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Oscillatory Dynamics of Urban Hierarchies 900–2000 Vulnerability and Resilience

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Book cover Computational Models of Complex Systems

Part of the book series: Intelligent Systems Reference Library ((ISRL,volume 53))

Abstract

We show the fallacies of the Zipfian and power-law views in quantitative analyses of city-size distributions and of the notion that they are superior, simpler, and more universal than q-exponential or Pareto II distributions because of the single-parameter assumption. Both sets of models have two parameters, but the q-exponential captures a scaling coefficient that is fundamental to understanding now the distribution of smaller sizes that is left out by the “cutoff” parameter of Zipfian and power-law. The additional parameter has a fundamental importance in understanding the historical dynamics of partially independent changes in the parameters of urban hierarchies and their interactions with the trading, larger resource bases and conflict networks (internal and external) in which city networks are embedded. We find, for the historical periods from 900 to 2000, combining Chandler and U.N. data, in three different regions of Eurasia, that q, as a small-city distribution parameter, has a time-lagged effect on \(\beta \), as a measure of only power-law inflection on the top 10 regional cities in China, Europe and Mid-Asia. Taking other time-lag measures into account, we interpret this as showing that trade, economic and conflict or socio-political instability in towns and smaller-cities of urban hierarchy have a greater effect on the health and productivity of larger cities as reflected in Zipfian size distributions, with growth proportional to size. As a means to help the reader understand our modeling efforts, we try to provide foundational intuitions about the basis in “nonextensive” physics used to improve our understanding how q-exponentials are derived specifically for non-equilibrium networks and distributions with long-range process that interconnect different parts, such as trade and transport systems, warfare and interpolity rivalries. The ordinary entropic measure e is “extensive” in that interactions of random effects are additive; the nonextensive generalization of \(e_{q}\) where \(e_{q=1} = e\) is ordinary Boltzmann-Gibbs entropy and the concept of multiplicative departures from randomness in the range \(1\ {<}\ q\ {<}\ 2\) helps to relate the physical processes subsumed in urban systems to the underlying foundation of certain Zipfian distributions from contributions to the non-Zipfian properties of the smaller cities in urban hierarchies.

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Notes

  1. 1.

    From 900 CE to 1970 his size estimates cover over 28 historical periods, usually spaced at 50-year intervals, always comprises a set of largest cities suitable for scaling in a single period. These large stable (and total) cities include 20(80) Chinese, 18(91) European, and 22(\({\sim }90\)) Mid-Asian.

  2. 2.

    Batty builds on an earlier working paper [36] on effects of interactions between cities, developed as a part of a common ISCOM project and now published as Chap. 9, In, G. Modelski, T. Devezas and W. Thompson, eds. pp. 190–225. London: Routledge.

  3. 3.

    As part of the same project ISCOM, see: Bettencourt, L. M. A., José Lobo, Dirk Helbing, Christian Kühnert , and Geoffrey B. West. [7].

  4. 4.

    Fujita, M. A., A. J. Venables, P. Krugman. [12].

  5. 5.

    Prima facie, because cities appear and disappear, preservation of a Zipfian distributional shape is impossible.

  6. 6.

    Zipfian rank-size for cities ranked 1 to n in size is also equivalent to the tendency to approximate a size of M/r, where r is a city’s rank compared to the largest city and M is a maximum city size that best fits the entire distribution. This formulation allows the rank 1 largest city size S1 to differ from its expected value under a Zipfian fitted to an extensive set of the larger cities.

  7. 7.

    See Clemente and Gonzalez-Val [10].

  8. 8.

    \(q=1\) is simply the standard free energy distribution of Boltzmann-Gibbs, \({\mathrm{e}_{\mathrm{q}=1=\mathrm{{BG}}}}^\mathrm{x}\), analogous to a cumulative distribution function (CDF) over a process with a Boltzmann constant k and in which independent events occur at a constant average rate, except that in \({\mathrm{e}_\mathrm{{BG}}}^{\mathrm{x}=\mathrm{W}}=k\ln W\) the average of equiprobable events in the interaction space W is logarithmic. Thus BG entropies are additive but \({\mathrm{e}_\mathrm{q}}^\mathrm{x}\) for \({q}>1\) are not.

