2000
DOI: 10.1002/(sici)1521-3951(200002)217:2<r10::aid-pssb999910>3.0.co;2-8
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Coarsened Lattice Spatial Disorder in the Thermodynamic Limit

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Cited by 3 publications
(3 citation statements)
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“…Now, the higher spatial inhomogeneity S ∆ (1) > S ∆ (2), see Fig.2d, favours the higher effective conductivity σ * (1) > σ * (2), while for the reverse cases we have the opposite relation, namely S ∆ (1-r) > S ∆ (2-r) and σ * (1-r) < σ * (2-r). Note the asymmetry of the S ∆ (p) curves regarding p = 0.5, which confirms the topological non-equivalence of H-and L-phases [20].…”
Section: Model and Resultsmentioning
confidence: 99%
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“…Now, the higher spatial inhomogeneity S ∆ (1) > S ∆ (2), see Fig.2d, favours the higher effective conductivity σ * (1) > σ * (2), while for the reverse cases we have the opposite relation, namely S ∆ (1-r) > S ∆ (2-r) and σ * (1-r) < σ * (2-r). Note the asymmetry of the S ∆ (p) curves regarding p = 0.5, which confirms the topological non-equivalence of H-and L-phases [20].…”
Section: Model and Resultsmentioning
confidence: 99%
“…c) The corresponding fractions of mixed bonds F M (p). d) The spatial inhomogeneity of coarsened lattice quantified by entropic measure S ∆ (p) in the thermodynamic limit [18,20].…”
Section: Model and Resultsmentioning
confidence: 99%
“…The morphological features of complex materials are vital for modelling and predicting their macroscopic properties, for instance, effective conductivity [1][2][3][4]. For binary micrographs of such materials, the quantitative characterization of the spatial distribution of pixels, in some cases allows correlate their properties and internal structure attributes.…”
Section: Introduction Sensitive Measuresmentioning
confidence: 99%