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論文資訊
- 類型：已發表論文
- 日期：2023-04-27
摘要
Due to the second principle of 熱力學s, the time dependence of 熵 for all kinds of systems under all kinds of physical circumstances always thrives interest. The logistic map …+1= 1 -…2 …& ISIN; [-1,1] (…& ISIN; [0,2]) is neither large, since it has only one degree of freedom, nor closed, since it is dissipative. It exhibits, nevertheless, a peculiar time 演化 of its natural 熵, which is the additive Boltzmann-Gibbs-Shannon one, …= - n-ary sumation …=1 …ln …, for all values of …for which the 李雅普諾夫 exponent is positive, and the nonadditive 1- n-ary sumation …=1 … one … = …-1 the number of windows of the phase space partition. We numerically show that, for increasing time, the phase-space-averaged 熵 overshoots above its stationary-state value in all cases. However, when …-+ & INFIN;, the overshooti
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