Abstract
The effective medium approximation (EMA) is derived to investigate the effective linear and nonlinear responses of two-component composites in which one component is nonspherical and distributed in shape. Both components with the volume fractions p and q are assumed to obey a current–field J–E relation of the form J = σiE + χi|E|2E, where σi and χi are the linear conductivity and nonlinear response of the component i (i = 1, 2) respectively. As the percolation threshold pc (or qc) is approached from above (or below), the effective linear conductivity σe and effective nonlinear response χe behave as σe ∼ [p − pc(Δ)]t and χe ∼ [p − pc(Δ)]t2 in the conductor/insulator (C/I) limit, and σe ∼ [qc(Δ) − q]−s and χe ∼ [qc(Δ) − q]−s2 in the superconductor/conductor (S/C) limit, where the exponents are found to be t = s = 1 and t2 = s2 = 2, independent of the shape variance parameter Δ, and pc(Δ) (or qc(Δ)) is a monotonically decreasing (or increasing) function with Δ. For a finite-conductivity ratio h = σ1/σ2, numerical results show that σe may be increased or decreased with increasing Δ, dependent on whether the first component is a good or a poor conductor, while χe can exhibit a monotonic increase, monotonic decrease and nonmonotonic behaviour. Therefore, χe can be greatly enhanced by the adjustment of the shape variance parameter, and thereby provides an alternative way to achieve large enhancement of effective nonlinear response. The results of EMA with shape distribution are also compared with exact solutions in the dilute limit and reasonable agreement is found.
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