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  • Reptation  (2)
  • PACS. 83.20.Fk Reptation theories - 83.20.Jp Computer simulation - 83.10.Nn Polymer dynamics  (1)
  • 1
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 10 (1999), S. 105-117 
    ISSN: 1434-6036
    Keywords: PACS. 83.20.Fk Reptation theories - 83.20.Jp Computer simulation - 83.10.Nn Polymer dynamics
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract: We study the diffusive motion of a (non-selfinteracting) chain through a quenched random environment, constructed such that it influences only the local dynamics but not the equilibrium configuration of the chain. Our Monte Carlo results show that this type of disorder, which we call kinematic, does not ruin reptation. This is in sharp contrast to disorder including also entropic traps and it supports the view that reptation prevails in melts, where in contrast to a gel entropic trapping is absent. Our data show the characteristic features of reptation, irrespective of the dilution or randomness of the kinematic obstacles. Our Monte Carlo results are in quantitative agreement with our recent detailed analytical evaluation of the reptation model (J. Stat. Phys. 90, 1325 (1998)). The analysis suggests that we effectively see reptation of a “blob”-chain, where the size of the blob rapidly increases with decreasing obstacle concentration.
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of statistical physics 90 (1998), S. 1375-1400 
    ISSN: 1572-9613
    Keywords: Reptation ; polymer dynamics ; Monte Carlo simulations
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We present simulation data for the motion of a polymer chain through a regular lattice of impenetrable obstacles (Evans–Edwards model). Chain lengths range from N= 20 to N= 640, and time up to 107Monte Carlo steps. For N≥ 160, for the central segment we find clear t 1/4behavior as an intermediate asymptote. The expected t 1/2range is not yet developed. For the end segment also the t l/4behavior is not reached. All these data compare well to our recent analytical evaluation of the reptation model, which shows that for shorter times (t≲104) the discreteness of the elementary motion cannot be neglected, whereas for longer times and short chains (N≲100) tube renewal plays an essential role also for the central segment. Due to the very broad crossover behavior, both the diffusion coefficient and the reptation time within the range of our simulation do not reach the asymptotic power laws predicted by reptation theory. We present results for the center-of-mass motion, showing the expected intermediate t 1/2behavior, but again only for very long chains. In addition we show results for the motion of the central segment relative to the center of mass, where in some intermediate range we see the expected increase of the effective power beyond the t 1/4law, before saturation sets in. Analysis and simulations agree on defining a new set of criteria as characteristic for reptation of finite chains.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Journal of statistical physics 90 (1998), S. 1325-1373 
    ISSN: 1572-9613
    Keywords: Reptation ; polymer dynamics
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We analyze the motion of individual beads of a polymer chain using a discrete version of De Gennes' reptation model that describes the motion of a polymer through an ordered lattice of obstacles. The motion within the tube can be evaluated rigorously; tube renewal is taken into account in an approximation motivated by random walk theory. We find microstructure effects to be present for remarkably large times and long chains, affecting essentially all present-day computer experiments. The various asymptotic power laws commonly considered as typical for reptation hold only for extremely long chains. Furthermore, for an arbitrary segment even in a very long chain, we find a rich variety of fairly broad crossovers, which for practicably accessible chain lengths overlap and smear out the asymptotic power laws. Our analysis suggests observables specifically adapted to distinguish reptation from motions dominated by disorder of the environment.
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