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Article: On perturbation procedure for limit cycle analysis
Title | On perturbation procedure for limit cycle analysis |
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Authors | |
Issue Date | 1991 |
Publisher | Pergamon. The Journal's web site is located at http://www.elsevier.com/locate/nlm |
Citation | International Journal Of Non-Linear Mechanics, 1991, v. 26 n. 1, p. 125-133 How to Cite? |
Abstract | In the use of perturbation procedure for analysing the limit cycle of an autonomous system, people usually assumed an initial condition ẋ(0) = 0. However, this initial condition is often simplified to x ̇nh(0) = 0, (n= 0, 1, 2,...) and taken as an additional condition to determine a constant, say bn, of the homogeneous solution xn = an cosτ + bn sin τ of the perturbation equation of each order. Nevertheless, this commonly accepted procedure will lead to large errors, especially for the case of larger values of the parameter ε. In this paper, a condition of constant phase angle Øn in the homogeneous solutions xnh = Ancos (τ + Øn) (n = 0, 1, 2,...) is adopted, i.e. Ø1 = Ø2 = ... = Ø. The limit cycles obtained by use of the present condition and corresponding perturbation procedure are in good agreement with the numerical results of the Runge-Kutta integration, and with the analytical expression obtained by the incremental harmonic balance method even in the case of the parameter ε = 1. © 1990. |
Persistent Identifier | http://hdl.handle.net/10722/149958 |
ISSN | 2023 Impact Factor: 2.8 2023 SCImago Journal Rankings: 0.800 |
ISI Accession Number ID |
DC Field | Value | Language |
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dc.contributor.author | Chen, SH | en_US |
dc.contributor.author | Cheung, YK | en_US |
dc.contributor.author | Lau, SL | en_US |
dc.date.accessioned | 2012-06-26T06:00:47Z | - |
dc.date.available | 2012-06-26T06:00:47Z | - |
dc.date.issued | 1991 | en_US |
dc.identifier.citation | International Journal Of Non-Linear Mechanics, 1991, v. 26 n. 1, p. 125-133 | en_US |
dc.identifier.issn | 0020-7462 | en_US |
dc.identifier.uri | http://hdl.handle.net/10722/149958 | - |
dc.description.abstract | In the use of perturbation procedure for analysing the limit cycle of an autonomous system, people usually assumed an initial condition ẋ(0) = 0. However, this initial condition is often simplified to x ̇nh(0) = 0, (n= 0, 1, 2,...) and taken as an additional condition to determine a constant, say bn, of the homogeneous solution xn = an cosτ + bn sin τ of the perturbation equation of each order. Nevertheless, this commonly accepted procedure will lead to large errors, especially for the case of larger values of the parameter ε. In this paper, a condition of constant phase angle Øn in the homogeneous solutions xnh = Ancos (τ + Øn) (n = 0, 1, 2,...) is adopted, i.e. Ø1 = Ø2 = ... = Ø. The limit cycles obtained by use of the present condition and corresponding perturbation procedure are in good agreement with the numerical results of the Runge-Kutta integration, and with the analytical expression obtained by the incremental harmonic balance method even in the case of the parameter ε = 1. © 1990. | en_US |
dc.language | eng | en_US |
dc.publisher | Pergamon. The Journal's web site is located at http://www.elsevier.com/locate/nlm | en_US |
dc.relation.ispartof | International Journal of Non-Linear Mechanics | en_US |
dc.title | On perturbation procedure for limit cycle analysis | en_US |
dc.type | Article | en_US |
dc.identifier.email | Cheung, YK:hreccyk@hkucc.hku.hk | en_US |
dc.identifier.authority | Cheung, YK=rp00104 | en_US |
dc.description.nature | link_to_subscribed_fulltext | en_US |
dc.identifier.scopus | eid_2-s2.0-0025798211 | en_US |
dc.identifier.volume | 26 | en_US |
dc.identifier.issue | 1 | en_US |
dc.identifier.spage | 125 | en_US |
dc.identifier.epage | 133 | en_US |
dc.identifier.isi | WOS:A1991EU44000011 | - |
dc.publisher.place | United Kingdom | en_US |
dc.identifier.scopusauthorid | Chen, SH=13303161800 | en_US |
dc.identifier.scopusauthorid | Cheung, YK=7202111065 | en_US |
dc.identifier.scopusauthorid | Lau, SL=7401596228 | en_US |
dc.identifier.issnl | 0020-7462 | - |