Abstract

A continued fraction representation for the effective conductivity tensor σ* of a two-dimensional polycrystal is derived. This representation is in terms of a sequence of positive definite symmetric matrices which characterize the underlying geometric structure of the material. The proof is accomplished by considering a particular basis for the Hilbert space of fields in the composite in which the linear operators relevant to determining the effective conductivity take simple forms as infinite matrices. These infinite matrices are then used in the variational definition of the effective conductivity to formulate the continued fraction. This continued fraction is used to derive upper and lower bounds on σ*.

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