274 research outputs found

    Entropic Elasticity of Phantom Percolation Networks

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    A new method is used to measure the stress and elastic constants of purely entropic phantom networks, in which a fraction pp of neighbors are tethered by inextensible bonds. We find that close to the percolation threshold pcp_c the shear modulus behaves as (p−pc)f(p-p_c)^f, where the exponent f≈1.35f\approx 1.35 in two dimensions, and f≈1.95f\approx 1.95 in three dimensions, close to the corresponding values of the conductivity exponent in random resistor networks. The components of the stiffness tensor (elastic constants) of the spanning cluster follow a power law ∌(p−pc)g\sim(p-p_c)^g, with an exponent g≈2.0g\approx 2.0 and 2.6 in two and three dimensions, respectively.Comment: submitted to the Europhys. Lett., 7 pages, 5 figure

    Persistence distributions for non gaussian markovian processes

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    We propose a systematic method to derive the asymptotic behaviour of the persistence distribution, for a large class of stochastic processes described by a general Fokker-Planck equation in one dimension. Theoretical predictions are compared to simple solvable systems and to numerical calculations. The very good agreement attests the validity of this approach.Comment: 7 pages, 1 figure, to be published in Europhysics Letter

    Random pinning limits the size of membrane adhesion domains

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    Theoretical models describing specific adhesion of membranes predict (for certain parameters) a macroscopic phase separation of bonds into adhesion domains. We show that this behavior is fundamentally altered if the membrane is pinned randomly due to, e.g., proteins that anchor the membrane to the cytoskeleton. Perturbations which locally restrict membrane height fluctuations induce quenched disorder of the random-field type. This rigorously prevents the formation of macroscopic adhesion domains following the Imry-Ma argument [Y. Imry and S. K. Ma, Phys. Rev. Lett. 35, 1399 (1975)]. Our prediction of random-field disorder follows from analytical calculations, and is strikingly confirmed in large-scale Monte Carlo simulations. These simulations are based on an efficient composite Monte Carlo move, whereby membrane height and bond degrees of freedom are updated simultaneously in a single move. The application of this move should prove rewarding for other systems also.Comment: revised and extended versio

    The Effect of Thermal Fluctuations on Schulman Area Elasticity

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    We study the elastic properties of a two-dimensional fluctuating surface whose area density is allowed to deviate from its optimal (Schulman) value. The behavior of such a surface is determined by an interplay between the area-dependent elastic energy, the curvature elasticity, and the entropy. We identify three different elastic regimes depending on the ratio Ap/AsA_p/A_s between the projected (frame) and the saturated areas. We show that thermal fluctuations modify the elastic energy of stretched surfaces (Ap/As>1A_p/A_s> 1), and dominate the elastic energy of compressed surfaces (Ap/As<1A_p/A_s< 1). When Ap∌AsA_p\sim A_s the elastic energy is not much affected by the fluctuations; the frame area at which the surface tension vanishes becomes smaller than AsA_s and the area elasticity modulus increases.Comment: 12 pages, to appear in Euro. Phys. J.

    Globular Structures of a Helix-Coil Copolymer: Self-Consistent Treatment

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    A self-consistent field theory was developed in the grand-canonical ensemble formulation to study transitions in a helix-coil multiblock globule. Helical and coil parts are treated as stiff rods and self-avoiding walks of variable lengths correspondingly. The resulting field-theory takes, in addition to the conventional Zimm-Bragg (B.H. Zimm, I.K. Bragg, J. Chem. Phys. 31, 526 (1959)) parameters, also three-dimensional interaction terms into account. The appropriate differential equations which determine the self-consistent fields were solved numerically with finite element method. Three different phase states are found: open chain, amorphous globule and nematic liquid-crystalline (LC) globule. The LC-globule formation is driven by the interplay between the hydrophobic helical segments attraction and the anisotropic globule surface energy of an entropic nature. The full phase diagram of the helix-coil copolymer was calculated and thoroughly discussed. The suggested theory shows a clear interplay between secondary and tertiary structures in globular homopolypeptides.Comment: 26 pages, 30 figures, corrected some typo

