O pewnym ustalonym zagadnieniu przestrzennym termosprężystości
A steady-state three-dimensional thermo-elastic problem The object of this paper is to determine the temperature field T and the stress components (σij) in an elastic semi-space, assuming that the temperature in the region Γ of the plane bounding the semi-space is known and equal to T0(ξ, η), the r...
| Published in: | Engineering Transactions |
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| Main Author: | |
| Format: | Article |
| Language: | English |
| Published: |
Institute of Fundamental Technological Research Polish Academy of Sciences
1957-08-01
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| Online Access: | https://et.ippt.pan.pl/index.php/et/article/view/3303 |
| _version_ | 1848651238564954112 |
|---|---|
| author | Witold NOWACKI |
| author_facet | Witold NOWACKI |
| author_sort | Witold NOWACKI |
| collection | DOAJ |
| container_title | Engineering Transactions |
| description | A steady-state three-dimensional thermo-elastic problem
The object of this paper is to determine the temperature field T and the stress components (σij) in an elastic semi-space, assuming that the temperature in the region Γ of the plane bounding the semi-space is known and equal to T0(ξ, η), the region outside Γ being kept at T = 0.
The problem is solved by means of the Green's function. The temperature field T* is determined and the stress components (σij*), in the case where T = 0 over the whole plane z = 0 except an infinitely small region dΓ where T = T0. Using integral expressions (1.1) and (1.2), T and σij are determined for any temperature distribution T0(ξ, η) inside the region Γ. In the second part of the paper, the Green's functions T* and Φ* and the Galerkin's function φ are determined, using the Fourier transformation. The Green's functions obtained for the stress (σij*) are characterized by the fact that the three components σzz*, σzx*, and σzy* are zero.
In the third part of the paper, consideration is given to the particular case of T0 = const over a rectangle whose sides are 2a and 2b, and that of T0 = const over an infinite strip of width 2a. In the latter case, only the stress σyy* differs from zero.
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| format | Article |
| id | doaj-eafa08994be047efbed8ba3ccb1e6cd0 |
| institution | Directory of Open Access Journals |
| issn | 0867-888X 2450-8071 |
| language | English |
| publishDate | 1957-08-01 |
| publisher | Institute of Fundamental Technological Research Polish Academy of Sciences |
| record_format | Article |
| spelling | doaj-eafa08994be047efbed8ba3ccb1e6cd02025-11-03T01:15:54ZengInstitute of Fundamental Technological Research Polish Academy of SciencesEngineering Transactions0867-888X2450-80711957-08-0153O pewnym ustalonym zagadnieniu przestrzennym termosprężystościWitold NOWACKI0Instytut Podstawowych Problemów Techniki PANA steady-state three-dimensional thermo-elastic problem The object of this paper is to determine the temperature field T and the stress components (σij) in an elastic semi-space, assuming that the temperature in the region Γ of the plane bounding the semi-space is known and equal to T0(ξ, η), the region outside Γ being kept at T = 0. The problem is solved by means of the Green's function. The temperature field T* is determined and the stress components (σij*), in the case where T = 0 over the whole plane z = 0 except an infinitely small region dΓ where T = T0. Using integral expressions (1.1) and (1.2), T and σij are determined for any temperature distribution T0(ξ, η) inside the region Γ. In the second part of the paper, the Green's functions T* and Φ* and the Galerkin's function φ are determined, using the Fourier transformation. The Green's functions obtained for the stress (σij*) are characterized by the fact that the three components σzz*, σzx*, and σzy* are zero. In the third part of the paper, consideration is given to the particular case of T0 = const over a rectangle whose sides are 2a and 2b, and that of T0 = const over an infinite strip of width 2a. In the latter case, only the stress σyy* differs from zero. https://et.ippt.pan.pl/index.php/et/article/view/3303 |
| spellingShingle | Witold NOWACKI O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title | O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title_full | O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title_fullStr | O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title_full_unstemmed | O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title_short | O pewnym ustalonym zagadnieniu przestrzennym termosprężystości |
| title_sort | o pewnym ustalonym zagadnieniu przestrzennym termosprezystosci |
| url | https://et.ippt.pan.pl/index.php/et/article/view/3303 |
| work_keys_str_mv | AT witoldnowacki opewnymustalonymzagadnieniuprzestrzennymtermosprezystosci |
