Abstract
How can order arise from complex, irregular, and chaotic states of matter? In classical antiquity philosophers tried to take the complexity of natural phenomena back to first principles. Astronomers suggested mathematical models in order to reduce the irregular and complex planetary orbits as they are experienced to regular and simple movements of spheres. Simplicity was understood, still for Copernicus, as a feature of truth (Sect. 2.1). With Newton and Leibniz something new was added to the theory of kinetic models. The calculus allows scientists to compute the instaneous velocity of a body and to visualize it as the tangent vector of the body’s trajectory. The velocity vector field has become one of the basic concepts in dynamical systems theory. The cosmic theories of Newton and Einstein have been described by dynamical models which are completely deterministic (Sect. 2.2).
Keywords
Hamiltonian System Phase Portrait Dissipative System Vortex Point Dynamical System TheoryPreview
Unable to display preview. Download preview PDF.
References
- 2.1For historical sources of Sect. 2.1 compare Mainzer, K.: Symmetries in Nature. De Gruyter: New York (1994) (German original 1988) Chapter 1Google Scholar
- 2.2Diels, H.: Die Fragmente der Vorsokratiker, 6th ed., revised by W Kranz, 3 vol. Berlin (1960/1961) (abbrev.: Diels-Kranz), 12 A 10 (Pseudo-Plutarch)Google Scholar
- 2.3Diels-Kranz 13 A 5, B 1Google Scholar
- 2.4Diels-Kranz 22 B 64, B 30Google Scholar
- 2.5Heisenberg, W.: Physik und Philosophic Ullstein: Frankfurt (1970) 44Google Scholar
- 2.6Diels-Kranz 22 B8Google Scholar
- 2.7Diels-Kranz 31 B8Google Scholar
- 2.8Heisenberg, W.: Die Plancksche Entdeckung und die philosophischen Grundlagen der Atomlehre, in: Heisenberg, W.: Wandlungen in den Grundlagen der Naturwissenschaften. S. Hirzel: Stuttgart (1959) 163Google Scholar
- 2.9Cf. also Hanson, N.R.: Constellations and Conjectures. Boston (1973) 101CrossRefGoogle Scholar
- 2.10Hanson, NR. (see Note 9, 113) carried out corresponding calculations.Google Scholar
- 2.11Bohr, H.: Fastperiodische Funktionen. Berlin (1932)Google Scholar
- 2.12Forke, A.: Geschichte der alten chinesischen Philosophie. Hamburg (1927) 486;Google Scholar
- 2.12aFêng Yu-Lan: A History of Chinese Philosophy vol. 2: The Period of Classical Learning. Princeton NJ (1953) 120Google Scholar
- 2.13Mainzer, K.: Geschichte der Geometrie. B. I. Wissenschaftsverlag: Mannheim/ Wien/Zürich 1980 83;MATHGoogle Scholar
- 2.13aEdwards, C.H.: The Historical Development of the Calculus. Springer: Berlin (1979) 89MATHCrossRefGoogle Scholar
- 2.14Mainzer, K.: Geschichte der Geometrie (see Note 13) 100; Abraham, R.H., Shaw, C.D.: Dynamics — The Geometry of Behavior Part 1. Aerial Press: Santa Cruz (1984) 20Google Scholar
- 2.15Audretsch, J./Mainzer, K. (eds.): Philosophie und Physik der Raum-Zeit. B. I. Wissenschaftsverlag: Mannheim (1988) 30Google Scholar
- 2.16Audretsch, J./Mainzer, K. (eds.): Philosophie und Physik der Raum-Zeit (see Note 15) 40; Weyl, H.: Raum, Zeit, Materie. Vorlesung über Allgemeine Relativitätstheorie. Wissenschaftliche Buchgesellschaft: Darmstadt (1961) (Reprint of the 5th Edition (1923)) 141Google Scholar
- 2.17Mach, E.: Die Mechanik. Historisch-kritisch dargestellt. Wissenschaftliche Buchgesellschaft: Darmstadt (1976) (Reprint of the 9th Edition (1933)) 149; Abraham, R.H., Shaw, CD.: Dynamics — The Geometry of Behavior (see Note 14) 57MATHGoogle Scholar
