The generalized Rayleigh and van der Pol differential equations are given, respectively, by the following expressions [1-5]:
THE GREATEST NUMBER OF LIMIT CYCLES OF THE GENERALIZED RAYLEIGH–LIÉNARD OSCILLATOR
✍ Scribed by J.D. Bejarano; J. Garcia-Margallo
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 115 KB
- Volume
- 221
- Category
- Article
- ISSN
- 0022-460X
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✦ Synopsis
The limit cycles of the generalized Rayleigh-Lie´nard oscillator X + AX + 2BX 3 + o(z 3 + z 2 X 2 + z 1 X 4 + z 4 X 2 )X = 0, for A q 0, B q 0, and A Q 0, B q 0 are studied by using the Jacobian elliptic functions with the generalized harmonic balance method. For given values of the parameters z i $ 0, i = 1, 2, 3, 4, the values of A and B for which limit cycles exist are found as functions of a single parameter. There is one limit cycle in the region where the Hamiltonian, E say, is positive, i.e., a solution of type cn, and six limit cycles, three double values, in the region where E is negative, solution type dn.
📜 SIMILAR VOLUMES
We consider a class of planar differential equations which include the Lie´nard differential equations. By applying the Bendixson-Dulac Criterion for '-connected sets we reduce the study of the number of limit cycles for such equations to the condition that a certain function of just one variable do