1402:) and the force extension models, it is possible to devise numerical algorithms to both construct a faithful representative volume element of a network and to simulate the resulting mechanical stress as it is subjected to strain. An iterative relaxation algorithm is used to maintain approximate force equilibrium at each network node as strain is imposed. When the force constant obtained for kinks having 2 or 3 isoprene units (approximately one Kuhn length) is used in numerical simulations, the predicted stress is found to be consistent with experiments. The results of such a calculation are shown in Fig. 1 (dashed red line) for sulphur cross-linked natural rubber and compared with experimental data (solid blue line). These simulations also predict a steep upturn in the stress as network chains become taut and, ultimately, material failure due to bond rupture. In the case of sulphur cross-linked natural rubber, the S-S bonds in the cross-link are much weaker than the C-C bonds on the chain backbone and are the network failure points. The plateau in the simulated stress, starting at a strain of about 7, is the limiting value for the network. Stresses greater than about 7 MPa cannot be supported and the network fails. Near this stress limit, the simulations predict that less than 10% of the chains are taut, i.e. in the high chain extension regime and less than 0.1% of the chains have ruptured. While the very low rupture fraction may seem surprising, it is not inconsistent with the common experience of stretching a rubber band until it breaks. The elastic response of the rubber after breaking is not noticeably different from the original.
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unit within a kink into an extended conformation, slightly increasing the end-to-end distance of the chain, and the energy required to do this is less than that needed to continue extending all of the kinks simultaneously. Numerous experiments strongly suggest that stretching a rubber network is accompanied by a decrease in entropy. As shown in Fig. 2, an isoprene unit has three single C-C bonds and there are two or three preferred rotational angles (orientations) about these bonds that have energy minima. Of the 18 allowed rotational conformations, only 6 have extended end-to-end distances and forcing the isoprene units in a chain to reside in some subset of the extended states must reduce the number of rotational conformations available for thermal motion. It is this reduction in the number of available states that causes the entropy to decrease. As the chain continues to straighten, all of the isoprene units in the chain are eventually forced into extended conformations and the chain is considered to be "taut." A force constant for chain extension can be estimated from the resulting change in free energy associated with this entropy change. As with regime IA, the force model for this regime is linear and proportional to the temperature divided by the chain tortuosity.
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in the same manner as when it was stretched (i.e. uniformly). Experimental observations by Mrowca et al. suggest that this expectation is inaccurate. To capture the extremely fast retraction dynamics, they utilized an experimental method devised by Exner and Stefan in 1874. Their method consisted of a rapidly rotating glass cylinder which, after being coated with lamp black, was placed next to the stretched rubber sample. Styli, attached to the mid-point and free end of the rubber sample, were held in contact with the glass cylinder. Then, as the free end of the rubber snapped back, the styli traced out helical paths in the lamp black coating of the rotating cylinder. By adjusting the rotation speed of the cylinder, they could record the position of the styli in less than one complete rotation. The trajectories were transferred to a graph by rolling the cylinder on a piece of damp blotter paper. The mark left by a stylus appeared as a white line (no lamp black) on the paper.
476:, the ratio of its contour length to its end-to-end distance. As the chain is extended, in response to an applied strain, the induced elastic force is assumed to propagate uniformly along its contour. Consider a network chain whose end points (network nodes) are more or less aligned with the tensile strain axis. As the initial strain is applied to the rubber sample, the network nodes at the ends of the chain begin to move apart and all of the kink vectors along the contour are stretched simultaneously. Physically, the applied strain forces the kinks to stretch beyond their thermal equilibrium end-to-end distances, causing a decrease in their entropy. The increase in free energy associated with this change in entropy, gives rise to a (linear) elastic force that opposes the strain. The force constant for the low strain regime can be estimated by sampling
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displacement of 0 in) in a little over 6 Ms. The linear behaviour of the displacement vs. time indicates that, after a brief acceleration, both the end and the midpoint of the sample snapped back at a constant velocity of about 50 m/s or 112 mph. However, the midpoint stylus did not start to move until about 3 Ms after the end was released. Evidently, the retraction process travels as a wave, starting at the free end. At high extensions some of the energy stored in the stretched network chain is due to a change in its entropy, but most of the energy is stored in bond distortions (regime II, above) which do not involve an entropy change. If one assumes that all of the stored energy is converted to kinetic energy, the retraction velocity may be calculated directly from the familiar conservation equation
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lengths of the chains and most of them are not connected to the nearest neighbor network node. Both the chain length and its end-to-end distance are described by probability distributions. The term "morphology" refers to this complexity. If the cross-linking agent is thoroughly mixed, there is an equal probability for any isoprene unit to become a network node. For dicumyl peroxide, the cross linking efficiency in natural rubber is unity, but this is not the case for sulfur. The initial morphology of the network is dictated by two random processes: the probability for a cross-link to occur at any isoprene unit and the Markov random walk nature of a chain conformation. The probability distribution function for how far one end of a chain end can βwanderβ from the other is generated by a Markov sequence. This
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on the surroundings results in the disappearance of thermal energy in order to do the work (the elastic band grows cooler, like an expanding gas). This last phenomenon is the critical clue that the ability of an elastomer to do work depends (as with an ideal gas) only on entropy-change considerations, and not on any stored (i.e. potential) energy within the polymer bonds. Instead, the energy to do work comes entirely from thermal energy, and (as in the case of an expanding ideal gas) only the positive entropy change of the polymer allows its internal thermal energy to be converted efficiently into work.
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480:(MD) trajectories of a kink (i.e. short chains) composed of 2β3 isoprene units, at relevant temperatures (e.g. 300K). By taking many samples of the coordinates over the course of the simulations, the probability distributions of end-to-end distance for a kink can be obtained. Since these distributions (which turn out to be approximately Gaussian) are directly related to the number of states, they may be associated with the entropy of the kink at any end-to-end distance. By numerically differentiating the probability distribution, the change in entropy, and hence
425:) network are constrained by surrounding chains to remain within a "tube." Elastic forces produced in a chain, as a result of some applied strain, are propagated along the chain contour within this tube. Fig. 2 shows a representation of a four-carbon isoprene backbone unit with an extra carbon atom at each end to indicate its connections to adjacent units on a chain. It has three single C-C bonds and one double bond. It is principally by rotating about the C-C single bonds that a polyisoprene chain randomly explores its possible conformations.
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1382:(52 Kuhn lengths) and has a contour length of about 50 nm. Fig. 3 shows that a significant fraction of chains span several node spacings, i.e., the chain ends overlap other network chains. Natural rubber, cross-linked with dicumyl peroxide, has tetra-functional cross-links (i.e. each cross-link node has 4 network chains emanating from it). Depending on their initial tortuosity and the orientation of their endpoints with respect to the strain axis, each chain associated with an active cross-link node can have a different elastic
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1607:. When the chain is stretched, the entropy is reduced by a large margin because there are fewer conformations available. As such there is a restoring force which causes the polymer chain to return to its equilibrium or unstretched state, such as a high entropy random coil configuration, once the external force is removed. This is the reason why rubber bands return to their original state. Two common models for rubber elasticity are the freely-jointed chain model and the worm-like chain model.
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3915:{\displaystyle {\begin{aligned}\Delta F_{\text{def}}({\vec {R}})&=-{\frac {3k_{\text{B}}T{\vec {R}}^{2}}{2Nb^{2}}}=-{\frac {3k_{\text{B}}T\left(\left(R_{x}^{2}-R_{x0}^{2}\right)+\left(R_{y}^{2}-R_{y0}^{2}\right)+\left(R_{z}^{2}-R_{z0}^{2}\right)\right)}{2Nb^{2}}}\\&=-{\frac {3k_{\text{B}}T\left(\left(\lambda _{x}^{2}-1\right)R_{x0}^{2}+\left(\lambda _{y}^{2}-1\right)R_{y0}^{2}+\left(\lambda _{z}^{2}-1\right)R_{z0}^{2}\right)}{2Nb^{2}}}\end{aligned}}}
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mechanics analysis of a large sample. There are no other examples of how entropy changes can produce a force in our everyday experience. One may regard the entropic forces in polymer chains as arising from the thermal collisions that their constituent atoms experience with the surrounding material. It is this constant jostling that produces a resisting (elastic) force in the chains as they are forced to become straight.
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284:) was regarded mostly as a curiosity. Its most useful application was its ability to erase pencil marks on paper by rubbing, hence its name. One of its most peculiar properties is a slight (but detectable) increase in temperature that occurs when a sample of rubber is stretched. If it is allowed to quickly retract, an equal amount of cooling is observed. This phenomenon caught the attention of the English physicist
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change times the absolute temperature. This rule is only valid so long as the energy is restricted to thermal states of molecules. If a rubber sample is stretched far enough, energy may reside in nonthermal states such as the distortion of chemical bonds and the rule does not apply. At low to moderate strains, theory predicts that the required stretching force is due to a change in entropy in the network chains.
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36:
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strain of a stretched rubber sample was held fixed as the temperature was varied between 10 and 70 degrees
Celsius. For each value of fixed strain, it is seen that the tensile stress varied linearly (to within experimental error). These experiments provide the most compelling evidence that entropy changes are the fundamental mechanism for rubber elasticity.
