dc.contributor | Universidade Estadual Paulista (UNESP) | |
dc.date.accessioned | 2022-05-01T08:45:05Z | |
dc.date.accessioned | 2022-12-20T03:41:07Z | |
dc.date.available | 2022-05-01T08:45:05Z | |
dc.date.available | 2022-12-20T03:41:07Z | |
dc.date.created | 2022-05-01T08:45:05Z | |
dc.date.issued | 2021-01-01 | |
dc.identifier | Nonlinear Physical Science, p. 93-114. | |
dc.identifier | 1867-8459 | |
dc.identifier | 1867-8440 | |
dc.identifier | http://hdl.handle.net/11449/233485 | |
dc.identifier | 10.1007/978-981-16-3544-1_7 | |
dc.identifier | 2-s2.0-85114312280 | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/5413584 | |
dc.description.abstract | We discuss in this chapter some dynamical properties for the Fermi-Ulam model under different dissipative forces. The first type considered is through inelastic collisions that is when the particle has a fractional loss of energy upon collision. We will show that depending on the control parameters, stable and unstable manifolds obtained from the same saddle fixed point cross each other producing a crisis event. Such a crisis destroys the chaotic attractor which is replaced by a chaotic transient. Another type of dissipative force is when the particle crosses a viscous media hence losing energy along its trajectory. Three different types of drag forces will be considered: (i) proportional to the velocity of the particle; (2) proportional to square of the velocity and; (3) proportional to a power of the velocity different from the linear and from the quadratic. | |
dc.language | eng | |
dc.relation | Nonlinear Physical Science | |
dc.source | Scopus | |
dc.title | Dissipation in the Fermi-Ulam Model | |
dc.type | Capítulos de libros | |