Abstract
This paper deals with the critical elastic behavior of a two-dimensional micropolar (or "granular") network with randomly rigid or elastic bonds. It presents a new derivation of Feng's inequalities 1<s<s in the context of micropolar elasticity (where s is the conductivity exponent, s the elastic-moduli exponent). In addition, an exact calculation on a fractal model suggests that s=sΔS, where ΔS is a correction of order 20%. This correction results from the rotations of the rigid clusters, and differs from the "eccentricity" correction ΔE found in the elastic case.