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4461:{\displaystyle {\begin{aligned}\Delta F_{\text{def}}({\vec {R}})&=-{\frac {k_{\text{B}}Tn_{s}\langle R^{2}\rangle \left(\lambda _{x}^{2}+\lambda _{y}^{2}+\lambda _{z}^{2}-3\right)}{2Nb^{2}}}\\&=-{\frac {k_{\text{B}}Tn_{s}\langle R^{2}\rangle \left(\lambda _{x}^{2}+\lambda _{y}^{2}+\lambda _{z}^{2}-3\right)}{2R_{0}^{2}}}\end{aligned}}}
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260:, or joined to each other by the bonds made with the cross-linking molecules. Because each rubber polymer is very long, each one participates in many crosslinks with many other rubber molecules, forming a continuous network. The resulting molecular structure demonstrates elasticity, making rubber a member of the class of elastic
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initial equilibrium contour length by the distortion of the chemical bonds along its backbone. In this case, the restoring force is spring-like and is referred to as regime II. The three force mechanisms are found to roughly correspond to the three regions observed in tensile stress vs. strain experiments, shown in Fig. 1.
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mechanisms that produce the elastic forces and the complex morphology of the network must be treated simultaneously, simple analytic elasticity models are not possible; an explicit 3-dimensional numerical model is required to simulate the effects of strain on a representative volume element of a network.
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At some point in the low extension regime (i.e. as all of the kinks along the chain are being extended simultaneously) it becomes energetically more favourable to have one kink transition to an extended conformation in order to stretch the chain further. The applied strain can force a single isoprene
462:
for a fixed chain length (i.e. fixed number of isoprene units) is described by a random walk. It is the joint probability distribution of the network chain lengths and the end-to-end distances between their cross-link nodes that characterizes the network morphology. Because both the molecular physics
360:
There are actually several physical mechanisms that produce the elastic forces within the network chains as a rubber sample is stretched. Two of these arise from entropy changes and one is associated with the distortion of the molecular bond angles along the chain backbone. These three mechanisms are
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Temperature affects the elasticity of elastomers in an unusual way. When the elastomer is assumed to be in a stretched state, heating causes them to contract. Vice versa, cooling can cause expansion. This can be observed with an ordinary rubber band. Stretching a rubber band will cause it to release
389:
of the network, it is not possible to obtain simple analytic formulae to predict the macroscopic stress. It is only via numerical simulations on computers that it is possible to capture the complex interaction between the molecular forces and the network morphology to predict the stress and ultimate
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which is concerned with the study of large thermal systems, e.g. rubber networks at room temperature. Although the detailed behavior of the constituent chains are random and far too complex to study individually, we can obtain very useful information about their "average" behavior from a statistical
330:
All of the polyisoprene molecules are connected together at multiple points by these chemical bonds (network nodes) resulting in a single giant molecule and all information about the original long polymers is lost. A rubber band is a single molecule, as is a latex glove. The sections of polyisoprene
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store any potential energy in stretched chemical bonds or elastic work done in stretching molecules, when work is done upon them. Instead, all work done on the rubber is "released" (not stored) and appears immediately in the polymer as thermal energy. In the same way, all work that the elastic does
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When stretching a piece of rubber (e.g. a rubber band) it will deform lengthwise in a uniform manner. When one end of the sample is released, it snaps back to its original length too quickly for the naked eye to resolve the process. An intuitive expectation is that it returns to its original length
1423:
For molecular systems in thermal equilibrium, the addition of energy (e.g. by mechanical work) can cause a change in entropy. This is known from the theories of thermodynamics and statistical mechanics. Specifically, both theories assert that the change in energy must be proportional to the entropy
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The complex morphology of a natural rubber network can be seen in Fig. 3, which shows the probability density vs. end-to-end distance (in units of mean node spacing) for an "average" chain. For the common experimental cross-link density of 4x10 cm, an average chain contains about 116 isoprene units
453:
There are three distinct molecular mechanisms that produce these forces, two of which arise from changes in entropy that is referred to as the low chain extension regime, Ia and the moderate chain extension regime, Ib. The third mechanism occurs at high chain extension, as it is extended beyond its
436:
Since a kink is composed of several isoprene units, each having three carbon-carbon single bonds, there are many possible conformations available to a kink, each with a distinct energy and end-to-end distance. Over time scales of seconds to minutes, only these relatively short sections of the chain
471:
The
Molecular Kink Paradigm envisions a representative network chain as a series of vectors that follow the chain contour within its tube. Each vector represents the equilibrium end-to-end distance of a kink. The actual 3-dimensional path of the chain is not pertinent, since all elastic forces are
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Their data, plotted as the graph in Fig. 5, shows the position of end and midpoint styli as the sample rapidly retracts to its original length. The sample was initially stretched 9.5 in (~24 cm) beyond its unstrained length and then released. The styli returned to their original positions (i.e. a
519:
simulations and it is approximately 7 nN, about a factor of a thousand greater than the entropic chain forces at low strain. The angles between adjacent backbone C-C bonds in an isoprene unit vary between about 115β120 degrees and the forces associated with maintaining these angles are quite
509:
When all of the isoprene units in a network chain have been forced to reside in just a few extended rotational conformations, the chain becomes taut. It may be regarded as sensibly straight, except for the zigzag path that the C-C bonds make along the chain contour. However, further extension is
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While stretching a rubber sample is the most common example of elasticity, it also occurs when rubber is compressed. Compression may be thought of as a two dimensional expansion as when a balloon is inflated. The molecular mechanisms that produce the elastic force are the same for all types of
1427:
It is therefore expected that the force necessary to stretch a sample to some value of strain should be proportional to the temperature of the sample. Measurements showing how the tensile stress in a stretched rubber sample varies with temperature are shown in Fig. 4. In these experiments, the
322:
backbone units, connected head-to-tail (commonly referred to as chains). Every chain follows a random, three-dimensional path through the polymer liquid and is in contact with thousands of other nearby chains. When heated to about 150C, reactive cross-linker molecules, such as sulfur or dicumyl
528:
Although the network is completely described by only two parameters (the number of network nodes per unit volume and the statistical de-correlation length of the polymer, the Kuhn length), the way in which the chains are connected is actually quite complicated. There is a wide variation in the
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and is determined by the
Boltzmann probability factors for each state (rotational conformation). As a rubber network is stretched, some kinks are forced into a restricted number of more extended conformations having a greater end-to-end distance and it is the resulting decrease in entropy that
334:
Because of the enormous economic and technological importance of rubber, predicting how a molecular network responds to mechanical strains has been of enduring interest to scientists and engineers. To understand the elastic properties of rubber, theoretically, it is necessary to know both the
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as it resists the applied strain. To preserve force equilibrium (zero net force) on each cross-link node, a node may be forced to move in tandem with the chain having the highest force constant for chain extension. It is this complex node motion, arising from the random nature of the network
364:
Initially, the rubber feels quite stiff (i.e. the force must be increased at a high rate with respect to the strain). At intermediate strains, the required increase in force is much lower to cause the same amount of stretch. Finally, as the sample approaches the breaking point, its stiffness
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428:
Sections of chain containing between two and three isoprene units have sufficient flexibility that they may be considered statistically de-correlated from one another. That is, there is no directional correlation along the chain for distances greater than this distance, referred to as a
514:
rotations. These forces are spring-like and are not associated with entropy changes. A taut chain can be extended by only about 40%. At this point the force along the chain is sufficient to mechanically rupture the C-C covalent bond. This tensile force limit has been calculated via
5232:{\displaystyle \Delta f_{\text{def}}={\frac {\Delta F_{\text{def}}({\vec {R}})}{V}}=-{\frac {k_{\text{B}}Tv_{s}\beta \left(\lambda _{x}^{2}+\lambda _{y}^{2}+\lambda _{z}^{2}-3\right)}{2}}={\frac {k_{\text{B}}Tv_{s}\beta }{2}}\left(\lambda _{z}^{2}+{\frac {2}{\lambda _{z}}}-3\right)}
437:(i.e. kinks) have sufficient volume to move freely amongst their possible rotational conformations. The thermal interactions tend to keep the kinks in a state of constant flux, as they make transitions between all of their possible rotational conformations. Because the kinks are in
299:
showed that the change in mechanical energy required to stretch a rubber sample should be proportional to the increase in temperature. This would later be associated with a change in entropy. The connection to thermodynamics was firmly established in 1859 when the
English physicist
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is the number average molecular weight of a network strand between crosslinks. Here, this type of analysis links the thermodynamic theory of rubber elasticity to experimentally measurable parameters. In addition, it gives insights into the cross-linking condition of the materials.
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morphology, that makes the study of the mechanical properties of rubber networks so difficult. As the network is strained, paths composed of these more extended chains emerge that span the entire sample, and it is these paths that carry most of the stress at high strains.
331:
between two adjacent cross-links are called network chains and can contain up to several hundred isoprene units. In natural rubber, each cross-link produces a network node with four chains emanating from it. It is the network that gives rise to these elastic properties.
767:
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The initial morphology of the network, immediately after chemical cross-linking, is governed by two random processes: (1) The probability for a cross-link to occur at any isoprene unit and, (2) the random walk nature of the chain conformation. The end-to-end distance
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1101:
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that are due to the different molecular mechanisms. These regions can be seen in Fig. 1, a typical stress vs. strain measurement for natural rubber. The three mechanisms (labelled Ia, Ib, and II) predominantly correspond to the regions shown on the plot.
