In this work, we investigate a Lagrangian model describing a particle constrained to move along non-degenerate conic sections, parameterized by the orbital eccentricity . In the non-relativistic regime, we apply the Dirac–Bergmann algorithm to identify a set of four second-class constraints, compute the corresponding Dirac brackets, and isolate the true physical degrees of freedom. This procedure yields a unified Hamiltonian treatment of circular (), elliptical (), parabolic (), and hyperbolic () trajectories. We then extend the analysis to the relativistic case, where we observe a similar constraint structure and construct the associated Dirac brackets accordingly. Finally, using the Hamilton-Jacobi formalism, we identify a set of non-involutive constraints; by introducing generalized brackets, we restore integrability and derive the correct equations of motion. A comparative analysis of both formalisms highlights their complementary features and deepens our understanding of the dynamics governing particles restricted to conic geometries.

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