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Rubber network

Figure 11.15. Typical chemical groupings in a sulphur-vulcanised natural rubber network, (a) Monosulphide cross-link (b) disulphide cross-link (c) polysulphide cross-link (j = 3-6) (d) parallel vicinal cross-link (n = 1-6) attached to adjacent main-chain atoms and which have the same influence as a single cross-link (e) cross-links attached to common or adjacent carbon atom (f) intra-chain cyclic monosulphide (g) intra-chain cyclic disulphide (h) pendent sulphide group terminated by moiety X derived from accelerator (i) conjugated diene (j) conjugated triene (k) extra-network material (1) carbon-carbon cross-links (probably absent)... Figure 11.15. Typical chemical groupings in a sulphur-vulcanised natural rubber network, (a) Monosulphide cross-link (b) disulphide cross-link (c) polysulphide cross-link (j = 3-6) (d) parallel vicinal cross-link (n = 1-6) attached to adjacent main-chain atoms and which have the same influence as a single cross-link (e) cross-links attached to common or adjacent carbon atom (f) intra-chain cyclic monosulphide (g) intra-chain cyclic disulphide (h) pendent sulphide group terminated by moiety X derived from accelerator (i) conjugated diene (j) conjugated triene (k) extra-network material (1) carbon-carbon cross-links (probably absent)...
Vulcanization changes the physical properties of rubbers. It increases viscosity, hardness, modulus, tensile strength, abrasion resistance, and decreases elongation at break, compression set and solubility in solvents. All those changes, except tensile strength, are proportional to the degree of cross-linking (number of crosslinks) in the rubber network. On the other hand, rubbers differ in their ease of vulcanization. Since cross-links form next to carbon-carbon double bonds. [Pg.638]

Langley, N.R. and Polmanteer, K.E., Relation of elastic modulus to crosslink and entanglement concentrations in rubber networks. J. Polym. Sci. Polym. Phys. Ed., 12(6), 1023-1034 (1974). [Pg.708]

Miscibility or compatibility provided by the compatibilizer or TLCP itself can affect the dimensional stability of in situ composites. The feature of ultra-high modulus and low viscosity melt of a nematic liquid crystalline polymer is suitable to induce greater dimensional stability in the composites. For drawn amorphous polymers, if the formed articles are exposed to sufficiently high temperatures, the extended chains are retracted by the entropic driving force of the stretched backbone, similar to the contraction of the stretched rubber network [61,62]. The presence of filler in the extruded articles significantly reduces the total extent of recoil. This can be attributed to the orientation of the fibers in the direction of drawing, which may act as a constraint for a certain amount of polymeric material surrounding them. [Pg.598]

A rubber network which is deformed to three independent extension ratios Xt, X2 and X3 takes the form of a biaxially oriented aggregate defined by coefficients P,mo. For example, we have... [Pg.98]

Fig. 3a. P200 and P400 as a function of draw ration for the pseudo-affine deformation scheme (uniaxially oriented sample) b P20o and P400 as a function of draw ratio X for the rubber network affine deformation scheme (N = 6, uniaxially oriented sample). Reproduced from Journal of Polymer Science by permission of the publishers, John Wiley Sons Incs (C)... Fig. 3a. P200 and P400 as a function of draw ration for the pseudo-affine deformation scheme (uniaxially oriented sample) b P20o and P400 as a function of draw ratio X for the rubber network affine deformation scheme (N = 6, uniaxially oriented sample). Reproduced from Journal of Polymer Science by permission of the publishers, John Wiley Sons Incs (C)...
Such considerations appear to be very relevant to the deformation of polymethylmethacrylate (PMMA) in the glassy state. At first sight, the development of P200 with draw ratio appears to follow the pseudo-affine deformation scheme rather than the rubber network model. It is, however, not possible to reconcile this conclusion with the temperature dependence of the behaviour where the development of orientation reduces in absolute magnitude with increasing temperature of deformation. It was proposed by Raha and Bowden 25) that an alternative deformation scheme, which fits the data well, is to assume that the deformation is akin to a rubber network, where the number of cross-links systematically reduces as the draw ratio is increased. It is assumed that the reduction in the number of cross-links per unit volume N i.e. molecular entanglements is proportional to the degree of deformation. [Pg.99]

Consequently, the measurement of three spectra and the determination of a from the isotropic sample allow calculation of (P2) and (P4). This method has been applied successfully to PET [53] and rubber networks [52], and to study the... [Pg.316]

For a moderately crossllnked network, equation (13) predicts a declining stress with lamellae formation from the amorphous melt. A stress Increase can be achieved with this model only by reorientation of the chain axis to the directions perpendicular (or nearly so) to the stress direction. If then this model is suitable for lightly crystalline materials, its behavior is in good accord with the observations of Luch and Yeh (6) on stretched natural rubber networks. They reported simultaneous lamellae formation and declining network stress. [Pg.303]

Approximative Methods for the Evaluation of Equilibrium Moduli of Relaxing Rubber Networks... [Pg.517]

