Cargando…
Introduction to the finite element method in electromagnetics
This series lecture is an introduction to the finite element method with applications in electromagnetics. The finite element method is a numerical method that is used to solve boundary-value problems characterized by a partial differential equation and a set of boundary conditions. The geometrical...
Autor principal: | |
---|---|
Lenguaje: | eng |
Publicado: |
Morgan & Claypool Publishers
2006
|
Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1607354 |
_version_ | 1780931719030898688 |
---|---|
author | Polycarpou, Anastasis |
author_facet | Polycarpou, Anastasis |
author_sort | Polycarpou, Anastasis |
collection | CERN |
description | This series lecture is an introduction to the finite element method with applications in electromagnetics. The finite element method is a numerical method that is used to solve boundary-value problems characterized by a partial differential equation and a set of boundary conditions. The geometrical domain of a boundary-value problem is discretized using sub-domain elements, called the finite elements, and the differential equation is applied to a single element after it is brought to a "weak" integro-differential form. A set of shape functions is used to represent the primary unknown variable |
id | cern-1607354 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
publisher | Morgan & Claypool Publishers |
record_format | invenio |
spelling | cern-16073542021-04-21T22:23:44Zhttp://cds.cern.ch/record/1607354engPolycarpou, AnastasisIntroduction to the finite element method in electromagneticsEngineeringThis series lecture is an introduction to the finite element method with applications in electromagnetics. The finite element method is a numerical method that is used to solve boundary-value problems characterized by a partial differential equation and a set of boundary conditions. The geometrical domain of a boundary-value problem is discretized using sub-domain elements, called the finite elements, and the differential equation is applied to a single element after it is brought to a "weak" integro-differential form. A set of shape functions is used to represent the primary unknown variable Morgan & Claypool Publishersoai:cds.cern.ch:16073542006 |
spellingShingle | Engineering Polycarpou, Anastasis Introduction to the finite element method in electromagnetics |
title | Introduction to the finite element method in electromagnetics |
title_full | Introduction to the finite element method in electromagnetics |
title_fullStr | Introduction to the finite element method in electromagnetics |
title_full_unstemmed | Introduction to the finite element method in electromagnetics |
title_short | Introduction to the finite element method in electromagnetics |
title_sort | introduction to the finite element method in electromagnetics |
topic | Engineering |
url | http://cds.cern.ch/record/1607354 |
work_keys_str_mv | AT polycarpouanastasis introductiontothefiniteelementmethodinelectromagnetics |