<abstract xmlns="http://www.w3.org/1999/xhtml">In this work, necessary and sufficient conditions for oscillation of solutions of second-order neutral impulsive differential system<disp-formula><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_tmmp-2020-0025_eq_001.png"></graphic><math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo>{</mo><mrow><mtable><mtr><mtd><mrow><msup><mrow><mrow><mrow><mo>(</mo><mrow><mi>r</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><msup><mrow><mrow><mrow><mo>(</mo><mrow><msup><mi>z</mi><mo>′</mo></msup><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow></mrow></mrow><mi>γ</mi></msup></mrow><mo>)</mo></mrow></mrow></mrow><mo>′</mo></msup><mo>+</mo><mi>q</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><msup><mrow><mi>x</mi></mrow><mi>α</mi></msup><mrow><mo>(</mo><mrow><mi>σ</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></mtd><mtd><mrow><mi>t</mi><mo>≥</mo><msub><mrow><mi>t</mi></mrow><mn>0</mn></msub><mo>,</mo><mi> </mi><mi> </mi><mi> </mi><mi>t</mi><mo>≠</mo><msub><mrow><mi>λ</mi></mrow><mi>k</mi></msub><mo>,</mo></mrow></mtd></mtr><mtr><mtd><mrow><mi>Δ</mi><mrow><mo>(</mo><mrow><mi>r</mi><mrow><mo>(</mo><mrow><msub><mrow><mi>λ</mi></mrow><mi>k</mi></msub></mrow><mo>)</mo></mrow><msup><mrow><mrow><mrow><mo>(</mo><mrow><msup><mi>z</mi><mo>′</mo></msup><mrow><mo>(</mo><mrow><msub><mrow><mi>λ</mi></mrow><mi>k</mi></msub></mrow><mo>)</mo></mrow></mrow><mo>)</mo></mrow></mrow></mrow><mi>γ</mi></msup></mrow><mo>)</mo></mrow><mo>+</mo><mi>h</mi><mrow><mo>(</mo><mrow><msub><mrow><mi>λ</mi></mrow><mi>k</mi></msub></mrow><mo>)</mo></mrow><msup><mrow><mi>x</mi></mrow><mi>α</mi></msup><mrow><mo>(</mo><mrow><mi>σ</mi><mrow><mo>(</mo><mrow><msub><mrow><mi>λ</mi></mrow><mi>k</mi></msub></mrow><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></mtd><mtd><mrow><mi>k</mi><mo>∈</mo><mi>𝕅</mi></mrow></mtd></mtr></mtable></mrow></mrow></mrow></math><tex-math>\left\{ {\matrix{{{{\left( {r\left( t \right){{\left( {z'\left( t \right)} \right)}^\gamma }} \right)}^\prime } + q\left( t \right){x^\alpha }\left( {\sigma \left( t \right)} \right) = 0,} \hfill &amp; {t \ge {t_0},\,\,\,t \ne {\lambda _k},} \hfill \cr {\Delta \left( {r\left( {{\lambda _k}} \right){{\left( {z'\left( {{\lambda _k}} \right)} \right)}^\gamma }} \right) + h\left( {{\lambda _k}} \right){x^\alpha }\left( {\sigma \left( {{\lambda _k}} \right)} \right) = 0,} \hfill &amp; {k \in \mathbb{N}} \hfill \cr } } \right.</tex-math></alternatives></disp-formula> are established, where
<disp-formula><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_tmmp-2020-0025_eq_002.png"></graphic><math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mrow><mi>z</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>=</mo><mi>x</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>+</mo><mi>p</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mi>x</mi><mrow><mo>(</mo><mrow><mi>τ</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow></mrow></math><tex-math>z\left( t \right) = x\left( t \right) + p\left( t \right)x\left( {\tau \left( t \right)} \right)</tex-math></alternatives></disp-formula>Under the assumption <inline-formula><alternatives><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_tmmp-2020-0025_eq_003.png"></inline-graphic><math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo>∫</mo><mrow><msup><mrow></mrow><mo>∞</mo></msup><msup><mrow><mrow><mrow><mo>(</mo><mrow><mi>r</mi><mrow><mo>(</mo><mi>η</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow></mrow></mrow><mrow><mo>-</mo><mn>1</mn><mo>/</mo><mi>α</mi></mrow></msup><mi>d</mi><mi>η</mi><mo>=</mo><mo>∞</mo></mrow></mrow></mrow></math><tex-math>\int {^\infty {{\left( {r\left( \eta \right)} \right)}^{ - 1/\alpha }}d\eta = \infty }</tex-math></alternatives></inline-formula> two cases when <italic>γ>α</italic> and <italic>γ&lt;α</italic> are considered. The main tool is Lebesgue’s Dominated Convergence theorem. Examples are given to illustrate the main results, and state an open problem.</abstract>

