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Annals of Systems Research: Publikatie van de Systeemgroep Nederland Publication of the Netherlands Society for Systems Research PDF

139 Pages·1977·4.505 MB·English
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Preview Annals of Systems Research: Publikatie van de Systeemgroep Nederland Publication of the Netherlands Society for Systems Research

ANNALS OF SYSTEMS RESEARCH VOL. 5 In the ANNALS OF SYSTEMS RFSEARCH are published original papers in the field of general systems research, both of a mathematical and non-mathematical nature. Research reports on special subjects which are of importance for the general development of systems research activity as a whole are also acceptable for publication. Accepted languages are English, German and French. Manuscripts in three-fold should be typewritten and double spaced. Special symbols should be inserted by hand. The manuscripts should not contain directions to the printer, these have to be supplied on a separate sheet. The author must keep a copy of the manuscript. The title of the manuscript should be short and informative. An abstract and a mailing address of the author must complement the manuscript. Illustrations must be added in a form ready for reproduction. Authors receive 25 offprints free of charge. Additional copies may be ordered from the publisher. All manuscripts for publication and books for review should be sent to: H. Koppelaar Associate Editor Annals of Systems Research Institute for Methodology and Statistics State University Utrecht Oudenoord 6 Utrecht, the Netherlands ANNALS OF SYSTEMS RESEARCH VOLUME 5, 1976 PUBLIKA TIE VAN DE SYSTEEMGROEP NEDERLAND PUBLICATION OF THE NETHERLANDS SOCIETY FOR SYSTEMS RESEARCH EDITOR B. V AN ROOTSELAAR Social Sciences Division tMartinus~ijhoff CLeiden 1976 ISBN-IJ: 978-90-207-0657-4 e-ISBN-IJ: 978-1-4613-4243-4 001: 10.10071978-1-4613-4243-4 © 1976 H. E. Stenfert Kroese B.V./Leiden - The Netherlands PREFACE The Netherlands Society for Systems Research was founded on 9 May 1970 to promote interdisciplinary scientific activity on basis of a systems approach. It has its seat in Utrecht, The Netherlands. Officers for the years 1975/1976: President: G. Broekstra, University of Delft Secretaries: G. De Zeeuw, University of Amsterdam (acting secretary) G. R. Eyzenga, University of Groningen Treasurer: J. N. Herbschleb, Computer Laboratory, Department of Cardio logy, University Hospital, CatharijnesingellOl, Utrecht. All information about the society can be obtained from the acting secretary. The editor is happy to announce that H. Koppelaar from the State University Utrecht will act as associate editor of the Journal. Moreover, the following scientists have declared to be willing to act as member of the editiorial board: Professor G. Klir, State University of New York, Binghamton, New York, U.S.A. Professor S. Braten, Institute of Sociology, University of Oslo, Blindern, Norway Professor B. R. Gaines, Department of Electrical Engineering Science, Univer sity of Essex, Colchester, U.K. Professor Maria Nowakowska, Department of Praxiology, Polish Academy of Sciences, Warszawa, Poland. Professor F. Pichler, Department of Systems Theory, Johannes Kepler Univer sity, Linz-Auhof, Austria. Professor B. Zeigler, Department of Applied Mathematics, Weizmann Institute of Science, Rehovot, Israel. The editor ADDRESSES OF AUTHORS Broekstra, G., Graduate School of Management, Poortweg 6-8, Delft, The Netherlands. Dalenoort, G. J., Institute for experimental psychology, State University Groningen, Biological Centre, Section D, Kerklaan 30, Haren (Gr.), The Netherlands. Klir, G. J., School of Advanced Technology, State University New York, Binghamton, N.Y. 13901, U.S.A. Kooijman, S. A. L. M., Institute for theoretical biology, Stationsweg 25, Leiden, The Netherlands. Koppelaar, H., Institute for Methodology and Statistics, State University Utrecht, Oudenoord 6, Utrecht, The Netherlands. Masser, I., Institute for Urban and Regional Planning, Heidelberglaan 2, Utrecht, The Netherlands. Scheurwater, J., Institute for Urban and Regional Planning, Heidelberglaan 2, Utrecht, The Netherlands. Uyttenhove, Hugo J. J., School of Advanced Technology, State University New York, Binghamton, N.Y. 13901, U.S.A. CONTENTS Koppelaar, Ho: Predictive Power Theory 1-5 0 0 0 0 0 0 0 0 0 0 0 Dalenoort, Go Jo: Collectivity in information-processing systems 7-28 Klir, Go, Uyttenhove, Ho Jo Jo: Computerized methodology