In this paper we discuss some general aspects of the so-called geometrodyna
mical approach (GDA) to Chaos and present some results obtained within this
framework. We firstly derive a naive but nevertheless a general geometriza
tion procedure, and then specialize the discussion to the description of mo
tion within the framework of two among the most representative implementati
ons of the approach, namely the Jacobi and Finsler geometrodynamics. In ord
er to support the claim that the GDA is not simply a mere re-transcription
of the usual dynamics, but instead can give various hints on the understand
ing of the qualitative behaviour of dynamical systems (DS's), we then compa
re, from a formal point of view, the tools used within the framework of Ham
iltonian dynamics to detect the presence of Chaos with the corresponding on
es used within the GDA, i.e., the tangent dynamics and the geodesic deviati
on equations, respectively, pointing out their general inequivalence. Moreo
ver, to advance the mathematical analysis and to highlight both the peculia
rities and the analogies of the methods, we work out two concrete applicati
ons to the study of very different, yet typical in distinct contexts, dynam
ical systems. The first is the well-known Henon-Heiles Hamiltonian, which a
llows us to exploit how the Finsler GDA is well suited not only for testing
the dynamical behaviour of systems with few degrees of freedom, but even t
o get deeper insights into the sources of instability. We show the effectiv
eness of the GDA, both in recovering fully satisfactory agreement with the
most well-established outcomes and also in helping the understanding of the
sources of Chaos. Then, in order to point out the general applicability of
the method, we present the results obtained from the geometrical Bianchi I
X (BIX) cosmological model, whose peculiarity is well known as its very nat
ure has been debated for a long time. Using the Finsler GDA, we obtain resu
lts with a built-in invariance, which give evidence to the non-chaotic beha
viour of this system, excluding any global exponential instability in the e
volution of the geodesic deviation. (C) 1998 Elsevier Science Ltd. All righ
ts reserved.