- 2.18Ruelle, D.: Small random pertubations of dynamical systems and the definition of attractors. Commun. Math. Phys. 82 (1981) 137–151; Abraham, R.H., Shaw, CD.: Dynamics — The Geometry of Behavior (see Note 14) 45MathSciNetADSMATHCrossRefGoogle Scholar
- 2.19For an analytical elaboration cf. Stauffer, D./ Stanley, H.E.: From Newton to Mandelbrot. A Primer in Theoretical Physics. Springer: Berlin (1990) 26MATHCrossRefGoogle Scholar
- 2.20Nicolis, G./Prigogine, I.: Die Erforschung des Komplexen (see Chapter 1, Note 3) 132; Abraham, R.H./Shaw, CD.: Dynamics — The Geometry of Behavior (see Note 14) 168, 174Google Scholar
- 2.21For an analytical elaboration cf. Mainzer, K.: Symmetries in Nature (see Note 1) Chapter 3.31; Stauffer, D./Stanley, H.E.: From Newton to Mandelbrot (see Note 19) 24Google Scholar
- 2.22Arnold, V.I.: Mathematical Methods of Classical Mechanics. Springer: Berlin (1978);MATHGoogle Scholar
- 2.22aDavies, P.C.W.: The Principles of Time-Asymmetry. Surrey University Press (1974);Google Scholar
- 2.22bPenrose, R.: The Emperor’s New Mind. Oxford University Press: Oxford (1989) 181Google Scholar
- 2.23Lichtenberg, A.J./Liebermann, M.A.: Regular and Stochastic Motion. Springer: Berlin (1982);Google Scholar
- 2.23aSchuster, H.G.: Deterministic Chaos. An Introduction. Physik-Verlag: Weinheim (1984) 137MATHGoogle Scholar
- 2.24Poincaré, H.: Les Méthodes Nouvelles de la Méchanique Céleste. Gauthier-Villars: Paris (1892)Google Scholar
- 2.25Arnold, V.I.: Small Denominators II, Proof of a theorem of A.N. Kolmogorov on the preservation of conditionally-periodic motions under a small perturbation of the Hamiltonian, Russ. Math. Surveys 18 (1963), 5;ADSGoogle Scholar
- 2.25aKolmogorov, A.N.: On Conservation of Conditionally-Periodic Motions for a Small Change in Hamilton’s Function, Dokl. Akad. Nauk. USSR 98 (1954) 525;MathSciNetGoogle Scholar
- 2.25bMoser, J.: Convergent series expansions of quasi-periodic motions, Math. Anm. 169 (1967), 163Google Scholar
- 2.26Cf. Arnold, V.I.: Mathematical Methods of Classical Mechanics (see Note 22); Schuster, H.G.: Deterministic Chaos (see Note 23), 141Google Scholar
- 2.27Hénon, M./Heiles, C.: The applicability of the third integral of the motion: Some numerical experiments, Astron. J. 69 (1964), pp. 73; Schuster, H.G: Deterministic Chaos (see Note 23), 150; Figures 2.16a-d from M.V Berry in S. Jorna (ed.), Topics in nonlinear dynamics, Am. Inst. Phys. Conf. Proc. vol. 46 (1978)ADSCrossRefGoogle Scholar
- 2.28For mathematical details compare, e.g. Staufer, D./Stanley, H.E.: From Newton to Mandelbrot (see Note 19), 83Google Scholar
- 2.29Mainzer, K.: Symmetrien der Natur (see Note 1), 423; Primas, H./Müller-Herold, U.: Elementare Quantenchemie. Teubner: Stuttgart (1984) with an elementary introduction to the Galileo-invariant quantum mechanics (Chapter 3)Google Scholar
- 2.30Audretsch, J./Mainzer, K. (eds.): Wieviele Leben hat Schrödingers Katze? B. I. Wissenschaftsverlag: Mannheim (1990)Google Scholar
- 2.31Gutzwiller, M.C.: Chaos in Classical and Quantum Mechanics. Springer: Berlin (1990)MATHGoogle Scholar
- 2.32Friedrich, H.: ‘Chaos in Atomen’, in: Mainzer, K./Schirmacher, W (ed.), Quanten, Chaos und Dämonen (see Note 1 of Chapter 1); Friedrich, H./Wintgen, D.: The hydrogen atom in a uniform magnetic field, Physics Reports 183 (1989) 37–79MathSciNetADSCrossRefGoogle Scholar