for structure modelling 29-65 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Broekstra, Go: Constraint analysis and structure identification 67-80 Masser, I., Scheurwater, Jo: Spatial interaction in the Amersfoort region: a systems analysis 81-112 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Kooijman, So A. L. Mo: Some remarks on the statistical analysis of grids, especially with respect to ecology 113-132 Editor's note 133 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 PREDICTIVE POWER THEORY HENK KOPPELAAR Summary Mulder's 'Game for Power', published in [I], has been fully formalized in [2] according to a method originated by Popper. We exploit this psychological theory further. Our results pertain to an overall analysis of the theory, whereby encompassing computer-simulation. 1. Introduction After publication of [2] by Hezewijk et al., some work was left to be done on Mulder's Power Theory [1], because this publication provided a transformation of Mulder's theory in terms of Forresters programming language DYNAMO [3] and we expected it to be feasible to reformulate the DYNAMO - version into differential equations. Model formulations in terms of differential equations are most suitable for an overall analysis of the model. With 'overall analysis' we mean the phase plane method which facilitates the prediction of systems behaviour for any point in time and any parameter value. Hence the name 'predictive power theory' for our exposition in the sequel. The reformulation of DYNAMO-statements in terms of differential equa tions is quite straight-forward, as follows. By definition: d Xi() _ /. X(t+h) -X(t) - t - 1m ---"---'-------'-'- dt h~O h In view of this definition, the D YNA M0 equation X.K = X.J + DT * Y.K (1) where DT > 0, is reformulated in ~ X(t) = Y(t) (2) dt So (1) is the straight-forward Euler discretization of (2). Annals of Systems Research,S (1976), 1-5 2 H. KOPPELAAR 2. Reformulation of the theory Hezewijk et al. [2], formulate the following (p. 56) KOSWI.KL = (ljAT) (MA.K • PER VAl • REALI) (3) BATWI.KL = (ljAT) (MA.K • GENI • REALI) (4) + KOBAI.K = KOBAI.J (DT) (KOSWI.JK - BATWI.JK) (5) where pervai, geni and reali are personality constants. We reformulate (3), (4) and (5) in one equation (6) ~ KOBA l(t) = _1 . [(PERVA I - GENI)REALI] MA(t) (6) dt AT The rest of the statements in [2] are VERSTI.KL = (ljAT) (MA.K • PERVAI) (7) + MANST.K = MANST.J (DT) (VERSTI.JK) (8) BATWE.KL = (ljAT) (MA.K • GENE. REALE) (9) KOSWE.KL = (ljAT) (MA.K • PERVAE • REALE) (10) + KOBAE.K = KOBAE.J (DT) (KOSWE.JK-BATWE.JK) (11) VERSTE.KL = (ljAR) (MA.K • PERVAE) (l2) + MAVST.K = MAVST.J (DT) (VERSTE.JK) (13) MAN.KL = (lIAT) (MANST.K-KOBAI.K) (14) MA V.KL = (ljAT) (MAVST.K - KOBAE.K) (15) MA.K = MA.J + (DT) (MAV.JK-MAN.JK) (16) The reformulation in terms of differential equations is for (7), (8): ~ MANST(t) = (ljAT) (PERVAI)MA(t) (17) dt for (9), (10), (11): ~ KOBAE(t) = (ljAT) [(PER VAl -GENE)REALE] dt MA(t) (18) for (12), (13): ~ MAVST(t) = (1IAT) (PERVA E)MA(t) (l9) dt 3. The Formal Power Theory Our excursion into previous work [2] on Mulder's theory yields equations: (6), (14), (15), (17), (18), (19). As a matter of fact these can be substituted directly into (16) without loss of generality, pertaining to one second order equation: PREDICTIVE POWER THEORY 3 d2 dt MA(t) = ac2.MA(t) (20) 2 where a = PERVAE-PERVAl-(PERVAE-GEN)REALE (PER VAl - GEN/)REALI c = ItAT, AT >0 In algebraic format (20) reads: (0, ') ~ (21) (xo) = (xo) Xl ac 0 Xl where: Xo == xo(t) = MA(t) d and Xl == xl(t) = - MA(t) dt From our substitution of (14) and (15), in (16) we know ~ + MA(t)lr=o = (1tA]) (MAVST(O)-KOBAE(O)-MANST(O) dt +ro~~) ~ Formula (21) represents the whole model given in [2], where (22) represents an initial condition of X I. 4. Predictions from the model The model for Mulder's Power Theory [1] is d - x(t) = Ax(t) dt COc ~) where x(t) is a vector (xo(t), XI(t»T and A = 2 with constants a and c according to (20) and initial conditions. In the case det(A) = -ac2 > 0 we have in the phase-plane a centre point in the origin, fig. 1. ° In the case det(A) = -ac2 < we have in the phase-plane a saddle point in the origin, with asymptotes X I = ± Xo, fig. 2. The case det(A) = 0, that is if a = 0, means that the system is in equilibrium, psychologically this says that the power distance is constant, because of the personality structure between the more and the less powerful person.

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