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
where N is the total number of elements, Ω = ln k1/kM is the logaritmic "volume" of the system, 
 is the mean relative growth and 
 is the standard deviation of the relative growth. The entropy equation of state is
where 
 is a constant that accounts for dimensionality and 
 is the elementary volume in phase space, with 
 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
- ↑ 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.
 - ↑ 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.
 
![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},](../I/m/e23d4e954efcda7645edc519a32efc06.png)