In this work, necessary and sufficient conditions for oscillation of solutions of second-order neutral impulsive differential system{(r(t)(z′(t))γ)′+q(t)xα(σ(t))=0,t≥t0,   t≠λk,Δ(r(λk)(z′(λk))γ)+h(λk)xα(σ(λk))=0,k∈𝕅\left\{ {\matrix{{{{\left( {r\left( t \right){{\left( {z'\left( t \right)} \right)}^\gamma }} \right)}^\prime } + q\left( t \right){x^\alpha }\left( {\sigma \left( t \right)} \right) = 0,} \hfill & {t \ge {t_0},\,\,\,t \ne {\lambda _k},} \hfill \cr {\Delta \left( {r\left( {{\lambda _k}} \right){{\left( {z'\left( {{\lambda _k}} \right)} \right)}^\gamma }} \right) + h\left( {{\lambda _k}} \right){x^\alpha }\left( {\sigma \left( {{\lambda _k}} \right)} \right) = 0,} \hfill & {k \in \mathbb{N}} \hfill \cr } } \right. are established, where
z(t)=x(t)+p(t)x(τ(t))z\left( t \right) = x\left( t \right) + p\left( t \right)x\left( {\tau \left( t \right)} \right)Under the assumption ∫∞(r(η))-1/αdη=∞\int {^\infty {{\left( {r\left( \eta \right)} \right)}^{ - 1/\alpha }}d\eta = \infty } two cases when γ>α and γ<α are considered. The main tool is Lebesgue’s Dominated Convergence theorem. Examples are given to illustrate the main results, and state an open problem.

Necessary and Sufficient Conditions for Oscillation of Solutions to Second-Order Neutral Differential Equations with Impulses

Tatra Mountains Mathematical Publications

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

In this work, necessary and sufficient conditions for oscillation of solutions of second-order neutral impulsive differential...

Necessary and Sufficient Conditions for Oscillation of Solutions to Second-Order Neutral Differential Equations with Impulses

Data publikacji: 04 lis 2020

Zakres stron: 157 - 170

Otrzymano: 18 maj 2020

DOI: https://doi.org/10.2478/tmmp-2020-0025

Słowa kluczowe
Oscillation, non-oscillation, neutral, delay, Lebesgue’s Dominated Convergence theorem, impulses

© 2020 Shyam Sundar Santra, published by Sciendo

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

Necessary and Sufficient Conditions for Oscillation of Solutions to Second-Order Neutral Differential Equations with Impulses

Data publikacji: 04 lis 2020

Zakres stron: 157 - 170

Otrzymano: 18 maj 2020

DOI: https://doi.org/10.2478/tmmp-2020-0025

Słowa kluczoweOscillation, non-oscillation, neutral, delay, Lebesgue’s Dominated Convergence theorem, impulses

© 2020 Shyam Sundar Santra, published by Sciendo

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

Słowa kluczowe
Oscillation, non-oscillation, neutral, delay, Lebesgue’s Dominated Convergence theorem, impulses