Transport and Percolation Theory in Weighted Networks (original) (raw)

Current Flow in Random Resistor Networks: The Role of Percolation in Weak and Strong Disorder

We study the current flow paths between two edges in a random resistor network on a L ϫ L square lattice. Each resistor has resistance e ax , where x is a uniformly distributed random variable and a controls the broadness of the distribution. We find that: ͑a͒ The scaled variable u ϵ L / a , where is the percolation connectedness exponent, fully determines the distribution of the current path length ᐉ for all values of u. For u ӷ 1, the behavior corresponds to the weak disorder limit and ᐉ scales as ᐉ ϳ L, while for u Ӷ 1, the behavior corresponds to the strong disorder limit with ᐉ ϳ L d opt , where d opt = 1.22± 0.01 is the optimal path exponent. ͑b͒ In the weak disorder regime, there is a length scale ϳ a , below which strong disorder and critical percolation characterize the current path.

Conductance distributions in random resistor networks. Self-averaging and disorder lengths

Journal of Statistical Physics, 1994

The self averaging properties of the conductance g are explored in Random Resistor Networks (RRN) with a broad distribution of bond strengths P (g) ∼ g µ−1 . The RRN problem is cast in terms of simple combinations of random variables on hierarchical lattices. Distributions of equivalent conductances are estimated numerically on hierarchical lattices as a function of size L and the distribution tail strength parameter µ. For networks above the percolation threshold, convergence to a Gaussian basin is always the case, except in the limit µ → 0. A disorder length ξ D is identified, beyond which the system is effectively homogeneous. This length scale diverges as ξ D ∼ |µ| −ν , (ν is the regular percolation correlation length exponent) when the microscopic distribution of conductors is exponentially wide (µ → 0). This implies that exactly the same critical behavior can be induced by geometrical disorder and by strong bond disorder with the bond occupation probability p ↔ µ. We find that only lattices at the percolation threshold have renormalized probability distributions in a Levy-like basin. At the percolation threshold the disorder length diverges at a critical tail strength µ c as |µ − µ c | −z with z ∼ 3.2 ± 0.1, a new exponent. Critical path analysis is used in a generalized form to give the macroscopic conductance in the case of lattices above p c .

Anomalous Conductance and Diffusion in Complex Networks

We study transport properties such as conductance and diffusion of complex networks such as scale-free and Erdős-Rényi networks. We consider the equivalent conductance G between two arbitrarily chosen nodes of random scale-free networks with degree distribution P (k) ∼ k −λ and Erdős-Rényi networks in which each link has the same unit resistance. Our theoretical analysis for scale-free networks predicts a broad range of values of G (or the related diffusion constant D), with a power-law tail distribution ΦSF(G) ∼ G −g G , where gG = 2λ − 1. We confirm our predictions by simulations of scale-free networks solving the Kirchhoff equations for the conductance between a pair of nodes. The power-law tail in ΦSF(G) leads to large values of G, thereby significantly improving the transport in scale-free networks, compared to Erdős-Rényi networks where the tail of the conductivity distribution decays exponentially. Based on a simple physical "transport backbone" picture we suggest that the conductances of scale-free and Erdős-Rényi networks can be approximated by ckAkB/(kA + kB) for any pair of nodes A and B with degrees kA and kB. Thus, a single parameter c characterizes transport on both scale-free and Erdős-Rényi networks.

Conductivity in percolation networks with broad distributions of resistances

Physical Review B, 1986

Diluted resistor networks with a broad distribution of resistances are studied near the percolation threshold. A hierarchical model of the backbone of the percolation cluster is employed. Resistor networks are considered where the resistors, R, are chosen from a distribution having a power-law tail such that ProbI R~XI-X as X~ao, 0&a & 1. Such distributions arise natura11y in continuum percolation systems. The hierarchical model is studied numerically and using a renormalization-group transformation for the distribution of resistances. The conclusion is that the conductivity exponent t is the greater of t, and (d-2)v+1/a where t, is the universal value of the conductivity exponent and v is the correlation-length exponent. This result is in agreement with Straley's earlier predictions [

ε Expansion for the Conductivity of a Random Resistor Network

Physical Review Letters, 1984

We present a reanalysis of the renormalization-group calculation to first order in ε=6−d, where d is the spatial dimensionality, of the exponent, t, which describes the behavior of the conductivity of a percolating network at the percolation threshold. If we set t=(d−2)ν p +ζ, where ν p is the correlation-length exponent, then our result is ζ=1+(ε/42). This result clarifies several previously paradoxical results concerning resistor networks and shows that the Alexander-Orbach relation breaks down at order ε.

