Pointwise convergence of the combination technique for Laplace's equation:
Abstract: "For a simple model problem -- the Laplace equation on the unit square with a Dirichlet boundary function vanishing for x = 0, x = 1, and y = 1, and equaling some suitable g(x) for y = 0 -- we present a proof of convergence for the combination technique, a modern, efficient, and easil...
Gespeichert in:
Format: | Buch |
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Sprache: | English |
Veröffentlicht: |
München
1993
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Schriftenreihe: | Technische Universität <München>: TUM-I
9336 |
Schlagworte: | |
Zusammenfassung: | Abstract: "For a simple model problem -- the Laplace equation on the unit square with a Dirichlet boundary function vanishing for x = 0, x = 1, and y = 1, and equaling some suitable g(x) for y = 0 -- we present a proof of convergence for the combination technique, a modern, efficient, and easily parallelizable sparse grid solver for elliptic partial differential equations that recently gained importance in fields of applications like computational fluid dynamics. For full square grids with meshwidth h and O(h⁻²) grid points, the order O(h²) of the discretization error using finite differences was shown in [12], if g(x) [member of] C²[0,1]. In this paper, we show that the finite difference discretization error of the solution produced by the combination technique on a sparse grid with only O((h⁻¹ log₂ (h⁻¹)) grid points is of the order O(h² log₂ (h⁻¹)), if the Fourier coefficients b[subscript k] of g̃, the 2-periodic and 0-symmetric extension of g, fulfill [formula] for some arbitrary small positive [epsilon]. If 0 <[epsilon] [<or =] 1, this is valid for g [member of] C⁴[0,1] and g(0) = g(1) = g''(0) = g''(1) = 0, e.g.. A simple transformation even shows that g [member of] C⁴[0,1] is sufficient. Furthermore, we present results of numerical experiments with functions g of varying smoothness." |
Beschreibung: | 25 S. graph. Darst. |
Internformat
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245 | 1 | 0 | |a Pointwise convergence of the combination technique for Laplace's equation |c Hans-Joachim Bongartz, ... |
264 | 1 | |a München |c 1993 | |
300 | |a 25 S. |b graph. Darst. | ||
336 | |b txt |2 rdacontent | ||
337 | |b n |2 rdamedia | ||
338 | |b nc |2 rdacarrier | ||
490 | 1 | |a Technische Universität <München>: TUM-I |v 9336 | |
490 | 1 | |a Sonderforschungsbereich Methoden und Werkzeuge für die Nutzung paralleler Rechnerarchitekturen: SFB-Bericht / A |v 1993,16 | |
520 | 3 | |a Abstract: "For a simple model problem -- the Laplace equation on the unit square with a Dirichlet boundary function vanishing for x = 0, x = 1, and y = 1, and equaling some suitable g(x) for y = 0 -- we present a proof of convergence for the combination technique, a modern, efficient, and easily parallelizable sparse grid solver for elliptic partial differential equations that recently gained importance in fields of applications like computational fluid dynamics. For full square grids with meshwidth h and O(h⁻²) grid points, the order O(h²) of the discretization error using finite differences was shown in [12], if g(x) [member of] C²[0,1]. In this paper, we show that the finite difference discretization error of the solution produced by the combination technique on a sparse grid with only O((h⁻¹ log₂ (h⁻¹)) grid points is of the order O(h² log₂ (h⁻¹)), if the Fourier coefficients b[subscript k] of g̃, the 2-periodic and 0-symmetric extension of g, fulfill [formula] for some arbitrary small positive [epsilon]. If 0 <[epsilon] [<or =] 1, this is valid for g [member of] C⁴[0,1] and g(0) = g(1) = g''(0) = g''(1) = 0, e.g.. A simple transformation even shows that g [member of] C⁴[0,1] is sufficient. Furthermore, we present results of numerical experiments with functions g of varying smoothness." | |
650 | 4 | |a Differential equations, Partial | |
700 | 1 | |a Bungartz, Hans-Joachim |d 1963- |e Sonstige |0 (DE-588)112889832 |4 oth | |
810 | 2 | |a A |t Sonderforschungsbereich Methoden und Werkzeuge für die Nutzung paralleler Rechnerarchitekturen: SFB-Bericht |v 1993,16 |w (DE-604)BV004627888 |9 1993,16 | |
