Next: Field fluctuation result
Up: Exact solutions for
Previous: Small contrast of
Another general conductivity result, due to Keller and Mendelson [18,19], for a general 2-D isotropic two phase microstructure, is that
| σ(σ1, σ2) σ(σ2,σ1) = σ1σ2 | (57) |
where σ(σ1, σ2) means the effective conductivity obtained when phase 1 has conductivity σ1 and phase 2 has conductivity σ2, and σ(σ2, σ1) means the phase conductivities have been interchanged before determining the effective conductivity.