1008:, shorter chains are more probable than longer ones. Note that the number of statistically independent backbone segments is not the same as the number of isoprene units. For natural rubber networks, the Kuhn length contains about 2.2 isoprene units, so
5248:
2631:
1395:
To calculate the elastic response of a rubber sample, the three chain force models (regimes Ia, Ib and II) and the network morphology must be combined in a micro-mechanical network model. Using the joint probability distribution in equation
1891:
4785:
which is the ratio between the end-to-end distance of the chain and the theoretical distance that obey random walk statistics. If we assume incompressibility, the product of extension ratios is 1, implying no change in the volume:
1621:
The freely joined chain, also called an ideal chain, follows the random walk model. Microscopically, the 3D random walk of a polymer chain assumes the overall end-to-end distance is expressed in terms of the x, y and z directions:
5632:{\displaystyle E={\frac {d(\sigma _{\text{eng}})}{d\lambda _{z}}}=k_{\text{B}}Tv_{s}\beta \left.\left(1+{\frac {2}{\lambda _{z}^{3}}}\right)\right|_{\lambda _{z}=1}=3k_{\text{B}}Tv_{s}\beta ={\frac {3\rho \beta RT}{M_{s}}}}
343:
chain defines the network. The physical mechanisms that occur within short sections of the polymer chains produce the elastic forces and the network morphology determines how these forces combine to produce the macroscopic
2527:
1734:
190:
refers to the ability of solid rubber to be stretched up to a factor of 10 from its original length, and return to close to its original length upon release. This process can be repeated many times with no apparent
601:
2329:{\displaystyle {\begin{aligned}\langle R\rangle &=0\\\langle R^{2}\rangle &=\int _{0}^{\infty }R^{2}4\pi R^{2}P({\vec {R}})dR=Nb^{2}\\\langle R^{2}\rangle ^{\frac {1}{2}}&={\sqrt {N}}b\end{aligned}}}
2635:
2103:
Therefore, the ensemble average end-to-end distance is simply the standard integral of the probability distribution over all space. Note that the movement could be backwards or forwards, so the net average
4967:
785:
The probability that any isoprene unit becomes part of a cross-link node is proportional to the ratio of the concentrations of the cross-linker molecules (e.g., dicumyl-peroxide) to the isoprene units:
520:
large, so within each unit, the chain backbone always follows a zigzag path, even at bond rupture. This mechanism accounts for the steep upturn in the elastic stress, observed at high strains (Fig. 1).
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is temperature dependent. If rubber temperature increases, the elastic coefficient increases as well. This is the reason why rubber under constant stress shrinks when its temperature increases.
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825:
1435:(i.e. the length of a sample shrinks when heated). Experiments have shown conclusively that, like almost all other materials, the coefficient of thermal expansion natural rubber is positive.
4008:
4644:{\displaystyle \Delta f_{\text{def}}={\frac {\Delta F_{\text{def}}({\vec {R}})}{V}}=-{\frac {k_{\text{B}}Tv_{s}\beta \left(\lambda _{x}^{2}+\lambda _{y}^{2}+\lambda _{z}^{2}-3\right)}{2}}}
1888:
changes over time. The probability distribution of the chain is the product of the probability distributions of the individual components, given by the following
Gaussian distribution:
2531:
2362:
is the number of conformations of the polymer chain. Since the deformation does not involve enthalpy change, the change in free energy can simply be calculated as the change in entropy
484:, with respect to the kink end-to-end distance can be found. The force model for this regime is found to be linear and proportional to the temperature divided by the chain tortuosity.
2993:{\displaystyle f={\frac {dF({\vec {R}})}{d{\vec {R}}}}={\frac {d}{d{\vec {R}}}}\left({\frac {3k_{\text{B}}T{\vec {R}}^{2}}{2Nb^{2}}}\right)={\frac {3k_{\text{B}}T}{Nb^{2}}}{\vec {R}}}
5695:
327:
between adjacent chains. A crosslink can be visualized as the letter 'X' but with some of its arms pointing out of the plane. The result is a three dimensional molecular network.
304:
published the first careful measurements of the temperature increase that occurred as a rubber sample was stretched. This work confirmed the theoretical predictions of Lord Kelvin.
1350:{\displaystyle P(r,N)\;=\;P(N)P(r|N)\;=\;p_{x}{\left(1-p_{x}\right)}^{N-1}\,4\pi r^{2}\left({\frac {2nb^{2}\pi }{3}}\right)^{-{3}/{2}}\exp \left(-{\frac {3r^{2}}{2nb^{2}}}\right)}
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6607:
Buche, M.R.; Silberstein, M.N. (2020). "Statistical mechanical constitutive theory of polymer networks: The inextricable links between distribution, behavior, and ensemble".
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5942:{\displaystyle F\approx {\frac {k_{\text{B}}T}{L_{\text{p}}}}\left({\frac {1}{4\left(1-{\frac {r}{L_{\rm {c}}}}\right)^{2}}}-{\frac {1}{4}}+{\frac {r}{L_{\text{c}}}}\right)}
4724:
491:
Fig. 2 Isoprene backbone unit. composed of carbon atoms (dark grey) and hydrogen atoms (white). Carbon atoms labeled '1' and '6' are in adjacent units on the polymer chain.
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heat, while releasing it after it has been stretched will lead it to absorb heat, causing its surroundings to become cooler. This phenomenon can be explained with the
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5380:{\displaystyle \sigma _{\text{eng}}={\frac {d(\Delta f_{\text{def}})}{\lambda _{z}}}=k_{\text{B}}Tv_{s}\beta \left(\lambda _{z}-{\frac {1}{\lambda _{z}^{2}}}\right)}
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are distributed according to a normal distribution. Therefore, they are equal in space, and all of them are 1/3 of the overall end-to-end distance of the chain:
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We can further expand the Flory theory into a macroscopic view, where bulk rubber material is discussed. Assume the original dimension of the rubber material is
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found that natural rubber's elastic properties could be immensely improved by adding a small amount of sulfur to produce chemical cross-links between adjacent
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and its discussion about entropy, the force generated from the deformation of a rubber chain from its original unstretched conformation can be derived. The
6392:
Anthony, R.L.; Caston, R.H.; Guth, E. (1942). "Equations of state for natural and synthetic rubber-like materials. I. Unaccelerated natural soft rubber".
445:
and we may associate an entropy with its end-to-end distance. The probability distribution for the end-to-end distance of a Kuhn length is approximately
386:
1377:
Fig. 3 Probability density for an average network chain vs. end-to-end distance in units of mean cross-link node spacing (2.9 nm); n= 52, b= 0.96 nm.
288:. In 1805 he published some qualitative observations on this characteristic as well as how the required stretching force increased with temperature.
2094:{\displaystyle P({\vec {R}})=P(R_{x})P(R_{y})P(R_{z})=\left({\frac {2nb^{2}\pi }{3}}\right)^{-{3}/{2}}\exp \left({\frac {-3R^{2}}{2Nb^{2}}}\right)}
2338:
The Flory theory of rubber elasticity suggests that rubber elasticity has primarily entropic origins. By using the following basic equations for
859:
413:
Fig. 1 Stress vs. tensile strain for a natural rubber network. Experimental data by
Treloar (solid blue), theoretical simulation (dashed red).
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5988:), an infinite force is required, which is intuitive. Graphically, the force begins at the origin and initially increases linearly with
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53:
5245:(by definition) is the first derivative of the energy in terms of the extension ratio, which is equivalent to the concept of strain:
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174:
119:
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433:. These non-straight regions evoke the concept of "kinks" and are in fact a manifestation of the random-walk nature of the chain.
5753:
The worm-like chain model (WLC) takes the energy required to bend a molecule into account. The variables are the same except that
6418:
L. A. Wood and G. Martin, Journal of
Research of the National Bureau of Standards-A. Physics and Chemistry Vol 68A, No. 3 (1964).
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assumed to operate along the chain contour. In addition to the chain's contour length, the only other important parameter is its
285:
100:
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The positive linear behaviour of the stress with temperature sometimes leads to the mistaken notion that rubber has a negative
762:{\displaystyle P(r|n)=4\pi r^{2}\left({\frac {2nb^{2}\pi }{3}}\right)^{-{3}/{2}}\exp \left(-{\frac {3r^{2}}{2nb^{2}}}\right)\,}
72:
1050:
57:
4850:
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2778:{\displaystyle \Delta F({\vec {R}})\approx -T\Delta S_{d}({\vec {R}}^{2})=C+{\frac {3k_{\text{B}}T}{Nb^{2}}}{\vec {R}}^{2}}
79:
6313:
D. E. Hanson and J. L. Barber, Modelling and
Simulation in Materials Science and Engineering 21 (2013), LAPR-2013-017962
4120:{\displaystyle \langle R_{x0}^{2}\rangle =\langle R_{y0}^{2}\rangle =\langle R_{z0}^{2}\rangle =\langle R^{2}\rangle /3}
459:
1419:
Fig. 4 Variation of tensile stress with temperature as strain held constant at four values (100%, 200%, 300% and 380%).
318:
Before it is cross-linked, the liquid natural rubber consists of very long polymer molecules, containing thousands of
226:. A rubber polymer follows a random winding path in three dimensions, intermingling with many other rubber polymers.
6674:
1473:. Numerical simulations, based on the molecular kink paradigm, predict velocities consistent with this experiment.
