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In the case of quenched disorder, we utilize two complementary ways to discover specific expressions for the stress. 1st method is based on direct combinatorial arguments. In the second method, we frame the model with regards to arbitrary matrices; pressure is then represented as an averaged logarithm of this trace of an item of random 3×3 matrices-either uncorrelated (Model I) or sequentially correlated (Model II).We develop the framework of classical observational entropy, that will be
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