Effective-medium theory for two-component nonlinear composites

Abstract
The effective-medium approximation (EMA) is employed to study the effective nonlinear response of a two-component composite. The first component, of fraction p, is nonlinear and obeys a current-field (J-E) characteristic of the form J=σ1 E+χ1‖E 2 E while the second component, of fraction q, is linear with J=σ2 E. Near the percolation threshold (pc or qc), we examine the conductor-insulator (C/I) limit (σ2=0) and the superconductor-conductor (S/C) limit (σ2=∞). For the C/I limit and p>pc, the effective linear- and nonlinear-response functions behave as σe≊(p-pc )t and χe≊(p-pc )2t, respectively. For the S/C limit and q<qc, σe and χe are found to diverge as σe≊(qc-q)s and χe≊(qc-q)2s. Explicit calculations are done in two dimensions and generalized to d dimensions. The exponents are found to be s=t=1 and s2=t2=2; pc=1/d and qc=(d-1)/d within EMA. For a finite-conductivity ratio h and at percolation, σe and χe are found to cross over from the fractal (h=0) to homogeneous (h=1) behavior. In the limits of small h and p-pc (or qc-q), the EMA results can be rescaled to collapse onto a universal curve. The scaling function is extracted and compared to a general scaling theory and an excellent agreement is found.