Due to the second principle of thermodynamics, time dependence entropy for all kinds systems under physical circumstances always thrives interest. The logistic map $x_{t+1}=1-a x_t^2 \in [-1,1]\;(a\in [0,2])$ is neither large, since it has only one degree freedom, nor closed, dissipative. It exhibits, nevertheless, a peculiar evolution its natural entropy, which additive Boltzmann-Gibbs-Shannon...