86:
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The factor of two comes about because two isoprene units (one from each chain) participate in the cross-link. The
46:
6008:. The force then plateaus but eventually increases again and approaches infinity as the chain length approaches
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68:
1447:
Fig. 5 Displacement of the end and midpoint of a rubber sample vs. time as it snaps back from high extension.
222:. This process builds polymers up by sequentially adding short molecular backbone units to the chain through
6679:
6475:
Guth, Eugene; James, Hubert M. (May 1941). "Elastic and
Thermoelastic Properties of Rubber like Materials".
5642:
349:
192:
1575:) than when it is under tension. Thus, when the tension is removed, the reaction is spontaneous, leading Ξ
442:
6049:
2339:
985:. The equation can be understood as simply the probability that an isoprene unit is NOT a cross-link (1β
487:
481:
374:
366:
6362:
Treloar, L.R.G. (1944). "Stress-Strain Data for
Vulcanized Rubber under Various Types of Deformation".
6237:
D. E. Hanson, J. L. Barber and G. Subramanian, Journal of Chemical Physics 139 (2013), LAPR-2014-018991
3345:
3308:
3271:
3234:
3197:
3160:
3005:
2107:
1603:
Invoking the theory of rubber elasticity, a polymer chain in a cross-linked network may be seen as an
6626:
6511:
6440:
6044:
1616:
1485:
203:
6465:
G. S. Whitby, "Plantation Rubber and the Testing of Rubber", Longmans and Green, London, 1920. p 461
5958:
417:
The Molecular Kink Paradigm proceeds from the intuitive notion that molecular chains that make up a
6249:
D. E. Hanson and R. L. Martin, The Journal of Chemical Physics 130, 064903 (2009), LAPR-2009-006764
4681:
446:
438:
211:
6161:
6011:
5756:
3268:). So microscopically, the deformed polymer chain can also be expressed with the extension ratio:
3133:
2626:{\displaystyle S=k_{\text{B}}\ln \Omega \,\approx {\frac {-3k_{\text{B}}{\vec {R}}^{2}}{2Nb^{2}}}}
1821:
6684:
6650:
6616:
5242:
477:
345:
207:
5388:
2365:
1011:
93:
6642:
6588:
6564:
6088:
2437:
1498:
516:
223:
2345:
1571:
must be negative, implying that the rubber in its natural state is more entangled (with more
962:
6634:
6519:
6484:
6448:
6401:
6371:
6211:
D. E. Hanson and J. L. Barber, Contemporary Physics 56 (3), 319β337 (2015), LAPR-2015-022971
308:
5720:
5700:
4654:
3981:
3954:
3927:
3106:
3079:
3052:
6543:
6223:
D. E. Hanson and R. L. Martin, Journal of Chemical Physics 133, 084903 (084908 pp.) (2010)
2398:
6630:
6536:
6515:
6444:
6343:
D. E. Hanson and J. L. Barber, Phys. Chem. Chem. Phys. 20, 8460 (2018), LAPR-2018-029488
6202:
Joule JP. On thermodynamic properties of solids. Phil Trans R Soc Lond. 1859;149:91β131.
1848:
6059:
5991:
5783:
5393:
2392:
1871:
1801:
1781:
1761:
1741:
1604:
1383:
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834:
576:
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536:
511:
418:
292:
277:
219:
295:
was being developedand within this framework, the English mathematician and physicist
6668:
6654:
2130:
will be zero. However, the root mean square can be a useful measure of the distance.
1587:
1564:
324:
253:
250:
242:
230:
6137:
6113:
510:
still possible by bond distortions (e.g. bond angle increases), bond stretches, and
3130:, a deformed shape can then be expressed by applying an individual extension ratio
1579:
to be negative. Consequently, the cooling effect must result in a positive ΞH, so Ξ
441:, the probability that a kink resides in any rotational conformation is given by a
361:
immediately apparent when a moderately thick rubber sample is stretched manually.
312:
281:
234:
5410:
is defined as derivative of the stress with respect to strain, which measures the
3924:
Assume that the rubber is cross-linked and isotropic, the random walk model gives
6261:
P. Flory, N. Rabjohn and M. Shaffer, Journal of Polymer Science 4, 435β455 (1949)
5955:=0), the force required to do so is zero, and to fully extend the polymer chain (
17:
6638:
1481:
430:
373:
The concept of entropy comes to us from the area of mathematical physics called
336:
301:
296:
35:
2440:
can be used on cross-linked polymers to predict their stress-strain relations:
2391:. Note that the force equation resembles the behaviour of a spring and follows
4678:
is the number of strands in network, the subscript "def" means "deformation",
3379:. The free energy change due to deformation can then be expressed as follows:
2522:{\displaystyle \Omega =C\exp \left({\frac {-3{\vec {R}}^{2}}{2Nb^{2}}}\right)}
473:
257:
6452:
6431:
Mrowca, B.A.; Dart, S.L.; Guth, E. (1944). "Retraction of stressed rubber".
6080:
5411:
276:
Following its introduction to Europe from America in the late 15th century,
265:
218:, or large, chain-like molecules. Polymers are produced by a process called
6646:
4127:. Plugging in the change of free energy equation above, it is easy to get:
1868:. Above the glass transition temperature, the polymer chain oscillates and
256:
to the cross-linking molecule. These bonds cause rubber polymers to become
1729:{\displaystyle {\vec {R}}=R_{x}{\hat {x}}+R_{y}{\hat {y}}+R_{z}{\hat {z}}}
1415:
245:. During the process, a small amount of a cross-linking molecule, usually
6299:
D. E. Hanson, Journal of Chemical Physics 131, 224904 (224905 pp.) (2009)
6273:
D. E. Hanson, Journal of Chemical Physics 134, 064906 (064906 pp.) (2011)
6054:
1526:
422:
365:
increases markedly. What the observer is noticing are the changes in the
319:
199:
6488:
1443:
323:
peroxide, can decompose and the subsequent chemical reactions produce a
1625:
340:
261:
238:
215:
6523:
6405:
6375:
348:
that is observed when a rubber sample is deformed (e.g. subjected to
246:
1551:. Since stretching is nonspontaneous, as it requires external work,
6621:
6138:"Polymerization | Definition, Classes, & Examples | Britannica"
6114:"Polymerization | Definition, Classes, & Examples | Britannica"
1442:
1414:
1372:
486:
408:
335:
physical mechanisms that occur at the molecular level and how the
6563:, vol. 1, Madison, WI: The University of Wisconsin Press,
1586:
The result is that an elastomer behaves somewhat like an ideal
385:
When these elastic force models are combined with the complex
131:
29:
6561:
Chemical Demonstrations: A Handbook for Teachers of Chemistry
6184:
Proc. Lit. and Phil. Soc., Manchester, 2d ser., 1, 288 (1805)
4962:{\displaystyle \lambda _{x}=\lambda _{y}=\lambda _{z}^{-1/2}}
6502:
Brown, J. B. (May 1963), "Thermodynamics of a Rubber Band",
4726:, which is the number density per volume of polymer chains,
1488:
proposed the entropic origins of rubber elasticity in 1941.
6322:
J. P. Joule, Phil. Trans. R. Soc. London 149, 91β131 (1859)
5500:
1590:, inasmuch as (to good approximation) elastic polymers do
5951:
Therefore, when there is no distance between chain ends (
936:{\displaystyle P(N)=p_{x}{\left(1-p_{x}\right)}^{N-1}\,,}
6079:
Pal, Sanjay; Das, Mithun; Naskar, Kinsuk (2023-05-17),
249:, is added. When heat is applied, sections of rubber's
4969:. So the previous free energy per volume equation is:
4893:{\displaystyle \lambda _{x}\lambda _{y}\lambda _{z}=1}
4832:{\displaystyle \lambda _{x}\lambda _{y}\lambda _{z}=1}
4778:{\displaystyle \beta =\langle R^{2}\rangle /R_{0}^{2}}
6537:
http://scifun.chem.wisc.edu/HomeExpts/rubberband.html
6162:"Polymerization - an overview | ScienceDirect Topics"
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is the distance between the fixed and free ends, and
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A. A. Markov, Izv. Peterb. Akad. 4 (1), 61β80 (1907)
60:. Unsourced material may be challenged and removed.
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820:{\displaystyle p_{x}=2{\frac {\text{}}{\text{}}}}
394:The Molecular Kink Paradigm for rubber elasticity
6285:D. E. Hanson, Polymer 45 (3), 1058β1062 (2004)
390:failure of a rubber sample as it is strained.
6193:Lord Kelvin, Quarterly J. Math., 1, 57 (1857)
291:By the mid-nineteenth century, the theory of
8:
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1411:Variation of tensile stress with temperature
1093:) between its terminating cross-link nodes:
6547:
4470:The free energy change per volume is just:
450:produces an elastic force along the chain.
1477:Historical approaches to elasticity theory
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5800:. Then, the force follows this equation:
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5414:of the rubber in laboratory experiments.
