp. These structures were assumed to be aldehydes. The aldehydes might exist already in unbleached pulps, but chlorine dioxide bleaching was also found to generate new aldehyde groups. The reactive groups were concluded to originate both from carbohydrates and lignin.


1961 ◽  
Vol 34 (2) ◽  
pp. 493-505 ◽  
Author(s):  
F. Bueche

Abstract The physical phenomena now widely known as the “Mullins effect” was apparently first studied in detail by Holt in about 1930. He showed that if a vulcanized rubber which contains carbon black is stretched to a relative elongation αm=L/L0 and released, it will not follow the same stress-strain curve when it is stretched once again to this same elongation. Instead, the rubber appears much softer on the second stretch for elongations below αm. Holt examined this behavior in some detail and showed that additional pre-stretches to αm softened the rubber further, but to a lesser degree than was observed on the first prestretch. In addition, Holt showed that the rubber regains a portion of its stiffness if allowed to rest in the relaxed state. Although this recovery was very slow at room temperature, up to about 50% recovery was noted after about an hour at 100° C. Similar softening effects were noted in gum stocks at exceedingly high elongations, but the effects were much less marked than in the filled stocks. This same effect was examined in more detail by Mullins after 1940. His results confirmed and greatly extended the earlier results of Holt. In addition, Mullins speculated about the mechanisms involved but came to no definite conclusion in that regard. Later, however, he and Tobin presented a phenomenological theory for the effect wherein they considered the rubber to be composed of hard and soft regions. They showed that their data could be described by assuming that some fraction of the hard regions became soft after a prestretch. No definite molecular basis for this process was proposed by Mullins and Tobin, although they speculated that either the breaking up of filler particle aggregates or the breaking loose of rubber to filler bonds might be involved. Later work by Blanchard and Parkinson confirmed and extended the data of Holt and Mullins. Further, these authors concluded that the softening was due to the breaking of rubber to filler bonds. They incorporated this idea into a semiempirical theory which agreed with their experiments. In addition, they obtained what they believed to be a distribution for the strength of the rubber-filler bonds. It will be seen in that which is to follow that their distribution probably does not represent what they thought it did, even though their basic ideas were correct.


1960 ◽  
Vol 33 (4) ◽  
pp. 953-958
Author(s):  
G. L. Slonimskiĭ ◽  
G. P. Drugova

Abstract 1. The basis of the process of ply separation of multiply rubber articles under repeated deformations is fatigue of the material in the region of the joint of the plies, which is a mechanochemical process, as previously studied, consisting of the development of chain chemical processes initiated by free radicals which are formed in the mechanical scission of chemical bonds in the molecules. 2. By the addition of substances inhibiting chain radical processes to the polymer it is possible to raise considerably the strength of the bond between elements of multiply vulcanized rubber articles.


Under repeated stressing, cracks in a specimen of vulcanized rubber may propagate and lead to failure. It has been found, however, that below a critical severity of strain no propagation occurs in the absence of chemical corrosion. This severity defines a fatigue limit for repeated stressing below which the life can be virtually indefinite. It can be expressed as the energy per unit area required to produce new surface ( T 0 ), and is about 5 x 10 4 erg/cm 2 . In contrast with gross strength properties such as tear and tensile strength, T 0 does not correlate with the viscoelastic behaviour of the material and varies only relatively slightly with chemical structure. It is shown that T 0 can be calculated approximately by considering the energy required to rupture the polymer chains lying across the path of the crack. This energy is calculated from the strengths of the chemical bonds, secondary forces being ignored. Theory and experiment agree within a factor of 2. Reasons why T 0 and the gross strength properties are influenced by different aspects of the structure of the material are discussed.


1983 ◽  
Vol 56 (1) ◽  
pp. 210-225 ◽  
Author(s):  
A. Y. Coran ◽  
R. Patel

Abstract Nylon resins and CPE rubber can be melt-blended to give compositions which have useful properties. If the rubber is cured by dynamic vulcanization, high strength oil resistant thermoplastic elastomers result. Cold milling of melt-mixed compositions results in nylon-reinforced rubber which can be mixed with curatives and press cured or statically vulcanized to give reinforced rubber compositions which resemble vulcanized rubber-short fiber composites. The reason for the high integrity of either the statically or the dynamically vulcanized composition appears to be that chemical bonds form between the rubber and plastic.