    Pseudo-boundaries in discontinuous 2-dimensional maps

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    It is known that Kolmogorov-Arnold-Moser boundaries appear in sufficiently smooth 2-dimensional area-preserving maps. When such boundaries are destroyed, they become pseudo-boundaries. We show that pseudo-boundaries can also be found in discontinuous maps. The origin of these pseudo-boundaries are groups of chains of islands which separate parts of the phase space and need to be crossed in order to move between the different sub-spaces. Trajectories, however, do not easily cross these chains, but tend to propagate along them. This type of behavior is demonstrated using a ``generalized'' Fermi map.Comment: 4 pages, 4 figures, Revtex, epsf, submitted to Physical Review E (as a brief report

    Microscopic formulation of the Zimm-Bragg model for the helix-coil transition

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    A microscopic spin model is proposed for the phenomenological Zimm-Bragg model for the helix-coil transition in biopolymers. This model is shown to provide the same thermophysical properties of the original Zimm-Bragg model and it allows a very convenient framework to compute statistical quantities. Physical origins of this spin model are made transparent by an exact mapping into a one-dimensional Ising model with an external field. However, the dependence on temperature of the reduced external field turns out to differ from the standard one-dimensional Ising model and hence it gives rise to different thermophysical properties, despite the exact mapping connecting them. We discuss how this point has been frequently overlooked in the recent literature.Comment: 11 pages, 2 figure

    Características físico-químicas de meis produzidos por espécies de meliponíneos.

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    AlĂ©m da abelhas Africanizadas (Apis mellifera L.), as abelhas indĂ­genas sem ferrĂŁo ou meliponĂ­neos (Meliponinae) sĂŁo potenciais produtoras de mel. Esse produto apresenta carcterĂ­sticas distintas do mel produzido pelas abelhas do gĂȘnero Apis, sendo muito apreciado pelos consumidores. Entretanto, sĂŁo escassos os dados cientĂ­ficos a respeito da composição desse mel na literatura nacional e internacional. A proposta deste trabalho Ă© avaliar as caracterĂ­sticas fĂ­sico-quĂ­micas do mel produzido por meliponĂ­neos. As anĂĄlises fĂ­sico-quĂ­mico foram realizadas de acordo com as tĂ©cnicas descritas pela AOAC (Association of Official Analytical Chemists), e pela European Honey Comission, conforme recomendado pela CAC (Codex Alimentarius Comission). Os resultados obtidos reforçam a necessidade do desenvolvimento de um padrĂŁo prĂłprio para os mĂ©is de abelhas sem ferrĂŁo, incluindo critĂ©rios microbiolĂłgicos.DisponĂ­vel tambĂ©m em: Cadernos de Agroecologia, V. 5, n.1, 2010

    Elasticity of Gaussian and nearly-Gaussian phantom networks

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    We study the elastic properties of phantom networks of Gaussian and nearly-Gaussian springs. We show that the stress tensor of a Gaussian network coincides with the conductivity tensor of an equivalent resistor network, while its elastic constants vanish. We use a perturbation theory to analyze the elastic behavior of networks of slightly non-Gaussian springs. We show that the elastic constants of phantom percolation networks of nearly-Gaussian springs have a power low dependence on the distance of the system from the percolation threshold, and derive bounds on the exponents.Comment: submitted to Phys. Rev. E, 10 pages, 1 figur

    Non-universality of elastic exponents in random bond-bending networks

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    We numerically investigate the rigidity percolation transition in two-dimensional flexible, random rod networks with freely rotating cross-links. Near the transition, networks are dominated by bending modes and the elastic modulii vanish with an exponent f=3.0\pm0.2, in contrast with central force percolation which shares the same geometric exponents. This indicates that universality for geometric quantities does not imply universality for elastic ones. The implications of this result for actin-fiber networks is discussed.Comment: 4 pages, 3 figures, minor clarifications and amendments. To appear in PRE Rap. Com
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