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1997:
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1176:
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1103:
1078:
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1013:
996:β1 successive units along a chain. Since
964:
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538:
175:Learn how and when to remove this message
120:Learn how and when to remove this message
1624:
531:conditional probability density function
241:and then solidified in a process called
198:Rubber, like all materials, consists of
6071:
4847:In a uniaxial deformed rubber, because
1563:is always positive (it can never reach
237:, are extracted from plants as a fluid
6426:
6424:
6387:
6385:
6339:
6337:
6309:
6307:
6305:
6295:
6293:
6291:
5690:{\displaystyle v_{s}=\rho N_{a}/M_{s}}
6331:L.D. Loan, Pure Appl. Chem. 30 (1972)
6281:
6279:
6269:
6267:
6257:
6255:
6245:
6243:
6233:
6231:
6229:
7:
6219:
6217:
1778:is the number of segments of length
1095:
1053:) relates the network chain length (
853:
595:
58:adding citations to reliable sources
5780:, the persistence length, replaces
496:Moderate chain extension regime, Ib
5879:
5717:is the mass density of the chain,
5274:
4995:
4976:
4496:
4477:
4138:
3392:
3002:Note that the elastic coefficient
2672:
2639:
2557:
2447:
2375:
2349:
2199:
1758:is the length of a rigid segment,
1391:Numerical network simulation model
147:tone or style may not reflect the
25:
4843:Case study: Uniaxial deformation:
3372:{\displaystyle \lambda _{z}R_{z}}
3335:{\displaystyle \lambda _{y}R_{y}}
3298:{\displaystyle \lambda _{x}R_{x}}
3261:{\displaystyle \lambda _{z}L_{z}}
3224:{\displaystyle \lambda _{y}L_{y}}
3187:{\displaystyle \lambda _{x}L_{x}}
3039:{\displaystyle 3k_{\text{B}}T/Nb}
2123:{\displaystyle \langle R\rangle }
1629:Model of the freely jointed chain
1433:coefficient of thermal expansion
157:guide to writing better articles
136:
34:
6559:Shakhashiri, Bassam Z. (1983),
831:for finding a chain containing
505:High chain extension regime, II
45:needs additional citations for
5981:{\displaystyle r=L_{\text{c}}}
5448:
5435:
5287:
5271:
5023:
5017:
5008:
4524:
4518:
4509:
4166:
4160:
4151:
3459:
3420:
3414:
3405:
2984:
2901:
2862:
2835:
2821:
2815:
2806:
2763:
2707:
2695:
2685:
2660:
2654:
2645:
2590:
2482:
2436:is the distance. Usually, the
2248:
2242:
2233:
1973:
1960:
1954:
1941:
1935:
1922:
1913:
1907:
1898:
1720:
1695:
1670:
1645:
1157:
1150:
1143:
1137:
1131:
1120:
1108:
1051:joint probability distribution
872:
866:
622:
615:
608:
467:Low chain extension regime, Ia
307:In 1838 the American inventor
27:Property of crosslinked rubber
1:
6081:"Origin of Rubber Elasticity"
4719:{\displaystyle v_{s}=n_{s}/V}
6585:Physics of Rubber Elasticity
6028:{\displaystyle L_{\text{c}}}
5773:{\displaystyle L_{\text{p}}}
3150:{\displaystyle \lambda _{i}}
1838:{\displaystyle L_{\text{c}}}
1037:. The product of equations (
851:isoprene units is given by:
553:in units of the Kuhn length
6639:10.1103/PhysRevE.102.012501
6587:, Oxford University Press,
6504:American Journal of Physics
2432:is the spring constant and
1845:is the "contour length" or
1398:
1073:) and end-to-end distance (
1045:
1039:
573:to the end-to-end distance
6701:
2384:{\displaystyle -T\Delta S}
1614:
1611:Freely-jointed chain model
1533:is the entropy, we obtain
1030:{\displaystyle N\sim 2.2n}
533:relates the chain length
229:Natural rubbers, such as
214:. Rubber's molecules are
1583:will be positive there.
1559:must be negative. Since
460:probability distribution
6583:L.R.G. Treloar (1975),
6535:Rubber Bands and Heat,
6453:10.1103/PhysRev.66.30.2
6085:Elasticity of Materials
2355:{\displaystyle \Omega }
978:{\displaystyle N\geq 1}
151:used on Knowledge (XXG)
6029:
6002:
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3097:
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2779:
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2523:
2418:
2385:
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2124:
2095:
1882:
1862:
1839:
1812:
1792:
1772:
1752:
1730:
1630:
1599:Polymer chain theories
1448:
1420:
1378:
1351:
1087:
1067:
1031:
979:
937:
845:
821:
763:
587:
567:
547:
492:
443:Boltzmann distribution
414:
356:Molecular-level models
210:that occur due to its
155:See Knowledge (XXG)'s
6166:www.sciencedirect.com
6050:Hyperelastic material
6030:
6003:
5983:
5944:
5795:
5775:
5749:Worm-like chain model
5739:
5737:{\displaystyle M_{s}}
5712:
5710:{\displaystyle \rho }
5692:
5634:
5405:
5382:
5234:
4964:
4895:
4834:
4780:
4721:
4673:
4671:{\displaystyle n_{s}}
4646:
4463:
4122:
4000:
3998:{\displaystyle R_{z}}
3973:
3971:{\displaystyle R_{y}}
3946:
3944:{\displaystyle R_{x}}
3917:
3374:
3337:
3300:
3263:
3226:
3189:
3152:
3125:
3123:{\displaystyle L_{z}}
3098:
3096:{\displaystyle L_{y}}
3071:
3069:{\displaystyle L_{x}}
3041:
2995:
2780:
2628:
2524:
2419:
2386:
2357:
2340:Helmholtz free energy
2331:
2125:
2096:
1883:
1863:
1840:
1813:
1793:
1773:
1753:
1731:
1628:
1446:
1418:
1376:
1352:
1088:
1068:
1032:
980:
938:
846:
822:
764:
588:
568:
548:
490:
412:
375:statistical mechanics
367:modulus of elasticity
6045:Elasticity (physics)
6012:
5992:
5959:
5804:
5784:
5757:
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5701:
5643:
5420:
5394:
5249:
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4904:
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4790:
4730:
4682:
4655:
4474:
4131:
4009:
3982:
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3928:
3385:
3346:
3309:
3272:
3235:
3198:
3161:
3134:
3107:
3080:
3053:
3006:
2788:
2636:
2532:
2444:
2417:{\displaystyle F=kx}
2399:
2366:
2346:
2136:
2108:
1892:
1872:
1849:
1822:
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1617:Freely Jointed Chain
1521:is the free energy,
1102:
1077:
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963:
860:
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790:
602:
577:
557:
537:
54:improve this article
6631:2020PhRvE.102a2501B
6516:1963AmJPh..31..397T
6489:10.1021/ie50377a017
6445:1944PhRv...66...30M
5532:
5369:
5197:
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4900:it is assumed that
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439:thermal equilibrium
212:molecular structure
208:molecular processes
69:"Rubber elasticity"
6548:Shakhashiri (1983)
6542:2019-06-13 at the
6364:Trans. Faraday Soc
6142:www.britannica.com
6118:www.britannica.com
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5243:engineering stress
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2091:
1878:
1861:{\displaystyle Nb}
1858:
1835:
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1768:
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1449:
1439:Snap-back velocity
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524:Network morphology
493:
478:molecular dynamics
415:
224:chemical reactions
6675:Rubber properties
6570:978-0-299-08890-3
6524:10.1119/1.1969535
6406:10.5254/1.3540117
6376:10.5254/1.3546701
6094:978-1-83969-961-0
6022:
6001:{\displaystyle r}
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5823:
5793:{\displaystyle b}
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5445:
5403:{\displaystyle E}
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2438:neo-Hookean model
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2010:
1910:
1881:{\displaystyle r}
1832:
1811:{\displaystyle R}
1791:{\displaystyle b}
1771:{\displaystyle N}
1751:{\displaystyle b}
1723:
1698:
1673:
1648:
1499:Gibbs free energy
1371:
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1340:
1264:
1086:{\displaystyle r}
1066:{\displaystyle N}
1004:) decreases with
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844:{\displaystyle N}
815:
814:
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783:
782:
751:
675:
586:{\displaystyle r}
566:{\displaystyle b}
546:{\displaystyle n}
517:quantum chemistry
188:Rubber elasticity
185:
184:
177:
149:encyclopedic tone
130:
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18:Rubber Elasticity
16:(Redirected from
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6544:Wayback Machine
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3500:
3479:
3472:
3452:
3439:
3435:
3423:
3395:
3383:
3382:
3359:
3349:
3344:
3343:
3322:
3312:
3307:
3306:
3285:
3275:
3270:
3269:
3248:
3238:
3233:
3232:
3211:
3201:
3196:
3195:
3174:
3164:
3159:
3158:
3157:to the length (
3137:
3132:
3131:
3110:
3105:
3104:
3083:
3078:
3077:
3056:
3051:
3050:
3012:
3004:
3003:
2965:
2961:
2947:
2943:
2921:
2914:
2894:
2881:
2877:
2871:
2852:
2825:
2799:
2786:
2785:
2756:
2743:
2739:
2725:
2721:
2688:
2675:
2634:
2633:
2610:
2603:
2583:
2573:
2566:
2541:
2530:
2529:
2502:
2495:
2475:
2468:
2462:
2442:
2441:
2397:
2396:
2364:
2363:
2344:
2343:
2323:
2322:
2305:
2290:
2280:
2274:
2273:
2263:
2220:
2204:
2182:
2169:
2163:
2162:
2152:
2134:
2133:
2106:
2105:
2074:
2067:
2056:
2049:
2043:
1993:
1986:
1980:
1979:
1963:
1944:
1925:
1890:
1889:
1870:
1869:
1847:
1846:
1825:
1820:
1819:
1800:
1799:
1780:
1779:
1760:
1759:
1740:
1739:
1704:
1679:
1654:
1634:
1633:
1619:
1613:
1605:entropic spring
1601:
1534:
1501:. Rearranging Ξ
1494:
1486:Hubert M. James
1479:
1466:
1462:
1461:
1441:
1413:
1408:
1393:
1363:
1329:
1322:
1311:
1307:
1301:
1297:
1247:
1240:
1234:
1233:
1223:
1188:
1181:
1177:
1175:
1165:
1100:
1099:
1075:
1074:
1055:
1054:
1010:
1009:
990:
961:
960:
949:
901:
894:
890:
888:
878:
858:
857:
833:
832:
793:
788:
787:
775:
740:
733:
722:
718:
712:
708:
658:
651:
645:
644:
634:
600:
599:
575:
574:
555:
554:
535:
534:
526:
507:
498:
469:
407:
403:
399:
397:
396:
358:
274:
254:chemically bond
206:is produced by
195:to the rubber.
