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A strange attractor! pp 273-312 | Steklov Math. Shimada I., 1979, “Gibbsian distribution on the Lorenz attractor,” Prog. 82, 137. 26, 683. Phys. Phys. Johnson, R. A., K. J. Palmer, and G. Sell, 1984, “Ergodic properties of linear dynamical systems,” preprint, Minneapolis. 4, 21 [Russian Math. Mahé, R., 1983, “Liapunov exponents and stable manifolds for compact transformations,” in Geometrical Dynamics, Lecture Notes in Mathematics 1007 (Springer, Berlin), pp. Young, L: S., 1984, “Dimension, entropy and Liapunov exponents in differentiable dynamical systems,” Physica A 124, 639. 114, 309. The systematic investigation of these quantities provides us for the first time with a reasonable understanding of dynamical systems, excited well beyond the quasiperiodic regimes. Math. The evolution of the weather thus boils down to following trajectories in a vector field. 2, 1. Caffarelli, R., R. Kohn, and L. 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A phase space model of a pendulum will chart a series of points growing closer to the low point each time their trajectory takes them past it, until they cluster around the low point in a stable configuration. Math. Grebogi, C., E. Ott, and J. Mandelbrot, B., 1982, The Fractal Geometry of Nature ( Freeman, San Francisco). McCluskey, H., and A. Manning, 1983, “Hausdorff dimension for horseshoes,” Ergod. Lett. Croquette, V., 1982, “Déterminisme et chaos,” Pour la Science 62, 62. Math. These keywords were added by machine and not by the authors. A 57, 397. 53, 242. The Lorenz Equations, Bifurcations, Chaos, and Strange Attractors (New York: Springer-Verlag, 1982). Young, L.-S., 1981, “Capacity of attractors,” Ergod. Mat. Theor. 73, 115. Strange attractors appear in both natural and theoretical diagrams of phase space models. 2, 109. Lorenz discovered this sensitivity to initial conditions in his model. Guckenheimer, J., 1982, “Noise in chaotic systems,” Nature 298, 358. Math. All this is of course very simplistic in comparison with the real weather phenomena, but it illustrates the fact that mathematicians love simple things. Hénon, M., 1976, “A two-dimensional mapping with a strange attractor,” Commun. Sci. Ruelle, D., 1982b, “Large volume limit of the distribution of characteristic exponents in turbulence,” Commun. Ressler, O. E., 1976, “An equation for continuous chaos,” Phys. Phys. Rev. 4, 55 (1977)]. Math. © 2020 Springer Nature Switzerland AG. Henri Poincaré, 42, 109. Newhouse, S., 1974, “Diffeomorphisms with infinitely many sinks,” Topology 13, 9. Wilkinson, J. H., and C. Reinsch, 1971, Linear Algebra (Springer, Berlin). 3 (237), 3. Sinai, Ya. Wolf, A., J. Cvitanovié, P., 1984, Ed., Universality in Chaos ( Adam Hilger, Bristol). How do the internal dynamics behave? Foias, C., and R. Temam, 1979, “Some analytic and geometric properties of the solutions of the evolution Navier-Stokes equations,” J. 177–215. G., 1972, “Gibbs measures in ergodic theory,” Usp. IHES 51, 137. But actually science works mainly by metaphor. Fenn. 19, 179 Moscow Math. Carverhill, A., 1984a, “Flows of stochastic systems: ergodic theory,” Stochastics, in press. Phys. 1, 381. Phys. Math. Mat. The notion of strange attractors and chaos goes further and suggests that no single mindset should be seen as the appropriate to all settings. Adler, R. L., A. G. Konheim, and M. H. McAndrew, 1965, “Topological entropy,” Trans. ... A strange attractor! Lieb, E. H., 1984, “On characteristic exponents in turbulence,” Commun. II, 343. Theory Dynam. A 14, 2338. Phys. As the Navier-Stokes equations that describe fluid dynamics are very difficult to solve, he simplified them drastically.Â The model he obtained probably has little to do with what really happens in the atmosphere.

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