Integrable equations with Ermakov–Pinney nonlinearities and Chiellini damping

"We introduce a special type of dissipative Ermakov-Pinney equations of the form vζζ + g(v)vζ + h(v) = 0, where h(v) = h0(v) + cv−3 and the nonlinear dissipation g(v) is based on the corresponding Chiellini integrable Abel equation. When h0(v) is a linear function, h0(v) = λ2v, general solution...

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Bibliographic Details
Author: HARET CODRATIAN ROSU
Format: article
Status:Versión aceptada para publicación
Publication Date:2015
Country:México
Institution:Instituto Potosino de Investigación Científica y Tecnológica
Repository:Repositorio Institucional del IPICYT
Language:English
OAI Identifier:oai:ipicyt.repositorioinstitucional.mx:1010/899
Online Access:http://ipicyt.repositorioinstitucional.mx/jspui/handle/1010/868
http://ipicyt.repositorioinstitucional.mx/jspui/handle/1010/899
Access Level:Open access
Keyword:info:eu-repo/classification/Autor/Dissipative Ermakov-Pinney equation
info:eu-repo/classification/Autor/Chiellini damping
info:eu-repo/classification/Autor/Reid nonlinearities
info:eu-repo/classification/Autor/Abel equation
info:eu-repo/classification/cti/1
Description
Summary:"We introduce a special type of dissipative Ermakov-Pinney equations of the form vζζ + g(v)vζ + h(v) = 0, where h(v) = h0(v) + cv−3 and the nonlinear dissipation g(v) is based on the corresponding Chiellini integrable Abel equation. When h0(v) is a linear function, h0(v) = λ2v, general solutions are obtained following the Abel equation route. Based on particular solutions, we also provide general solutions containing a factor with the phase of the Milne type. In addition, the same kinds of general solutions are constructed for the cases of higher-order Reid nonlinearities. The Chiellini dissipative function is actually a dissipation-gain function because it can be negative on some intervals. We also examine the nonlinear case h0(v) = Ω20(v − v2) and show that it leads to an integrable hyperelliptic case."