Geometrically constrained particle dynamics revisited: Equation of motion in terms of the normal curvature of the constraint manifold
We revisit the problem of the particle dynamics subject to a geometric holonomic constraint of codimension 1 in spatial dimensions d =2 and 3. In the absence of dissipation, we show that by solving the Lagrangian multiplier in a general fashion, the external potential independent part, the net norma...
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Format | Journal Article |
Language | English |
Published |
04.01.2024
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Subjects | |
Online Access | Get full text |
DOI | 10.48550/arxiv.2401.02631 |
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Summary: | We revisit the problem of the particle dynamics subject to a geometric
holonomic constraint of codimension 1 in spatial dimensions d =2 and 3. In the
absence of dissipation, we show that by solving the Lagrangian multiplier in a
general fashion, the external potential independent part, the net normal force,
of the equation of motion corresponds to precisely to the curvature of the
trajectory on the constraint space multiplied by twice the kinetic energy. The
tangent the trajectory is the instantaneous velocity. In d = 3, this term
equals the second fundamental form II of the constraint surface evaluated on
the unit tangent vector in the direction of velocity. Using these result we
establish the relation between constrained particle dynamics with geodesic
equations and derive intriguing kinematic implications using theorems from
fundamental differential geometry. |
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DOI: | 10.48550/arxiv.2401.02631 |