Investigation of the conductivity of random networks

Physica A: Statistical Mechanics and its Applications, 1999

This work presents the results of numerical simulations concerning the electrical conductivity of two-component random resistor networks in d = 3 as a model of composite media. Finite di erence calculations have been carried out for several system sizes, conductance ratios and occupation numbers. Using an electric analogy an equation is developed empirically which ÿts the data at conductivity ratios of f = 0:5-0.01. At f = 0:001 enhanced deviations occur which are diminished by introducing an additional parameter in the epirical equation. The percolation threshold was determined to be about p * = 0:25.

Anomalous Transport in Scale-Free Networks

To study transport properties of scale-free and Erdős-Rényi networks, we analyze the conductance G between two arbitrarily chosen nodes of random scale-free networks with degree distribution Pk k ÿ in which all links have unit resistance. We predict a broad range of values of G, with a power-law tail distribution SF G G ÿg G , where g G 2 ÿ 1, and confirm our predictions by simulations. The power-law tail in SF G leads to large values of G, signaling better transport in scale-free networks compared to Erdős-Rényi networks where the tail of the conductivity distribution decays exponentially. Based on a simple physical ''transport backbone'' picture we show that the conductances of scale-free and Erdős-Rényi networks are well approximated by ck A k B =k A k B for any pair of nodes A and B with degrees k A and k B , where c emerges as the main parameter characterizing network transport.

Scaling Law of Resistance Fluctuations in Stationary Random Resistor Networks

Physical Review Letters, 2000

In a random resistor network we consider the simultaneous evolution of two competing random processes consisting in breaking and recovering the elementary resistors with probabilities W D and W R . The condition W R . W D ͑͞1 1 W D ͒ leads to a stationary state, while in the opposite case, the broken resistor fraction reaches the percolation threshold p c . We study the resistance noise of this system under stationary conditions by Monte Carlo simulations. The variance of resistance fluctuations ͗dR 2 ͘ is found to follow a scaling law j p 2 p c j 2k0 with k 0 5.5. The proposed model relates quantitatively the defectiveness of a disordered media with its electrical and excess-noise characteristics. PACS numbers: 85.40.Qx, 05.40.Ca, 68.35.Rh, 72.70.+m Random resistor networks (RRN) have proven to be a useful model of electronic transport through disordered media . To this purpose, several percolation approaches have been applied to RRNs to investigate complex interactions where structural or electronic rearrangements modify the properties of the system under investigation. Examples include biological systems [2], electronic transport in composite materials , amorphous and crystalline semiconductors , or breakdown of electrical properties . Recently, degradation toward failure has been addressed successfully with standard and biased percolation models .

Transfer matrix calculation of conductivity in three-dimensional random resistor networks at percolation threshold

Journal de Physique Lettres, 1983

2014 Pour des barreaux de taille n x n x L, avec L ~ n et n ~ 18, nous calculons la conductivité d'un réseau aléatoire de conducteurs et d'isolants. Au seuil de percolation sur un réseau cubique simple, nos résultats Monte Carlo donnent une conductivité qui décroît comme n-2,1 quand la largeur n du barreau augmente pour la percolation de sites et celle de liens. Quand on tient compte des corrections au scaling avec un exposant de correction 03C9 d'ordre 1, notre meilleure estimation pour l'exposant t de la conductivité est t/v = 2,2 ± 0,1 à la fois pour le cas des liens et celui des sites. Ces résultats sont en accord avec la conjecture de Alexander-Orbach t/v ~ 2,26 pour l'exposant de la conductivité en dimension 3. Abstract. 2014 For very long bars of size n x n x L, with L ~ n, and n up to 18, we calculate the conductivity of a random network of resistors and insulators. At the percolation threshold in a simple cubic lattice our Monte Carlo data give a conductivity decreasing with bar diameter n as n-2.1 for site and bond percolation. Taking into account corrections to scaling with a correction exponent 03C9

Conduction in rectangular quasi-one-dimensional and two-dimensional random resistor networks away from the percolation threshold

Physical Review E, 2009

In this study we investigate electrical conduction in finite rectangular random resistor networks in quasione and two dimensions far away from the percolation threshold p c by the use of a bond percolation model. Various topologies such as parallel linear chains in one dimension, as well as square and triangular lattices in two dimensions, are compared as a function of the geometrical aspect ratio. In particular we propose a linear approximation for conduction in two-dimensional systems far from p c , which is useful for engineering purposes. We find that the same scaling function, which can be used for finite-size scaling of percolation thresholds, also applies to describe conduction away from p c . This is in contrast to the quasi-one-dimensional case, which is highly nonlinear. The qualitative analysis of the range within which the linear approximation is legitimate is given. A brief link to real applications is made by taking into account a statistical distribution of the resistors in the network. Our results are of potential interest in fields such as nanostructured or composite materials and sensing applications.