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for the motions of the bodies. Even in a three body system the motions of the bodies become chaotic and unpredictable at a detailed level. In 1890 Poincare demonstrated that it is actually impossible to solve the equations for a three body system in a simple field system, so even a system as simple as t
and accurate enough measurement today, the future course of the universe could be predicted. For mathematicians, that dictum was dashed in 1899 by Poincare's proof of the existence of chaos. PoincarE showed that not only was it impossible to derive a formula which could predict 165 EFTA00625293 the
, entropy is not maximised, but is being produced continuously; as heat flows continuously from hot to cold. 199 EFTA00625327 What Paltridge and Lorenz discovered was that the earth appeared to act in a 'deliberate' manner, by adjusting the temperatures across the globe, to a give a maximum possible
1864 Steriade, M., McCarley, R.W. (1990) Brainstem Control of Wakefulness and Sleep. Plenum. N.Y. 289 HOUSE_OVERSIGHT_013789 Stillwell, J. (1985) Poincare’s Papers on Fuchsian Groups. Springer-Verlag, N.Y. pp 1-50 Stockbridge,L.L., French,A.S. (1989) Characterization of a calcium-activated potassium ch
ormly divergent (and convergent), “hyperbolic” chaotic systems, such as brain systems, behave in Euclidean space, an intuitive similarity about which Poincare experienced his famous vacation bus trip epiphany (Stillwell, 1985). It should also be noted that encoding neural spike trains in one dimension for s
in dimension greater than two (for orbits to be more than a fixed point or limit cycle, able to snake around without necessarily intersecting ), the Lorenz attractor has dimension just a little over two, our difficulties with establishing the “true” physiological dimension of real biological observables
blished a model of it through internal reconstructions of sequential sensory experiences that_accompanied our exploratory movements. A world. It was Poincare’s habit to topologize the dynamics of motion in mathematical problems that lacked analytic solutions. In this way, simple algebraic operations repla
eer, George Birkoff (1922), was computing the output of a very reduced subset of Saltzman’s differential equations for predicting the weather (1962). Lorenz found that numerically integrated trajectories manifested unpredictable times and directions of motion between the two spiral orbits of what has come
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