Abstract
On the basis of the transformation to the rotating coordinates associated with the imbedded unstable limit cycles in the Lorenz system, we present a new representation for the long time averages, which may be applicable to any three-dimensional dissipative dynamical systems producing chaos. By employing the dynamics of the phases of the imbeddid limit cycles, we show that the time average is expressible in terms of two types of the weight factors; the residence time probability density and the factor inbersely proportional to the speed of the phase.

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