181:
170:
164:
161:
154:
145:This article's
141:
137:
126:
115:
109:
106:
63:
61:
51:
39:
28:
23:
22:
15:
12:
11:
5:
6698:
6696:
6688:
6687:
6682:
6680:Thermodynamics
6677:
6667:
6666:
6661:
6660:
6599:
6593:
6575:
6569:
6551:
6528:
6494:
6483:(5): 624β629.
6477:Ind. Eng. Chem
6467:
6458:
6439:(1β2): 30β32.
6420:
6411:
6381:
6370:(4): 813β825.
6354:
6345:
6333:
6324:
6315:
6301:
6287:
6275:
6263:
6251:
6239:
6225:
6213:
6204:
6195:
6186:
6177:
6153:
6129:
6105:
6093:
6087:, IntechOpen,
6070:
6069:
6067:
6064:
6063:
6062:
6060:Thermodynamics
6057:
6052:
6047:
6040:
6037:
6018:
5997:
5971:
5967:
5964:
5937:
5925:
5921:
5916:
5911:
5908:
5903:
5895:
5890:
5881:
5876:
5872:
5867:
5864:
5860:
5855:
5851:
5845:
5833:
5828:
5819:
5812:
5809:
5789:
5763:
5750:
5747:
5731:
5727:
5706:
5684:
5680:
5675:
5669:
5665:
5661:
5658:
5653:
5649:
5624:
5620:
5615:
5612:
5609:
5606:
5603:
5597:
5594:
5589:
5585:
5581:
5572:
5568:
5565:
5560:
5557:
5552:
5548:
5542:
5538:
5530:
5525:
5521:
5517:
5512:
5509:
5505:
5501:
5497:
5492:
5488:
5484:
5475:
5471:
5463:
5459:
5455:
5450:
5441:
5437:
5434:
5428:
5425:
5399:
5375:
5367:
5362:
5358:
5354:
5349:
5344:
5340:
5335:
5331:
5326:
5322:
5318:
5309:
5305:
5298:
5294:
5289:
5280:
5276:
5273:
5270:
5264:
5255:
5227:
5223:
5220:
5213:
5209:
5205:
5200:
5195:
5190:
5186:
5181:
5175:
5171:
5166:
5162:
5158:
5149:
5142:
5137:
5132:
5128:
5125:
5120:
5115:
5111:
5107:
5102:
5097:
5093:
5089:
5084:
5079:
5075:
5070:
5066:
5061:
5057:
5053:
5044:
5037:
5034:
5029:
5025:
5019:
5016:
5010:
5001:
4997:
4991:
4982:
4978:
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4948:
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4927:
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4914:
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4889:
4886:
4881:
4877:
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4867:
4861:
4857:
4828:
4825:
4820:
4816:
4810:
4806:
4800:
4796:
4772:
4767:
4763:
4758:
4754:
4749:
4745:
4741:
4738:
4735:
4715:
4711:
4705:
4701:
4697:
4692:
4688:
4665:
4661:
4638:
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4626:
4621:
4616:
4612:
4608:
4603:
4598:
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4567:
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4417:
4412:
4408:
4404:
4399:
4394:
4390:
4386:
4381:
4376:
4372:
4367:
4363:
4358:
4354:
4350:
4345:
4341:
4337:
4328:
4321:
4318:
4315:
4313:
4311:
4303:
4299:
4295:
4292:
4286:
4282:
4279:
4274:
4269:
4265:
4261:
4256:
4251:
4247:
4243:
4238:
4233:
4229:
4224:
4220:
4215:
4211:
4207:
4202:
4198:
4194:
4185:
4178:
4175:
4172:
4170:
4168:
4162:
4159:
4153:
4144:
4140:
4137:
4136:
4116:
4112:
4108:
4103:
4099:
4095:
4092:
4089:
4084:
4079:
4076:
4072:
4068:
4065:
4062:
4057:
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4022:
4018:
4014:
3992:
3988:
3965:
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3898:
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3891:
3885:
3879:
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3832:
3827:
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3803:
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3793:
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3784:
3780:
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3767:
3763:
3758:
3754:
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3727:
3723:
3714:
3710:
3704:
3701:
3698:
3696:
3694:
3686:
3682:
3678:
3675:
3669:
3664:
3658:
3653:
3650:
3646:
3642:
3637:
3632:
3628:
3623:
3619:
3615:
3609:
3604:
3601:
3597:
3593:
3588:
3583:
3579:
3574:
3570:
3566:
3560:
3555:
3552:
3548:
3544:
3539:
3534:
3530:
3525:
3520:
3516:
3507:
3503:
3497:
3494:
3486:
3482:
3478:
3475:
3468:
3461:
3458:
3451:
3442:
3438:
3432:
3429:
3426:
3424:
3422:
3416:
3413:
3407:
3398:
3394:
3391:
3390:
3366:
3362:
3356:
3352:
3329:
3325:
3319:
3315:
3292:
3288:
3282:
3278:
3255:
3251:
3245:
3241:
3218:
3214:
3208:
3204:
3181:
3177:
3171:
3167:
3144:
3140:
3117:
3113:
3090:
3086:
3063:
3059:
3035:
3032:
3028:
3024:
3015:
3011:
2986:
2983:
2972:
2968:
2964:
2959:
2950:
2946:
2940:
2936:
2928:
2924:
2920:
2917:
2910:
2903:
2900:
2893:
2884:
2880:
2874:
2864:
2861:
2855:
2851:
2846:
2837:
2834:
2828:
2823:
2817:
2814:
2808:
2805:
2802:
2796:
2793:
2772:
2765:
2762:
2750:
2746:
2742:
2737:
2728:
2724:
2718:
2715:
2712:
2709:
2704:
2697:
2694:
2687:
2682:
2678:
2674:
2671:
2668:
2665:
2662:
2656:
2653:
2647:
2644:
2641:
2617:
2613:
2609:
2606:
2599:
2592:
2589:
2576:
2572:
2569:
2563:
2559:
2556:
2553:
2544:
2540:
2537:
2517:
2509:
2505:
2501:
2498:
2491:
2484:
2481:
2474:
2471:
2465:
2461:
2458:
2455:
2452:
2449:
2428:is the force,
2413:
2410:
2407:
2404:
2380:
2377:
2374:
2371:
2351:
2321:
2316:
2311:
2308:
2306:
2301:
2298:
2293:
2287:
2283:
2279:
2276:
2275:
2270:
2266:
2262:
2259:
2256:
2253:
2250:
2244:
2241:
2235:
2232:
2227:
2223:
2219:
2216:
2211:
2207:
2201:
2196:
2192:
2188:
2185:
2183:
2181:
2176:
2172:
2168:
2165:
2164:
2161:
2158:
2155:
2153:
2151:
2148:
2145:
2142:
2141:
2119:
2116:
2113:
2089:
2081:
2077:
2073:
2070:
2063:
2059:
2055:
2052:
2046:
2042:
2039:
2033:
2028:
2023:
2019:
2014:
2009:
2005:
2000:
1996:
1992:
1989:
1983:
1978:
1975:
1970:
1966:
1962:
1959:
1956:
1951:
1947:
1943:
1940:
1937:
1932:
1928:
1924:
1921:
1918:
1915:
1909:
1906:
1900:
1897:
1877:
1857:
1854:
1828:
1807:
1787:
1767:
1747:
1738:In the model,
1722:
1719:
1711:
1707:
1703:
1697:
1694:
1686:
1682:
1678:
1672:
1669:
1661:
1657:
1653:
1647:
1644:
1615:Main article:
1612:
1609:
1600:
1597:
1493:
1492:Thermodynamics
1490:
1478:
1475:
1440:
1437:
1412:
1409:
1407:
1404:
1392:
1389:
1384:force constant
1369:
1368:
1359:
1357:
1345:
1336:
1332:
1328:
1325:
1318:
1314:
1310:
1304:
1300:
1296:
1293:
1287:
1282:
1277:
1273:
1268:
1263:
1259:
1254:
1250:
1246:
1243:
1237:
1230:
1226:
1222:
1219:
1213:
1210:
1207:
1201:
1195:
1191:
1187:
1184:
1180:
1172:
1168:
1163:
1159:
1156:
1152:
1148:
1145:
1142:
1139:
1136:
1133:
1130:
1126:
1122:
1119:
1116:
1113:
1110:
1107:
1082:
1062:
1026:
1023:
1020:
1017:
988:
974:
971:
968:
955:
954:
945:
943:
932:
926:
923:
920:
914:
908:
904:
900:
897:
893:
885:
881:
877:
874:
871:
868:
865:
840:
808:
805:
800:
796:
781:
780:
771:
769:
756:
747:
743:
739:
736:
729:
725:
721:
715:
711:
707:
704:
698:
693:
688:
684:
679:
674:
670:
665:
661:
657:
654:
648:
641:
637:
633:
630:
627:
624:
621:
617:
613:
610:
607:
582:
562:
542:
525:
522:
512:dihedral angle
506:
503:
497:
494:
468:
465:
419:natural rubber
395:
392:
357:
354:
350:tensile strain
339:nature of the
293:thermodynamics
278:natural rubber
273:
270:
251:polymer chains
220:polymerization
183:
182:
144:
142:
135:
128:
127:
42:
40:
33:
26:
24:
14:
13:
10:
9:
6:
4:
3:
2:
6697:
6686:
6683:
6681:
6678:
6676:
6673:
6672:
6670:
6656:
6652:
6648:
6644:
6640:
6636:
6632:
6628:
6623:
6618:
6615:(1): 012501.
