Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations

The main purpose of this paper is to study the oscillatory properties of solutions of the third-order quasi-linear delay differential equation ℒy(t)+f(t)yβ(σ(t))=0{\cal L}y(t) + f(t){y^\beta }(\sigma (t)) = 0 where ℒy(t) = (b(t)(a(t)(y0(t)) )0)0 is a semi-canonical differential operator. The main id...

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Main Authors: Saranya K., Piramanantham V., Thandapani E.
Format: Article
Language:English
Published: De Gruyter 2021-11-01
Series:Nonautonomous Dynamical Systems
Subjects:
Online Access:https://doi.org/10.1515/msds-2020-0135
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author Saranya K.
Piramanantham V.
Thandapani E.
author_facet Saranya K.
Piramanantham V.
Thandapani E.
author_sort Saranya K.
collection DOAJ
description The main purpose of this paper is to study the oscillatory properties of solutions of the third-order quasi-linear delay differential equation ℒy(t)+f(t)yβ(σ(t))=0{\cal L}y(t) + f(t){y^\beta }(\sigma (t)) = 0 where ℒy(t) = (b(t)(a(t)(y0(t)) )0)0 is a semi-canonical differential operator. The main idea is to transform the semi-canonical operator into canonical form and then obtain new oscillation results for the studied equation. Examples are provided to illustrate the importance of the main results.
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spelling doaj.art-11d05cd83e444c2980c8870cdf52e2422022-12-21T17:17:28ZengDe GruyterNonautonomous Dynamical Systems2353-06262021-11-018122823810.1515/msds-2020-0135Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential EquationsSaranya K.0Piramanantham V.1Thandapani E.2Department of Mathematics, Bharathidasan University, Tiruchirappalli-620024, IndiaDepartment of Mathematics, Bharathidasan University, Tiruchirappalli-620024, IndiaRamanujan Institute for Advanced Study in Mathematics, University of Madras, Chennai-600005, IndiaThe main purpose of this paper is to study the oscillatory properties of solutions of the third-order quasi-linear delay differential equation ℒy(t)+f(t)yβ(σ(t))=0{\cal L}y(t) + f(t){y^\beta }(\sigma (t)) = 0 where ℒy(t) = (b(t)(a(t)(y0(t)) )0)0 is a semi-canonical differential operator. The main idea is to transform the semi-canonical operator into canonical form and then obtain new oscillation results for the studied equation. Examples are provided to illustrate the importance of the main results.https://doi.org/10.1515/msds-2020-0135semi- canonicalthird-orderdelay differential equationsoscillation34c1034k11
spellingShingle Saranya K.
Piramanantham V.
Thandapani E.
Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
Nonautonomous Dynamical Systems
semi- canonical
third-order
delay differential equations
oscillation
34c10
34k11
title Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
title_full Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
title_fullStr Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
title_full_unstemmed Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
title_short Oscillation Results for Third-Order Semi-Canonical Quasi-Linear Delay Differential Equations
title_sort oscillation results for third order semi canonical quasi linear delay differential equations
topic semi- canonical
third-order
delay differential equations
oscillation
34c10
34k11
url https://doi.org/10.1515/msds-2020-0135
work_keys_str_mv AT saranyak oscillationresultsforthirdordersemicanonicalquasilineardelaydifferentialequations
AT piramananthamv oscillationresultsforthirdordersemicanonicalquasilineardelaydifferentialequations
AT thandapanie oscillationresultsforthirdordersemicanonicalquasilineardelaydifferentialequations