By Professor Dr. Wolfgang Weidlich, Dr. Günter Haag (auth.)
While the volumes hitherto released within the Springer sequence in Synergetics were committed nearly completely to the self-organized formation of constructions in physics, chemistry and biology, the current monograph by means of Weidlich and Haag offers with the formation of "structures" (or "patterns") in society. initially look it can appear a bold firm to house the complicated tactics in society utilizing suggestions and strategies first constructed in physics. yet over the last decade it's been proven that there's a huge type of phenomena in various fields to which unifying techniques might be utilized. this can be particulary actual of events within which a approach composed of many components or participants acquires a brand new constitution on macroscopic scales. certainly, this can be the definition of synergetics which I formulated greater than a decade in the past, and which shaped the root of my survey at the profound analogies within the behaviour of advanced structures, includ ing these of sociology (H. Haken: Synergetics. An creation, quantity 1 of this series). As i've got mentioned on many events, the common validity of those suggestions is neither unintended neither is it because of a trifling extension of actual ideas to different fields, yet is in its place a end result of deep-rooted struc tural houses of platforms of interacting elements that are as a result of rigorous mathe maticallaws. in most cases conversing, suggestions and strategies initially utilized in physics will be utilized to sociological phenomena in ways.
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Additional info for Concepts and Models of a Quantitative Sociology: The Dynamics of Interacting Populations
94) and initially confined between x_ and x+ will never overlap x+ or x_. Case d) Fluctuation Dominated Motion. An initial distribution P (x; 0) concentrated at the potential minima x- and x+ neighbouring the unstable point Xo will now be considered. In this case a slow equilibration process will take place by means of a probability flux between the modes until the stationary distribution Pst (x) is established. Since the drift force k (x) is directed towards the minima x_ and x+, it cannot be primarily responsible for this process.
0. 2 ... 6 V cy V ~ I? AI v: I} /. 0. 0. 0. 0. 0. /. 6 / .. V .... 0. 0. 0. 0. 0. 2 V [/ . 2 --). 6 /. 0. 3a-d. Graphical solutions ofthe transcendental equation x = tanh (0 + KX) in typical cases. 36, 47] can now be made. Despite the apparent oversimplications in the model, the main assumptions of only two opinions and of one homogeneous population described by the same trend parameters seem to find some justification: In liberal societies a trend to two main parties, usually representing "progressive" and "conservative" opinions, can often be observed.
02 the expected large probability peak at x+ corresponding to the prevalence 15 > 0 is found. 5 as can be seen by comparison with Fig. 4; the strong adaptation trends present exaggerate a given preference and shift the opinion configuration to more extreme values. Even more interesting is the small probability peak at L < O. It could be assumed that - because of, say, previous history - the sample society does not belong to the large but to the small probability peak. ) This would imply that in this society a collectively stabilized opinion configuration x_ < 0 exists in contradiction to the sign and magnitude of the individual preference parameter 15 > 0 of all its individual members.