The present paper builds on the previous contribution by the second author, S. Fiori, Synchronization of first-order autonomous oscillators on Riemannian manifolds, Discrete and Continuous Dynamical Systems – Series B, Vol. 24, No. 4, pp. 1725 – 1741, April 2019. The aim of the present paper is to optimize a previously-developed control law to achieve synchronization of first-order non-linear oscillators whose state evolves on a Riemannian manifold. The optimization of such control law has been achieved by introducing a transverse control field, which guarantees reduced control effort without affecting the synchronization speed of the oscillators. The developed non-linear control theory has been analyzed from a theoretical point of view as well as through a comprehensive series of numerical experiments.
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Figure 1. Simulation of the evolution of the master system (in green color), controlled systems $ \Sigma_L $ (26) (in red color) and $ \Sigma_G $ (27) (in blue color) on the sphere $ \mathbb{S}^2 $, displayed in terms of state components, together with the values taken by the Lyapunov function (7) during evolution (in blue color for $ \Sigma_G $ and in red color for $ \Sigma_L $)
Figure 4. Synchronization of a master/slave pair oscillators on the sphere $ \mathbb{S}^7 $ – with and without the transverse field $ \tau_G $ – illustrated in terms of control efforts and Lypunov function values (in red color for the system without transverse component and blue color for the system with transverse component). The left-bottom panes shows the course of the difference $ \|u\|_{z_s}^2-\|u+\tau_G\|_{z_s}^2 $ which takes non-negative values
Figure 6. Synchronization of two master/slave oscillators on $ \mathbb{SO}(3) $ by the control field (4). In the top panel, the evolution of the squared Riemannian distance $ d^2(z^s, z^m) $ is represented versus time. In the bottom panel, the evolution of the squared control effort related to the control law $ u $ is represented over times
Figure 7. Synchronization of two master/slave oscillators on $ \mathbb{SO}(3) $ by the control field $ \tilde{u} $ with (48) as transverse control field. In the top panel, the evolution of the squared Riemannian distance $ d^2(z^s, z^m) $ is represented versus time. In the bottom panel, the evolution of the squared control effort associated to the control field $ \tilde{u} $ is represented
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Simulation of the evolution of the master system (in green color), controlled systems
Simulation of the evolution of the controlled systems
Synchronization of a master/slave pair oscillators on the sphere
Synchronization of a master/slave pair oscillators on the sphere
Synchronization of a master/slave pair oscillators on the sphere
Synchronization of two master/slave oscillators on
Synchronization of two master/slave oscillators on
Synchronization of two master/slave oscillators on