6614:
6610:
6603:
6600:
6596:
6594:9780198570271
6590:
6586:
6579:
6576:
6572:
6566:
6562:
6555:
6552:
6549:
6545:
6541:
6538:
6532:
6529:
6525:
6521:
6517:
6513:
6509:
6505:
6498:
6495:
6490:
6486:
6482:
6478:
6471:
6468:
6462:
6459:
6454:
6450:
6446:
6442:
6438:
6434:
6427:
6425:
6421:
6415:
6412:
6407:
6403:
6399:
6395:
6394:J. Phys. Chem
6388:
6386:
6382:
6377:
6373:
6369:
6365:
6358:
6355:
6349:
6346:
6340:
6338:
6334:
6328:
6325:
6319:
6316:
6310:
6308:
6306:
6302:
6296:
6294:
6292:
6288:
6282:
6280:
6276:
6270:
6268:
6264:
6258:
6256:
6252:
6246:
6244:
6240:
6234:
6232:
6230:
6226:
6220:
6218:
6214:
6208:
6205:
6199:
6196:
6190:
6187:
6181:
6178:
6167:
6163:
6157:
6154:
6143:
6139:
6133:
6130:
6119:
6115:
6109:
6106:
6096:
6090:
6086:
6082:
6075:
6072:
6065:
6061:
6058:
6056:
6053:
6051:
6048:
6046:
6043:
6042:
6038:
6036:
6016:
5995:
5969:
5965:
5962:
5954:
5949:
5935:
5923:
5919:
5914:
5909:
5906:
5901:
5893:
5888:
5874:
5870:
5865:
5862:
5858:
5853:
5849:
5843:
5831:
5826:
5817:
5810:
5807:
5787:
5761:
5748:
5746:
5729:
5725:
5704:
5682:
5678:
5673:
5667:
5663:
5659:
5656:
5651:
5647:
5622:
5618:
5613:
5610:
5607:
5604:
5601:
5595:
5592:
5587:
5583:
5579:
5570:
5566:
5563:
5558:
5555:
5550:
5546:
5540:
5536:
5528:
5523:
5519:
5515:
5510:
5507:
5503:
5495:
5490:
5486:
5482:
5473:
5469:
5461:
5457:
5453:
5439:
5432:
5426:
5423:
5415:
5413:
5397:
5390:
5373:
5365:
5360:
5356:
5352:
5347:
5342:
5338:
5333:
5329:
5324:
5320:
5316:
5307:
5303:
5296:
5292:
5278:
5268:
5262:
5253:
5244:
5239:
5225:
5221:
5218:
5211:
5207:
5203:
5198:
5193:
5188:
5184:
5179:
5173:
5169:
5164:
5160:
5156:
5147:
5140:
5135:
5130:
5126:
5123:
5118:
5113:
5109:
5105:
5100:
5095:
5091:
5087:
5082:
5077:
5073:
5068:
5064:
5059:
5055:
5051:
5042:
5035:
5032:
5027:
5014:
4999:
4989:
4980:
4954:
4950:
4946:
4943:
4938:
4934:
4930:
4925:
4921:
4917:
4912:
4908:
4887:
4884:
4879:
4875:
4869:
4865:
4859:
4855:
4845:
4844:
4840:
4826:
4823:
4818:
4814:
4808:
4804:
4798:
4794:
4770:
4765:
4761:
4756:
4747:
4743:
4736:
4733:
4713:
4709:
4703:
4699:
4695:
4690:
4686:
4663:
4659:
4636:
4631:
4627:
4624:
4619:
4614:
4610:
4606:
4601:
4596:
4592:
4588:
4583:
4578:
4574:
4569:
4565:
4560:
4556:
4552:
4543:
4536:
4533:
4528:
4515:
4500:
4490:
4481:
4468:
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2209:
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2057:
2053:
2050:
2044:
2040:
2037:
2031:
2026:
2021:
2017:
2012:
2007:
2003:
1998:
1994:
1990:
1987:
1981:
1976:
1968:
1964:
1957:
1949:
1945:
1938:
1930:
1926:
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1916:
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1598:
1596:
1593:
1589:
1588:monatomic gas
1584:
1582:
1578:
1574:
1570:
1566:
1565:absolute zero
1562:
1558:
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1128:
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1111:
1105:
1098:
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1080:
1060:
1052:
1048:
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1042:
1041:
1024:
1021:
1018:
1015:
1007:
1003:
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995:
991:
972:
969:
966:
953:
946:
944:
930:
924:
921:
918:
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906:
902:
898:
895:
891:
883:
879:
875:
869:
863:
856:
855:
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838:
830:
806:
803:
798:
794:
779:
772:
770:
754:
745:
741:
737:
734:
727:
723:
719:
713:
709:
705:
702:
696:
691:
686:
682:
677:
672:
668:
663:
659:
655:
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635:
631:
628:
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619:
611:
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560:
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532:
523:
521:
518:
513:
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502:
495:
489:
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483:
479:
475:
466:
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461:
455:
451:
448:
444:
440:
434:
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426:
424:
420:
411:
402:
393:
391:
388:
383:
379:
376:
371:
368:
362:
355:
353:
351:
347:
342:
338:
332:
328:
326:
325:chemical bond
321:
316:
314:
310:
305:
303:
298:
294:
289:
287:
283:
279:
271:
269:
267:
263:
259:
255:
252:
248:
244:
243:Vulcanization
240:
236:
232:
231:polybutadiene
227:
225:
221:
217:
213:
209:
205:
201:
196:
194:
189:
179:
176:
168:
158:
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150:
143:
134:
133:
124:
121:
113:
102:
99:
95:
92:
88:
85:
81:
78:
74:
71: β
70:
66:
65:Find sources:
59:
55:
49:
48:
43:This article
41:
37:
32:
31:
19:
6612:
6609:Phys. Rev. E
6608:
6602:
6584:
6578:
6560:
6554:
6531:
6507:
6503:
6497:
6480:
6476:
6470:
6461:
6436:
6432:
6414:
6397:
6393:
6367:
6363:
6357:
6348:
6327:
6318:
6207:
6198:
6189:
6180:
6169:. Retrieved
6165:
6156:
6145:. Retrieved
6141:
6132:
6121:. Retrieved
6117:
6108:
6098:, retrieved
6084:
6074:
5952:
5950:
5752:
5416:
5240:
4846:
4842:
4841:
4469:
3923:
3381:
3048:
3001:
2433:
2429:
2425:
2337:
2132:
2102:
1737:
1632:
1620:
1602:
1591:
1585:
1580:
1576:
1568:
1560:
1556:
1552:
1547:
1543:
1539:
1535:
1530:
1522:
1518:
1514:
1510:
1506:
1502:
1495:
1480:
1470:
1457:
1454:
1450:
1430:
1426:
1422:
1397:
1394:
1380:
1361:
1044:
1038:
1005:
1001:
997:
993:
986:
958:
947:
784:
773:
527:
508:
499:
470:
456:
452:
435:
427:
423:polyisoprene
416:
384:
380:
372:
363:
359:
333:
329:
317:
313:polyisoprene
306:
290:
282:polyisoprene
275:
258:cross-linked
235:polyisoprene
228:
197:
187:
186:
171:
162:
146:
116:
107:
97:
90:
83:
76:
64:
52:Please help
47:verification
44:
6400:: 826β840.
2393:Hooke's law
1573:microstates
1482:Eugene Guth
1406:Experiments
829:probability
482:free energy
431:Kuhn length
337:random-walk
315:molecules.
