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11 Socio-Economic Modeling
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           Fig. 11.1. Angra dos Reis, Brazil: on the w = o(1)-part of the Pareto distribution


























           Fig. 11.2. Salvador de Bahia, Brazil: on the w = o(1)-part of the Pareto distribution


           same effect can also be obtained by simply allowing the random variables in the
           trading laws (11.6) to assume values on the whole real axis, and at the same time
           discarding those trades for which one of the post-trade wealths is non-positive.
              A critical analysis of the discussed collision=trading rules reveals a deep
           analogy between the economic models described above and the granular ma-
           terial flows modeling framework of Chapter 3. They share the property that
           the steady (or, more generally, the self-similar asymptotic) states are different
           from the classical Maxwell distribution of the Boltzmann equation of gas dy-
           namics presented in Chap. 1. Another analogy becomes evident when looking
           at the non-conservative properties of the economic and granular Boltzmann
           equations, resulting from inelastic binary collision models.
              Conservativeexchangedynamicsbetweenindividualsredistributethewealth
           among people. Without conservation, the best way to extract information on the
           large-time behavior of the solution relies on scaling the solution itself to keep
           the average wealth constant after scaling. Nevertheless, the explicit form of the
           limit distribution of the kinetic equation remains extremely difficult to recover,
           and often requires the use of suitable numerical methods.
              A complementary method to extract information on the steady state distri-
           bution was linked in [5] to the possibility of obtaining particular asymptotics,
           which mimic the characteristics of the solution of the original problem for large
           times. The main result in this direction was to show that the kinetic model
           converges (under appropriate assumptions) in a suitable scaling limit to a par-
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