Abstract
Abstract
At first we study Galiullin’s construction of Bertrand problem and compare it with Szebehely’s method, latter is based on a first order partial differential equation for the unknown potential that produces a prescribed monoparametric family of planar trajectories. In the second part of the paper we study the inverse problem of the trajectories such that the corresponding force is a nonconservative position dependent one, satisfying the non-vanishing curl condition and not the gradient of a potential function. Recently this force has been introduced and popularized by Berry and Shukla (J. Phys. A 45 (2012) 305 201). We connect the inverse problem dynamics of these curl force trajectories with the generalized potentials obtained by Sarlet-Mestdag-Prince (Rep. Math. Phys. 72(2013) 65-84) from the inverse problem of ϕ(x, y) = xy
m
for m ≠ 0, m ≠ –1. Finally we show that the analog of these curly trajectories in momentum space can be manifested as kinetic energies of the pair of Calogero-Leyvraz Hamiltonians (J. Nonlinear Math. Phys. 26 (2019) 147-154) describing the motion of a particle in a magnetic field with friction.
Funder
Khalifa University of Science, Technology and Research
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