1963 ◽  
Vol 36 (2) ◽  
pp. 365-376 ◽  
Author(s):  
V. V. Lavrentev

Abstract a) The true static friction of vulcanized rubber is in practice immeasurably small (equal to zero, according to theory). b) The static friction as usually determined is an initial friction force. c) The initial friction force is equal to the sliding friction force in accelerated movement. It depends on the contact time, the rate of growth of the tangential force and the other conditions of experiment. d) With long contact times, particularly at higher temperatures, strong chemical bonds are formed between the vulcanized rubber and the track, leading to true static friction. e) The theoretical law of friction agrees well with the experimental results over the whole range of normal pressures. f) Good approximations are given in the range of low normal pressures by Coulomb's law (5) and in the rubber of high normal pressures by that of Thirion (7).


1940 ◽  
Vol 13 (1) ◽  
pp. 48-48 ◽  
Author(s):  
P. A. Thiessen ◽  
W. Kirch

Abstract Crystallization can be brought about in weakly vulcanized rubber by the method described by Thiessen and Kirsch for natural rubber. When samples of this type of vulcanized rubber were exposed to x-rays below + 6° C, but not under pressure, then Debye-Scherrer diagrams corresponding to those of a crystallized latex film were obtained. To determine the influence of pressure on these vulcanizates, samples were subjected to pressure on all sides in the chambers of the pressure apparatus described in the earlier work. After having been exposed for 100 days the sample which had been kept at + 6° C under 30 atmospheres' pressure showed a very marked Debye-Scherrer diagram, whereas samples kept at the same temperature but at normal pressure showed only the halo of an amorphous substance. Consequently pressure has an influence on the crystallization of vulcanized rubber as well as of raw rubber. The melting point of the crystalline phase lies between + 11° C. and +13° C. Obviously then an increase in pressure raises the temperature range of supercooling.


1989 ◽  
Vol 62 (1) ◽  
pp. 143-156 ◽  
Author(s):  
Gary R. Hamed ◽  
S. Hatfield

Abstract A simple model of filler dispersion has been used to approximate particle spacing and the portion of rubber that is restricted as a result of particulate reinforcement. For N330 black, which has an equivalent radius of 20.2 nm, the critical concentration (in SBR of Mw=344 000) for coherent carbon-gel formation upon solvent immersion is 30 phr. At this level of filler, particle-particle spacing is approximately the diameter of the average SBR random coil. In the second part of the study, compositions in which portions of free rubber had been extracted were compared to conventional mixes at the same black concentrations. Conventional and extracted vulcanizates had similar cure behavior and resistance to deformation, however, extracted samples, with excessive bound rubber had reduced strengths, consistent with the presence of inherent flaws. Apparently, the extracted samples, which are torn apart upon mastication are unable to fully reknit together even after compression molding and vulcanization.


1957 ◽  
Vol 30 (2) ◽  
pp. 689-704
Author(s):  
Joseph Green ◽  
E. F. Sverdrup

Abstract Scrap vulcanized rubber has been used principally for the manufacture of reclaimed rubber, which exhibits properties inherent in the original polymers of the scrap. Little has been found in the literature on the utilization of scrap vulcanized rubber as a low-cost starting material for controlled polymer synthesis. In the present investigation scraps containing natural and Type S synthetic rubbers have been modified to produce chemically different polymers possessing properties not usually associated with the initial elastomers. The authors believe that reactions with vulcanized rubber are not usually the same as reactions with the raw polymers and in this work the physical means of accomplishing the reaction are different. In 1938 Bacon and Farmer reported that when masticated raw natural rubber and maleic anhydride were dissolved in a solvent and the solution was heated in the presence of benzoyl peroxide, the ingredients reacted, yielding a variety of tough, fibrous, or resinous products. When vulcanized natural and Type S synthetic rubber scraps were reclaimed in a Reclaimator (a specially designed extruder type plasticator, made by the U. S. Rubber Reclaiming Co., Inc.) in the presence of a critical concentration of certain activated unsaturated compounds, a reaction occurred between the unsaturated compound and the scrap vulcanized rubber. With maleic anhydride, the resulting product was a carboxylated and replasticized rubber. This elastomer exhibited vulcanizing versatility via the carboxyl groups—i.e., curing with bivalent metallic oxides, diamines, glycols, epoxy resins, and diisocyanates. The polarity imparted by the carboxyl groups and the degree of crosslinking of the polymer appear responsible for its oil resistance, a property not normally present in a tire reclaim. The blocking of the double bonds, either by reaction at the double bond or by steric hindrance, added to the good aging properties anticipated with nonsulfur vulcanizates.


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