A general method to describe Hamiltonian chaos in the thermodynamic limit is presented which is based on a model equation independent of the dynamics. This equation is derived from a geometric approach to Hamiltonian chaos recently proposed, and provides an analytic estimate of the largest Lyapunov exponent λ. The particular case of the Fermi-Pasta-Ulam β-model Hamiltonian is considered, showing an excellent agreement between the values of λ predicted by the model and those obtained with computer simulations of the tangent dynamics.
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Casetti et al. (1995) studied this question.
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