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Differential effective medium theory and effective particle mapping

Differential effective medium theory (D-EMT) [19] was chosen as the best candidate for the concrete problem as shown in Fig. 1 for the following reason. The accuracy of an EMT is often linked to how well its percolation properties match those of the experimental system being considered [17,20]. In D-EMT, the inclusions are always discontinous, and the matrix is always continuous. This is the same situation for concrete, with discontinuous aggregates embedded in a continuous matrix. So it might be expected that D-EMT would work well for concrete.

One should note, however, that several modeling and experimental studies have shown that in a typical concrete, the ITZ regions are themselves percolating [21,22,23]. The form of D-EMT considered in this paper will not reflect this fact, although it will take the ITZ into account. However, whether or not percolation of a phase matters to the overall properties depends on the contrast of its properties with those of the surrounding phases [9,24]. For the case of diffusion through concrete, the ITZ property is at most ten times that of the matrix, which is not enough of a contrast for percolation to matter particularly [9]. So this deficiency in D-EMT should not significantly affect the accuracy of D-EMT for this problem. However, if the problem of fluid permeability were being considered [9], where the contrast between ITZ and matrix is on the order of 100, then most likely D-EMT would fail, as the percolation of the ITZ regions would then matter greatly. In that case, any approach not taking ITZ percolation into account is unlikely to be accurate.




Next: Standard D-EMT Up: Main Previous: Introduction