Higher-order saddle potentials, nonlinear curl forces, trapping and dynamics
Autor: | Partha Guha, Sudip Garai |
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Rok vydání: | 2021 |
Předmět: |
Physics
Degree (graph theory) Applied Mathematics Mechanical Engineering Aerospace Engineering Order (ring theory) Ocean Engineering Type (model theory) 01 natural sciences Matrix (mathematics) Central force Control and Systems Engineering 0103 physical sciences Tensor Electrical and Electronic Engineering 010301 acoustics Energy (signal processing) Saddle Mathematical physics |
Zdroj: | Nonlinear Dynamics. 103:2257-2272 |
ISSN: | 1573-269X 0924-090X |
DOI: | 10.1007/s11071-021-06212-w |
Popis: | The position-dependent non-conservative forces are called curl forces introduced recently by Berry and Shukla (J Phys A 45:305201, 2012). The aim of this paper is to study mainly the curl force dynamics of non-conservative central force $$\ddot{x} = -xg(x,y)$$ and $$\ddot{y} = -yg(x,y)$$ connected to higher-order saddle potentials. In particular, we study the dynamics of the type $$\ddot{x}_i = -x_ig \big (\frac{1}{2}(x_{1}^{2} - x_{2}^{2}) \big )$$ , $$i=1,2$$ and its application towards the trapping of ions. We also study the higher-order saddle surfaces, using the pair of higher-order saddle surfaces and rotated saddle surfaces by constructing a generalized rotating shaft equation. The complex curl force can also be constructed by using this pair. By the direct computation, we show that all these motions of higher-order saddles are completely integrable due to the existence of two conserved quantities, viz. energy function and the Fradkin tensor. The Newtonian system $$\ddot{x} = {{\mathcal {X}}}(x,y)$$ , $$\ddot{y} = {{\mathcal {Y}}}(x,y)$$ has also been studied with an energy like first integral $$I(\mathbf{x}, \dot{\mathbf{x}}) = \frac{1}{2}\dot{\mathbf{x}}^TM(\mathbf{x})\dot{\mathbf{x}} + U(\mathbf{x})$$ , where $$M(\mathbf{x})$$ is a $$(2 \times 2)$$ matrix of which the components are polynomials of degree less than or equal to two and the condition on $${{\mathcal {X}}}$$ and $${{\mathcal {Y}}}$$ for which the curl is non-vanishing is also obtained. |
Databáze: | OpenAIRE |
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