- 2.33Birkhoff. G.D.: Nouvelles Recherches sur les Systems Dynamiques, Mem. Pont. Acad. Sci. Novi Lyncaei 1 (1935) 85Google Scholar
- 2.34Enz, C.P.: Beschreibung nicht-konservativer nicht-linearer Systeme I–II, Physik in unserer Zeit 4 (1979) 119–126,ADSCrossRefGoogle Scholar
- 2.34aEnz, C.P.: Beschreibung nicht-konservativer nicht-linearer Systeme I–II, Physik in unserer Zeit 5 (1979) 141–144 (II)ADSCrossRefGoogle Scholar
- 2.35Lorenz, E.N.: Deterministic nonperiodic flow, J. Atoms. Sci. 20 (1963) 130; Schuster, H.G.: Deterministic Chaos (see Note 23) 9ADSCrossRefGoogle Scholar
- 2.36Eckmann, J.P.: Roads to turbulence in dissipative dynamical systems, Rev. Mod. Phys. 53 (1981) 643;MathSciNetADSMATHCrossRefGoogle Scholar
- 2.36aComputer simulation of Fig. 2.21 from Lanford, O.E., Turbulence Seminar, in: Bernard, P./Rativ, T. (eds.): Lecture Notes in Mathematics 615, Springer: Berlin (1977) 114Google Scholar
- 2.37Mandelbrot, B.B.: The Fractal Geometry of Nature, Freeman: San Fransisco (1982);MATHGoogle Scholar
- 2.37aGrassberger, P.: On the Hausdorff Dimension of Fractal Attractors, J. Stat. Phys. 19 (1981) 25; Lichtenberg, A.J./Liebermann, M.A.: Regular and Stoachstic Motions (see Note 23)Google Scholar
- 2.38Collet, P./Eckmann, J.P.: Iterated Maps of the Interval as Dynamical Systems, Birkhäuser: Boston (1980) (see Figures 2.22–2.24)Google Scholar
- 2.39Großmann, S./Thomae, E.: Invariant distributions and stationary correlation functions of one-dimensional discrete processes, Z. Naturforsch. 32 A (1977) 1353; Feigenbaum, M.J.: Quantitative universality for a class of nonlinear transformations, J. Stat. Phys. (1978) 25MathSciNetADSGoogle Scholar
- 2.40Mainzer, K.: Symmetrien der Natur (see Note 1)Google Scholar
- 2.41Cf. Nicolis, G./Prigogine, I.: Die Erforschung des Komplexen (see Note 3, Chapter 1)205Google Scholar
- 2.42Cf. Prigogine, I.: From Being to Becoming — Time and Complexity in Physical Sciences, Freemann: San Fransisco (1980);Google Scholar
- 2.42aCf. Prigogine, I.: Introduction to Thermodynamics of Irreversible Processes, Wiley: New York (1961)MATHGoogle Scholar
- 2.43Fig. 2.26 from Feynman, R.P./Leighton, R.B./Sands, M.: The Feynman Lectures of Physics vol. II, Addison-Wesley (1965)Google Scholar
- 2.44Haken, H.: Synergetics (see Note 4, Chapter 1) 5Google Scholar
- 2.45Haken, H.: Synergetics (see Note 4, Chapter 1) 202; Haken, H.: Advanced Synergetics. Instability Hierarchies of Self-Organizing Systems and Devices. Springer: Berlin (1983) 187;MATHGoogle Scholar
- 2.45aWeinberg, S.: Gravitation and Cosmology. Principles and Applications of the General Theory of Relativity. Wiley: New York (1972)Google Scholar
- 2.46Cf. Mainzer, K.: Symmetrien der Natur (see Note 1) Chapter 4Google Scholar
- 2.47Curie, P.: Sur la Symétrie dans les Phénomènes Physiques, Journal de Physique 3 (1894) 3Google Scholar
- 2.48Audretsch, J./Mainzer, K. (eds.): Vom Anfang der Welt. C.H. Beck: München (21990);Google Scholar
- 2.48aMainzer, K.: Symmetrien der Natur (see Note 1) 515; Fritzsch, H.: Vom Urknall zum Zerfall. Die Weltzwischen Anfang und Ende. Piper: München (1983) 278Google Scholar
- 2.49Hawking, S.: A Brief History of Time. From the Big Bang to Black Holes. Bantam Press: London (1988)Google Scholar
- 2.50Audretsch, J./Mainzer, K. (eds.): Vom Anfang der Welt (see Note 48) 165Google Scholar