Scale-free ideal gas

The scale-free ideal gas (SFIG) is a physical model assuming a collection of non-interacting elements with an stochastic proportional growth. It is the scale-invariant version of an ideal gas. Some cases of city-population, electoral results and cites to scientific journals can be approximately considered scale-free ideal gases.[1]

In a one-dimensional discrete model with size-parameter k, where k1 and kM are the minimum and maximum allowed sizes respectively, and v = dk/dt is the growth, the bulk probability density function F(k, v) of a scale-free ideal gas follows


F(k,v)=\frac{N}{\Omega k^2}\frac{\exp\left[-(v/k-\overline{w})^2/2\sigma_w^2\right]}{\sqrt{2\pi}\sigma_w},

where N is the total number of elements, Ω = ln k1/kM is the logaritmic "volume" of the system, \overline{w}=\langle v/k \rangle is the mean relative growth and \sigma_w is the standard deviation of the relative growth. The entropy equation of state is

S=N\kappa\left\{\ln\frac{\Omega}{N}\frac{\sqrt{2\pi}\sigma_w}{H'}+\frac{3}{2}\right\},

where \kappa is a constant that accounts for dimensionality and H'=1/M\Delta\tau is the elementary volume in phase space, with \Delta\tau the elementary time and M the total number of allowed discrete sizes. This expression has the same form as the one-dimensional ideal gas, changing the thermodynamical variables (N, V, T) by (N, Ω,σw).

Zipf's law may emerge in the external limits of the density since it is a special regime of scale-free ideal gases.[2]

References

  1. Hernando, A.; Vesperinas, C.; Plastino, A. (2010). "Fisher information and the thermodynamics of scale-invariant systems". Physica A: Statistical Mechanics and its Applications 389 (3): 490–498. arXiv:0908.0504. Bibcode:2010PhyA..389..490H. doi:10.1016/j.physa.2009.09.054.
  2. Hernando, A.; Puigdomènech, D.; Villuendas, D.; Vesperinas, C.; Plastino, A. (2009). "Zipf's law from a Fisher variational-principle". Physics Letters A 374 (1): 18–21. arXiv:0908.0501. Bibcode:2009PhLA..374...18H. doi:10.1016/j.physleta.2009.10.027.
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