193 research outputs found

    The cross-over from 2D to 3D percolation and its relationship to glass transition in thin films. Theory and numerical simulations

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    We consider here the percolation problem in thin films, both in the direction normal to the film and in the direction parallel to the film. We thereby describe here the cross-over between 2D and 3D percolation, which we do on cubic and square lattices. The main relations are derived using scaling and real space renormalisation arguments. They are checked by numerical simulations, which also provide the numerical prefactors. We calculate in particular the correlation length parallel to the film, the average mass and the mass distribution n(m)n(m) of the clusters. In particular, we show that the latter is given by a master function of hD+1/σ2ν3ppc(h)1/σ2mh^{-D+1/\sigma_{2}\nu_{3}}| p-p_{c}(h)|^{1/\sigma_{2}} m, where hh is the thickness of the film and D,ν3,σ2D,\nu_3,\sigma_2 are tabulated 2D and 3D critical exponents. pc(h)p_c(h) is the percolation threshold of the film which we also calculate. These results are of interest in particular for describing the glass transition in thin polymer films.Comment: 14 figure

    Dragging a polymer chain into a nanotube and subsequent release

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    We present a scaling theory and Monte Carlo (MC) simulation results for a flexible polymer chain slowly dragged by one end into a nanotube. We also describe the situation when the completely confined chain is released and gradually leaves the tube. MC simulations were performed for a self-avoiding lattice model with a biased chain growth algorithm, the pruned-enriched Rosenbluth method. The nanotube is a long channel opened at one end and its diameter DD is much smaller than the size of the polymer coil in solution. We analyze the following characteristics as functions of the chain end position xx inside the tube: the free energy of confinement, the average end-to-end distance, the average number of imprisoned monomers, and the average stretching of the confined part of the chain for various values of DD and for the number of monomers in the chain, NN. We show that when the chain end is dragged by a certain critical distance xx^* into the tube, the polymer undergoes a first-order phase transition whereby the remaining free tail is abruptly sucked into the tube. This is accompanied by jumps in the average size, the number of imprisoned segments, and in the average stretching parameter. The critical distance scales as xND11/νx^*\sim ND^{1-1/\nu}. The transition takes place when approximately 3/4 of the chain units are dragged into the tube. The theory presented is based on constructing the Landau free energy as a function of an order parameter that provides a complete description of equilibrium and metastable states. We argue that if the trapped chain is released with all monomers allowed to fluctuate, the reverse process in which the chain leaves the confinement occurs smoothly without any jumps. Finally, we apply the theory to estimate the lifetime of confined DNA in metastable states in nanotubes.Comment: 13pages, 14figure

    Quantificação da biomassa na floresta estadual do Amapá: alometria e estimativas de estoque de carbono.

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    Material e métodos; Localização e caracterização da área; Inventário de biomassa; Inventário florestal das parcelas de biomassa; Estimativas de biomassa; Compartimentos da biomassa área e raízes das árvores; Equação de biomassa; Inventário florestal; Estimativa da biomassa fresca na FLOTA do Amapá; Estoque de carbono na FLOTA do Amapá; Teor de umidade; Teor de carbono; Estoque de carbono; Custo do levantamento de dados em campo para a quantificação da biomassa.bitstream/item/114961/1/CPAF-AP-2012-Quantificacao-da-biomassa.pd
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