The time and temperature dependent properties of crosslinked polymers including epoxy resins (1-3) and rubber networks (4-7) have been studied in the past. Crosslinking has a strong effect on the glass transition temperature (Tg), on viscoelastic response, and on plastic deformation. Although experimental observations and empirical expressions have been made and proposed, respectively, progress has been slow in understanding the nonequilibrium mechanisms responsible for the time dependent behavior. [Pg.124]

Tristar polybutadienes prepared by the intermediacy of lithium acetal initiators were also converted to three dimensional networks in a liquid rubber formulation using a diisocyanate curing agent. Table IV shows normal stress-strain properties for liquid rubber networks at various star branch Hn s. It can be seen that as the branch Mn increases to 2920, there is a general increase in the quality of the network. Interestingly, the star polymer network with a star branch Mn of 2920 (Mc=5840) exhibits mechanical properties in the range of a conventional sulfur vulcani-zate with a Me of about 6000-8000. [Pg.434]

Kramer,O., Greco,R., Ferry,J.D. Viscoelastic properties of butyl rubber networks containing reptating polyisobutylene. Paper presented at the San Diego meeting of the American Physical Society, March, 1973. [Pg.176]

Some further remarks concerning the Mooney-Rivlin equation are in place (14, 112). In dry rubber networks Ca in extension is often of the same order of magnitude as Cx, so that we are by no means confronted with a minor correction. In unilateral compression C2 is almost zero, and perhaps slightly negative. The constant Cx increases with the crosslinking density and with the temperature the ratio C2/C( in extension seems... [Pg.60]

Bobear, W. J. Chain density in rubber networks. Rubber Chem. Technol. 40, 1560 (1967). [Pg.95]

In homogeneous networks such as that of crosslinked rubber, the equilibrium degree of swelling qm depends on the molecular weight of the network chain Mc, satisfying the following relation for a given rubber network-solvent system [56],... [Pg.103]

The spin-lattice relaxation process is usually exponential. Theoretically, the effect of spin-diffusion, characterized by the coefficient D (order of 1(T12 cm2 s 1), has an influence on T, relaxation times when ix > L2/D, where Lis the diffusion path length. NMR studies of model systems f6r rubber networks, based on a styrene-butadiene-styrene block copolymer (SBSy, in which styrene blocks act as a crosslink for polybutadiene rubber segments of known and uniform length, indicate that spin diffusion operating between PS and PB phases causes a lowering of Tg for the PS component in SBS (as compared to the pure PS) and hindering of the motion of the PB component (as compared to the pure PB)51). [Pg.21]

Under suitable conditions when viscous flow is not dominant, it has been proposed that the reactions within the rubber network may be related to stress changes as follows. [Pg.304]

With an unaccelerated sulfur-natural-rubber system, the poor crosslinking efficiency results m sulfur being incorporated into the rubber network as long polysulfide crosslinks, cyclic monosulfides, and vicinal crosslinks, which are very close together and act physically as a single cross-link (see Fig. 2). [Pg.1450]

Figure 7.11 Double-quantum images of a strained rubber band with a cut (a) image, (b) 2H image of deuterated spy molecules incorporated into the rubber network by swelling, (c) finite element simulation of the stress distribution... Figure 7.11 Double-quantum images of a strained rubber band with a cut (a) image, (b) 2H image of deuterated spy molecules incorporated into the rubber network by swelling, (c) finite element simulation of the stress distribution...

See other pages where Rubber network is mentioned: [Pg.98]    [Pg.98]    [Pg.80]    [Pg.797]    [Pg.518]    [Pg.519]    [Pg.521]    [Pg.523]    [Pg.525]    [Pg.527]    [Pg.529]    [Pg.531]    [Pg.53]    [Pg.161]    [Pg.44]    [Pg.199]    [Pg.104]    [Pg.115]    [Pg.104]    [Pg.87]    [Pg.53]    [Pg.304]    [Pg.98]    [Pg.539]    [Pg.46]    [Pg.87]    [Pg.209]   
See also in sourсe #XX -- [ Pg.303 ]

See also in sourсe #XX -- [ Pg.601 ]




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Affine network model, rubber elasticity

Cavitation rubber network

Double networking cured rubber

Double networking rubber

Fibrillation, rubber network

Filled rubbers network structure

Network Structure in Oil-Extended Rubbers - Effect of Chain Entanglements

Network theory, rubber elasticity

Polymer networks rubber reinforcement theories

Relaxing rubber networks

Rubber elasticity cross-linked polymer network

Rubber elasticity phantom network

Rubber elasticity swollen networks

Rubber elasticity temporary networks

Rubber elasticity three-dimensional network

Rubber elastomeric networks

Rubber interpenetrating networks

Rubber network elasticity

Rubber network structure

Rubber network toughening

Rubber particles network cavitation

Rubber-like networks

Styrene-butadiene rubber network structure

Subject rubber network

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