The local isochronism of the periodic oscillations of x¨=g(x) (g(x)=−xf(x), f(0)>0, so that x=0 is a center) is equivalent to the Lyapunov stability of (0,0) for the system: x¨=g(x), y¨=yg′(x). The generalization of this property for the system x¨=g(x), y¨=y[g′(x)+3αg(x)(1+αx)−1], g′(0)<0, is studied by introducing an "artificial time'' τ, τ(t,x0,x˙0)=∫t0m(x(ξ,x0,x˙0))dξ, where m is a strictly positive continuous map and x a periodic solution, and by defining a general m-isochronism relative to this "time''; e.g., the concept of m-isochronous center is used. In particular, f-isochronism and (1+αx)−2-isochronism are studied and applied.

### On the periodic oscillations of x¨=g(x)

#### Abstract

The local isochronism of the periodic oscillations of x¨=g(x) (g(x)=−xf(x), f(0)>0, so that x=0 is a center) is equivalent to the Lyapunov stability of (0,0) for the system: x¨=g(x), y¨=yg′(x). The generalization of this property for the system x¨=g(x), y¨=y[g′(x)+3αg(x)(1+αx)−1], g′(0)<0, is studied by introducing an "artificial time'' τ, τ(t,x0,x˙0)=∫t0m(x(ξ,x0,x˙0))dξ, where m is a strictly positive continuous map and x a periodic solution, and by defining a general m-isochronism relative to this "time''; e.g., the concept of m-isochronous center is used. In particular, f-isochronism and (1+αx)−2-isochronism are studied and applied.
##### Scheda breve Scheda completa Scheda completa (DC)
1989
Isochronism, generalized isochronism, Lyapunov stability
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Utilizza questo identificativo per citare o creare un link a questo documento: `https://hdl.handle.net/11562/393343`
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