  9. 9.

    Another parameter for each curve (derived from \(\uptheta \) and \(\upsigma \) of Pareto II) is the value of x where the line on the upper left of each graph as in Fig. 2 intersect with asymptotic power-law line of the tail. We do not use this cutoff for the Chandler data because the lowest city sizes are missing and the top of the graph is truncated. Bercher and Vignat’s [5] references [29,37] list standard statistical derivations for Pareto II, including those [32,34] that give MLE results, including Shalizi’s.

  10. 10.

    See Appendix A for the calculation and explanation of these 2 parameters. Bootstrap estimates of the standard error and confidence limits of the \(q,\kappa \) parameters derived from \(\Theta ,\sigma \) are provided by Shalizi’s [27] R program for MLE.

  11. 11.

    Variables q and \(\upbeta \) have the lowest cross-correlations for Mid-Asia, but detailed examination of the Mid-Asia time-lags shows a weak cyclical dynamic of Hi-\(\mathrm{q}{\rightarrow }{\text {Lo-}}{\upbeta } {\rightarrow }{\text {Lo-}}\mathrm{q}{\rightarrow }{\text {Hi-}}{\upbeta }\) that holds to 1950.

  12. 12.

    The dynamics is analyzed using an extrapolated Chandler [9] data such that the time lag is at 25 years.

  13. 13.

    Socio-political instability index (SPI), I, is binary with a value of 1 to indicate instability and 0 otherwise. The rules to indicate instability are as follows: (1) A higher number of wars that are not isolated and affected the areas of conflicting interests; (2) natural disasters that significantly affect population (ex: the Black Death); (3) a significant mobility of population due to domestic socio-political unrest (ex: the movement of Song Dynasty’s capital from north to south).

  14. 14.

    There are two additional constants (\(C\beta \) and Cq). All coefficients have \(\mathrm{p}<0.021\) for both equations. The specific coefficients are \(-0.441\), 0.363, 1.316, and \(-0.088\) for Eq. (1) and \(-0.907\), 0.573, and 1.580 for Eq. (2).

  15. 15.

    A two-equation reciprocal time-lag model such as Eqs. (1) and (2) produces fluctuations if the signs of the right hand elements are opposite, but convergence or divergence if they are the same. This can be verified in difference equations using initial values that generate a full time series.

  16. 16.

    Technically, the mathematics assigned to chaos is a deterministic departure from randomness in which a dynamic trajectory never settles down into equilibrium, and small differences in initial conditions lead to divergent trajectories. The link between empirical history and “edge of chaos” is typically done by simulation.

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Appendix A: Example of the European City-Size Distribution

Appendix A: Example of the European City-Size Distribution

Figures 16 and 17 show the raw European cumulative city-size distributions truncated to the top 20 cities for each of Chandler’s historical periods. The x-axis gives city rank. The y-axis in Fig. 16 is the natural log e of city size, unlabeled. Figure 17 shows the same data in a log10-log10 plot, where city rank is also logged and the y axis should be multiplied by 100. If the latter plot showed straight lines, the distributions would be Pareto I power-laws. Cutoffs can be seen for each of the lines, an indication that the Pareto II q-exponential is more relevant for these distributions. Minimum top-ranked city-sizes recorded by Chandler [9] are as small as 11,000 persons, but not lower, so that cities of sizes down to 5,000 are not included. Although the q-exponential has two parameters, a power-law fit to these data would also require a second parameter for each distribution, the size at which the distributions of higher sizes is power-law.

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White, D.R., Tambayong, L. (2014). Oscillatory Dynamics of Urban Hierarchies 900–2000 Vulnerability and Resilience. In: Mago, V., Dabbaghian, V. (eds) Computational Models of Complex Systems. Intelligent Systems Reference Library, vol 53. Springer, Cham. https://doi.org/10.1007/978-3-319-01285-8_10

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