Entropies above

Note that the Gibb s partition of the micro entropy above is not maximum for a near equilibrium situation. This follows from the fact that the function -xlnx 0 < x < 1, has a maximum for x = /e. Assuming that our correlation model in a more realistic dissipative system of varying occurrence of base pairs would prefer a "close to equilibrium" entropy, we find that a recalculation of our parameters above yields the trend... 

Left The mononuclear excess entropy (above that for a nonexpanded system) as a function of a self-similar expansion coordinate (inverse of scaled radius parameter, i.e., C = 1 no expansion), for unit (MeV) steps in the excitation energy per nucleon e. Right The level density parameter with expansion but m /m = 1 dotted), considering both expansion and the evolution of nik (dashed) and expansion with both mi, and (solid) are shown (Sobotka et al. 2004)... 

Despite of the rather approximate accuracy of such averaged calculations, we can make quite a reliable conclusion on the fact that business entropy, with the aggregation of its stmctures, sharply increases during the transition from the medium to large business as the quality of business processes decreases. The application of more accurate initial data allows obtaining specific values of business entropy, above which the process of economic relations can reach a critical level. 

Although the rigorous solution was not presented until 1972, Flory offered arguments in support of the scaling law Eq. (2.83) much earlier. The point of concern is the equilibrium conformation of a chain, being the result of a balance between repulsive excluded volume forces and retracting forces ar-ing from the decreasing conformational entropy. Above, with Eq. (2.78), we have already introduced Flory s expression for the potential produced by the excluded volume forces... 

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