Abstract

The unique exact analytical solutions of parabolic boundary value problems of mathematical physics in piecewise homogeneous wedge-shaped solid cylinder were constructed at first time by the method of integral and hybrid integral transforms in combination with the method of main solutions (matrices of influence and Green matrices). The cases of assigning on the verge of the wedge the boundary conditions of Dirichlet and Neumann and their possible combinations (Dirichlet – Neumann, Neumann – Dirichlet) are considered. Finite integral Fourier transform by an angular variable $\varphi \in (0; \varphi_0)$, a Fourier integral transform on the Cartesian segment $(-l_1;l_2)$ by an applicative variable $z$ and a hybrid integral transform of the Hankel type of the first kind on a segment $(0;R)$ of the polar axis with $n$ points of conjugation by an radial variable $r$ were used to construct solutions of investigated initial-boundary value problems. The consistent application of integral transforms by geometric variables allows us to reduce the three-dimensional initial boundary-value problems of conjugation to the Cauchy problem for a regular linear inhomogeneous 1st order differential equation whose unique solution is written in a closed form. The application of inverse integral transforms restores explicitly the solution of the considered problems through their integral image. The structure of the solution of the problem in the case of setting the Neumann boundary conditions on the wedge edges is analyzed. Exact analytical formulas for the components of the main solutions are written and the theorem on the existence of a single bounded classical solution of the problem is formulated. The obtained solutions are algorithmic in nature and can be used (using numerical methods) in solving applied problems.

Highlights

  • Ðîçãëÿíóòî âèïàäêè çàäàííÿ íà ãðàíÿõ êëèíà êðàéîâèõ óìîâ Äiðiõëå i Íåéìàíà òàõ ìîæëèâèõ êîìáiíàöié (Äiðiõëå Íåéìàíà, Íåéìàíà Äiðiõëå).

  • Çàñòîñóâàííÿ îáåðíåíèõ iíòåãðàëüíèõ ïåðåòâîðåíü âiäíîâëþ1 â ÿâíîìó âèãëÿäi ðîçâ'ÿçêè ðîçãëÿíóòèõ ïàðàáîëi÷íèõ ïî÷àòêîâî-êðàéîâèõ çàäà÷ ÷åðåçõ iíòåãðàëüíå çîáðàæåííÿ.

  • Ùî êðiì ìåòîäó âiäîêðåìëåííÿ çìiííèõ (ìåòîäó Ôóð'1) òà éîãî óçàãàëüíåíü, îäíèì ç âàæëèâèõ i åôåêòèâíèõ ìåòîäiâ âèâ÷åííÿ ëiíiéíèõ êðàéîâèõ i ìiøàíèõ çàäà÷ äëÿ äèôåðåíöiàëüíèõ ðiâíÿíü ç ÷àñòèííèìè ïîõiäíèìè â îäíîðiäíèõ ñåðåäîâèùàõ 1 ìåòîä iíòåãðàëüíèõ ïåðåòâîðåíü, ÿêèé äà1 ìîæëèâiñòü ïîáóäóâàòè â àíàëiòè÷íîìó âèãëÿäi òî÷íi ðîçâ'ÿçêè ðîçãëÿíóòèõ çàäà÷ ÷åðåçõ iíòåãðàëüíå çîáðàæåííÿ.

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Summary

Introduction

Ðîçãëÿíóòî âèïàäêè çàäàííÿ íà ãðàíÿõ êëèíà êðàéîâèõ óìîâ Äiðiõëå i Íåéìàíà òàõ ìîæëèâèõ êîìáiíàöié (Äiðiõëå Íåéìàíà, Íåéìàíà Äiðiõëå). Çàñòîñóâàííÿ îáåðíåíèõ iíòåãðàëüíèõ ïåðåòâîðåíü âiäíîâëþ1 â ÿâíîìó âèãëÿäi ðîçâ'ÿçêè ðîçãëÿíóòèõ ïàðàáîëi÷íèõ ïî÷àòêîâî-êðàéîâèõ çàäà÷ ÷åðåçõ iíòåãðàëüíå çîáðàæåííÿ.

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