The solvability of a boundary-value periodic problem

In the space of functions B a 3+ ={g(x, t)=−g(−x, t)=g(x+2π, t)=−g(x, t+T3/2)=g(x, −t)}, we establish that if the condition aT 3 (2s−1)=4πk, (4πk, a (2s−1))=1, k ∈ ℤ, s ∈ ℕ, is satisfied, then the linear problem u u −a 2 u xx =g(x, t), u(0, t)=u(π, t)=0, u(x, t+T 3 )=u(x, t), ℝ2, is always...

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Date:1997
Main Authors: Petrovskii, Ya. B., Khoma, G. P., Петрівський, Я. Б., Хома, Г. П.
Format: Article
Language:Ukrainian
English
Published: Institute of Mathematics, NAS of Ukraine 1997
Online Access:https://umj.imath.kiev.ua/index.php/umj/article/view/5006
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Journal Title:Ukrains’kyi Matematychnyi Zhurnal
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Ukrains’kyi Matematychnyi Zhurnal
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author Petrovskii, Ya. B.
Khoma, G. P.
Петрівський, Я. Б.
Хома, Г. П.
author_facet Petrovskii, Ya. B.
Khoma, G. P.
Петрівський, Я. Б.
Хома, Г. П.
author_sort Petrovskii, Ya. B.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
collection OJS
datestamp_date 2020-03-18T21:22:31Z
description In the space of functions B a 3+ ={g(x, t)=−g(−x, t)=g(x+2π, t)=−g(x, t+T3/2)=g(x, −t)}, we establish that if the condition aT 3 (2s−1)=4πk, (4πk, a (2s−1))=1, k ∈ ℤ, s ∈ ℕ, is satisfied, then the linear problem u u −a 2 u xx =g(x, t), u(0, t)=u(π, t)=0, u(x, t+T 3 )=u(x, t), ℝ2, is always consistent. To prove this statement, we construct an exact solution in the form of an integral operator.
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spelling umjimathkievua-article-50062020-03-18T21:22:31Z The solvability of a boundary-value periodic problem Розв'язність однієї крайової періодичної задачі Petrovskii, Ya. B. Khoma, G. P. Петрівський, Я. Б. Хома, Г. П. In the space of functions B a 3+ ={g(x, t)=−g(−x, t)=g(x+2π, t)=−g(x, t+T3/2)=g(x, −t)}, we establish that if the condition aT 3 (2s−1)=4πk, (4πk, a (2s−1))=1, k ∈ ℤ, s ∈ ℕ, is satisfied, then the linear problem u u −a 2 u xx =g(x, t), u(0, t)=u(π, t)=0, u(x, t+T 3 )=u(x, t), ℝ2, is always consistent. To prove this statement, we construct an exact solution in the form of an integral operator. У просторі функцій B a 3+ ={g(x, t)=−g(−x, t)=g(x+2π, t)=−g(x, t+T3/2)=g(x, −t)} встановлено, що при виконанні умови aT 3 (2s−1)=4πk, (4πk, a (2s−1))=1, k ∈ ℤ, s ∈ ℕ, лінійна задача u u −a 2 u xx =g(x, t), u(0, t)=u(π, t)=0, u(x, t+T 3 )=u(x, t), ℝ2 завжди сумісна. Для доведення цього твердження побудовано точний розв'язок у вигляді інтегрального оператора. Institute of Mathematics, NAS of Ukraine 1997-02-25 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/5006 Ukrains’kyi Matematychnyi Zhurnal; Vol. 49 No. 2 (1997); 302–308 Український математичний журнал; Том 49 № 2 (1997); 302–308 1027-3190 uk en https://umj.imath.kiev.ua/index.php/umj/article/view/5006/6711 https://umj.imath.kiev.ua/index.php/umj/article/view/5006/6712 Copyright (c) 1997 Petrovskii Ya. B.; Khoma G. P.
spellingShingle Petrovskii, Ya. B.
Khoma, G. P.
Петрівський, Я. Б.
Хома, Г. П.
The solvability of a boundary-value periodic problem
title The solvability of a boundary-value periodic problem
title_alt Розв'язність однієї крайової періодичної задачі
title_full The solvability of a boundary-value periodic problem
title_fullStr The solvability of a boundary-value periodic problem
title_full_unstemmed The solvability of a boundary-value periodic problem
title_short The solvability of a boundary-value periodic problem
title_sort solvability of a boundary-value periodic problem
url https://umj.imath.kiev.ua/index.php/umj/article/view/5006
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