Periodic solutions of Lienard differential equations via averaging theory of order two

Abstract For ε ≠ 0sufficiently small we provide sufficient conditions for the existence of periodic solutions for the Lienard differential equations of the form x ′′ + f ⁢ ( x ) ⁢ x ′ + n 2 ⁢ x + g ⁢ ( x ) = ε 2 ⁢ p 1 ⁢ ( t ) + ε 3 ⁢ p 2 ⁢ ( t ) , where n is a positive integer, f : ℝ → ℝis a C 3func...

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Bibliographic Details
Main Author: LLIBRE,JAUME (author)
Other Authors: NOVAES,DOUGLAS D. (author), TEIXEIRA,MARCO A. (author)
Format: article
Language:eng
Published: 2015
Subjects:
Online Access:http://old.scielo.br/scielo.php?script=sci_arttext&pid=S0001-37652015000501905
Country:Brazil
Oai:oai:scielo:S0001-37652015000501905
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Summary:Abstract For ε ≠ 0sufficiently small we provide sufficient conditions for the existence of periodic solutions for the Lienard differential equations of the form x ′′ + f ⁢ ( x ) ⁢ x ′ + n 2 ⁢ x + g ⁢ ( x ) = ε 2 ⁢ p 1 ⁢ ( t ) + ε 3 ⁢ p 2 ⁢ ( t ) , where n is a positive integer, f : ℝ → ℝis a C 3function, g : ℝ → ℝis a C 4function, and p i : ℝ → ℝfor i = 1 , 2are continuous 2 ⁢ π–periodic function. The main tool used in this paper is the averaging theory of second order. We also provide one application of the main result obtained.