830 | 0 | |a Technische Universität <München>: TUM-I |v 9336 |w (DE-604)BV006185376 |9 9336 | |
999 | |a oai:aleph.bib-bvb.de:BVB01-006478081 |
Datensatz im Suchindex
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author_GND | (DE-588)112889832 |
building | Verbundindex |
bvnumber | BV009791800 |
ctrlnum | (OCoLC)31897458 (DE-599)BVBBV009791800 |
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id | DE-604.BV009791800 |
illustrated | Illustrated |
indexdate | 2024-07-09T17:40:56Z |
institution | BVB |
language | English |
oai_aleph_id | oai:aleph.bib-bvb.de:BVB01-006478081 |
oclc_num | 31897458 |
open_access_boolean | |
owner | DE-12 DE-91G DE-BY-TUM |
owner_facet | DE-12 DE-91G DE-BY-TUM |
physical | 25 S. graph. Darst. |
publishDate | 1993 |
publishDateSearch | 1993 |
publishDateSort | 1993 |
record_format | marc |
series | Technische Universität <München>: TUM-I |
series2 | Technische Universität <München>: TUM-I Sonderforschungsbereich Methoden und Werkzeuge für die Nutzung paralleler Rechnerarchitekturen: SFB-Bericht / A |
spelling | Pointwise convergence of the combination technique for Laplace's equation Hans-Joachim Bongartz, ... München 1993 25 S. graph. Darst. txt rdacontent n rdamedia nc rdacarrier Technische Universität <München>: TUM-I 9336 Sonderforschungsbereich Methoden und Werkzeuge für die Nutzung paralleler Rechnerarchitekturen: SFB-Bericht / A 1993,16 Abstract: "For a simple model problem -- the Laplace equation on the unit square with a Dirichlet boundary function vanishing for x = 0, x = 1, and y = 1, and equaling some suitable g(x) for y = 0 -- we present a proof of convergence for the combination technique, a modern, efficient, and easily parallelizable sparse grid solver for elliptic partial differential equations that recently gained importance in fields of applications like computational fluid dynamics. For full square grids with meshwidth h and O(h⁻²) grid points, the order O(h²) of the discretization error using finite differences was shown in [12], if g(x) [member of] C²[0,1]. In this paper, we show that the finite difference discretization error of the solution produced by the combination technique on a sparse grid with only O((h⁻¹ log₂ (h⁻¹)) grid points is of the order O(h² log₂ (h⁻¹)), if the Fourier coefficients b[subscript k] of g̃, the 2-periodic and 0-symmetric extension of g, fulfill [formula] for some arbitrary small positive [epsilon]. If 0 <[epsilon] [<or =] 1, this is valid for g [member of] C⁴[0,1] and g(0) = g(1) = g''(0) = g''(1) = 0, e.g.. A simple transformation even shows that g [member of] C⁴[0,1] is sufficient. Furthermore, we present results of numerical experiments with functions g of varying smoothness." Differential equations, Partial Bungartz, Hans-Joachim 1963- Sonstige (DE-588)112889832 oth A Sonderforschungsbereich Methoden und Werkzeuge für die Nutzung paralleler Rechnerarchitekturen: SFB-Bericht 1993,16 (DE-604)BV004627888 1993,16 Technische Universität <München>: TUM-I 9336 (DE-604)BV006185376 9336 |
spellingShingle | Pointwise convergence of the combination technique for Laplace's equation Technische Universität <München>: TUM-I Differential equations, Partial |
title | Pointwise convergence of the combination technique for Laplace's equation |
title_auth | Pointwise convergence of the combination technique for Laplace's equation |
title_exact_search | Pointwise convergence of the combination technique for Laplace's equation |
title_full | Pointwise convergence of the combination technique for Laplace's equation Hans-Joachim Bongartz, ... |
title_fullStr | Pointwise convergence of the combination technique for Laplace's equation Hans-Joachim Bongartz, ... |
title_full_unstemmed | Pointwise convergence of the combination technique for Laplace's equation Hans-Joachim Bongartz, ... |
title_short | Pointwise convergence of the combination technique for Laplace's equation |
title_sort | pointwise convergence of the combination technique for laplace s equation |
topic | Differential equations, Partial |
topic_facet | Differential equations, Partial |
volume_link | (DE-604)BV004627888 (DE-604)BV006185376 |
work_keys_str_mv | AT bungartzhansjoachim pointwiseconvergenceofthecombinationtechniqueforlaplacesequation |