302:James Joule
297:Lord Kelvin
202:. Rubber's
193:degradation
6669:Categories
6622:2004.07874
6510:(5): 397,
6171:2024-07-25
6147:2024-07-25
6123:2024-07-25
6100:2024-07-25
6066:References
474:tortuosity
387:morphology
286:John Gough
266:elastomers
204:elasticity
80:newspapers
6685:Mechanics
6655:215814600
6546:, citing
6433:Phys. Rev
5902:−
5866:−
5811:≈
5705:ρ
5660:ρ
5608:β
5605:ρ
5593:β
5547:λ
5520:λ
5496:β
5458:λ
5440:σ
5412:stiffness
5357:λ
5348:−
5339:λ
5330:β
5293:λ
5275:Δ
5254:σ
5219:−
5208:λ
5185:λ
5170:β
5124:−
5110:λ
5092:λ
5074:λ
5065:β
5036:−
5018:→
4996:Δ
4977:Δ
4944:−
4935:λ
4922:λ
4909:λ
4876:λ
4866:λ
4856:λ
4815:λ
4805:λ
4795:λ
4753:⟩
4740:⟨
4734:β
4625:−
4611:λ
4593:λ
4575:λ
4566:β
4537:−
4519:→
4497:Δ
4478:Δ
4421:−
4407:λ
4389:λ
4371:λ
4362:⟩
4349:⟨
4320:−
4278:−
4264:λ
4246:λ
4228:λ
4219:⟩
4206:⟨
4177:−
4161:→
4139:Δ
4107:⟩
4094:⟨
4088:⟩
4067:⟨
4061:⟩
4040:⟨
4034:⟩
4013:⟨
3854:−
3840:λ
3802:−
3788:λ
3750:−
3736:λ
3703:−
3641:−
3592:−
3543:−
3496:−
3460:→
3431:−
3415:→
3393:Δ
3351:λ
3314:λ
3277:λ
3240:λ
3203:λ
3166:λ
3139:λ
2985:→
2902:→
2863:→
2836:→
2816:→
2764:→
2696:→
2673:Δ
2667:−
2664:≈
2655:→
2640:Δ
2591:→
2568:−
2562:≈
2558:Ω
2555:
2483:→
2470:−
2460:
2448:Ω
2376:Δ
2370:−
2350:Ω
2292:⟩
2278:⟨
2243:→
2218:π
2200:∞
2191:∫
2180:⟩
2167:⟨
2150:⟩
2144:⟨
2118:⟩
2112:⟨
2051:−
2041:
2018:−
2004:π
1908:→
1721:^
1696:^
1671:^
1646:→
1303:−
1295:
1272:−
1258:π
1221:π
1209:−
1186:−
1019:∼
970:≥
922:−
899:−
714:−
706:
683:−
669:π
632:π
200:molecules
165:July 2024
110:July 2024
6647:32794915
6540:Archived
6055:Polymers
6039:See also
5387:and the
2424:, where
1567:), the Ξ
1527:enthalpy
1517:, where
447:Gaussian
382:strain.
320:isoprene
262:polymers
216:polymers
6627:Bibcode
6512:Bibcode
6441:Bibcode
1525:is the
1509:−
1465:⁄
1049:) (the
1043:) and (
341:polymer
272:History
264:called
239:colloid
94:scholar
6653:
6645:
6591:
6567:
6091:
5639:where
4651:where
1529:, and
959:where
398:": -->
346:stress
247:sulfur
96:
89:
82:
75:
67:
6651:S2CID
6617:arXiv
992:) in
101:JSTOR
87:books
6643:PMID
6589:ISBN
6565:ISBN
6089:ISBN
5241:The
3978:and
3103:and
1484:and
400:edit
233:and
73:news
6635:doi
6613:102
6520:doi
6485:doi
6449:doi
6402:doi
6372:doi
5444:eng
5283:def
5258:eng
5004:def
4985:def
4505:def
4486:def
4147:def
3401:def
2457:exp
2038:exp
1592:not
1546:β Ξ
1542:= Ξ
1292:exp
1022:2.2
703:exp
352:).
56:by
6671::
6649:.
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6633:.
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6290:^
6278:^
6266:^
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6216:^
6164:.
6140:.
6116:.
6083:,
6035:.
5697:,
4839:.
3951:,
3342:,
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3231:,
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3076:,
2552:ln
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1798:,
1505:=Ξ
1471:mv
1460:=
593::
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6657:.
6637::
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6522::
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6491:.
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3762:R
3757:)
3753:1
3745:2
3740:x
3731:(
3726:(
3722:T
3717:B
3713:k
3709:3
3700:=
3685:2
3681:b
3677:N
3674:2
3668:)
3663:)
3657:2
3652:0
3649:z
3645:R
3636:2
3631:z
3627:R
3622:(
3618:+
3614:)
3608:2
3603:0
3600:y
3596:R
3587:2
3582:y
3578:R
3573:(
3569:+
3565:)
3559:2
3554:0
3551:x
3547:R
3538:2
3533:x
3529:R
3524:(
3519:(
3515:T
3510:B
3506:k
3502:3
3493:=
3485:2
3481:b
3477:N
3474:2
3467:2
3457:R
3450:T
3445:B
3441:k
3437:3
3428:=
3421:)
3412:R
3406:(
3397:F
3365:z
3361:R
3355:z
3328:y
3324:R
3318:y
3291:x
3287:R
3281:x
3254:z
3250:L
3244:z
3217:y
3213:L
3207:y
3180:x
3176:L
3170:x
3143:i
3116:z
3112:L
3089:y
3085:L
3062:x
3058:L
3034:b
3031:N
3027:/
3023:T
3018:B
3014:k
3010:3
2982:R
2971:2
2967:b
2963:N
2958:T
2953:B
2949:k
2945:3
2939:=
2935:)
2927:2
2923:b
2919:N
2916:2
2909:2
2899:R
2892:T
2887:B
2883:k
2879:3
2873:(
2860:R
2854:d
2850:d
2845:=
2833:R
2827:d
2822:)
2813:R
2807:(
2804:F
2801:d
2795:=
2792:f
2771:2
2761:R
2749:2
2745:b
2741:N
2736:T
2731:B
2727:k
2723:3
2717:+
2714:C
2711:=
2708:)
2703:2
2693:R
2686:(
2681:d
2677:S
2670:T
2661:)
2652:R
2646:(
2643:F
2616:2
2612:b
2608:N
2605:2
2598:2
2588:R
2579:B
2575:k
2571:3
2547:B
2543:k
2539:=
2536:S
2516:)
2508:2
2504:b
2500:N
2497:2
2490:2
2480:R
2473:3
2464:(
2454:C
2451:=
2434:x
2430:k
2426:F
2412:x
2409:k
2406:=
2403:F
2379:S
2373:T
2320:b
2315:N
2310:=
2300:2
2297:1
2286:2
2282:R
2269:2
2265:b
2261:N
2258:=
2255:R
2252:d
2249:)
2240:R
2234:(
2231:P
2226:2
2222:R
2215:4
2210:2
2206:R
2195:0
2187:=
2175:2
2171:R
2160:0
2157:=
2147:R
2115:R
2088:)
2080:2
2076:b
2072:N
2069:2
2062:2
2058:R
2054:3
2045:(
2032:2
2027:/
2022:3
2013:)
2008:3
1999:2
1995:b
1991:n
1988:2
1982:(
1977:=
1974:)
1969:z
1965:R
1961:(
1958:P
1955:)
1950:y
1946:R
1942:(
1939:P
1936:)
1931:x
1927:R
1923:(
1920:P
1917:=
1914:)
1905:R
1899:(
1896:P
1876:r
1856:b
1853:N
1831:c
1827:L
1806:R
1786:b
1766:N
1746:b
1718:z
1710:z
1706:R
1702:+
1693:y
1685:y
1681:R
1677:+
1668:x
1660:x
1656:R
1652:=
1643:R
1581:S
1577:G
1569:S
1561:T
1557:S
1555:Ξ
1553:T
1548:G
1544:H
1540:S
1538:Ξ
1536:T
1531:S
1523:H
1519:G
1515:S
1513:Ξ
1511:T
1507:H
1503:G
1467:2
1463:1
1458:E
1399:4
1396:(
1366:)
1364:4
1362:(
1344:)
1335:2
1331:b
1327:n
1324:2
1317:2
1313:r
1309:3
1299:(
1286:2
1281:/
1276:3
1267:)
1262:3
1253:2
1249:b
1245:n
1242:2
1236:(
1229:2
1225:r
1218:4
1212:1
1206:N
1200:)
1194:x
1190:p
1183:1
1179:(
1171:x
1167:p
1162:=
1158:)
1155:N
1151:|
1147:r
1144:(
1141:P
1138:)
1135:N
1132:(
1129:P
1125:=
1121:)
1118:N
1115:,
1112:r
1109:(
1106:P
1081:r
1061:N
1046:3
1040:1
1025:n
1016:N
1006:N
1002:N
1000:(
998:P
994:N
989:x
987:p
973:1
967:N
952:)
950:3
948:(
931:,
925:1
919:N
913:)
907:x
903:p
896:1
892:(
884:x
880:p
876:=
873:)
870:N
867:(
864:P
839:N
807:2
804:=
799:x
795:p
778:)
776:1
774:(
755:)
746:2
742:b
738:n
735:2
728:2
724:r
720:3
710:(
697:2
692:/
687:3
678:)
673:3
664:2
660:b
656:n
653:2
647:(
640:2
636:r
629:4
626:=
623:)
620:n
616:|
612:r
609:(
606:P
581:r
561:b
541:n
421:(
404:]
280:(
178:)
172:(
167:)
163:(
153:.
123:)
117:(
112:)
108:(
98:Β·
91:Β·
84:Β·
77:Β·
50:.
20:)
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