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Differential Equations with a Small Parameter Attached to the Highest Derivatives and Some Problems in the Theory of Oscillations
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References
1960
Year
Numerical AnalysisPeriodic SolutionsHamiltonian TheorySmall Parameter AttachedPhysicsSuch Periodic SolutionsAlgebraic AnalysisOscillation TheoryGeometric Singular Perturbation TheoryNonlinear EquationHighest DerivativesDifferential EquationsCalculus Of VariationNonlinear Oscillation
This paper presents a brief review, for the most part, of the authors' results concerning systems of differential equations of the form <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">\epsilon \dot{x}^1 = f^i(x^1,\cdots,x^k,y^1,\cdots,y^l) i =1, 2,\cdots,k</tex> <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">\dot{y}^i = g^i(x^1,\cdots,x^k,y^1,\cdots,y^l) j =1,2,\cdots,</tex> where <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">\epsilon</tex> is a small positive parameter. The emphasis is on periodic solutions of such systems which are close to discontinuous solutions. Such periodic solutions are mathematical representations of relaxation oscillations which are encountered in various mechanical, electrical and radio systems.
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