Abstract:The model of rigid linear heat conductor with memory is reconsidered focussing the interest on the heat relaxation function. Thus, the definitions of heat flux and thermal work are revised to understand where changes are required when the heat flux relaxation function k is assumed to be unbounded at the initial time t = 0. That is, it is represented by a regular integrable function, namely k ∈ L 1 (R + ), but its time derivative is not integrable, that isk / ∈ L 1 (R + ). Notably, also under these relaxed assu… Show more
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