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AbstractNonholonomic mechanics describes the motion of systems constrained by nonintegrable constraints. One of its most remarkable properties is that the derivation of the nonholonomic equations is not variational in nature. However, in this paper, we prove (Theorem 1.1) that for kinetic nonholonomic systems, the solutions starting from a fixed pointqare true geodesics for a family of Riemannian metrics on the image submanifold$${{\mathcal {M}}}^{nh}_q$$Mqnhof the nonholonomic exponential map. This implies a surprising result: the kinetic nonholonomic trajectories with starting pointq, for sufficiently small times, minimize length in$${{\mathcal {M}}}^{nh}_q$$Mqnh!
nonholonomic mechanics, Mathematics - Differential Geometry, Nonholonomic systems related to the dynamics of a system of particles, radial geodesics, FOS: Physical sciences, Methods of global Riemannian geometry, including PDE methods; curvature restrictions, Mathematical Physics (math-ph), 70G45 (Primary), 53B20, 53C21, 37J60, 70F25 (Secondary), nonholonomic geodesics, exponential map, Local Riemannian geometry, Differential geometric methods (tensors, connections, symplectic, Poisson, contact, Riemannian, nonholonomic, etc.) for problems in mechanics, Differential Geometry (math.DG), FOS: Mathematics, Riemannian geometry, Nonholonomic dynamical systems, Mathematical Physics
nonholonomic mechanics, Mathematics - Differential Geometry, Nonholonomic systems related to the dynamics of a system of particles, radial geodesics, FOS: Physical sciences, Methods of global Riemannian geometry, including PDE methods; curvature restrictions, Mathematical Physics (math-ph), 70G45 (Primary), 53B20, 53C21, 37J60, 70F25 (Secondary), nonholonomic geodesics, exponential map, Local Riemannian geometry, Differential geometric methods (tensors, connections, symplectic, Poisson, contact, Riemannian, nonholonomic, etc.) for problems in mechanics, Differential Geometry (math.DG), FOS: Mathematics, Riemannian geometry, Nonholonomic dynamical systems, Mathematical Physics
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